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A survey of hard spectrum ROSAT sources 2 optical identification of hard sources

A survey of hard spectrum ROSAT sources 2 optical identification of hard sources
A survey of hard spectrum ROSAT sources 2 optical identification of hard sources

a r X i v :a s t r o -p h /0103055v 1 3 M a r 2001

Mon.Not.R.Astron.Soc.000,000–000(0000)Printed 1February 2008

(MN L A T E X style ?le v1.4)

A Survey of hard spectrum ROSAT sources 2:optical

identi?cation of hard sources

M.J.Page 1,J.P.D.Mittaz 1,F.J.Carrera 1,2

1Mullard Space Science Laboratory,University College London,Holmbury St Mary,Dorking,Surrey RH56NT,UK.2Instituto

de F′?sica de Cantabria (Consejo Superior de Investigaciones Cient′??cas–Universidad de Cantabria),39005Santander,Spain.

ABSTRACT

We have surveyed 188ROSAT PSPC ?elds for X–ray sources with hard spectra

(α<0.5);such sources must be major contributors to the X–ray background at faint ?uxes.In this paper we present optical identi?cations for 62of these sources:28AGN which show broad lines in their optical spectra (BLAGN),13narrow emission line galaxies (NELGs),5galaxies with no visible emission lines,8clusters and 8Galactic stars.

The BLAGN,NELGs and galaxies have similar distributions of X–ray ?ux and spectra.Their ROSAT spectra are consistent with their being AGN obscured by columns of 20.5

We propose that BLAGN are likely to constitute a signi?cant fraction of the faint,hard,0.5-2keV population and could be important to reproducing the shape of the X–ray background,because they are the most numerous type of object in our sample (comprising almost half the identi?ed sources),and because all our high redshift (z >1)identi?ed hard sources have broad lines.

1

INTRODUCTION

The origin of most of the X–ray emission in the Uni-verse is still unknown because the sources that produce most of the >2keV X–ray background (XRB)are still to be resolved.ROSAT surveys have succeeded in resolv-ing ~80%of the 1-2keV XRB into individual sources (Hasinger et al.1998),and optical identi?cation and X–ray spectroscopy has been possible for brighter sources which produce ~40%of the 1-2keV background.The majority of these sources are broad line AGN (hereafter BLAGN),and at faint ?uxes narrow emission line galaxies (hereafter NELGs,McHardy et al.1998);Schmidt et al.(1998)argued that the NELGs are also AGN,but with low luminosity or obscured broad line regions.On aver-age,faint NELGs have harder X–ray spectra (f ν∝ν?αwith α~0.5,Romero-Colmenero et al.1996,Almaini et al.1996)than the broad line AGN which have mean α~1(Mittaz et al.1999,Ciliegi et al.1994).

Despite the success of ROSAT surveys,the XRB can-not be synthesised by extrapolating the observed source populations to faint ?uxes,because the resultant spec-trum would be softer than that of the background;this

discrepancy is present for all energy bands between 0.5and 40keV.This means that at faint ?uxes there must be a population of sources with spectra that are harder than the background.According to leading models,these hard sources (eg Fabian 1999,Gilli,Risaliti &Salvati 1999)are obscured AGN.However,the physical nature and observa-tional appearance of the XRB producing population is not yet known,and is the subject of some debate.For exam-ple,Gilli,Risaliti &Salvati (1999)examined a model in-tended to reproduce the XRB by extrapolating the X–ray emission of present epoch AGN to high redshift using the observed soft X–ray luminosity function.In contrast,the model of Fabian (1999)has a large fraction of the XRB due to a population of high redshift,heavily obscured,growing AGN,which are di?erent to anything observed in the local universe.

In Page et al.(2000),hereafter paper 1,we presented a catalogue of 147serendipitous ROSAT sources which have spectra harder than that of the XRB.These sources have a steep N (S )relation down to the sensitivity limit of our survey (~10?14erg cm ?2s ?1),and are therefore likely to be the bright tail of the population of hard sources that

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2Page,Mittaz&Carrera

dominate the source counts at faint?uxes.As such,they could o?er us a preview of the faint,hard and dominant, X-ray source population.We have therefore undertaken a programme of optical and infrared observations of our ROSAT hard source sample to?nd out what these sources are.In this paper we present the hard source identi?ca-tions obtained from our optical(spectroscopic)campaign together with those found in existing catalogues.Section2 details our method and observations,the results of which are given in Section3.These results are discussed in the context of absorbed AGN and the XRB in Section4.Fi-nally,we present our conclusions in Section5.

