Chem.Soc.Rev.,2012,41,7938–Defect-related luminescent materials
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Efficient Photocyclization of Dithienylethene Dimer,Trimer, and Tetramer:Quantum Yield and Reaction DynamicsTeruaki Kaieda,†Seiya Kobatake,†Hiroshi Miyasaka,*,‡Masataka Murakami,‡Nobuyuki Iwai,§Yasushi Nagata,§Akira Itaya,§and Masahiro Irie*,†Contribution from the Department of Chemistry and Biochemistry,Graduate School ofEngineering,Kyushu Uni V ersity,and CREST,Japan Science and Technology Corporation,Higashi-ku,Fukuoka812-8581,Japan,Department of Chemistry,Graduate School of Engineering Science,Osaka Uni V ersity,Toyonaka,Osaka560-8531,Japan,and Department of Polymer Science and Engineering,Kyoto Institute of Technology,Matsugasaki,Sakyo,Kyoto606-8585,JapanReceived June27,2001.Revised Manuscript Received October22,2001Abstract:Multi-dithienylethene arrays,in which two,three,or four1,2-bis(2,4-dimethylthiophen-3-yl)-perfluorocyclopentenes are ethynylene-bridged,were synthesized.Upon irradiation with ultraviolet light the hexane solutions of the arrays turned violet-blue and the color disappeared by irradiation with visible light.The quantum yields of photocyclization reactions successively increased from0.21to0.40by increasing the number of the dithienylethene moieties in the arrays from one to four.Picosecond laser photolysis as well as the fluorescence depolarization experiment confirmed that efficient excited energy migration in the arrays from the photochemically inactive parallel conformer to the photoactive antiparallel conformer resulted in the high quantum yields.IntroductionConsiderable attention has been paid to photochromic dyes which show reversible photoisomerizations upon irradiation with light of appropriate wavelengths because of their potential applicability to optoelectronic devices.1In general,photoge-nerated colored isomers of photochromic dyes are thermally unstable and return to the initial colorless isomers in the dark. Recently,several thermally irreversible photochromic com-pounds,such as furylfulgides,2diarylethenes,3and phenoxy-naphthacenequinones,4have been developed.The photogener-ated colored isomers are stable and never return back to the initial colorless isomers in the dark.Among the compounds, diarylethenes with heterocyclic aryl rings are the most promising for the optoelectronic devices,5-8such as optical memory,photooptical switching,display,and photodriven actuators, because of their fatigue-resistant property.6,7For practical applications it is required to further improve the performance of the photochromic diarylethenes,such as efficient photore-activity(high cyclization quantum yields),high absorption coefficients of the colored isomers,rapid response,and reactivity in the solid state.In the present study,we have prepared sensitive multi-dithienylethene arrays with high cyclization quantum yields.The open-ring isomers of dithienylethenes in solution have two conformations,antiparallel and parallel,in almost equal amounts,as shown in Scheme1.9,10The interconversion rate between the two conformations is much slower than the lifetime of photoexcited states.9Therefore,both conformers are photo-excited independently.Among the two conformers,only the antiparallel conformer has a chance to be converted to the closed-ring isomer.11Therefore,the maximum cyclization quantum yield cannot exceed0.5.12There are two strategies to increase the cyclization quantum yield in solution.One is to increase the ratio of the antiparallel conformers in the ground state.When a sodium sulfonate derivative of bis(2-methyl-1-benzothiophen-3-yl)perfluorocy-clopentene was included in the -cyclodextrin cavity,the molecule was force to adopt an antiparallel conformation.The†Kyushu University.‡Osaka University.§Kyoto Institute of Technology.(1)(a)Du¨rr,H.;Bouas-Laurent,H.Photochromism,Molecules and Systems;Elsevier:Amsterdam,1990.(b)McArdle,C.B.Applied Photochromic Polymer Systems;Blankie:Glasgow,1992.(c)Crano,J.C.;Guglielmetti, anic Photochromic and Thermochromic Compounds;Plenum Press:New York,1999.(2)(a)Heller,H.G.;Oliver,S.J.Chem.Soc.,Perkin Trans.11981,197.(b)Darcy,P.J.;Heller,H.G.;Strydom,P.J.;Whittall,J.J.Chem.Soc.,Perkin Trans.11981,202.(3)(a)Irie,M.;Mohri,.Chem.1988,53,803.(b)Hanazawa,M.;Sumiya,R.;Horikawa,Y.;Irie,M.J.Chem.Soc.,mun.1992, 206.(4)Buchholtz,F.;Zelichenok,A.;Krongauz,V.Macromolecules1993,26,906(5)Irie,M.Photoreacti V e Materials for Ultrahigh-Density Optical Memory;Elsevier:Amsterdam,1994.(6)Irie,M.;Uchida,K.Bull.Chem.Soc.Jpn.1998,71,985.(7)Irie,M.Chem.Re V.2000,100,1685.(8)Irie,M.;Kobatake,S.;Horichi,M.Science2001,291,1769.(9)Uchida,K.;Nakayama,Y.;Irie,M.Bull.Chem.Soc.Jpn.1990,63,1311.(10)Irie,M.;Miyatake,O.;Uchida,K.;Eriguchi,T.J.Am.Chem.Soc.1994,116,9894.(11)Nakamura,S.;Irie,.Chem.1988,53,6136.(12)Irie,M.;Sakemura,K.;Okinaka,M.;Uchida,.Chem.199560,8305.Published on Web02/09/200210.1021/ja0115722CCC:$22.00©2002American Chemical Society J.AM.CHEM.SOC.9VOL.124,NO.9,20022015cyclization quantum yield was found to increase from 0.32to 0.49.13Zerbi et al.14also ascribed the high cyclization quantum yield of a polymer having dithienylethenes in the main chain to the enforced antiparallel conformation of the dithienylethene moieties in the ground state.The other strategy is to increase the ratio of antiparallel conformers in the photoexcited state.When photoexcited energy can be transferred from the photo-chemically inactive parallel conformation unit to the photoactive antiparallel one,the quantum yield is expected to increase.Such energy transfer is probable in dithienylethene dimer,trimer,or tetramer,in which the dithienylethene moieties are ethynylene-bridged.15-18Recently,Branda et al .19reported limited photo-chromic reactivity of dithienylethene dimers,in which two dithienylethene moieties are connected by a single bond.When N dithienylperfluorocyclopentene moieties are con-nected with conjugated bonds,the system has 2N conformations by a combination of parallel and antiparallel conformations.Among the 2N conformations,only one conformation,in which all dithienylethene moieties are in the parallel conformation,cannot cyclize to the closed-ring isomer by photoirradiation,while (2N -1)other conformations can undergo the photocy-clization reaction by transferring the photoexcited energy to the antiparallel conformation unit.Figure 1lists all conformations of the monomer,dimer,trimer,and tetramer systems.From the list it is inferred that the ratio of photoactive systems increases from 0.5to 0.94by increasing the number of dithienylethene moieties in the arrays from one to four,resulting in high quantum yields.In this work,the dimer,trimer,and tetramer in Scheme 2were synthesized and the quantum yields and the mechanism of the cyclization reactions were studied by irradia-tion with continuous as well as picosecond laser pulse light.Results and DiscussionPhotochromism of Dimer in Hexane.Figure 2shows the absorption spectral change of the dimer in hexane by photoir-radiation.Upon irradiation with 320nm light,the colorless solution of the open-ring form dimer with the absorptionmaximum at 320nm ( ,2.3×104M -1cm -1)turned violet,in which characteristic absorption maxima were observed at 365and 584nm.The violet color indicates formation of the closed-ring isomer.6Upon visible (λ>540nm)light irradiation,the violet color disappeared indicating return to the initial open-ring isomer.The coloration/decoloration cycle could be repeated more than 10times and a clear isosbestic point was observed at 338nm even after 10cycles.The photoirradiated sample was analyzed with high perfor-mance liquid chromatography (HPLC,silica gel column,Wa-kosil 5SIL,eluent hexane/ethyl acetate (96:4)).When monitored at the isosbestic point of 338nm,two peaks were observed.When the monitoring wavelength was shifted to 584nm,at which wavelength only the closed-ring form absorbs,only one peak was observed in the HPLC chart.This indicates that only one closed-ring isomer was produced by UV irradiation.Even after prolonged irradiation any other photoproduct was not(13)(a)Takeshita,M.;Choi,C.N.;Irie,mun.1997,2265.(b)Takeshita,M.;Kato,N.;Kawauchi,S.;Imase,T.;Watanabe,J.;Irie,.Chem.1998,63,9306.(14)Stellacci,F.;Bertarelli,C.;Toscano,F.;Gallazzi,M.C.;Zolti,G.;Zerbi,G.Ad V .Mater.1999,11,292.(15)Hsiao,J.-S.;Krueger,B.P.;Wagner,R.W.;Johnson,T.E.;Delaney,J.K.;Mauzerall,D.C.;Fleming,G.R.;Lindsey,J.S.;Bocian,D.F.;Donohoe,R.J.J.Am.Chem.Soc.1996,118,11181.(16)Yang,S.I.;Lammi,R.K.;Seth,J.;Riggs,J.A.;Arai,T.;Kim,D.;Bocian,D.F.;Holten,D.;Lindsey,J.S.J.Phys.Chem.B 1998,102,9426.(17)Li,J.;Ambroise A.;Yang,S.R.;Diers,J.R.;Seth,J.;Wack,C.R.;Bocian,D.F.;Holten,D.;Lindsey,J.S.J.Am.Chem.Soc.1999,121,8927.(18)Lammi,R.K.;Ambroise A.;Balasubramanian,T.;Wagner,R.W.;Bocian,D.F.;Holten,D.;Lindsey,J.S.J.Am.Chem.Soc.2000,122,7579.(19)Peters,A.;Branda,N.R.Ad V .Mater.Opt.Electron.2000,10,245.Scheme 1.Photochromism ofDithienyletheneFigure 1.Conformations of monomer,dimer,trimer,and tetramermolecules.Figure 2.Absorption spectral change of the dimer in hexane upon irradiation with 320nm light:(s )before photoirradiation and (---)after UV-light irradiation for 11min.The fluorescence spectrum of the (O -O)dimer in hexane was also shown (---).Scheme 2.Structure of Monomer,Dimer,Trimer,andTetramerA R T I C L E SKaieda et al.2016J.AM.CHEM.SOC.9VOL.124,NO.9,2002detected.The absence of the isomer having two closed-ring forms in the photoirradiated dimer agrees to the result observed in the dimers reported by Branda et al .19The colored isomer was collected and the structure was analyzed by 1H NMR spectroscopy.The methyl protons of the colored dimer showed seven signals,as shown in Figure 3a.In the NMR spectrum there existed a characteristic signal at 2.00ppm assigned to the methyl protons of the closed-ring form and a characteristic signal at 2.04ppm assigned to the methyl protons of the open-ring form.20The ratio of the two signals was 1:1,which means that the colored isomer is an (O -C)dimer having an open-ring form (O)and a closed-ring form (C).The isomer in which both dithienylethenes are in the closed-ring form (C -C)was not detected.To search for the reason the isomer having two closed-ring forms (C -C)was not produced,fluorescence spectra of the initial open-ring form (O -O)dimer and the photogenerated (O -C)dimer were measured in hexane.When excited at 320nm,the (O -O)dimer gave fluorescence at 440nm,while the (O -C)dimer did not give fluorescence.As can be seen from Figure 2,there is an overlap of the fluorescence of the (O -O)dimer and the absorption of the (O -C)dimer.The overlap suggests that the intramolecular energy transfer is possible from the excited open-ring unit to the closed-ring unit.In other words,when the (O -C)dimer is excited with UV light,the excited energy of the open-ring form unit is efficiently transferred to the closed-ring form unit in the same molecule,as shown inScheme 3.Therefore,the cyclization reaction of the remaining open-ring form unit cannot take place.The efficient intramo-lecular energy transfer process will be discussed in detail in later sections,using the fluorescence depolarization experiment and picosecond laser photolysis.Photochromism of Trimer in Hexane.Figure 4shows the absorption spectral change of the trimer by UV irradiation in hexane.Upon irradiation with 320nm light,the colorless solution of all open-ring form (O -O -O)trimer with the absorption maximum at 325nm ( ,4.6×104M -1cm -1)turned blue,in which characteristic absorption maxima were observed at 365and 620nm.Upon visible (λ>540nm)light irradiation,the blue color disappeared.The HPLC chromatogram (monitoring wavelength 342nm)of the solution after UV irradiation is shown in Figure 5.Four peaks were observed.When the monitoring wavelength was changed to 600nm where the open-ring form unit has no absorption,three peaks except the second peak were observed,indicating that there existed three kinds of closed-ring form isomers.The four peaks were isolated and their structures were determined by UV -vis absorption spectral measurement and 1H NMR spectroscopy.The first peak trimer had the absorption maximum at 635nm ( ,2.4×104M -1cm -1).The third and fourth peak trimers had the maxima at 584nm.These colored isomers converted(20)In the NMR spectrum of the monomer,the methyl signals of the open-ring isomer were observed at 2.04and 2.29ppm,while they shifted to 2.00and 2.14ppm in the closed-ringisomer.Figure 3.1H NMR methyl signals of the (O -C)dimer (a)and the (O -C -O)trimer(b).Figure 4.Absorption spectral change of the trimer in hexane upon irradiation with 320nm light:(s )before photoirradiation and (---)after UV-light irradiation for 11min.Figure 5.HPLC chromatogram of the trimer irradiated with 320nm for 11min in hexane.A UV detector was used for monitoring at 342nm.The column was silica gel (Wakosil 5SIL)and the eluent was hexane/ethyl acetate (98:2).Scheme 3.Intramolecular Energy Transfer in the ExcitedStatePhotocyclization of Dithienylethene Di-,Tri-,and Tetramers A R T I C L E SJ.AM.CHEM.SOC.9VOL.124,NO.9,20022017to the open-ring form trimer by irradiation with visible light (λ>540nm).The absorption maxima suggest that the first peak trimer has the closed-ring form in the middle,while the third and fourth peak trimers have the closed-ring form unit(s)at the end,because the absorption maximum of 584nm was the same as the maximum of the (O -C)dimer.The structures were further examined by 1H NMR measurement.The methyl protons of the second peak trimer were observed at 2.04,2.11,and 2.29ppm,which are assigned to an all open-ring form (O -O -O)trimer.The methyl protons of the first peak trimer showed five signals,as shown in Figure 3b.In the NMR spectrum there was no characteristic signal at 2.00ppm,which is assigned to the methyl protons of the terminal closed-ring form.This result indicates that the product does not contain the terminal closed-ring form.Thus,the first peak is the (O -C -O)trimer having one closed-ring form unit at the middle.The methyl protons of the third peak trimer showed six peaks.In the NMR spectrum there existed a characteristic signal at 2.00ppm assigned to the terminal closed-ring form and a characteristic signal at 2.04ppm assigned to the terminal open-ring form.The ratio of the two signals was 1:1,which means the colored isomer is the (O -O -C)trimer having one closed-ring form at the one end.The absorption coefficient of the fourth peak trimer (584nm; ,2.9×104M -1cm -1)was twice as large as that of the third peak trimer (584nm; ,1.4×104M -1cm -1),which is the same as that of the (O -C)dimer.This indicates that the peak is due to the (C -O -C)trimer having two closed-ring form units at both ends.The fourth peak is not due to the (O -C -C)trimer,because the absorption maxima was observed at 584nm (assigned to the terminal closed-ring form),not at 635nm (assigned to the middle closed-ring form),and the characteristic signal at 2.04ppm assigned to the terminal open-ring form was not observed.Any isomer in which neighboring two dithienylethene units are converted to the closed-ring forms was not detected.The time-course of formation of the three isomers (O -C -O,O -O -C,C -O -C)was measured by HPLC,as shown in Figure 6.Upon UV-light irradiation,the amount of all open-ring form (O -O -O)trimer decreased.At the same time the amount of two trimers,O -C -O and C -O -O,having closed-ring form units increased.After 11min of photoirradiation,the ratio of (C -O -C),(O -C -O),and (O -O -C)isomers was 3:54:39.The amount of (C -O -C)trimer having two closed-ring form units at both ends increased gradually.The rate for formation of the (O -C -O)trimer having one closed-ring formunit in the middle was faster than that of the (O -O -C)trimer having one closed-ring form unit at the end.Photochromism of Tetramer in Hexane.The absorption spectral change of the tetramer in hexane is shown in Figure 7.Upon irradiation with 320nm light,the colorless solution of the open-ring form tetramer with the absorption maximum at 325nm ( ,6.9×104M -1cm -1)turned greenish-blue,in which characteristic absorption maxima were observed at 354and 625nm.Upon visible (λ>540nm)light irradiation,the greenish-blue color disappeared.Figure 8shows the HPLC chromatogram (monitoring wave-length 346nm)of the solution after UV irradiation.Five peaks were observed.When the monitoring wavelength was changed to 600nm,where the open-ring form has no absorption,four peaks except the third peak were observed.These four peaks were ascribed to the closed-ring form isomers.The first peak tetramer had the absorption maximum at 635nm,while the maximum shifted to 620nm in the second peak tetramer.The fourth and fifth peaks had the absorption maximum at 584nm.These colored compounds converted to the open-ring form isomer by irradiation with visible light (λ>540nm).These colored and colorless isomers were isolated and their structures were determined by 1H NMR and absorption spectroscopy.The methyl protons of the third peak tetramer were observed at 2.04,2.11,and 2.29ppm,which are identical to those of the open-ring form isomer.The methyl protons of the first peak tetramer showed six signals,in which there was no characteristic signal at 2.00ppm.This indicates that the first peak is due to the tetramer having no closed-ring form unit at the end and having one inner closed-ring form unit.The methyl protonsofFigure 6.The change in the content of the isomers of the trimer upon irradiation with 320nm:the (O -O -O)trimer (O ),the (O -C -O)trimer (0),the (O -O -C)trimer ()),and the (C -O -C)trimer (×).Figure 7.Absorption spectral change of the tetramer in hexane upon irradiation with 320nm light:(s )before photoirradiation and (---)after UV-light irradiation for 8min.Figure 8.HPLC chromatogram of the tetramer irradiated with 320nm in hexane.A UV detector was used for monitoring at 346nm.The column was silica gel (Wakosil 5SIL)and the eluent was hexane/ethyl acetate (96:4).A R T I C L E S Kaieda et al.2018J.AM.CHEM.SOC.9VOL.124,NO.9,2002the second peak tetramer showed six peaks.In the spectrum there existed characteristic signals at 2.00and 2.04ppm assigned to the terminal closed-ring and open-ring forms,respectively.The peak intensity of a characteristic signal at 2.17ppm,which is assigned to the methyl protons at the quantarnary carbons in the closed-ring form units,indicates that two closed-ring form units are included in the molecule.This means that the colored isomer is the (O -C -O -C)tetramer having one terminal closed-ring form unit and one inner closed-ring form unit.This peak is not due to the (O -O -C -C)tetramer,because the signal at 2.33ppm was 3times larger than the signal at 2.29ppm.The fourth and fifth peaks had the same absorption maximum at 584nm.The absorption coefficient of the fifth peak ( ,2.8×104M -1cm -1)was twice as large as that of the fourth peak ( ,1.4×104M -1cm -1)at 584nm,indicating that the fourth peak is due to the (O -O -O -C)tetramer having one closed-ring form at the end.The fifth peak is the (C -O -O -C)tetramer having two closed-ring form units at both ends.Even in the tetramer any isomer,in which both neighboring dithienylethene units are converted to the closed-ring form,was not detected.The time-course of formation of the four isomers,(O -C -O -O),(O -O -O -C),(O -C -O -C),and (C -O -O -C),was measured by HPLC,as shown in Figure 9.Upon UV irradiation,the amount of all open-ring tetramer immediately decreased and at the same time the amount of two closed-ring isomers,(O -C -O -O)and (O -O -O -C),increased.The amount of the (C -O -O -C)tetramer having two closed-ring form units at both ends and the (O -C -O -C)tetramer having both inner and terminal closed-ring form units increased gradually.The rate of formation of the (O -C -O -O)tetramer having an inner closed-ring form unit was faster than that of the (O -O -O -C)tetramer having a terminal closed-ring form unit.Quantum Yields of Dimer,Trimer,and Tetramer.The cyclization quantum yields of dimer,trimer,and tetramer were measured at room temperature.The quantum yield measurement was carried out as follows.The dimer and the trimer were dissolved in hexane and the solutions were irradiated with ultraviolet light (λ)340nm).Cyclohexane was used as the solvent for the tetramer because of its low solubility in hexane.A 500W xenon lamp was used as the light source and the irradiation wavelength (λ)340nm)was isolated by passing the light through a monochromator.In the case of the monomer and the dimer the rate of cyclization reaction was followed by measuring the absorption increase at 534nm ( ,5.0×103M -1cm -1)21and 584nm ( ,1.4×104M -1cm -1),respectively.Inthe case of the trimer and the tetramer the irradiated hexane or cyclohexane solutions were passed through HPLC and the ratio change of each product upon irradiation was analyzed by setting the monitoring wavelength to the quasi-isosbestic point.The absorption increase at 584and 635nm was also followed to confirm the accuracy of the quantum yield determination.The light intensity was monitored by a photometer,which was cali-brated by the photoreaction of furylfulgide in hexane solution.The quantum yield measurement was carried out three times for each multi-dithienylethene arrays and the average values were adopted as the quantum yields.The error of the relative quantum yields among the oligomers was less than (5%,while the error of absolute values was on the order of (10%.The quantum yield of the open-ring form (O -O)dimer to the (O -C)dimer was determined to be 0.31.The yields of the trimer from the all open-ring form (O -O -O)isomer to the (O -C -O)isomer having one closed-ring form unit at the middle and the (O -O -C)isomer having one closed-ring form unit at the end were 0.20and 0.16,respectively.The total cyclization yield of the trimer was 0.36.The cyclization quantum yields of the tetramer from the all open-ring form (O -O -O -O)isomer to the (O -C -O -O)isomer having one inner closed-ring form unit and the (O -O -O -C)isomer having one terminal closed-ring form unit were determined to be 0.30and 0.10,respectively.The total cyclization quantum yield was 0.40.The photocyclization quantum yields increased by increasing the number of dithienylethene moieties in the arrays.The increase in the quantum yields is attributed to the intramolecular energy migration from the photochemically inactive parallel conforma-tion unit to the photoactive one,as described in the introductory section.Fluorescence Depolarization.To confirm the intramolecular energy migration in the arrays,depolarization of fluorescence was measured in a 2-methyltetrahydrofuran rigid glass at 77K.An excitation wavelength of 320nm was selected.Dithie-nylethenes undergo photochromic reactions even in the solid state at low temperature.22Fluorescence spectra of the dimer,the trimer and the tetramer gave a similar emission at 440nm,while the emission of the monomer was observed at 420nm.The fluorescence polarization values (p )(I ||-I ⊥)/(I ||+I ⊥))were determined to be 0.51(monomer),0.23(dimer),0.17(trimer),and 0.14(tetramer),respectively.For the monomer,the polarization of the fluorescence directly correlates with the direction of the polarized excitation light.In the case of the multi-dithienylethene arrays,depolarization took place.The p values decreased by increasing the number of the dithienylethene moieties in the arrays.This result clearly indicates that the excited energy migrates in the arrays.23Reaction Dynamics.To reveal the dynamics of the excited energy migration,a laser photolysis experiment was carried out with use of a picosecond laser pulse.Figure 10a shows the time-resolved transient absorption spectra of the dimer in a hexane solution excited with a picosecond 355nm laser pulse.A broad absorption spectrum with maxima around 490and 750nm appeared within the time resolution of the apparatus,followed(21)Uchida,K.;Irie,M.Chem.Lett.1995,969.(22)(a)Kobatake,S.;Yamada,T.;Uchida,K.;Kato,N.;Irie,M.J.Am.Chem.Soc.1999,121,2380.(b)Irie,M.;Lifka,T.;Kobatake,S.;Kato,N.J.Am.Chem.Soc.2000,122,4871.(23)(a)David,C.;Baeyens-Volant,D.;Geuskens,G.Eur.Polym.J.1976,12,71.(b)David,C.;Putman-de Lavareille,N.;Geuskens,G.Eur.Polym.J.1977,13,15.Figure 9.The change in the content of the isomers of the tetramer upon irradiation with 320nm:the (O -O -O -O)tetramer (O ),the (O -O -C -O)tetramer (0),the (O -O -O -C)tetramer ()),the (O -C -O -C)tetramer (×),and the (C -O -O -C)tetramer (4).Photocyclization of Dithienylethene Di-,Tri-,and Tetramers A R T I C L E SJ.AM.CHEM.SOC.9VOL.124,NO.9,20022019by the growth of sharp absorption maximum at 465nm in the time region of a few hundred picoseconds and the apparent decrease in absorption intensity in the wavelength region >650nm.No spectral change was observed in subnanoseconds to nanoseconds time region.Figure 10b shows the time profile of the transient absorption band at 780nm.The solid line in Figure 10b shows the results calculated on the basis of the double-exponential function as eq 1,where τ1and τ2are 35and 100ps,and A 1,A 2,and A 3are 46,46,and 8%,respectively.The pulse widths of the excitation and the monitoring pulses were convoluted in the curve.Since the broad spectrum appeared within the time resolution of the apparatus and the time constant of the fluorescence decay was obtained to be ca.100ps,24it is concluded that the broad absorption observed immediately after the excitation is due to the S 1state.To explore the spectral evolution in the early stage after the excitation,the difference spectrum between that at 100ps and that at 0ps was plotted in Figure 10c.Both of the spectra used for the calculation were normalized at 750nm.A sharp absorption peak at 465nm and a broad absorption band at 580nm were obtained as the difference.Since the former sharp absorption at 465nm did not decrease in the time window examined here (6ns),this band is ascribed to a long-living species such as a triplet state.On the other hand,the absorption band at 580nm is ascribed to the (O -C)dimer.On the basis of the above results,the spectral evolution around 580nm is attributable to the formation of the closed-ring form.To quantitatively elucidate the formation process of the closed-ring form,the time profiles of various wavelength points were analyzed.However,all the time profiles except for the wavelength region around 465nm showed only the decay behaviors,indicating that the broad absorption due to the S 1state has rather large extinction coefficients in the entire wavelength region >650nm.The absorption signals in the longer wavelength region are mainly due to the S 1state.Accordingly,we subtracted the contribution of this S 1spectrum (the spectrum at 0ps)from each of the spectra observed at various delay times after the excitation by adjusting the intensity of the spectrum at 750nm to those at various delay times.The transient spectra thus obtained are shown Figure 11a.The absorption spectra with maxima at 465and 580nm increase with an increase in the delay time after the excitation.The time profile of the transient absorbance at 580nm due to the closed-ring form (O -C)is exhibited in Figure 11b.The solid line in this figure shows the result calculated on the basis of the double-exponential rise function (eq 2).The initial instaneous rise was eliminated for the calculation,where τf and τs are (35(5)and (100(10)ps,respectively.The relative preexponential factors,A f and A s ,are 47and 53%.These time constants were in agreement with those for the decay of the S 1state monitored at 780nm (Figure 10b).Similar biphasic rise behavior was also observed for the transient absorbance at 465nm.To precisely elucidate the production pathways of the closed-ring form,the difference spectra between those at several delay times were plotted.Figure 12exhibits the difference spectra between those at 500ps and 120ps and between those at 120ps and 20ps.As is clearly shown in these spectra,the latter spectrum actually shows the formation of the closed-ring form(24)Single photon counting with a subnanosecond light pulse was used for thefluorescence measurement.Since the time resolution is not so sufficient to precisely determine the biphasic decay behaviors,single-exponential decay was assumed for the fluorescencedecay.Figure 10.(a)Time-resolved transient absorption spectra of the open-ring form (O -O)dimer in hexane,excited with a picosecond 355nm laser pulse.(b)Time profile of transient absorbance at 780nm.This solid line is the result calculated on the basis of the double-exponential function (see text).(c)Difference spectrum between that at 100ps and that at 0ps for the time-resolved transient absorption spectra of the open-ring form (O -O)dimer in hexane,excited with a picosecond 355nm laser pulse.A 780(t ))A 1exp(-t /τ1)+A 2exp(-t /τ2)+A 3(1)A (t ))A -{A f exp(-t /τf )+A s exp(-t /τs )}(2)A R T I C L E S Kaieda et al.2020J.AM.CHEM.SOC.9VOL.124,NO.9,2002。
盐酸左旋咪唑稀土化合物的制备及其对三元乙丙橡胶胶料性能的影响吴启浩,岑 兰*,黄 坤(广东工业大学材料与能源学院,广东广州 510006)摘要:采用稀土氧化钇与盐酸左旋咪唑制备盐酸左旋咪唑稀土化合物(LHLC),考察LHLC对三元乙丙橡胶(EPDM)/炭黑胶料的硫化特性和物理性能的影响。
红外光谱分析结果表明,盐酸左旋咪唑与稀土元素发生了配位反应。
试验结果表明:LHLC对胶料的硫化促进效率与促进剂M相当;LHLC用量增大,胶料的表观交联密度和M H增大,t90缩短;促进剂TRA/促进剂BZ/LHLC硫黄硫化体系有利于提高胶料的物理性能,随着LHLC用量的增大,硫化胶的拉伸强度、撕裂强度、硬度、100%定伸应力都有所增大,拉断伸长率呈下降趋势;LHLC对硫化胶的喷霜和耐热氧老化性能影响不大;LHLC 用量超过0.8份后,胶料的阿克隆磨耗量减小,随着LHLC用量的增大,硫化胶的耐磨性能变好。
关键词:稀土;盐酸左旋咪唑;硫化促进剂;三元乙丙橡胶中图分类号:TQ333.4;TQ330.38+5 文献标志码:A 文章编号:1000-890X(2017)06-0340-04盐酸左旋咪唑(Levamisole Hydrochloride,简称LH)是一种普通医疗用药,分子结构中含有—N=C—S—基团,类似于橡胶硫化促进剂的基团,倘若能够用作硫化促进剂,在硫化过程中不会释放出亚硝胺,属于安全胺的范畴;本课题组前期研究表明,LH能够促进SBR的硫化,但直接使用时促进效果不理想。
另一方面,稀土元素具有独特的4f电子层结构及较大的原子转矩和较强的自旋耦合等特性,因此具有独特的物理化学性质,稀土元素倾向于与硬碱原子生成配合物,如稀土元素能够与橡胶硫化促进剂配合,提高其硫化促进性能[1-2]。
三元乙丙橡胶(EPDM)主链饱和而侧链含有少量的不饱和键,采用硫黄体系硫化时,其硫化反应活性较低,且硫黄和极性促进剂在胶料中的分散性不好,胶料容易喷霜。