Throughout this paper we de?ne power law spectral indexαsuch that fν∝ν?α.

2OPTICAL IDENTIFICATION

2.1Strategy

To produce a systematic and e?cient optical identi?-cation programme,we divided the hard X-ray sources into two groups depending on the ease of optical iden-ti?cation.Sources which had one or two plausible candi-dates present in APM data and/or the DSS were consid-ered suitable for optical spectroscopy and make up the ‘spectroscopic sample’,while sources with no plausible candidates,or more than two,were considered unsuit-able for spectroscopy and became the‘imaging sample’. There are103sources in the spectroscopic sample and 44sources in the imaging sample.This paper will deal only with identi?ed sources from the spectroscopic sam-ple(except for two sources,RXJ005812.20-274217.8and RXJ101112.05+554451.3,which are fainter than our spec-troscopic sample limit but have catalogue identi?cations). The properties of sources in the imaging sample,and their relationship to the spectroscopic sample sources,will be discussed brie?y in Section3.2and in more detail in Car-rera et al.(in preparation)where we will present the re-sults of our optical and infrared imaging.The three sources of data for the identi?cation process were spectra taken on the William Herschel Telescope(WHT)and the Eu-ropean Southern Observatory3.6m Telescope(ESO3.6), and databases of existing catalogues.The optical spectra will be presented in Mittaz et al.(2001)along with a full description of the observations and data reduction.

Catalogue identi?cations were obtained by search-ing the NASA Extragalactic Database(NED)and SIM-BAD around all the ROSAT hard source positions (not just the spectroscopic sample).One further source (RXJ043420.48-082136.7)was identi?ed from a WHT ISIS spectrum taken during the RIXOS programme,but was not part of the?nal RIXOS sample presented in Mason et al.(2000).

3RESULTS

Table1contains the list of optical identi?cations.We have categorised our sources as follows.X-ray sources with an optical counterpart which is a Galactic star,of any type, have been classi?ed as stars,and X-ray sources which are clusters of galaxies have been classi?ed as clusters.X-ray Table2.Di?erent types of identi?ed hard sources and their mean properties.N is the number of sources, S is the mean ?tted?ux in units of10?14erg cm?2s?1, α is the mean ?tted spectral slope, z is the mean redshift and log L is the mean of the log of observed0.5-2keV luminosity in erg s?1,calculated as described in Section3.3.For comparison,the unidenti?ed sources from the spectroscopic sample are listed as No ID(S),while the unidenti?ed sources from the imaging sample are listed as‘No ID(I)’.

N S α z log L offset BLAGN288.1-0.29 1.0043.71 6.1 NELGs1313.6-0.740.2542.687.2 galaxies5 4.0-0.430.1241.85 6.5 clusters819.90.210.2343.38-stars8 3.1-0.91--11.45 No ID(S)43 3.9-0.52---

No ID(I)42 3.2-0.54---sources with an extragalactic optical counterpart which has one or more broad emission lines,or a broad compo-nent(>2000km s?1)to an emission line,is classi?ed as a broad line AGN(BLAGN).X-ray sources with galaxy op-tical counterparts showing narrow emission lines(<2000 km s?1)but no broad emission lines are classed as narrow emission line galaxies(NELGs).Note that none of the nar-row line objects in this survey would be classi?ed as nar-row line Seyfert1s(eg by the criteria given in Goodrich 1989).Galaxies with no discernable emission lines were classed as galaxies.The numbers of objects in each cate-gory,and their mean properties are given in Table2.The sample is dominated by extragalactic sources,and of these over half are broad line AGN.

The distributions of o?sets between the X-ray posi-tions and the optical counterparts for the di?erent classes of hard source are shown in Fig.1.The mean o?sets for each source type are given in Table2and are6–7arc-seconds for all source types except for the Galactic stars, which have a mean o?set of12arcseconds and a?at dis-tribution of o?sets(Fig.1);this suggests that the‘star’identi?cations are less secure than the others.

We have systematically checked the redshifts of the extragalactic hard sources for similarity to the redshifts of the targets of the PSPC observations in which they were detected.Only two sources,RXJ111926.34+210646.1and RXJ120403.79+280711.2,both clusters of galaxies,have redshifts similar to the observation targets.

3.1X-ray slopes and?uxes

The?tted X-ray spectral slopes and?uxes of the di?erent types of sources are shown in Fig.2,and their mean slopes and?uxes are given in Table2.A noticeable feature of Fig. 2is that the clusters of galaxies are concentrated towards the top right(soft spectrum,high?ux)corner compared to the other sources.This trend is con?rmed by a two dimensional Kolmogorov Smirnov(2DKS)test(Fasano& Franceschini1987):the cluster distribution of(α,S)is dif-ferent to that for any(or all)of the other source types with >99%con?dence.Because they are not particularly hard, and because they are predominantly bright and therefore do not have as steep an N(S)relation as the rest of the hard sources,the clusters are unlikely to be important contributors to the faint hard source population.

c 0000RAS,MNRAS000,000–000

A Survey of hard spectrum ROSAT sources2:optical identi?cation of hard sources3 Table1.Hard source optical counterparts

Source optical position origin type z cat name notes

RA dec

RXJ001144.43-362638.0001144.54-362639.0EFOSC BLAGN0.900

RXJ004651.98-204329.0004651.83-204328.6cat BLAGN0.380[HB89]0044-209

RXJ005734.78-272827.4005734.94-272828.0EFOSC BLAGN 2.185

RXJ005736.81-273305.9005736.75-273304.6cat NELG0.213GSGP4X:069

RXJ005746.75-273000.8005746.83-273000.9cat galaxy0.019ESO411-G034

RXJ005801.64-275308.6005801.32-275310.2EFOSC NELG0.416GSGP4X:091

RXJ005812.20-274217.8005813.57-274211.4cat NELG0.597GSGP4X:100

RXJ013555.47-183210.2013555.71-183224.9EFOSC star0.000

RXJ013707.63-183846.4013707.75-183849.9EFOSC star0.000Unlikely to be X-ray source RXJ013721.47-182558.3013721.94-182603.0EFOSC NELG0.336

RXJ014159.22-543037.0014159.81-543039.6EFOSC BLAGN0.168

RXJ031456.58-552006.8031456.30-552006.1cat galaxy0.387[GZd97]1.4GHz38

RXJ033340.22-391833.4033339.54-391841.4EFOSC BLAGN 1.436

RXJ033402.54-390048.7033403.26-390036.9EFOSC galaxy0.061PKS0332-39W AT radio source

RXJ034119.02-441033.3034119.23-441029.9cat BLAGN0.505QSF3X:51

RXJ043420.48-082136.7043420.19-082131.3cat BLAGN0.155

RXJ045558.99-753229.1045558.82-753228.0cat NELG0.018ESO033-G002

RXJ052839.93-325148.5052839.83-325144.7cat cluster0.273[VMF98]042

RXJ082640.20+263112.3082640.52+263114.1ISIS NELG0.182

RXJ085340.52+134924.9085341.01+134919.7cat NELG0.190MS0850.8+1401Uncertain ID

RXJ085851.49+141150.7085850.75+141154.5ISIS NELG0.453

RXJ090518.27+335006.0090517.94-335016.1ISIS NELG0.425

RXJ090923.64+423629.2090923.82+423623.3ISIS BLAGN0.177

RXJ091908.27+745305.6091910.56+745311.2ISIS galaxy0.073

RXJ094144.51+385434.8094144.61+385439.1ISIS BLAGN 1.819

RXJ095340.67+074426.1095340.12+074412.3cat BLAGN0.760RIXOS F218

001

RXJ111926.34+210646.1111925.93+210647.4cat cluster0.176

RXJ111942.16+211518.1111942.13+211516.6cat BLAGN 1.288

RXJ112056.87+132726.2112057.48+132708.0ISIS star0.000Unlikely to be X-ray source RXJ114621.27+285320.6114619.93+285306.6cat cluster0.170part of[VMF98]107

RXJ115952.10+553212.1115952.28+553206.1cat cluster0.081MS1157.3+5548

RXJ120403.79+280711.2120403.55+280701.3cat cluster0.167MS1201.5+2824

RXJ121017.25+391822.6121016.61+391816.6ISIS NELG0.022

RXJ121115.30+391146.8121115.67+391154.2cat cluster0.340MS1208.7+3928

RXJ121803.82+470854.612184.54+470851.0ISIS BLAGN 1.743

RXJ124913.86-055906.2124913.85-055919.4cat BLAGN 2.212[HB89]1246-057BALQSO

RXJ131635.62+285942.7131634.72+285929.3cat BLAGN0.277RIXOS F224

026

RXJ133152.51+111643.5133152.25+111649.6cat BLAGN0.090RIXOS F278

011

RXJ140134.94+542029.2140134.59+542031.1ISIS galaxy0.069

RXJ140416.61+541618.2140416.79+541614.6ISIS BLAGN 1.405

RXJ142754.71+330007.0142754.51+325959.8cat BLAGN0.420RIXOS F110

4Page,Mittaz&

Carrera

Figure1.Histogram of o?sets,in bins of2arcseconds,between

the X–ray positions and optical counterparts for the di?erent

classes of identi?ed sources.