Vol.412020年12月No.122766~2773CHEMICAL JOURNAL OF CHINESE UNIVERSITIES高等学校化学学报胺基膦钌卡宾化合物的合成及催化烯烃复分解反应王晋宇,柳春丽,陈延辉(天津科技大学化工与材料学院,天津卤水化工与资源生态化利用重点实验室,天津300457)摘要合成并表征了一类含新型胺基膦配体的Grubbs 二代型钌卡宾烯烃复分解催化剂[RuCl 2(H 2IMes)·(R 1HNPR 22)(=CHPh)],采用核磁共振波谱和单晶X 射线衍射确定了催化剂的结构.在室温条件下,以N,N -二烯丙基-对甲苯磺酰胺的关环复分解反应(RCM)为模型,考察了不同胺基膦配体对钌卡宾催化反应速率的影响.结果表明,G 2⁃1表现出最佳的催化活性.通过底物研究发现,G 2⁃1催化剂(摩尔分数,1%)对双端烯及多端烯的RCM 反应具有较好的活性和官能团适应性,产物收率均>95%;G 2⁃1催化剂同样适用于同(异)端烯底物的交叉复分解反应(CM),其催化苯乙烯与3-苯氧基丙烯的CM 反应时产物收率高达92%.关键词胺基膦配体;钌卡宾配合物;关环复分解;交叉复分解中图分类号O621.2文献标志码A烯烃复分解反应是指烯烃的碳碳双键在金属化合物的作用下被切断并重组为新分子结构的一类反应,是一种简单、快速、绿色且高效构建复杂分子的有效手段[1~10].目前,含有钼、钨和钌金属的催化剂已被广泛用于生物医药和有机合成等领域[11~13].与钼和钨催化剂相比,钌基催化剂对官能团兼容性好,对水和氧不敏感,因而备受关注[14].1996年,具有代表性和开创性的钌催化剂—二(三环己基膦)亚苄基二氯化钌被发现,该催化剂对空气稳定、催化活性高,为钌催化剂的发展奠定了基础,被称为Grubbs 一代催化剂(G 1,结构见图1)[15].G 1催化剂存在寿命短的缺点,在催化一些难以关环底物的反应时收率较低.1999年,Grubbs 等[16]利用空间位阻较大的N -杂环卡宾(NHC )取代G 1中的一个三环己基膦,开发出Grubbs 二代催化剂(G 2,结构见图1).与G 1催化剂相比,G 2催化剂的活性提升了2个数量级,显著降低了反应中催化剂的使用量,为工业化的大规模应用提供了可能性[17~19].随后,G 2催化剂的一个膦配体被双吡啶取代,发展成为Grubbs 三代催化剂(G 3,结构见图1)[20].G 3催化剂能够快速引发反应,且具有良好的官能团适应性.另外,G 3催化剂还可通过开环交叉聚合反应(ROMP )制备分子量可控和低分散的聚合物[21~24].纵观G 1~G 3钌基催化剂的发展历程,辅助配体的使用与调变起着关键作用,这为钌催化剂的进一步优化和发展指明了方向.基于卡宾钌G 2催化剂,已有大量研究集中于卡宾配体和膦配体的修饰和调变,以求提高催化剂的性能.2018年,Grubbs 等[25]首次将膦胺配体引入G 2钌基催化剂体系,开发出Fig.1Grubbs ruthenium olefin metathesis catalystsdoi :10.7503/cjcu20200420收稿日期:2020-07-02.网络出版日期:2020-10-07.基金项目:国家自然科学基金(批准号:21371131)资助.联系人简介:陈延辉,男,博士,教授,主要从事金属有机均相催化应用研究.E -mail:************.cnNo.12王晋宇等:胺基膦钌卡宾化合物的合成及催化烯烃复分解反应具有膦胺配体的Grubbs 二代钌烯烃复分解催化剂(Scheme 1),并系统地研究了膦胺配体对其催化性能的影响.研究发现,P —N 键插入膦配体骨架能有效加速G 2催化剂的引发,提高初始反应速率.这种速率的提高可能与膦胺配体(相对于三环己基膦配体)更易于从钌金属中心解离有关[26,27].这一过程促使G 2催化剂转变为一个14电子的活性钌中间体,进而引发烯烃复分解反应.由此可见,在G 2催化剂体系中,辅助膦配体的解离速率直接决定反应的初始速率和催化剂活性.理论上,通过调变G 2催化剂膦配体中取代基的电子效应和空间效应,即可有效降低膦配体和钌中心的结合力,促使配体从金属中心解离.胺基膦是一种重要的有机膦配体,具有独特的P —N 双齿配位特性,已经被广泛应用于各种金属有机化合物的合成和应用研究中.双烷基取代膦胺配体已经被应用于G 2钌基催化剂体系,迄今胺基膦在钌基烯烃复分解催化剂领域的应用尚未见报道.与双烷基取代的膦胺配体相比,胺基膦具有更低的磷上电子云密度,可使配体更易于从钌金属中心解离,利于提高催化剂的活性.本文从Grubbs 第三代催化剂出发,设计合成了一系列含胺基膦配位的钌卡宾化合物G 2-1~G 2-6(Scheme 1),通过调变取代基效应研究了催化剂的烯烃复分解反应特性.目标化合物的结构经核磁共振波谱和单晶X 射线衍射表征.利用模型反应,比较了合成的系列催化剂的性能,发现G 2⁃1表现出最佳的催化活性,并且优于同等反应条件下的商用催化剂G 2和G 3.另外,从底物取代基的电子效应、杂原子效应和空间效应等几个方面,系统评价了G 2⁃1催化剂对关环复分解反应(RCM )和交叉复分解反应(CM )的催化性能.1实验部分1.1试剂与仪器环己胺、正丙胺、异丙胺、叔丁胺、二苯基氯化膦、二异丙基氯化膦和二环己基氯化膦均为分析纯,购于百灵威科技有限公司;正己烷、甲苯和四氢呋喃均为分析纯,购于天津江天化工有限公司.所用溶剂均在氮气气氛下经Na 或CaH 2干燥.参照文献[28]方法合成胺基膦配体,并采用核磁共振波谱进行表征.德利斯手套箱(成都德利斯实业有限公司);Agilent 7890A 型气相色谱仪(GC ,美国Agilent 公司,HP -5色谱柱);AV Ⅲ400MB 型核磁共振波谱仪(NMR ,德国Bruker 公司),TMS 为内标,1H NMR 频率为400MHz ,31P NMR 频率为162MHz ;Brucker SMART APEX Ⅱ型单晶X 射线衍射仪(XRD ,德国Bruker 公司),采用单色化的Mo Kα辐射源(λ=0.071073nm ),在低温(113.15K )下收集衍射数据.1.2实验过程胺基膦钌卡宾化合物的合成路线如Scheme 2所示.Scheme 1Structures of aminophosphine rutheniumcomplexesScheme 2Synthesis of aminophosphine ruthenium complexes2767Vol.41高等学校化学学报在氮气气氛下,将2.90g (4.00mmol )钌卡宾配合物G 3加入到含有15mL 甲苯的圆底烧瓶中,再缓慢滴加1.11g (4.00mmol )N -叔丁基-1,1-二环己基膦胺的甲苯溶液(5mL ),搅拌10min ;反应结束后,抽干溶剂甲苯,固体用正己烷洗涤,经过滤、干燥,得到化合物G 2⁃1(2.75g ,3.28mmol ),收率为81%.参照化合物G 2⁃1的合成方法制备钌卡宾化合物G 2⁃2~G 2⁃6,收率在72%~77%之间.化合物G 2⁃1~G 2⁃6的1H NMR 和31P NMR 数据见表1.图2示出了化合物G 2⁃3晶体的分子结构,其晶体数据及结构参数列于表2和表3.由图2可见,化合物G 2⁃3的胺基膦配体通过磷原子和钌中心配位,而氮原子不参与配位,钌中心呈现一个五配位的三角方锥构型.钌原子分别与2个氯、2个卡宾碳和1个磷原子配位.其中,2个钌氯键的键长分别为0.24079(12)和0.23923(13)nm,相差不大.但金属钌中心和两个卡宾碳原子的键长相差较大,分别为0.2085(5)和0.1833(5)nm,充分显示出钌碳单键和双键的配位特性.钌膦键的键长为0.24220(13)nm,在正常的范围之内。
j. am. chem. soc.的文章类型-回复首先,需要明确的是,j. am. chem. soc. 是《美国化学学会杂志》(Journal of the American Chemical Society)的简称。
作为一个高影响力的学术期刊,它涉及的文章类型非常广泛,覆盖了化学领域的各个方向。
下面以中括号内的内容为主题,我们来一步一步回答和解析这个问题。
[文章类型]:以这个主题为基础,我们可以选择一种比较通用的文章类型进行分析,例如综述文章(review article)。
综述文章通常对某个领域的最新进展和研究成果进行总结和评述,把相关文献进行归类整理,可以为该领域的学者提供一个全面的概览及从中获得灵感和启发。
在综述文章中,我们可以对该主题进行全面的研究回顾、对比、综合和分析,以期帮助读者了解并深入探讨该主题。
下面是一份可能的文章大纲:Ⅰ. 引言A. 引入主题:介绍[文章类型] 这个主题的研究背景和意义B. 论述目的:说明本文的目的和构成Ⅱ. 研究历史与进展A. 回顾过去:通过文献回顾,介绍过去在[文章类型] 方面的研究和发展情况B. 当前挑战:讨论目前研究领域的挑战和问题Ⅲ. [文章类型]方法与技术A. 介绍常用的[文章类型] 实验方法和技术B. 分析这些方法和技术的优缺点Ⅳ. [文章类型]应用与前景A. 阐述[文章类型] 在不同领域的应用案例B. 展望[文章类型] 的未来发展方向和可能的研究热点Ⅴ. 结论A. 总结本文的主要内容和观点B. 强调[文章类型] 的重要性和潜在的贡献在这份大纲的基础上,我们可以逐步展开文章内容,提取相关文献进行综述,并且可以加入自己的观点和分析。
总体而言,一篇关于[文章类型] 主题的综述文章应该具备以下特点:全面回顾、系统综合、观点独特、观点支持。
通过这样的文章,我们可以向读者传达对该主题的全面理解和深入见解,并为进一步研究和创新性思考提供思路和基础知识。
需要注意的是,以上仅仅是对一种可能的文章类型进行解析和概述,并不能代表所有的j. am. chem. soc. 文章类型。
Cite this:Chem.Soc.Rev.,2013,42,794Three dimensional macroporous architectures and aerogels built of carbon nanotubes and/or graphene:synthesis and applicationsStefania Nardecchia,Daniel Carriazo,M.Luisa Ferrer,Marı´a C.Gutie ´rrez and Francisco del Monte*Carbon nanotubes and graphene are some of the most intensively explored carbon allotropes in materials science.This interest mainly resides in their unique properties with electrical conductivities as high as 104S cm À1,thermal conductivities as high as 5000W m À1K and superior mechanical properties with elastic moduli on the order of 1TPa for both of them.The possibility to translate the individual properties of these monodimensional (e.g.carbon nanotubes)and bidimensional (e.g.graphene)building units into two-dimensional free-standing thick and thin films has paved the way for using these allotropes in a number of applications (including photocatalysis,electrochemistry,electronics and optoelectronics,among others)as well as for the preparation of biological and chemical sensors.More recently and while recognizing the tremendous interest of these two-dimensional structures,researchers are noticing that the performance of certain devices can experience a significant enhancement by the use of three-dimensional architectures and/or aerogels because of the increase of active material per projected area.This is obviously the case as long as the nanometre-sized building units remain accessible so that the concept of hierarchical three-dimensional organization is critical to guarantee the mass transport and,as consequence,performance enhancement.Thus,this review aims to describe the different synthetic processes used for preparation of these three-dimensional architectures and/or aerogels containing either any or both allotropes,and the different fields of application in which the particular structure of these materials provided a significant enhancement in theefficacy as compared to their two-dimensional analogues or even opened the path to novel applications.The unprecedented compilation of information from both CNT-and graphene-based three-dimensional architectures and/or aerogels in a single revision is also of interest because it allows a straightforward comparison between the particular features provided by each allotrope.Nanoparticles (NPs)and nanocomposites benefiting from the synergy between inorganic and organic compounds are indeed playing a major role in the development of advanced functional materials for a number of emerging applications (e.g.,catalysis,storage and controlled release systems,smart fillers,and bio-technologies).1Within this context,assembling NPs into struc-turally macroscopic structures is of special relevance for the realistic development of any of the above-cited applications because the resulting materials would offer a desirable combi-nation of high internal reactive surface area and straightforward molecular transport through broad ‘‘highways’’leading to such a surface.2These morphologies are also obtained in monolithsexhibiting hierarchical structures that combine micro-,meso-,and macropores—so that the micro and mesoporosity provide high surface areas while the macroporosity guaranties accessi-bility to this surface.Besides morphology,it is obvious that the chemical nature of the monolith also plays a role and will ultimately determine the particular application of these materi-als.For instance,the use of monolithic aerogels based on silica as columns in high-pressure liquid chromatography (HPLC)is quite extended 3–5whereas the electrically conductive framework of monolithic carbon aerogels has determined their preferred application as electrodes in electrochemical devices (supercapa-citors,fuel cells,batteries,etc.).6–8Interestingly,sol–gel chemis-try is one of the most common synthetic processes used for preparation of both silica and carbon hierarchical monoliths.Thus,Tanaka and coworkers first described the preparation of silica columns for HPLC in 19969using a sol–gel process basedInstituto de Ciencia de Materiales de Madrid (ICMM),Consejo Superior deInvestigaciones Cientı´ficas (CSIC),Cantoblanco 28049,Madrid,Spain.E-mail:delmonte@icmm.csic.es;Fax:+34913720623;Tel:+34913349033Received 24th August 2012DOI:10.1039/c2cs35353a/csrChem Soc RevP u b l i s h e d o n 16 N o v e m b e r 2012. D o w n l o a d e d b y U n i v e r s i t y o f S c i e n c e a n d T e c h n o l o g y o f C h i n a o n 01/10/2013 09:10:35.on the hydrolysis and polycondensation of tetramethoxysilane (TMOS)in the presence of polyethylene oxide (PEO)as a tem-plate.10,11Meanwhile and inspired by the seminal work on silica aerogels by Kistler in 1931,12Pekala et al.13first reported on the use of sol–gel chemistry for the achievement of highly cross-linked organic gels that,after supercritical drying and subsequent thermal treatment in an inert atmosphere,resulted in carbon monoliths.The main features that determined the popularization of the sol–gel process are the capability to produce materials in a variety of forms that includes thin films and three-dimensional (3D)architectures,the textural and chemical characteristics of which can be easily tuned for the achievement of co-continuous structures with well defined hierarchical structures for bare silica-or carbon-based materials as well as hybrids and composites.14–18While recognizing the tremendous relevance of silica,hybrid-silica and carbon mono-liths,the focus of this review will not be on these particular materials because there are already excellent reviews and books that cover most of the recent advances in this area.19–25Less revised has been however the preparation and application of composite-based monolithic aerogels and,in particular,of those containing carbon nanotubes (CNTs)and/or Ts and graphene are both allotropes of Ts exhibit a cylindrical hollow nanostructure with the walls formed by one-atom-thick sheets of carbon that are rolled at specific and discrete angles,which ultimately determine whether the individual nanotube shell is a metal or a Ts are categorized as single-,double-or multi-walled CNTs (SWCNTs,DWCNTs or MWCNTs,respectively)depending on the number of the rolled walls.Mean-while,graphene is a planar monolayer of carbon atoms arranged into a two-dimensional (2D)honeycomb lattice with a C–C bond length of 0.142nm.These two well-known allotropes of carbon have attracted much attention from the scientific community because they exhibit unique properties (electrical conductivities as high as 104S cm À1,thermal conductivities as high as 5000W m À1K and superior mechanical properties with elastic moduli on the order of 1TPa,for both of them)26–31that,eventually,can be translated into any architecture built up with any of them.In this review,we will summarize the use of CNTs and graphene oxide (GO)as,respectively,monodimensional (1D)and 2D building units in the synthesis of 3D macroporous architectures and aerogels.We will also describe the great potential of the resulting hydrogels and aerogels in the field of actuators,supercapacitors and polymer composites.T-based 3D architectures and aerogelsSince their discovery in 1991,32CNTs have been the subject of numerous research works given their unique properties,for example,extremely high electrical conductivities,very high thermal conductiv-ities,and outstanding mechanical properties.However,the proces-sing of CNT-based materials into engineered 3D macroporous structures is still in its infancy and most of the arrays prepared to date with controlled areas and nanotube lengths are 2D-type;e.g.well vertically aligned CNT architectures,33,34self-assembled CNTStefania Nardecchia,Francisco del Monte,M.Luisa Ferrer,Daniel Carriazo and Marı´a C.Gutie ´rrez Stefania Nardecchia graduated in Industrial Chemistry in 2005at the University of Roma ,obtained her PhD from the University of Madrid in 2012.In 2008she joined the Group of Bioinspired Materials at the Institute of Materials Science of Madrid (ICMM-CSIC)where she is currently working.Her research interests focused on materials for drug release and biomaterials for bone and neural tissue regeneration.Daniel Carriazo obtained his PhD from the University of Salamanca in 2008on the synthesis of layered double hydroxides and porous oxides for catalytic applications.In 2009he joined the Group of Bioinspired Materials at the Institute of Materials Science of Madrid (ICMM-CSIC)where he is currently working.During 2011he spent eight monthsworking in the group headed by Prof.Niederberger at the ETH-Zu¨rich on the synthesis of nano-materials by non-aqueous routes.His present scientific interest is focused on the synthesis of carbonaceous materials with hierarchical porosity for energy storage and environmental applications.Marı´a Luisa Ferrer is a tenured scientist at the Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC).After an MSc degree in Polymer Science (1992),she completed her PhD in chemistry at the University Autonoma of Madrid (1995).She was a postdoctoral fellow over the next three years ,first at the University of Patras (Greece)and ,after that ,at UCLA (USA).After that ,she got a teaching appointment at the UMH (Spain).She joined the ICMM-CSIC in 2000to work on the preparation of hierarchical materials with applications in both energy and biomaterials.Marı´a C.Gutie ´rrez obtained her PhD in Organic Chemistry at the University of Granada in 2001.From 2001to 2003,she worked as a postdoctoral fellow with Prof.Furstoss in Biocatalysis and Fine Chemistry at the Universite´de la Me ´diterrane ´e (France),and participated in European projects from IV and V Framework Programmes.In 2004,she joined the Group of Bioinspired Materials at the ICMM-CSIC in Spain and became a tenured scientist in 2009.Her research interest is the development of New Routes for Preparation of Hierarchical and Multifunctional Materials for Applications in Biotechnology and Biomedicine.Francisco del Monte is a Scientist at the Instituto de Ciencia de Materiales de Madrid (ICMM-CSIC)in Spain.He received a BSc degree in organic chemistry in 1991,an MSc degree in polymer science in 1992,and a PhD in chemistry in 1996.He then spent two years as a post-doctoral fellow at the University of Los Angeles ,California.Since 2004,he leads the Group of Bioinspired Materials at the ICMM-CSIC.His current scientific interest is the use of biomimetic chemistry and deep eutectic solvents for the preparation of hierarchically organized materials.Review ArticleChem Soc RevP u b l i s h e d o n 16 N o v e m b e r 2012. D o w n l o a d e d b y U n i v e r s i t y o f S c i e n c e a n d T e c h n o l o g y o f C h i n a o n 01/10/2013 09:10:35.sheets 35or textiles containing nanotube-fiber capacitors woven in orthogonal directions,36among others.37Eventually,3D sieve architectures have also been constructed,38although the length of the third dimension of the regular patterned cavities is typically limited to that of some few CNTs,39,40except for those composites where the CNT fraction is minor.41The valuable contribution of these works to different applications has been highlighted in recent reviews 42–48and,for this reason,will not be the subject of this review either.Chemical vapor deposition (CVD)techniques have been recently used to prepare 3D structures composed of freestanding films of vertically aligned carbon nanotubes.49Considering the valuable contribution of these 3D structures to different applications,50it is our belief that ‘‘true’’3D architectures—in which the third dimen-sion is within the range of the other two—produced by chemical routes could exhibit interesting properties (e.g.in terms of both electrical conductivity and mechanical properties)for industrial applications.This belief is actually corroborated by the increased number of works dealing with CNT-based 3D architectures pub-lished within the last two years;i.e.ca.65%of the works revised herein correspond to the 2011–2012period.The main reason behind this tremendous activity is that,as a general trend for any catalytic application,the performance of any device based on CNTs can experience a significant enhancement by the use of 3D architectures rather than 2D ones because of the obvious increase of active material in the former case.Hydrogels,organogels,and aerogels based on silica or carbon and consisting of micro-,meso-and even macroporous networks forming a hierarchical structure that guaranties molecular transport throughout the entire 3D architecture to gain access to the internal reactive surface are illustrative examples of 3D macroscopic assemblies corroborating this issue.19–25Thus,the aim of this review with regard to CNTs will be to summarize those self-assembling processes described to date that have been capable of building ‘‘true’’3D hierarchical macro-structures and have explored those applications where silica and carbon monoliths have already proved efficient (e.g.membranes and columns for water treatment and chromatographic separa-tions,electrodes for supercapacitors,fuel cells and batteries,and catalytic substrates,among others).1.1Organogels and aerogels from CNT suspensionsThe organic functionalization of either SWCNTs or MWCNTs with an organogelator can result in the formation of freestanding CNT organogels.For instance,SWCNTs functionalized by ferrocene-grafted poly(p -phenyleneethynylene)can gelate common organic solvents such as chloroform to form robust 3D nanotube networks that cannot be re-dispersed in any organic solvent.51Thermally annealed CNT aerogels were mechanically stable and stiff(Fig.1),highly porous (99%),and exhibited excellent electrical conductivity (ca.1–2S cm À1)and large specific surface area (590–680m 2g À1).52Moreover,Fmoc-protected-amino-acid-based (Fmoc-Phe-OH,where Fmoc stands for N -fluorenyl-9-methoxycarbonyl and Phe for Phenyl-alanine)hydrogels have also been used to incorporate and disperse SWCNT within the gel phase at physiological pH and temperature.53The resulting hydrogels exhibited an intriguing 1D alignment of SWCNTs on the surface of the gel nanofibers that enhanced theelastic properties as well as the thermal stability,and provided a notorious electrical conductivity of 3.1S cm À1to the resulting hydrogels.Meanwhile,the presence of functional groups on MWCNTs that remained available after gelation allowed the conjugation of the properties of gels and nanostructured car-bon materials.54The benefits of using organogelators were therefore multiple considering that,besides inducing gelation and conferring additional properties to the resulting gels,functionalization helps for CNT dispersion at the solution stage and hence,to the achievement of a homogeneous distribution of CNT throughout the resulting gel.Within the context of monomers and polymers,Zhang et al.demonstrated that embedding either MWCNTs or acid-treated MWCNTs into a poly(3,4-ethylenedioxythiophene)–poly(styrene-sulfonate)(PEDOT–PSS)aerogel matrix can significantly enhance the specific surface areas (280–400m 2g À1)of the resulting compo-site aerogels while maintaining good thermal stability and electrical conductivities (1.2–6.9Â10À2S cm À1).55Poly (3-(trimethoxysilyl)propylmethacrylate)(PTMSPMA)can also be used to disperse and functionalize MWCNTs.In this case,strong and permanent chemical bonding between percolated MWCNTs in the resulting free-standing monolithic aerogel was obtained upon the hydrolysis and condensation of PTMSPMA.The entangled MWCNTs generated mesoporous structures on the honeycomb walls,creating aerogels with a surface area of 580m 2g À1(nearly 2-fold the surface area of pristine MWCNTs),remarkable elastic properties and good electrical conductivity (e.g.up to 0.67S cm À1).All these features determined the exceptional pressure and chemical vapor sensing capabilities of these aerogels.56Surfactants have also been used for dispersion of CNT and subsequent formation of aerogels.For instance,Ostojic solubilized SWCNTs in 1%w/v sodium dodecyl sulphate (SDS)aqueous solution.Streptavidin phosphate and DNA complexes were there-after used for SDS replacement and so induce SWCNT gelation.Ethanol and ethanol–water solvent exchange and subsequent critical-point-drying resulted in the formation of SWCNT aerogels exhibiting a previously unobserved peak at 1.3eV in the photo-luminescence spectrum that corresponds to a phonon-assisted recombination of photoexcited charges.57In another interesting example,Yodh and coworkers suspended different concentrations of as-received CNTs (e.g.weight fractions ranging from 5to 13mg mL À1)in water with sodium dodecylbenzene sulfonate.58The suspensions were left overnight to set into elastic gels thatwereFig.1Picture of SWCNT aerogels weighing 17.4mg (density:9.8mg mL À1)before (a),during (b)and after (c)application of a 20g weight.Monoliths were obtained from SWCNTs functionalized with ferrocene-graftedpoly(p -phenyleneethynylene).(Reproduced with permission from ref.52.Copyright (2011)Elsevier Publishing Group).Chem Soc RevReview ArticleP u b l i s h e d o n 16 N o v e m b e r 2012. D o w n l o a d e d b y U n i v e r s i t y o f S c i e n c e a n d T e c h n o l o g y o f C h i n a o n 01/10/2013 09:10:35.subsequently soaked at 901C in aqueous solutions of polyvinyl alcohol (PVA)for structural reinforcement.Reinforced and non-reinforced gels were thereafter submitted to either freeze-or critical-point-drying processes for the achievement of the aero-gel structure.PVA-reinforced aerogels exhibited outstanding mechanical properties (for instance,they were able to hold 8000times their weight,Fig.2)whereas much better conductiv-ities were found for non-reinforced ones (e.g.0.6S cm À1for non-reinforced versus ca.10À5S cm À1for reinforced ones).More recently,Islam and coworkers,using a similar approach in which they substituted PVA by polydimethylsiloxane (PDMS),produced transparent (ca.93%of transmittance for a 3m m-thick aerogel)and stretchable conductors,the electrical conductivity of which (ranging 0.7–1.1S cm À1)remained basically the same under high bending strain.59Transparent SWCNT aerogels can also be obtained using silica as binder (Fig.3a).In this case,SWCNTs were dispersed in water using SDS or sodium deoxy-cholate and then reacted with a silica precursor like TMOS either by a chemical vapor-into-liquid sol–gel process—in which the low boiling point of TMOS allows vapours diffusion through the SWCNT aqueous suspension—or by a regular liquid-phase sol–gel process—in which small aliquots of TMOS are added into the SWCNT aqueous suspension.60After CO 2supercritical drying,the resulting solution-free and surfactant-free SWCNT-silica aerogels provided access to new photophysical properties of SWCNT and hence,converted this solid-state nanomaterial into not only an ideal system for making fundamental optical measurements,but also a novel and suitable platform for the development of applications in sensing,photonics,and opto-electronics in the near future (Fig.3b–d).Within the context of dispersing CNTs in aqueous solutions that also contain a certain molecular precursor in charge of building up the 3D architecture where the CNT will be finally immobilized,the sol–gel polymerization of resorcinol andformaldehyde offers interesting perspectives.For instance,Baumann and coworkers have recently performed a quite extensive and stimulating work on SWCNTs and DWCNTs 3D architectures synthesized by resorcinol–formaldehyde polycondensation.By intro-ducing low concentrations of the sol–gel precursors to a suspension of highly purified SWCNTs,the polymerization was primarily induced on the walls of the CNT bundles and,more importantly,at the junctions between adjacent bundles to form an organic binder.The resulting assembly was dried and subsequently pyrolyzed to convert the organic binder into carbon.61TheaerogelsFig.2(a)Picture of SWCNT aerogels (density:7.5mg mL À1)non-reinforced (left,black coloured)and reinforced (right,gray coloured)with 1wt%PVA.(b)Three PVA-reinforced aerogel monoliths (total mass =13.0mg)supporting 100g (ca.8000times their weight).(c)SEM micrograph revealing themacroporus architecture of PVA-reinforced aerogel (0.5wt%PVA,10mg mL À1CNT content).(d)TEM micrograph of non-reinforced CNT aerogel.(Reproduced with permission from ref.58.Copyright (2007)Wiley-VCH).Fig.3(a)Picture of aerogels without (blank)and with SWCNTs.(b)PL spectrum of aerogels exposed to CO 2,THF,and ether vapors.The PL spectrum of non-exposed (e.g.in vacuum)is also included for comparison.(c)Shift in PL emission wavelength relative to the signal collected under vacuum as a function of SWCNT diameter after exposure of SWNT-aerogels to air (green square),CO 2(red dots),THF (blue triangle),and ether (yellow star).(d)Emission wavelength shifts for SWCNTs with different diameter after alternating exposure to ether and vacuum:(9,5)light blue squares;(7,6)red dots;(7,5)green triangle;and (8,3)blue triangle.(Adapted with permission from ref.60.Copyright (2011)American Chemical Society).Review Article Chem Soc RevP u b l i s h e d o n 16 N o v e m b e r 2012. D o w n l o a d e d b y U n i v e r s i t y o f S c i e n c e a n d T e c h n o l o g y o f C h i n a o n 01/10/2013 09:10:35.could be also prepared with varying SWCNT loading (0–55wt%).62At nanotube loadings of 55wt%,shrinkage of the aerogel monoliths during carbonization and drying was almost completely eliminated and the electrical conductivities improved by an order of magnitude as compared to those of foams without SWCNTs.Particularly interesting in terms of conductivity (up to 8S cm À1)and surface area (above 500m 2g À1)were those composites based on DWCNTs.63Interestingly,the porous network of these architectures can be surface decorated with oxide coatings (Fig.4).64In this case,sol–gel deposition of SiO 2,SnO 2or TiO 2produced a conformal overlayer on the primary ligament structure of the SWCNT-based support,thus preserving open porosity within the monolithic part.The result-ing aerogels (SWCNT-CA)exhibited good electrical conductivity (up to 1S cm À1)and an enhancement in the mechanical properties relative to the uncoated SWCNT-CA support that should prove advantageous for a number of applications,such as battery electrodes,sensing devices,and catalysts.Morerecently,Gutie´rrez et al.have studied the polycondensation of not only resorcinol and formaldehyde 65but also furfuryl alco-hol 66in deep eutectic solvents (DES)because of their capability to homogeneously disperse high amounts of CNTs.In the furfuryl alcohol case,the presence of DES induced the formation of monolithic carbons with a bimodal porosity that comprises from micro-up to macropores.The morphology of the resulting carbons (C FA ,without CNTs)consisted of a bicontinuous porous network built of highly cross-linked clusters that aggregated and assembled into a stiff,interconnected structure (Fig.5).This sortof morphology is typical of carbons obtained via spinodal decomposition processes where the formation of a rich-polymer phase by polycondensation is accompanied by the segregation of the non-condensed matter (creating first a poor-polymer phase that,ultimately,becomes a depleted-polymer phase),the elimina-tion of which (either before carbonization by washing or during carbonization by thermal decomposition)results in the formation of the above-mentioned bicontinuous porous structure.67In this particular case,furfuryl alcohol condensated on the walls of the MWCNTs so that the resulting bicontinuous porous network resembled a skeleton network composed of interconnected MWCNTs ‘‘glued’’by the carbon resulting from the furfuryl alcohol condensation and pyrolysis (C FACNT ).The presence of a carbon shell that coated every MWCNT and formed strong junctions between them was reflected in both the electrical conductivity (up to 4.8S cm À1,as measured by the four-probe method)and the elastic character (Young’s modulus,11MPa)of the monoliths having the largest MWCNT content.The combi-nation of high electrical conductivity,hierarchical structure and pseudo elastic properties contributed to retain 75%of theinitialFig.4SEM images of (a and b)as-synthesized and (c and d)annealed at 3201C TiO 2/SWCNT-CA composites at low and high magnifications.TEM images of annealed (e and f)TiO 2–SWCNT-CA composites at low and high magnifications.Inset in (f)is the electron diffraction pattern of the annealed TiO 2/SWCNT-CA.(Reproduced with permission from ref.64.Copyright (2011)American ChemicalSociety).Fig.5SEM micrographs of C FA (a,b and c),C FACNT1(d)and C FACNT5(f,h and i).TEM micrographs of colloidal carbon corresponding to C FA and C FACNT1(c),and fibrillar carbon corresponding to C FACNT1and C FACNT5(e and g).