Note that the very hard mean spectral index of the

Galactic stars(see Table2)is due to the three objects with

best?tα

with best?tα=?1.65and RXJ133146.37+111420.4with

best?tα=?1.472)are unlikely to be correct identi?ca-

tions(see Section3.6).

The other three types of sources(BLAGN,NELGs

and galaxies)have distributions of(α,S)which are indis-

tinguishable from one another according to the2DKS test;

any(or all)could be signi?cant contributors to the faint,

hard population.

For comparison Figure2also shows the unidenti?ed

sources.Unidenti?ed objects in the spectroscopic sample

are found with similar spectral slopes and?uxes to the

identi?ed sources(except the clusters which are softer and

brighter).The sources in the imaging sample are more

concentrated toward faint?uxes and comprise most of the

faintest(S~10?14erg cm?2s?1)hard sources.

3.2The unidenti?ed sources

We now consider brie?y how fair a subsample the identi-

?ed sources are of the whole ROSAT hard source sample.

Starting with the spectroscopic sample,candidates were

chosen for identi?cation on our WHT and ESO3.6m ob-

serving runs without regard to their optical magnitudes

and morphologies,(except to exclude sources with an ex-

isting catalogue identi?cation)and are hence an unbi-

ased subsample of the spectroscopic sample.The catalogue

identi?cations,although including a few optically bright

galaxies,are mostly from previous?ux limited X–ray sur-

veys.They therefore tend to have higher X–ray?uxes than

the spectroscopic sample as a whole,but are otherwise a

fair subsample.This means that except for a bias towards

higher X–ray?uxes,the identi?ed sources are a fair sub-

sample of the spectroscopic sample.

The spectroscopic sample is a signi?cant fraction of

the whole ROSAT hard source sample(103of147sources),

but it cannot be considered a fair subsample because it ex-

cludes the optically faint sources which form the imaging

sample.Without spectroscopically identifying the imaging

sample(which is currently impractical)it is not possible to

determine whether or not the imaging sample is actually

made up of the same mix of sources as the spectroscopic

sample.However we can examine whether it is possible,by

assuming that similar types of sources will have similar X–

ray to optical?ux ratios.Figure3shows the X–ray?ux

against the APM red(E or R)magnitude for the identi?ed

sources with available APM data.BLAGN,NELGs and

galaxies are found with similar ranges of X–ray to opti-

cal ratio.The optical counterparts to the imaging sample

sources are presumed to be fainter than the plate limit,

which we take to be20.5and21.0for sources with APM

data available for E and R plates respectively.The imag-

ing sample sources are plotted in Fig.3with these lower

limits except for two sources RXJ031956.76-663938.5and

RXJ101031.05+503458.6,which are in the imaging sam-

ple because there are too many potential counterparts for

practical spectroscopic follow up.The dashed line corre-

sponds to an X–ray to optical?ux ratio which is similar

to that of RXJ111750.51+075712.8,which has the high-

est X–ray to optical?ux ratio of the identi?ed spectro-

scopic sample sources excluding the clusters.Only six of

the imaging sample sources lie above the dashed line,and

therefore de?nitely have X–ray to optical?ux ratios di?er-

ent to those of the identi?ed sources.Therefore the limits

on the optical to X–ray ratios are consistent with the iden-

ti?ed sources being the same types of objects as constitute

almost the whole ROSAT hard source sample.

3.3Redshifts and luminosities

Fig.4shows the redshifts and0.5-2keV luminosities for

the extragalactic hard sources.Luminosities were calcu-

lated from the?tted?uxes,K corrected using the best?t

spectral slopes,and assuming H0=50km s?1Mpc?3,

q0=0.The majority of the BLAGN have higher lumi-

nosities and redshifts than the NELGs and galaxies;all

the high redshift(z>1)sources are BLAGN.This may

imply that either hard spectrum narrow line sources do

not exist at high luminosity/redshift or our spectroscopic

c 0000RAS,MNRAS000,000–000

A Survey of hard spectrum ROSAT sources2:optical identi?cation of hard sources

5 Figure2.X-ray spectral slopes and?uxes of the di?erent types of hard source.For comparison the unidenti?ed sources are shown in the last panel:the spectroscopic sample as?lled dots and the imaging sample as crosses(see Section2for de?nitions of the two

samples).

sample is not deep enough(in X–ray or optical?ux)to

?nd them.

3.4X–ray-optical-radio?ux ratios

It is common to parameterise the X–ray to optical and

optical to radio?ux ratios of AGN asαOX andαOR,where

αOX is the slope of the power law which(in the object’s

rest frame)would connect the?ux density(Fν)at2500?A

with the X–ray?ux density at2keV,andαOR is the slope

of the power law which would connect the?ux density at

2500?A with the?ux density at5GHz.

For all sources we have estimated the rest frame2500

?A?ux density using B photometry(taken from Carrera et

al.in preparation)and assuming a power law optical-UV

spectrum with slopeα=0.5,and using the B magnitude

to?ux conversion given by Wilkes et al.(1994).The B

magnitudes have been corrected for Galactic reddening

using the expression for E(B?V)in Bohlin,Savage&

Drake(1978)and assuming A B=4E(B V).

To estimate the rest frame5GHz?uxes we have

searched for potential radio counterparts to our X–ray

sources in the catalogues of radio sources in the VLA1.4

GHz FIRST(White et al.1997)and NVSS(Condon et al.

1998)surveys and the5GHz Parkes-MIT-NRAO(PMN,

Gri?th&Wright1993)survey.Additionally,radio images

from these surveys were searched by eye to ensure that any

extended radio sources associated with our X–ray sources

were not missed,and to ensure that there were no spuri-

ous radio counterparts associated with other extended ra-

dio sources.The uncertainty in radio source position from

these three surveys ranges from~better than1arcsecond

(FIRST)to around10arcseconds(PMN).The sky den-

sity of radio sources is su?ciently low(reaching around

100deg?2at the~1mJy completeness limit of FIRST)

that it is unlikely that there are any chance coincidences.

Where no suitable radio source appears in a survey cat-

alogue,we have taken the catalogue completeness limit

as the upper limit to the radio?ux of the X–ray source.

We took the best measurement(or upper limit)available

from the three surveys and assume a radio spectral slope

ofα=0.7.

The2keV?ux density has been estimated from the

c 0000RAS,MNRAS000,000–000

6Page,Mittaz &

Carrera

Figure 3.Optical magnitudes against X–ray ?uxes for the identi?ed sources inthe spectroscopic sample (symbols)and the sources in the imaging sample (lower limits).The gradient of the dashed line corresponds to a constant ratio of X–ray to optical ?ux.

?tted 0.5-2keV ?uxes and assuming an X–ray spectral slope of α=0.

We then computed αOX =0.384log[f ν(2500?A )/f ν(2keV)]and

αOR =?0.186log[f ν(2500?A )/f ν

(5GHz)]

αOX and αOR are shown in Fig.5for all the hard sources identi?ed as BLAGN,NELGs and galaxies.The horizontal dashed line marks αOR =0.35which is com-monly used to di?erentiate radio loud and radio quiet objects (Zamorani et al.1981).Seven hard sources (four BLAGN,2galaxies and 1NELG)lie above this line,and are therefore radio loud.This is a large radio loud fraction (15+7?5%where errors are the Poission 68%con?dence in-terval,Gehrels 1986)of the BLAGN,NELGs and galaxies compared to the fraction found in normal ROSAT surveys without spectral selection,eg Cilliegi et al.(1995)?nd that

only two of the eighty CRSS AGN and NELGs (2.5+3.3

?1.6%)are radio loud.On the other hand,the distribution of αOX of the hard sources is quite similar to that found in other AGN surveys (eg Ciliegi et al.1995,Wilkes et al.1994),with the majority of sources having 1<αOX <1.8.3.5

X–ray absorption

The leading hypothesis to explain the majority of faint hard sources which contribute substantially to the XRB

Figure 4.Redshifts and observed 0.5-2keV luminosities for the di?erent extragalactic source types

is that they are intrinsically absorbed AGN (eg Fabian &Iwasawa 1999,Setti &Woltjer 1989).This is also a likely hypothesis for our hard sources,because the optical spec-tra and colours of a signi?cant fraction of our BLAGN and NELGs suggest absorption (Mittaz et al.2001and Carrera et al.2001).Assuming that our BLAGN,NELGs and galaxies have hard spectra because of absorption,we have estimated their column densities from their 3colour ROSAT PSPC spectra.We assume that before absorp-tion they have power law X–ray spectra with energy in-dex α=1(typical for X-ray selected AGN,eg Mittaz et al.1999,Maccacaro et al.1988)and ?t their intrinsic cold gas column.The ?tting procedure was identical to that described in paper 1except that the free parameters in the ?t are intrinsic column and power law normalisa-tion rather than power law slope and normalisation.The results of these ?ts are given in Table 3.