(Reproduced with permission from ref.66.Copyright (2011)Wiley-VCH).Chem Soc Rev Review ArticleP u b l i s h e d o n 16 N o v e m b e r 2012. D o w n l o a d e d b y U n i v e r s i t y o f S c i e n c e a n d T e c h n o l o g y o f C h i n a o n 01/10/2013 09:10:35.capacitance at current densities of up to 765mA cm À2(29A g À1)when two of these monoliths (each monolith was 1.2cm in diameter and 1.1mm in height,and weighed 17mg)were assembled into a supercapacitor cell.It is also worth noting those works using polymers that can play an ‘‘all-in-one’’role as both dispersing agents helping to the achievement of homogeneous aqueous suspensions of CNT and structural binders holding the 3D architecture formed after any sort of processing (e.g.freeze-drying,electrospun,etc.).For instance,Tasis and coworkers used PVA as a dispersing-aid agent of KMnO 4-treated MWCNTs in water.The application of flash freezing to the MWCNT/PVA aqueous suspension (e.g.in liquid nitrogen)and subsequent freeze-drying resulted in MWCNT aerogels that exhibited interesting thermal and cata-lytic properties as well as absorption capacity of polynuclear aromatic substances.68This ‘‘all-in-one’’approach can be further extended upon the use of different polymers.For instance,del Monte and coworkers used chitosan for disper-sing HNO 3-treated MWCNTs (up to 8wt%)in water.69MWCNT aerogels were obtained upon the application of the ISISA (ice segregation induced self-assembly)process that basically con-sists of a unidirectional freezing of the sample (e.g.by dipping it into a nitrogen liquid bath at a constant rate)followed by freeze-drying.70In this case,unidirectional freezing allowed the achievement of macroporous structures with well-aligned micro-channels in the freezing direction and a well-patterned morphol-ogy between channels (mellar and microhoneycomb,respectively)(Fig.6).These ultralightweight aerogels (specific gravity ranging from 4.9Â10À2to 9.4Â10À2along with the MWCNT content)exhibited remarkable electrical conductivities of up to 2.5S cm À1for those aerogels composed of 89wt%MWCNTs and 11wt%CHI.Interestingly,the aerogel structure could be reinforced upon exposure to glutaraldehyde vapors without detri-mental effects on either the morphology or the electrical con-ductivity.71These features allowed the use of these aerogels as high-perfomance 3D electrodes in both direct methanol and microbial fuel cells (DMFCs and MFCs,respectively).69,72Particularly interesting was the microchanneled structure in this latter case,allowing the possibility to work in the ‘‘flow-through’’mode so that bacteria could colonize the entire internal structure of cylindrical aerogels of ca.4mm in diameter and 12mm in height (Fig.7)that,otherwise (e.g.in static conditions),was not possible.73The validity of these aerogels to work as high-perfo-mance 3D electrodes under ‘‘flow-through’’conditions was not only demonstrated in MFCs,but also for electrodeposition of a layer of calcium–phosphate salts homogenously distributed throughout the entire internal surface of the aerogels.Interest-ingly,the crystal habit of the deposited mineral was easily controlled by the electrodeposition conditions (Fig.8).74It is worth noting that,as in the previous case,homogeneous coatings were not attained upon chemical mineralization carried out under non-flow conditions.71More recently,the same group has explored the capability of different polysaccharides (e.g.chondroi-tin sulphate)and protein-like polymers (e.g.gelatin)for the preparation of analogue MWCNT aerogels.75The authors have also explored the potential application of these MWCNT aerogels as scaffolds for tissue engineering purposes.71,74–761.2.CNT-surface modified aerogelsCNT functionalization of the internal surface of preformed aerogels has recently gained increased interest because it offers a tremendous versatility considering the existing palette of 3D architectures that may be suitable for this purpose.For instance,Petrov and coworkers reported on the ice-mediated deposition of individual CNTs onto the inner surface of a pre-formed macroporous polymer cryogel.77Fig.6SEM micrographs of MWCNT scaffolds:(a)cross-section view,(b)longitudinal view according to plane 1and (c)longitudinal view according to plane 2.Bars are 200m m in every case.(Reproduced with permission from ref.74.Copyright (2012)Wiley-VCH).Fig.7SEM images (a–c)of biofilm at different magnifications taken from the inner part of the 3D scaffold.(Adapted with permission from ref.72.Copyright (2011)Royal Society of Chemistry).Review ArticleChem Soc RevP u b l i s h e d o n 16 N o v e m b e r 2012. D o w n l o a d e d b y U n i v e r s i t y o f S c i e n c e a n d T e c h n o l o g y o f C h i n a o n 01/10/2013 09:10:35.。
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Title: Understanding Chemical Physics Letters Journal and Its CategorizationIntroduction:In the realm of scientific research, academic journals play a pivotal role in disseminating knowledge and driving progress in various disciplines. Researchers and scholars often strive to publish their work in reputable journals, respected within their respective fields. Chemical Physics Letters is a prominent journal catering to the interdisciplinary niche of chemical physics. This article aims to provide a comprehensive explanation of Chemical Physics Letters, its significance, and its categorization within the scientific community.1. Chemical Physics Letters: An OverviewChemical Physics Letters (CPL) is an esteemed scientific journal that publishes groundbreaking research in the field of chemical physics. Founded in 1970, CPL has been instrumental in promotinginterdisciplinary research encompassing both chemistry and physics. It serves as a platform for scientists to share their discoveries, theories, and experimental data, facilitating collaboration and advancement in the field.2. Scope and Content:CPL focuses on a wide range of topics, including molecular dynamics, spectroscopy, quantum chemistry, computational chemistry, chemical kinetics, and surface science. The journal welcomes contributions that highlight the interface between chemistry and physics, encouraging scientists to explore novel approaches towards understanding chemical phenomena using physical principles.3. Editorial Process and Peer Review:Chemical Physics Letters adopts a rigorous peer-review process to ensure that publications meet high scientific standards. After submission, manuscripts undergo a thorough evaluation by subject matter experts, who scrutinize the quality, significance, and originality of the research. This critical appraisal helps maintain the journal's credibility by identifying flaws, suggesting revisions, and selecting the most cutting-edge research for publication.4. Impact Factor and Reputation:The impact factor (IF) is a widely used metric to assess the influence and relevance of academic journals. It quantifies the average number of citations received by articles published in a particular journal over a specific period. Chemical Physics Letters consistently achieves an excellent impact factor, implying that the research published within its pages garners substantial attention from the scientific community. A high IF reflects the journal's reputation and the significance of the research it showcases.5. Categorization and Ranking:To facilitate better navigation for researchers, academic journals are categorized, often referred to as journal indexing. Chemical Physics Letters falls into the Chemical Physics category, marking its specialization as a journal bridging the gap between chemistry and physics. Within this category, CPL has established itself as one of the leading publications, displaying a consistently impressive impact factor and attracting high-quality research submissions.6. Practical Implications:The categorization and reputation of Chemical Physics Letters holdpractical implications for researchers in the field of chemical physics. By submitting their research to CPL, scientists have the opportunity to gain exposure, reach a wide audience, and receive constructive feedback from experts in the field. Additionally, publications within Chemical Physics Letters can enhance researchers' academic credentials, contributing to career development and the potential for future collaborations.Conclusion:Chemical Physics Letters' consistent publication of cutting-edge research, interdisciplinary focus, and high impact factor make it a sought-after platform for researchers in the field of chemical physics. By bridging the gap between chemistry and physics, CPL facilitates the advancement of knowledge and fosters collaboration. Its categorization within the Chemical Physics index confirms its prominence and relevance within the scientific community. As research continues to push boundaries, Chemical Physics Letters is likely to maintain its pivotal role as a platform for groundbreaking discoveries and innovative ideas in the field.。
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20850.01330.806 409 4.50.027060.735 774 3.20.034350.762 15287.90.107180.745 739 5.40.053960.715 227.60.001180.774 105 5.10.007480.647 129 4.90.00780.74475 3.50.002990.639212 3.70.013920.784 201 5.60.009290.599 500 6.30.06138 1.238 >10.00.00042 1.049 290 6.10.019640.625 251 5.60.017330.895 12498.40.075460.68 241 2.20.005560.628 1341 6.70.120620.829 651 6.90.026690.572 224 5.10.010210.672 290 5.30.013220.702 194 1.60.002660.7278>10.00.000620.792 314>10.00.019270.649 32830.001390.381 520 6.30.034550.62153 5.20.004350.904 200 1.30.002460.856 109 3.70.00563143 5.80.013670.825 439 4.20.025470.66 441>10.00.03210.853 17290.80.002020.494 1527.40.009010.741 624 2.40.016810.714 337 6.40.02850.71 173 1.90.002010.614 124 6.30.008010.593 2207.60.010810.602 4708.20.028730.596 221 5.20.00853 1.29 4957.50.036490.714 967.20.003150.52311>10.00.000450.543 184 3.50.006730.588 1064 2.80.017560.666 2437.60.014140.744 257.10.002380.868 105130.022770.574 10130.003550.834 2518.20.017620.63 16669.90.081330.508 1478 4.10.10840.548 14830.008560.8753427.80.015630.587 559.80.002470.6496 1.50.001250.668648.10.002270.561 178 6.20.010850.6 247>10.00.011750.526 202 5.20.013550.701 1484 5.40.069550.546 116 6.40.005740.60572 2.10.00140.58954>10.00.004010.856 351 6.60.011110.57 960 3.90.021660.681 1549.50.006150.597 5790.008180.646 6720.0008353 2.30.00061176 2.60.005320.633 1947.80.016490.569 223 5.60.014960.968 25280.006360.457 1626 5.50.049760.537 1977.10.008730.585 128 5.40.00580.57919>10.00.001080.734 650 3.70.017210.673 9419.10.050830.59113>10.00.00130.598 21090.007690.475 906>10.00.066080.687 350 3.90.005590.396 2247.80.01640.479 1789 5.50.074220.539 419>10.00.014550.491 579 6.80.034280.585 11717.30.084950.73 918.60.003920.471 458.60.00220.655 100 6.20.007370.666 335 5.10.012850.644 964 5.50.038290.59199 5.20.004810.478 302 6.60.012460.48640 2.10.000610.345 392>10.00.021350.719339>10.00.01560.489 5138.90.025150.615 50 4.50.001620.659 1368.50.005580.639 353 5.90.018730.713 495 4.80.011170.321 1147.60.003960.391 156 6.70.022520.706 508 6.50.027410.476 82 5.10.003380.472 410>10.00.020760.421 400>10.00.012770.531 463 4.70.008250.53 728 5.70.012880.253 2367.10.012090.669 180 3.80.004490.45 360>10.00.018270.679 2957.80.035210.653 950 3.40.026580.586 218 5.20.006840.446 2547.50.007820.487。
刊名简称刊名全称ISSN PLOS PATHOG PLoS Pathogens1553-7366 REV MED VIROL REVIEWS IN MEDICAL VIROLOGY1052-9276 ADV VIRUS RES ADVANCES IN VIRUS RESEARCH0065-3527 AIDS AIDS0269-9370 ANTIVIR THER ANTIVIRAL THERAPY1359-6535 J VIROL JOURNAL OF VIROLOGY0022-538X RETROVIROLOGY Retrovirology 1742-4690 ANTIVIR RES ANTIVIRAL RESEARCH0166-3542 INFLUENZA OTHER RESP Influenza and Other Respiratory Viruses1750-2640 INT J MED MICROBIOL INTERNATIONAL JOURNAL OF MEDICAL MICROBIOLOGY1438-4221 J CLIN VIROL JOURNAL OF CLINICAL VIROLOGY1386-6532 J GEN VIROL JOURNAL OF GENERAL VIROLOGY0022-1317 J MED VIROL JOURNAL OF MEDICAL VIROLOGY0146-6615 J VIRAL HEPATITIS JOURNAL OF VIRAL HEPATITIS1352-0504 MICROBES INFECT MICROBES AND INFECTION1286-4579 VIROLOGY VIROLOGY0042-6822 ACTA VIROL ACTA VIROLOGICA0001-723X AIDS RES HUM RETROV AIDS RESEARCH AND HUMAN RETROVIRUSES0889-2229 ARCH VIROL ARCHIVES OF VIROLOGY0304-8608 CURR HIV RES CURRENT HIV RESEARCH1570-162X FOOD ENVIRON VIROL Food and Environmental Virology1867-0334 FUTURE 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收稿:2005年2月,收修改稿:2006年4月 3通讯联系人 e 2mail :zzm @离子液体中手性催化剂回收研究周智明3 姜 飞 莫凡洋(北京理工大学化工与环境学院 北京100081)摘 要 近年来,贵重的手性催化剂的回收与再利用越来越引起化学工作者的关注,而离子液体在催化剂回收方面有其独特的优势。
本文综述了离子液体在手性催化反应中的应用,在回收催化剂的同时,也能一定程度上提高催化剂的催化效率:着重介绍了新型含咪唑盐手性催化剂及其在不对称催化中的应用,由于它在离子液体和有机溶剂的显著差异可以很容易地得到回收,并且能一定程度地稳定催化剂,提高催化效率,这对我们设计合成新型可回收的催化剂具有重要的借鉴意义。
关键词 离子液体 不对称催化 对映选择性 回收中图分类号:O64514;O62113;O643136 文献标识码:A 文章编号:10052281X (2007)0120042209Advances of R ecycling Chiral C atalysts in Ionic LiquidsZhou Zhiming3 Jiang Fei Mo Fanyang(School of Chemical Engineering and Environment ,Beijing Institute of T echnology ,Beijing 100081,China )Abstract Recently ,m ore and m ore chemists are concerned about the recycle and reuse of expensive transition metal catalysts.I onic liquid has unique advantages in recycling catalysts.This article reviews the application of chiral catalyst reactions in ionic liquids ,which can not only recycle and reuse catalysts ,but als o im prove the efficiencies of catalysts.In addition ,novel imidazolium contained chiral catalysts and their applications in asymmetry catalytic reactions are summarized in detail.Because of their distinct s olubilities in ionic liquids and organic s olvents ,they can be easily recycled and reused ,and they can als o enhance the stability of catalysts ,im prove the efficiencies of catalysts ,which give us a guidance to design and synthesize novel recyclable catalysts.K ey w ords ionic liquids ;asymmetric catalysis ;enantioselectivity ;recycle 在传统的不对称催化反应中要用大量的有机溶剂,这些挥发性的溶剂给环境带来了很大的危害。
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第21卷第2期2021年2月过程工程学报The Chinese Journal of Process EngineeringVol.21 No.2Feb. 2021f 材料工程D O I : 10.12034/j .issn. 1009-606X.220091Preparation and physicochemical properties of cyclopropyl methylketazineWenzhao ZH A O 12, Peng ZH AO 1, Long L IU 1, Yangfeng X IA 12,Yanqiang ZH A N G 3 4*1. Beijing K e y Laboratory of Ionic Liquids Clean Process, Institute of Process Engineering, Chinese A c a d e m y of Sciences, Beijing100190, China2. School of Chemical Engineering, University of Chinese A c a d e m y of Sciences, Beijing 100049, China3. K e y Laboratory of Science and Technology on Particle Materials, Institute of Process Engineering, Chinese A c a d e m y of Sciences,Beijing 100190, China4. Zhengzhou Institute of Emerging Industrial Technology, Zhengzhou, H e n a n 450000, ChinaAbstract : Ketazines as useful intermediates have been〇extensively applied in many industrial fields , including dyes , pharmaceuticals , aviation fuels , photosensitive materials , as well as polymerizable monomers . In this work , a new ketazine derivative (cyclopropyl methyl ketazine , C10N2H16) was preparedfrom cyclopropyl methyl ketone and hydrazine hydrate . Under the atmospheric pressure , the reaction was studied under different mole ratios of cyclopropyl methyl ketone to hydrazine , reaction temperatures , and reaction times . With the optimized reaction conditions o f 2.0:1, 363.2 K , 101.3 kPa and 7 h , the yield ofcyclopropyl methyl ketazine was up to 93.6% through the chromatograph measurements . The structure o f cyclopropyl methyl ketazine was characterized by IR and NMR spectra after it was purified through distillation . In order to prove the existence o f isomers , Gaussian 09 program to optimize the structures was used and the energy values (single point energy ) of cyclopropyl methyl ketazine was calculated . Furthermore , a comprehensive set of the physicochemical parameters for cyclopropyl methyl ketazine was provided , including density [p =0.884〜0.947 g /cm3],dynamic viscosity (?/=1.39〜2.88 mPa .s),liquid heat capacity [Cp =2.03〜2.32 J/(g K )] and surface tension (a =22.1 〜25.0 mN /m ) in temperature range (280~400 K ). The data o fp , rj and o exhibited the negative correlations with temperature , while V m , a and Cp showed the positive correlations with temperature , which all had a good fitting degree for equations . Considering the cyclopropyl methyl ketazine reaction systems , the vapor-liquid equilibria (V L E ) o f binary system (cyclopropyl methyl ketone-cyclopropyl methyl ketazine ) was measured and correlated with NRTL model to acquire the binary interaction parameters . The obtained data and correlations are valuable for industrial processes , and could be the good references for industrial design .Key words : cyclopropyl methyl ketazine ; physicochemical properties ; vapor-liquid equilibria ; isomer收稿:2020-03-19,修回:2020-04-05,网络发表:2020-05-15,Received: 2020-03-19, Revised: 2020-04-05, Published online: 2020-05-15 基金项目:国家自然科学基金资助项目(编号:21878278:21676281);北京市自然科学基金资助项目(编号:2192054)作者简介:赵文昭(1995-),女,山东省泰安市人,硕士研宄生,应用化学专业,*********************.cn;张延强,通讯联系人,E-mail:**************.cn.引用格式:赵文昭,赵鹏,刘龙,等.环丙基甲基酮连氮的制备及物化性质.过程工程学报,2021,2丨(2): 183-192.Zhao W Z, Zhao P , Liu L , e t a l . Preparation and physicochemical p r o p e rties of cyclopropyl methyl ketazine (i n Chinese). Chin. J . Process Eng.,2021,21(2): 183-192, DOI: 10.12034/j .i s s n . 1009-606X.220091.I-M f o it l a(f u w /s v c /184过程工程学报第21卷环丙基甲基酮连氮的制备及物化性质赵文昭口,赵鹏\刘龙、夏洋峰口,张延强3,4*I.中国科学院过程工程研宂所离子液体清洁过程北京市重点实验室,北京1001902.中国科学院大学化学工程学院,北京1000493.中国科学院过程工程研宄所中国科学院粉体材料技术重点实验室,北京1001904.郑州中科新兴产业技术研究院,河南郑州450000摘要:以环丙基甲基酮和水合肼为原料,合成了一种新的酮连氮(环丙基甲基酮连氮)。
R E N A L C A R EHemoRO 4 ONESINGLE REVERSE OSMOSIS SYSTEMWITH HEAT DISINFECTION2HemoRO 4 ONESINGL E RE V ER SE O SMO SI S S Y S T EM W I T H HE AT DI SINF EC T ION5,7” colored touch screenRemovable handleDecalcification withinnovative tabsBuilt-in wheelsReduced operating noise with sound-insulated aluminum housingReduced footprintA safe, continuous supply of dialysis water is now available in a high performing, low maintenance system.Thanks to multiple built-in safety features – including internal heat disinfection – HemoRO 4 ONEfulfills the rigorous requirements of home and acute dialysis, ensuring the utmost in patient safety.This portable solution is ideal for dialysis centers or ICUs in need of mobility, as well as patients who wish to carry out their dialysis treatments in the comfort of home.3SAFE• Semi-automated heat disinfection ensures high water quality and microbiological safety for dialysis ― H eat disinfection of reverse osmosis (RO) membrane, permeate path, and connection hoses with>80°C hot water• Easy to decalcify with innovative tabs―No softener needed for hard water up to 15 °dH (2,67 mmol/l) without affecting water quality or safety ―Higher security and better performances ―No handling of citric acid solution required• Short connection cables to minimize exposure to environmental contaminants • Internal leakage monitoring to protect against water damage • P re-treatment accessories:― U ltrafiltration membranes that offer extra protection frommicrobials and endotoxins― Water softener ―Water leakage detector• S ampling set accessory ensures a straightforward andstandardized microbiological sampling• Multiple access levels for end users and maintenance personnelProvides up to 70 l/h of dialysis water at inlet temperature of 10°C (2,5 bar counter-pressure). No softener needed for hard water up to 15°dH(2,67mmol/l).EASY TO USE• R eady within 10 minutes• D isinfect with the push of a button• L ow noise operation so it can be used beside the patient without any disturbance • 14,5 cm touch screen for easy to read, instant access to settings and mainfunctions• I ntegrated SD-card stores data for maintenance and service purposes • USB and Ethernet connectivity• Low care and maintenance requirements • Can be mounted to a wall for convenience4MOBILE• R obust metal housing and compact design (69 x 31,5 x 26,5 cm)• Lightweight: 35 kg (dry), 40 kg (wet)• E asy to move thanks to built-in wheels and handle• O ptional trolleys (small or large) for easier handling and transport,especially for frequent movements or long distances56Possible combinationsHemoRO 4 ONE : ECOHemoRO 4 ONE : MAXConformity declared with directive 93/42/EEC concerning medical devices.We reserve the right to make technical changes.Product range overviewHemoRO 4 ONE is available in 2 ranges: ECO and MAXECO70 l/h peak flow*70 l/h permanent on soft water supply*50 l/h permanent on hard water supply*MAX70 l/h permanent flow*Other configurations, accessories, and spare parts are available upon request.115 V, 60 Hz, NEMA 5-15P01HRO415CCNXX-UG 01HRO417CCNXX-UG •01HRO415CCNXS-UG01HRO417CCNXS-UG ••01HRO415CCNXM-UG 01HRO417CCNXM-UG ••••01HRO415CCN1X-UG 01HRO417CCN1X-UG ••01HRO415CCN1S-UG 01HRO417CCN1S-UG •••01HRO415CCN3X-UG 01HRO417CCN3X-UG ••01HRO415CCN3S-UG 01HRO417CCN3S-UG •••230 V, 60 Hz, CEE 7/701HRO415DXNXX-UG 01HRO417DXNXX-UG •01HRO415DXNXS-UG01HRO417DXNXS-UG ••01HRO415DXNXM-UG 01HRO417DXNXM-UG ••••01HRO415DXN1X-UG 01HRO417DXN1X-UG ••01HRO415DXN1S-UG 01HRO417DXN1S-UG •••01HRO415DXN3X-UG 01HRO417DXN3X-UG ••01HRO415DXN3S-UG01HRO417DXN3S-UG•••Technical specificationsA. Applies to soft water feedB. Applies to REF 01HRO4ONE2 and REF 01HRO4ONE2CC. Applies to REF 01HRO4ONE and REF 01HRO4ONECD. A switchable permanent connection must be provided in home dialysis environmentsE. Using permeate as feed water is forbiddenF. NHN: German reference “Normalhöhennull” (normal height zero)7NIPRO MEDICAL AUSTRIA GMBH :Divischgasse 4, 1210 Wien, AUSTRIA | T: +43 1 532 23 14 | F: +43 1 532 23 14 89NIPRO EUROPE EGYPT :Nile City Towers, 22nd Floor, North Tower, Nile City, Towers, Cornich El Nile, 11624 Ramelt Beaulac, Cairo, EGYPT NIPRO MEDICAL FRANCE S.A. :Biopôle Clermont-Limagne, 63360 Saint Beauzire, FRANCE | T: +33 (0)473 33 41 00 | F: +33 (0)473 33 41 09NIPRO MEDICAL GERMANY GMBH :Am Gierath 20d, 40885 Ratingen, GERMANY | T: +49 (0)2102 565 98 30 | F: +49 (0)2102 565 98 40NIPRO MEDICAL EUROPE NV - ITALY :Centro Direzionale Milanofiori, Strada 1 - Palazzo F1, 20090 Assago (Milano), ITALY | T: +39 (0)2 57 50 00 57 | F: +39 (0)2 57 51 81 11NIPRO MEDICAL IVORY COAST :Selmer Lot n°18, Abidjan-Cocody Riviera, Abidjan, Ivory Coast NIPRO MEDICAL EUROPE NV NETHERLANDS :Verlengde Poolseweg 16, 4818 CL Breda, NETHERLANDS | T: +31 (0)76 524 50 99 | F: +31 (0)76 524 46 66NIPRO MEDICAL NIGERIA LTD. :9 Adelabu Close, Off Toyin Street, 100271 Ikeja, Lagos State, NIGERIA | T: +234 (0)802 706 7065NIPRO MEDICAL POLAND SP. Z O.O. :Ul. Panska 73, 00-834 Warszawa, POLAND | T: +48 (0)22 31 47 155 | F: +48 (0)22 31 47 152NIPRO EUROPE PORTUGAL :Avd. Da Liberdade 249, 1° Andar, 1205-143 Lisboa, PORTUGAL | T: +34 (0)91 878 29 21 | F: +34 (0)91 878 28 40NIPRO MEDICAL EUROPE RUSSIAN REPRESENTATIVE OFFICE :12 Krasnopresnenskaya Nab., Office 1407, entrance 6, 123610 Moscow, RUSSIA | T: +7 (0)495 258 1364 | T: +7 (0)495 258 1365NIPRO MEDICAL SENEGAL S.U.A.R.L. : 27 Avenue Georges Pompidou, Dakar, SENEGAL NIPRO MEDICAL D.O.O. BEOGRAD :Bastovanska 68a, 11000 Belgrade, SERBIA | T: +381 (0)11 75 15 578NIPRO MEDICAL SOUTH AFRICA (PTY) LTD :4B Dwyka Street, Stikland Industria, Cape Town, 7530, SOUTH AFRICA | T: + 27 21 949-2635 | F: +27 21 949-2397Unit 20&21, Falcon Lane, Lanseria Business Park, Erf 805 Lanseria Corporate Estate, Pelindaba Rd.,Lanseria Ext. 26, Gauteng, SOUTH AFRICA | T: + 27 11 431 1114 / 26 | F: +27 11 431 1115NIPRO MEDICAL EUROPE NV SPAIN :Poligono Los Frailes n° 93 y 94, Daganzo, 28814 Madrid, SPAIN | T: +34 (0)91 884 5531 | F: +34 (0)91 878 2840NIPRO MEDIKAL SAĞ.HIZ.TIC.LTD.ŞTI. :Mustafa Kemal Mah. 2139, Cad No. 2/17-18-19, 06510 Çankaya-Ankara, TURKEY | T: +90 (0)312 442 21 12 | F: +90 (0)312 442 21 92NIPRO MEDICAL UK LTD. :25 Barnes Wallis Road, Segensworth East, Fareham Hampshire PO15 5TT, UNITED KINGDOM | T: +44 148 985 48 30Nipro Medical Europe : European Headquarters, Blokhuisstraat 42, 2800 Mechelen, Belgium T: +32 (0)15 263 500 | F: +32 (0)15 263 510 |***********************| ENNipro Renal Care is part of Nipro Corporation Japan, a leading global healthcare company established in 1954. With over 28.000 employees worldwide, Nipro serves the Medical Device, Pharmaceutical, and Pharmaceutical Packaging industries.Nipro Renal Care is a global market leader with over 5 decades providing renal solutions for dialysis and dialysis-related treatment. We specialize in developing dialysis machines, water treatment systems, and a comprehensive portfolio of disposable medical equipment.In order to address the needs of patients, healthcare professionals, and procurement managers alike, Nipro Renal Care is driven by innovation and patient safety to offer the highest quality products that optimize time, effort, and costs.BECAUSE EVERY LIFE DESERVES AFFORDABLE CAREB r o -H e m o R O 4 O N E - E N - 08.N o v .19P r o d u c t s a r e c o n t i n u o u s l y u n d e r r e v i e w i n t h e l i g h t o f t e c h n i c a l a d v a n c e m e n t ; t h e a c t u a l s p e c i f i c a t i o n s m a y t h e r e f o r e b e s u b j e c t t o i m p r o v e m e n t o r m o d i f i c a t i o n w i t h o u t n o t i c e . S o m e f e a t u r e s a n d /o r a c c e s s o r i e s d i s p l a y e d a n d d e s c r i b e d c o u l d b e o p t i o n a l o n d i f f e r e n t m a r k e t s . T h e i n f o r m a t i o n p r o v i d e d d o e s n o t c o n s t i t u t e a n o f f e r t o s e l l a n d i s p r o v i d e d f o r m e r e l y i n f o r m a t i o n a l p u r p o s e s . I m a g e s p u b l i s h e d i n t h e p r e s e n t d o c u m e n t a r e s h o w n e x c l u s i v e l y f o r d e m o p u r p o s e s , a r e r e p r e s e n t a t i v e o f t h e p o s s i b l e a p p l i c a t i o n s a n d m i g h t b e a d a p t e d f o r g r a p h i c n e e d s . A l l r i g h t s r e s e r v e d .。
原子与分子物理学报JOURNAL OF ATOMIC AND MOLECULAR PHYSICS第38卷第1期2021年2月Vol. 38 No. 1Feb. 2021分子动力学模拟研究方解石表面润湿性反转机理刘汝敏打康晓东2,辛 晶1,吴 英打柴汝宽3(1.中海油田服务股份有限公司油田生产事业部,天津300459;.中海油研究总院有限责任公司,北京100028 ;3.中国石油大学(北京)油气资源与探测国家重点实验室,北京102249)摘要:利用分子动力学模拟技术从分子尺度探究方解石表面润湿性反转机理.首先,研究方解石表面润 湿性反转过程;而后,从原油分子-方解石表面与原油分子-原油分子/水分子相互作用两个方面系统揭示方解石表面润湿性反转机理.结果:(1)水分子能够驱离方解石表面弱吸附的非极性分子造成润湿性的改变,但不能驱离强吸附的极性分子使润湿性反转难以实现;(2)原油分子极性越强与方解石表面相互作 用越强,极性分子与方解石表面之间主要为静电力,非极性分子与方解石表面之间主要为范德华力;(3)原油分子极性越相近分子之间的相互作用越强,分子极性相差越大分子之间的相互作用越弱.非极性分子之间 主要是范德华力,极性分子之间主要是静电力;(4)原油分子在方解石表面和水分子的共同作用下形成乙酸-毗睫-水-甲苯-己烷的稳定吸附序列.本研究为靶向提高采收率技术的设计与应用提供理论基础. 关键词:分子动力学模拟;方解石表面;原油分子;润湿性;反转机理中图分类号:TE319; TE357 文献标识码:A DOI : 10.19855/j.l000-0364.2021.011006Wettability alteration mechanism of calcite surface :Molecular dynamics simulation studyLIU Ru-Min 1, KANG Xiao-Dong 2, XIN Jing 1, WU Ying 1, CHAI Ru-Kuan 3(1. China Oilfield Services Ltd. COSL Production Optimization , Tianjin 300459 , China ;2. CNOOC Research Institute , Beijing 100028 ,China;3. State key Laboratory of Petroleum Resources and Prospecting , China University of Petroleum ( Beijing ) , Beijing102249 , China )Abstract : Molecular dynamic simulation is used to study the wettability alteration mechanism of calcite surface inmolecular scale. Firstly , the wettability alteration process is investigated with molecular dynamic simulation. Then , the wettability alteration mechanism is explained in two aspects , including crude oil molecules 一 calcitesurface and crude oil molecules 一 crude oil/water molecules interactions. Results show that (1 ) water can dis place the weaker absorbed nonpolar crude oil molecules and result in the wettability alteration , while it can not displace the stronger absorbed polar molecules and calcite surface stays oil - wet ; (2 ) The stronger the polarityof crude oil molecule is , the stronger the interaction between crude oil molecule and calcite surface is. Electro static force contributes most in polar molecule 一 calcite surface interactions ,while van der Waals force is moreimportant in non 一 polar molecule 一 calcite surface interactions ; ( 3 ) The smaller the polarity difference of the crude oil molecules ,the stronger the interaction among molecules ,vice versa. The van der Waals force contrib utes most among non 一 polar molecules interactions ; the electrostatic force plays a major role among polar mole cules interactions ; (4) The stable adsorption sequence of acetic acid 一 pyridine 一 water 一 toluene 一 hexane isformed with the combination influence of water molecules and calcite surfaces. This study provides a theoretical basis for the design and application of targeted enhanced oil recovery technology.Key words : Molecular dynamics simulation ; Calcite surface ; Crude oil molecule ; Wettability alteration mechanism收稿日期:2020-04-23基金项目:国家科技重大专项(大型油气田及煤层气开发2016ZX05025)作者简介:刘汝敏(1976—)女,高级工程师,主要从事油气田开发开采研究工作• E-mail : **************.cn第38卷原子与分子物理学报第1期1引言碳酸盐岩油气田是全球油气资源的重要组成部分,已发现的碳酸盐岩油藏储量约占世界油藏总储量的50%左右,产量占60%左右[1-3L碳酸盐岩油藏采收率普遍较低,润湿性作为储层基本性质对油藏采收率具有重要影响⑷•当前油气田开发/提高采收率领域关于润湿性的研究多集中于润湿角法[5'6〕、渗吸与排驱法"8〕等宏观物理实验方法,其具体微观作用机理尚不明朗,这也直接阻碍了与润湿性相关提高采收率技术的发展与应用•工程应用倒逼理论研究,非常有必要从分子尺度入手,详细探究碳酸盐岩油藏润湿性反转机理[9_11近年,分子动力学模拟被广泛的应用于矿物表面润湿性相关研究[12_15].与物理实验相比,分子动力学模拟可以从分子尺度研究矿物表面特性以及有机小分子吸附、解吸的作用特征进而解释润湿性改变机理•Van Duin[16'17]和Zhong】18〕研究4种原油分子在云母、石英和方解石表面的吸附,面从湿油湿的建立两步的润湿性反转机理.Murgich[19]研究了沥青质和胶质在高岭石表面的吸附过程中的分子间相互作用,提出沥青和胶质主要受范德华力作用吸附于高岭石表面.Liu[20]和Yuan®]运用分子动力学模拟研究油湿性石英/方解石表面的形成并分析表面活性剂造成表面润湿性反转的机理.当前关于矿物表面润湿性的分子动力学模拟研究多重矿物面与油分子的应了油分子之间的相互作用.此外,现有研究过分强调某一类分子吸附的作用而忽略原油整体性特征.因此,当前研究并不能全面的解释方解石表面润湿性反转机理.本文利用分子动力学模拟研究乙酸、毗睫、甲苯和己烷等4种不同极性的有机小分子作为代油分子方石润湿机理.先,分子动力学模拟研究方解石表面润湿性反转过程•而后,从原油分子-方解石表面的相互作用和体系内部分子之间的相互作用等两个方面探究润湿性反转机理•本文研究在分子尺度阐释方石面润湿与机理,酸盐岩储层润湿性的针对性调整奠定理论基础.2模型与方法2.1吸附体系模型利用Materials Studio软件中Amorphous Cell 模块和Forcite模块完成模拟体系的构建以及动力学弛豫•利用COMPASS力场血,3〕描述原子间相互作用,作为第一个从头算力场已被证明能够准确的预测有机和无机物质之间的相互作用,势能函数如下:昭=I E b()+£E e(0)+工化(°)+ bond angle dihedralI E(,,)+£E^()+E“e+E”』”cross oui—of—plane(1)式中,前5项为成键相互作用,分别表示键长、键角、二面角、交叉项和离平面的势能函数,b, 0,,分别为键长、键角、二面角和离平面振动的角度.E eie=£如为静电相互作用,£城=W r i.ji怡G「3G门相互用.Ti i Ti i其中,i和j分别代表不同的原子;g为原子电荷; r为不同原子距离;£为势阱深度.采用周期性边界平板模型,建立水分子单元-混合原油分子单元-方解石表面三元体系模型、单一原油分子单元-方解石表面、单一原油分子单元-水分子单元和单一原油分子单元-单一原油分子元等二元体系,分用研究方石面润湿性反转过程、原油分子与方解石表面相互作用、原油分子与原油分子/水分子之间的相互作用.其中,选取最为稳定的CaCO3{104}表面[24-26]进行润湿性相关研究,建立尺寸为2.934nm x2.920 nm X1.50nm的CaCO3{104}表面,如图1a.混合原油分子单元包含己烷分子15个、甲苯分子14、分子16和乙酸分子22,元度与CaCO3{104}表面相匹配,如图1b.单一原油分子单元分别包含乙酸分子89个、毗睫分子67个、甲苯分子58个和己烷分子62个,以保持体系密度为0.75g/cm3.水分子单元包含400个水分子,单元大小与CaCO3{104}表面相匹配,如图1c.2.2分子动力学模拟采用NVT系综对体系进行分子动力学模拟,分子初始速度按照Maxwell-Boltzmann分布随机产生,运用Velocity Verlet[27]算法求解牛顿运动方程;体系温度设置为298K,采用Andersen恒温第38卷刘汝敏,等:分子动力学模拟研究方解石表面润湿性反转机理第1期(a)(b)构型图:(a)CaC03{104}表面;(b)混合原油分子单元;(c)水分子单元图1研究单元构型图Fig.1Configurations of system units(c)模式3;长程静电作用力计算采用Ewald求和方法旳,范德华相互作用计算采用Atom Based方法网,设 1.2nm,能以外的分子间相互作用能按平均密方法进行校正;拟面原子自,固定其子持结构•此外,为避维周期性边界引起的周期性晶胞相互作用,在的顶部4nm厚的.模拟步长为1.0fs,二元、三元体系进行10ns的分子学模拟,采用最后1ns的统计平均值来计算相关参量•3结果与讨论3・1润湿性反转过程为探究方解石表面润湿性反转机理,构建水分子单元-混合原油分子单元-方石表面三元行研究,图2a和图2b分元体系的初始和平衡构型•对比图2a和图2b可得:部分原油分子已分子驱离方解石表面润湿性的部分反转•在方解石表面的吸引作用下,水分子已功穿油的甲苯和己烷部分,上述分子分子驱离方解石表面而位于.其,甲苯与在微弱的互溶距方解石表面相,烷与水分子完全分分油水体系最外层•,分子继续向方石面分子溶分子方解石表面;最终,水分子并不能稳的乙酸分子方解石表面依持一的油湿性,润湿生的•3・2方解石表面润湿性反转机理方解石表面、原油分子和水分子共同参与原油分子在方解石表面的用,直接方解石表面润湿•因此有必要详细研究原图2原油分子单元-水分子单元-方解石三元体系构Fig.2Configurations of the crude oil unit-water unit -calcite unit ternary system(a)初始(b)平衡油分子-方解石表面、原油分子-原油分子/水分子的相互作用,系统、准确的方解石表面润湿性的机理•3.2.1原油分子与方解石表面相互作用图3油分子单元-方石表面二元体系的平衡构型•可,4种不同极性的油分子在方石界面的在的异.由图3a和图3b可:极性分子(乙酸、毗)在方解石表面形成排列紧密、规则的:吸,其中乙酸分子在方解石表面自组分子层,分子排列较双•由图3c和图3d可:非极性分子(甲苯、己烷)在方解石表面,其有第排列较为规则,方解石表面分布越来越乱.此外,:甲苯和己烷等非极性分子与方解石表面的距大于乙酸和等极分子,极油分子与方石面的相互用极分子.第38卷原子与分子物理学报第1期图3油分子单元-方解石表面的平衡构型Fig.3Equilibrium configurations of crude oil unit-calcite surface binary system不极油分子在方石面的分,建立各原油分子沿z方的相对浓分,如图4.由图4可:极性原油分子的吸附峰主要位于0.144-1.326nm,其中乙酸主要吸附峰位于0.144-0.425nm,卩比睫主要分布于0.197-0.385nm.非极性分子距离方解石表面的距离明显较远,甲苯分0.263-1.510nm,己烷分布于0.230-1.739nm.说明方解石表面对不同极油分子的在较大的差异,分子极性越强与方解石表面的相互作用越强,距离方解石表面越近.,.距离表面较远.uolallu①。
大学化学Univ. Chem. 2022,37 (12), 2209053 (1 of 8)•专题• doi: 10.3866/PKU.DXHX202209053 二氧化碳的捕获和转化——第54届国际化学奥林匹克试题第3题解析郑捷1,张振杰2,程方益2,李恺3,王颖霞1,*1北京大学化学与分子工程学院,北京1008712南开大学化学学院,天津3000713郑州大学化学学院,郑州450001摘要:二氧化碳是引起温室效应的“罪魁祸首”,其吸收和转化一直是科学研究的热点之一。
第54届国际化学奥林匹克试题第3题围绕CO2的处理,从NaOH碱液吸收CO2出发,结合H2辅助的电化学循环实现吸收剂重生和高纯CO2回收、新型类沸石咪唑骨架多孔材料的结构和催化CO2转化,讲述了一个从经典到前沿、从普通的溶液体系到新型固体材料应用而解决科学问题的故事。
藉此,引导年轻的学子关注气候变化,了解基础化学原理在解决环境问题中的重要作用,鼓励学生打好学科基础,投身探索和发展新方法和创制新材料的研究之中。
关键词:二氧化碳;捕获和转化;类沸石咪唑骨架;催化;电化学中图分类号:G64;O6Capture and Transformation of Carbon Dioxide: Analysis on Problem 3 of the 54th International Chemistry OlympiadJie Zheng 1, Zhenjie Zhang 2, Fangyi Cheng 2, Kai Li 3, Yingxia Wang 1,*1 College of Chemistry and Molecular Engineering, Peking University, Beijing 100871, China.2 College of Chemistry, Nankai University, Tianjin 300071, China.3 College of Chemistry, Zhengzhou University, Zhengzhou 450001, China.Abstract:Carbon dioxide is considered as the “culprit” of the greenhouse effect, and the study on the capture and transformation of carbon dioxide has been being one of the hot topics of scientific research. The problem 3 of the 54th International Chemistry Olympiad focused on this topic: starting from the absorption of CO2 by NaOH solution, then presenting the development of the electrochemical cycle assisted by H2 to realize the regeneration of absorbent and the recovery of CO2with high-purity, and finally introducing the structure of new porous materials with zeolite-like imidazolate framework and their application in catalytic conversion of CO2. A story was told about solving the problem by the strategy from conventional mothed to frontier research, from ordinary solution systems to new solid materials. The young students are expected to pay attention to the climate change, to have a comprehensive understanding of the fundamental chemical principles in solving environmental problems, and to devote themselves to developing new methods and materials in the field.Key Words: Carbon dioxide; Capture and transformation; Zeolitic imidazolate framework; Catalysis;Electrochemistry收稿:2022-09-20;录用:2022-10-08;网络发表:2022-10-25*通讯作者,Email:**************.cn气候变化是人类面临的最严峻的挑战之一。
Cite this:Chem.Soc.Rev .,2012,41,7938–7961Defect-related luminescent materials:synthesis,emission properties and applicationsCuimiao Zhang ab and Jun Lin*aReceived 25th March 2012DOI:10.1039/c2cs35215jLuminescent materials have found a wide variety of applications,including information displays,lighting,X-ray intensification and scintillation,and so on.Therefore,much effort has been devoted to exploring novel luminescent materials so far.In the past decade,defect-related luminescent materials have inspired intensive research efforts in their own right.This kind of luminescent material can be basically classified into silica-based materials,phosphate systems,metal oxides,BCNO phosphors,and carbon-based materials.These materials combine several favourable attributes of traditional commercially available phosphors,which are stable,efficient,and less toxic,being free of the burdens of intrinsic toxicity or elemental scarcity and the need for stringent,intricate,tedious,costly,or inefficient preparation steps.Defect-related luminescentmaterials can be produced inexpensively and on a large scale by many approaches,such as sol–gel process,hydro(solvo)thermal reaction,hydrolysis methods,and electrochemical methods.This review article highlights the recent advances in the chemical synthesis and luminescent properties of the defect-related materials,together with their control and tuning,and emission mechanisms (solid state physics).We also speculate on their future and discuss potential developments for their applications in lighting and biomedical fields.1.IntroductionLuminescent materials (or phosphors)are generally characterized by the emission of light in the visible range but can also be in other spectral regions (such as ultraviolet or infrared)with energy beyond thermal equilibrium.1,2The ever-growing demand for advanced luminescent materials has motivated scientific andaState Key Laboratory of Rare Earth Resources Utilization,Changchun Institute of Applied Chemistry,Chinese Academy of Sciences,Changchun 130022,P.R.China.E-mail:jlin@;Fax:(+86)431-85698041bCollege of Chemistry and Environmental Science,Hebei University,Baoding 071002,P.R.China.E-mail:cuimiaozhang@Cuimiao ZhangCuimiao Zhang was born in Hebei,China,in 1980.She received her BS (2004)in chemistry from Hebei Univer-sity.Then she has been a grad-uate student in Jun Lin’s group at Changchun Institute of Applied Chemistry (CIAC),Chinese Academy of Sciences,and received a PhD degree in 2010.After graduation,she has been working as a research fellow in Nanyang Technolo-gical University (Singapore,2010–2012).Her current research interests include thesynthesis of environmentally-friendly luminescence materials and their bioapplication.She came back to China in 2012,and since then has been working as an assistant professor in Hebei University.Jun LinJun Lin was born in Chang-chun,China,in 1966.He received BS and MS degrees in inorganic chemistry from Jilin University,China,in 1989and 1992,respectively,and a PhD degree (inorganic chemistry)from the Chang-chun Institute of Applied Chemistry (CIAC),Chinese Academy of Sciences,in 1995.Then he went to CityU (HK,1996),INM (Germany,1997),VCU and UNO (USA,1998–1999)working as a postdoctor.He came back toChina in 2000,and since then has been working as a professor in CIAC.His research interests include luminescent materials and multifunctional composite materials together with their applica-tions in display,lighting and biomedical fields.Chem Soc RevDynamic Article Links/csrCRITICAL REVIEWP u b l i s h e d o n 27 S e p t e m b e r 2012. D o w n l o a d e d o n 06/01/2015 10:49:26.View Article Online / Journal Homepage / Table of Contents for this issuetechnological efforts dedicated to improving existing phos-phors and to developing new effective luminescent materials.3Generally,inorganic luminescent materials can be classified into two groups:metal-activator based and non-activator based luminescent materials.The first case is represented by transitions between energy levels of metal activator ions containing the rare earth and/or transition metal ions (e.g.f–f transitions of Eu 3+in Y 2O 3:Eu 3+)4–7or complex ions (e.g.the charge-transfer transition on [WO 4]2Àin CaWO 4).8,9These kinds of luminescent materials are often expensive and contain non-environmentally friendly elements,such as Ag (in ZnS:Ag +)and lanthanides.1–15On the other hand,it is necessary for most metal-activator-based phosphors to be excited by short-wavelength ultraviolet (UV)light for operation,which results in the extensive use of a mercury vapor plasma in fluorescent lighting products.1,10The excess usage of mercury vapor will give rise to environmental contamination and technical difficulties.The other group of luminescent materials consists of semiconductors and defect-related materials.For most semiconductors,the luminescence normally results from band-to-band excitation between impurity states within the bandgap.However,some serious intrinsic toxicity and potential environmental hazards associated with many of these semiconductors are critically pronounced,which have limited their applications.For the defect-related luminescent materials,although the roots can be traced to 1986,16they have had a remarkable growth since Sailor et al.reported the white phosphors from a silicate-carboxylate sol–gel precursor.17Since then,the emerging defect-related luminescent materials,which do not contain any transition metal or rare earth activators,appear to be promising alternatives to traditional phosphors in many applications because of their advantages of low toxicity,stability,tunable emission color,and low cost.17–30Although the origins of photoluminescence (PL)are not yet entirely understood in defect-related materials,there is mounting evidence that emission arises from the special defects.Typically,the defects in these kind of materials contain vacancies,impurities,radical impurities,donor–acceptor pairs,etc.,22,27,31–33which may arouse charge imbalances at these defect sites.The charge imbalances must be rectified by localization of electrons and electron holes or give rise to impurity states within the bandgap.Therefore,the defect sites are apparently the precursors for various centers containing the emission center for defect-related luminescent materials and impart them with excellent photo-luminescent emission.On the other hand,in modern chemistry and materials science,there have been tremendous developments in the synthetic control of size,shape,and composition,thus allowing the tailoring of their properties.34–40Therefore,the synthesis methods have been inten-sively pursued for their technological and fundamental scientific importance.41,42Among them,the luminescence properties of defect-related luminescent materials can also be influenced by their phase,surface chemistry,size distribution,morphology and/or porosity.43–45Thus,the rational control over these factors has become an important research issue in recent years.46So far,valuable explorations have been carried out based on soft chemical synthetic strategies [such as Pechini sol–gel (PSG)method,hydro-thermal process,and so on]to luminescent materials as well as controlled morphologies,formation,and luminescence properties.As we know,the tremendous recent advances in functionalized nanomaterials with distinct fluorescent properties,47–54mesoporous properties,55and biocompatability 56,57have received considerable attention in the past decades,since nanomaterials provide a new platform for biomedical applications such as drug delivery,bio-separation,fluorescent labeling,58diagnosis and treatment of disease.59–68During the past decades,the use of semiconductor fluorescent nanocrystals or quantum dots has notably extended the scope of possible biological applications (fluorescent probes,labeling and tracking,etc.)due to their high quantum yield and high photostability.69,70However,their disadvantages of blinking,potential cytotoxicity in vivo ,and complex functionalization strategies have limited their use.Additionally,some serious problems of photobleaching and quenching of fluorescent organic molecules are critically pronounced,which have seriously limited their applications in biomedical areas.60,71,72In contrast to traditional fluorescent materials in biological areas such as organic dyes and quantum dots,the novel defect-related luminescent nanomaterials may be promising fluorescent materials in biological fields due to their good optical properties,high chemical stability,and low toxicity.29,30,73–77Especially,multifunctional defect-related materials with excellent luminescent,structural,and/or surface properties seem to be ideal systems for biomedical applications.To date,many recent reports have shown that multifunctional defect-related materials,as the most efficient fluorescent materials,can be used for the intracellular imaging,drug delivery,and so on.26,29,30,78In this review article,we mainly focus on the recent progress in various chemical syntheses and luminescent properties of defect-related luminescent materials,together with their tuning and possible emission mechanisms as well as their applications in lighting,display,and biological fields (including bioimaging and tracking in drug delivery systems),based on our recent efforts and those of others in this area.Moreover,we hope to inspire research into the origins of the unique properties of this emergent class of novel luminescent materials and to encourage their exploration in a multitude of exciting areas from lighting to display and medical diagnostics.2.Synthetic methodsGenerally,as the defect sites are mainly created in the preparing process,the luminescent properties of defect-related materials seem to be dominated by the preparation methods.In recent years,a large number of synthetic methods have been developed for generating defect-related luminescent materials.These methods can be divided into several categories:sol–gel method,hydro-(solvo)thermal reaction,hydrolysis method,electrospinning process,sonochemical synthesis,chemical vapor deposition (CVD),and so on.Typically,the common features of all these methods of synthesis are the need of heat treatments (high or low temperature)and/or organic groups (surfactants,organic additives,templates,etc.).2.1.Sol–gel methodUndoubtedly,the sol–gel technique is one of the most well-known soft solution processes,which can be generally divided into three types:sol–gel route based on the hydrolysis andP u b l i s h e d o n 27 S e p t e m b e r 2012. D o w n l o a d e d o n 06/01/2015 10:49:26.condensation of molecular precursors,gelation route based on concentration of aqueous solutions containing metal-chelates (called ‘‘chelate gel’’route),and polymerizable complex route (named Pechini-type sol–gel process).79–81Commonly,silicon alkoxides,metal alkoxides,or organic additives [such as citric acid and polyethylene glycol (PEG)]are employed in the sol–gel process,following heat treatment to remove the organic groups produced by alcoholysis of alkoxides or organic additives.Interestingly,it is also possible to utilize some defects (such as carbon impurities and vacancies)as emission centers to get novel defect-related luminescent materials.17,79It has been reported that sol–gel-derived SiO 2-based materials,including silica gels (xerogels or aerogels),28,82porous silica,83multicomponent silica-based oxide materials,84silicate-carboxylate,17and inorganic–organic hybrids,18,85all show strong luminescence from the blue to red spectral region,17–19,27and even ultraviolet photoluminescence.83They can potentially be used as environ-mentally friendly luminescent materials without expensive or toxic metal elements as activators.Pechini-type sol–gel process (PSG),which uses common metal salts as precursors,citric acid as a chelating ligand of metal ions and polyhydroxy alcohol as a cross-linking agent to form a polymeric resin on the molecular level,can reduce segregation of particles and ensure compositional homogene-ity.These advantages can overcome most of the difficulties and disadvantages that frequently occur in the alkoxide-based sol–gel process (high cost,fast hydrolysis rate,and so on).Pechini-type sol–gel method followed by heat treatment at moderate temperature can remove organic additives and generate a pure phase of multiple components (Scheme 1).79During this annealing process,hydrocarbon residues cannot be removed completely,which may induce carbon impurities and form other kinds of defects in the host lattice (such as the oxygen defects).It is possible to utilize these defects as emission centers to obtain novel phosphors without rare earth or transition metal ions as activators.In the past several years,our group has synthesized various kinds of highly efficient defect-related phosphors by PSG.We found that the PSG process-derived BPO 4exhibits a weak purple-colored emission under UV irradiation caused by the carbon impurities.Doping it with alkaline earth metal and alkali metal ions 86,87or mixing with SiO 2or Al 2O 388produced a series of BPO 4-based materials that emit an efficient bluish-white light with a quantum yield more than 31%,which is induced by carbon impurities,peroxyl radicals,and/or oxygen vacancies defects,respectively.Besides BPO 4-based phosphors,the same phenomena were also observed in Al 2O 3,89ZrO 2,43and silica/apatite composite 90prepared by PSG process (Fig.1),whichcan also show efficient,stable,and/or tunable luminescence.In addition,some titanates (CaTiO 3,SrTiO 3,and BaTiO 3)exhibiting an intense photoluminescence were also prepared by PSG method followed by calcination at 300–4001C.91,92For the sol–gel method,the annealing procedure (temperature and annealing time)is the key step in the synthesis process,which can seriously affect the types and quantities of the defects in the materials and their luminescent properties.2.2.Hydro(solvo)thermal reactionIt is well known that the hydrothermal method is a typical solution-based method that exploits water or organic solvents under certain temperatures and pressures,and has received much attention.93Over the past decade,various micro-and/or nano-crystals,which exhibit many interesting shape-and size-dependent phenomena and properties,have been synthesized by the hydrothermal process and extensively investigated for both their scientific and technological applications.94–99Especially,the water-based systems with environmentally acceptable and relatively low cost advantages provide a relatively green chemical alternative to the preparation of various inorganic materials.38,100–102To date,different defect-related luminescentScheme 1Basic principle of Pechini sol–gel process to synthesize phosphors (reproduced with permission from ref.79,copyright 2007,American Chemical Society).Fig.1Representative shapes of defect-related luminescent materials obtained by Pechini-type sol–gel process.SEM images of BPO 4:6%Li +(a),Al 2O 3(b),ZrO 2(c)(reproduced with permission from ref.87,89and 43,copyright 2009,2008,and 2007,American Chemical Society),and silica/apatite composite (d)(reproduced with permission from ref.90,copyright 2011,Royal Society of Chemistry).P u b l i s h e d o n 27 S e p t e m b e r 2012. D o w n l o a d e d o n 06/01/2015 10:49:26.materials have been successfully prepared by the simple hydro-thermal method.For instance,based on the hydrothermal treatment at designated reaction conditions (such as reaction temperature and time,chelating ligands,organic additives,etc.),a systematic study has been carried out to investigate the controlled formation of a series of apatite structure micro-/nano-crystals with environmentally friendly defect-related luminescent properties.103–106The general synthetic methodology for the apatite structures is shown in the top of Fig.2.As an example,the hydroxyapatite (HAp)phosphors via hydrothermal process [trisodium citrate as chelating ligands and hexadecyltri-methylammonium bromide (CTAB)as surfactants]with narrow size distribution and novel morphologies and architectures,such as nanorods,nanowires,nanoparticles,microspheres,micro-flowers,microsheets,and microspheres (Fig.2a–f),are of special significance in understanding the growth behavior and influence on defect-related luminescent properties.103Moreover,there are several important key factors for final shapes of HAp nano/microcrystals,which contains pH values,organic additive (CTAB),and trisodium citrate (Fig.2).107,108The metal-chelating trisodium citrate ligands can not only affect the morphology of the sample,but also the key factor for the defect-related luminescent properties.During the crystal growth of HAp,the trisodium citrate can slow down the nucleation and subsequent crystal growth of HAp particles and change the relative surface energy of different crystal facets,which results in the formation of different HAp structures.109On the other hand,the electron paramagnetic resonance (EPR)results indicates that the lumi-nescent-related paramagnetic defects (CO 2 À)can be induced by trisodium citrate during the hydrothermal process.Under the high pressure and thermal process,bond cleavages can occur in some citrate anions,which result in R–C and CO 2 À.Small amounts of CO 2 Àradicals resulting from the bond cleavages are trapped by the already formed hydroxyapatite lattice or interstitial positions.The residual fragmented bonds (CO 2 À)are apparently the precursors for various centers,such as luminescent centers.Apart from the investigation of the HAp nano/microcrystals,we also utilized a similar method to synthesize other apatite structures with defect-related luminescent properties,such as calcium fluorapatite (FAP)nanorods,strontium hydroxyapatite (SrHAp)with various morphologies (nanorods and architecture microspheres).Fig.2g–i shows the representative morpho-logies of FAP and SrHAp products.We found that the molar ratio of metal ions and chelating ligands,reaction time,and acetone treatment are also critical to obtain the apatite structures.Especially,multifunctional strontium hydroxy-apatite nanorods with luminescent and mesoporous properties can be easily synthesized at a low temperature,and have good biocompatibility,stability,nontoxicty,and water-soluble properties.106In addition,the defect-related fluoride materials prepared by the solvothermal method were also reported.97,110The as-obtained alkaline earth metal fluoride (CaF 2,SrF 2,BaF 2)nanocrystals based on the solvothermal method exhibit a narrow size distribution,and can be well dispersed in nonpolar solvents.The colloidal solutions of these three fluoride nano-crystals dispersed in cyclohexane present a strong emissionFig.2The general synthetic methodology for a series of apatite nano/microstructures by hydrothermal method and the typical methodologies for defect-related luminescent apatite structures by hydrothermal method.Typical TEM and SEM images of calcium hydroxyapatite (a–f)(reproduced with permission from ref.103,copyright 2009,American Chemical Society),SEM images of calcium fluorapatite (g)(reproduced with permission from ref.105,copyright 2010,Royal Society of Chemistry),and strontium hydroxyapatite (h,i)(reproduced with permission from ref.106and 104,copyright 2010,2009,Elsevier and American Chemical Society)with multiform shapes.P u b l i s h e d o n 27 S e p t e m b e r 2012. D o w n l o a d e d o n 06/01/2015 10:49:26.band around 400nm in the PL spectra.97In addition,a series of well-dispersed KRE 3F 10(RE =rare earth:Sm–Lu,Y)colloidal nanocrystals with a rich variety of morphologies,such as hexagonal nanoplates,nanocubes and nanoparticles have been synthesized by a facile solvothermal route.The as-prepared nanocrystals are highly crystalline and can be well dispersed in nonpolar solvents such as cyclohexane and chloroform to form stable and clear colloids,which all display self-activated luminescence.1102.3.Hydrolysis methodIt is well known that the hydrolysis method is often used to prepare hydroxide and oxide materials using alkoxides as precursors.Over the past decade,monodisperse nano-/microspheres,which exhibit tunable or size-dependent photoluminescent properties,have been synthesized by the hydrolysis method and extensively investigated.111–115Our group has reported the simple synthesis of nearly monodisperse zirconia spheres (ZrO 2)with defect-related tunable luminescent properties (Fig.3a and b)by the controlled hydrolysis of zirconium butoxide in ethanol,followed by heat treatment in air at low temperature from 300to 5001C.106,116In addition,the well-known Sto ber method,117based on hydro-lysis of tetraethylorthosilicate (TEOS)in an alcohol medium in the presence of water and ammonia,has been extensively employed to prepare the monodisperse silica (SiO 2)spheres with different sizes by a modified procedure (Fig.3).These monodisperse SiO 2spheres could be further annealed at low temperature (generally less than 6001C),and exhibited bright,stable,and tunable defect-related luminescence.111,113Apart from the methodology presented by Sto ber and modified Sto ber methods,other hydrolysis-related strategies have recently been developed,based mainly on reverse microemulsions using a stable and macroscopically isotropic dispersion of a surfactant and water in a hydrocarbon (Fig.3c),114,118,119or on direct micelles as templates.120,1212.4.Electrospinning processThe electrospinning technique was developed for the synthesis of one-dimensional (1D)nanomaterials.122–128During the synthesis process,the as-synthesized 1D precursor needs to be annealed to remove the organic additives.Moreover,it is also possible to form some carbon-related impurities induced by residual organic additives and other oxygen-related defects as emission centers during the annealing process.Recently,the electrospinning method was employed to prepare multifunctional silica fibers,which possess irregular porous structure,and display fiber-like morphology with dimensions of several hundred nanometers in width and several millimeters in length (Fig.4).129Furthermore,the as-obtained silica fibers exhibit an intense broad bluish emission,which might be attributed to impurities and/or defects in the silica fibers.In addition,Qiu and co-workers reported tunable emission of BCNO nanoparticle-embedded polymer electrospun nano-fibers.130Firstly,BCNO nanoparticles were prepared by a low-temperature method.Then,the BCNO nanoparticle-embedded polymer electrospun nanofibers were synthesized by an electrospinning process using synthesized BCNO phosphors as raw materials.Photoluminescence properties of these nanofibers indicate that the emission can be readily tuned by adjusting the C concentration in the BCNO phosphors.Fig.3Typical SEM images for unannealed ZrO 2(a),heat-treated ZrO 2spheres (b)(reproduced with permission from ref.112,copyright 2009,American Chemical Society),and (c–f)SiO 2spheres with different size (reproduced with permission from ref.114,copyright 2010,Elsevier).Fig.4Typical SEM images of the as-formed precursor (a)and porous silica fibers annealed at 6001C (b).The possible formation process of the porous structures in silica fibers (c)(reproduced with permission from ref.129,copyright 2010,Wiley).P u b l i s h e d o n 27 S e p t e m b e r 2012. D o w n l o a d e d o n 06/01/2015 10:49:26.2.5.Sonochemical synthesisThe sonochemical method has been widely used to prepare a variety of nanostructured materials.131,132During the sonication process,propagation of pressure waves is intense enough to cause the formation,growth and implosive collapse of bubbles in liquid medium.These bubbles generate localized hotspots,which exhibit extreme temperatures,pressure and high cooling rates.133Sonochemical effects can primarily drive a variety of chemical reactions such as oxidation,reduction,and so on.During this special process,some defects can also be formed as a result of localized hotspots.Recently,Uchino and co-workers 134synthesized luminescent silica crystals without luminescent activator ions via a sonochemical reduction route.The neutral oxygen vacancy or the F center induced by the sonochemical process might be the emission centers and give a broad visible PL band peaking at B 500nm under UV irradiation.The sonochemical reduction of TEOS by a colloidal solution of sodium performed by Gedanken’s group led to the formation of silicon.135Ultrasound-induced reduction was further applied to a system with silicon alkoxides and colloidal sodium to prepare luminescent silicon nanoparticles.2.6.Chemical vapor depositionThe chemical vapor deposition (CVD)system is believed as an important synthesis method with several advantages,such as relatively low temperature and low cost,adaptable to a wide variety of structures,rapid growth,and direct growth on a large number of substrates.136Controlling the different reaction conditions (such as substrate temperature,pressure,reactant composition,reactant pre-treatment,supply rates,etc.),a number of forms of CVD are in wide use,including atmospheric pressure CVD (APCVD),aerosol-assisted CVD (AACVD),plasma-enhanced CVD (PECVD),and so on.137–139So far,a large number of compounds,including oxides,sulfides,semiconduc-tors,carbon-based materials,etc.,have been grown by these CVD methods.140Among them,some defect-related luminescent materials can also be obtained by this kind of method.Previously,off-stoichiometric silicon oxide (SiO x ,x o 2)thin films can often be synthesized via chemical vapor deposition.141,142In addition,Becher’s group reported the fluorescence and polarization spectroscopy of single silicon vacancy centers in heteroepitaxial nanodiamonds on iridium using microwave plasma chemical vapor deposition.143Yang and co-workers have successfully fabricated the In 2O 3–ZnO one-dimensional nanosized heterostructures constructed by In 2O 3quadrangular columns and ZnO hexagonal disks by thermal chemical vapor transport.144Besides the above methods,multistep heat treatment,145thermal decomposition,16flame spray pyrolysis,146microwave irradiation method,147etc.can also be employed to prepare the defect-related luminescent materials.3.Classification and optical propertiesDefect-related luminescent materials can be classified intosilica-based materials,phosphate systems,metal oxides,BCNO phosphors,and carbon-based materials,etc .Here we will elucidate the luminescent properties together with theircontrol and tuning,and emission mechanisms (solid state physics)of these materials.3.1.Silica and silica-based materialsEarlier defect-related luminescent materials were mainly based upon silica and silica-based materials,including silicate-carboxylate,17SiO 2glass,18,22SiO 2gels,27,28SiO 2spheres,111,114organic/inorganic hybrid silicones,23–25silica nanotubes,148molecular sieves,31,149etc.150–156As the most promising materials for environmentally friendly phosphors,these kinds of luminescent materials have been the focus of research efforts since the pioneering work of Sailor and co-workers.17,121It has been reported that a kind of white phosphor with high emissive broadband spectra (Fig.5a)(emission maximum between 450and 600nm)can be synthesized from a sol–gel precursor and a variety of organic carboxylic acid with a low heat treatment.The PL quantum yield of these materials ranged from 20%to 45%under UV (365nm)excitation with PL lifetime less than 10ns.In addition,it is worth pointing out that the bright white photoluminescence was first attributed to carbon defect centers and the detailed scheme of the carbon substitutional defect for Si as the luminescent species in the lattice is shown in Fig.5b.Apart from this,silica gels have been also extensively investigated as defect-related phosphors.Among them,silica aerogels,which are well-known to show photoluminescence generally from the blue to red spectral regions,exhibited several structural defects advantageous to photoluminescent properties,such as a non-bridged oxygen hole center (NBOHC)(described as SiOH -SiO + H;this defect was connected with bands at 1.8and 1.9eV),151–153peroxy linkage (POL)(labeled as ROO ,where R represents an unspecified radical or part of the structure),154and E 0center (R Si )on the basis of the basic emission characteristic band at 2.2eV in the PL spectra.152,156Inaddition,Hinic’s group has reported PL spectra measured Fig.5Optical characterization of SiO 2-based materials.Emission spectra (337nm excitation at 298K)of sol–gel-prepared SiO 2-based phosphors (a)and a scheme of the carbon substitutional defect for Si as the luminescent species in the lattice (b)(reproduced with permission from ref.17,copyright 1997,).Emission spectra of monodisperse SiO 2spheres excited at 300nm (c)and the corresponding photographs (d)under a 365nm lamp (reproduced with permission from ref.111,copyright 2006,American Chemical Society).P u b l i s h e d o n 27 S e p t e m b e r 2012. D o w n l o a d e d o n 06/01/2015 10:49:26.。