The BLAGN,NELG and galaxies’?tted absorbing columns and luminosities (before absorption)are shown in Fig.6.Most of the high luminosity sources (near the top of Fig.6)are BLAGN,while most of the galaxies are found with low luminosities;the mean log L (in erg s ?1,0.5-2keV)for the BLAGN,NELGs and galaxies are 44.4,43.2and 42.2respectively.We note that the trend in Fig.6for the most absorbed sources to have the highest luminosity is probably a selection e?ect due to the shifting of the rest frame emitted passband to higher energy with increasing redshift.This means that sources detectable in the PSPC and satisfying our spectral selection criterion

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A Survey of hard spectrum ROSAT sources2:optical identi?cation of hard sources7

Table3.Hard sourceαOX,αOR and?tted columns

Source———X–ray———B mag A B————radio————αOXαOR—X–ray column?t—?ux aαlog L b?uxνsurvey N H norm c

(mJy)(GHz)(cm?2)

RXJ001144.43-362638.0 4.19+0.60

?0.56-0.14+0.27

?0.35

43.97+0.06

?0.06

20.38±0.120.08<2.50 1.4NVSS 1.32+0.04

?0.04

<0.3321.34+0.43

?0.29

2.32+0.52

?0.39

RXJ004651.98-204329.019.37+1.95

?1.560.32+0.13

?0.11

44.05+0.04

?0.04

18.60±0.300.11<2.50 1.4NVSS 1.30+0.06

?0.06

<0.2120.72+0.08

?0.09

9.91+0.89

?0.92

RXJ005734.78-272827.4 1.15+0.31

?0.20-0.34+0.56

?0.99

43.91+0.10

?0.08

18.62±0.160.13<2.50 1.4NVSS 1.84+0.06

?0.06

<0.2122.60+0.26

?0.48

0.90+0.33

?0.27

RXJ005736.81-273305.9 1.25+0.23

?0.250.00+0.36

?0.64

42.34+0.07

?0.10

20.72±0.300.13<2.50 1.4NVSS 1.42+0.08

?0.07

<0.3621.07+0.40

?0.46

0.79+0.22

?0.18

RXJ005746.75-273000.8 1.75+0.26

?0.280.08+0.34

?0.32

40.42+0.06

?0.08

13.53±0.100.13 3.80±0.70 1.4NVSS 2.45+0.04

?0.04

-0.16+0.02

?0.02

20.80+0.29

?0.28

1.02+0.21

?0.18

RXJ005801.64-275308.6 5.09+0.50

?0.52-0.35+0.31

?0.29

43.45+0.04

?0.05

21.43±0.150.13<2.50 1.4NVSS 1.09+0.04

?0.04

<0.4121.55+0.17

?0.25

3.31+0.71

?0.54

RXJ005812.20-274217.80.90+0.24

?0.22-0.30+0.58

?1.02

42.97+0.10

?0.12

22.63±0.300.13<2.50 1.4NVSS 1.21+0.09

?0.09

<0.5121.75+0.29

?0.57

0.65+0.29

?0.17

RXJ013721.47-182558.3 3.91+0.57

?0.460.03+0.19

?0.27

43.22+0.06

?0.05

20.87±0.110.07<2.50 1.4NVSS 1.23+0.04

?0.04

<0.3620.84+0.17

?0.15

2.02+0.30

?0.26

RXJ014159.22-543037.08.81+1.51

?1.51-0.22+0.41

?0.57

42.98+0.07

?0.08

17.38±0.100.17<37.00 5.0PMN 1.60+0.05

?0.04

<0.3921.37+0.20

?0.46

5.98+1.77

?1.54

RXJ031456.58-552006.8 3.45+0.54

?0.48-1.66+0.70

?0.85

43.04+0.06

?0.06

21.72±0.130.18 1.25±0.11 1.4FIRST 1.10+0.05

?0.04

0.37+0.02

?0.02

22.12+0.10

?0.15

4.42+1.18

?1.03

RXJ033340.22-391833.4 3.37+0.70

?0.75-0.24+0.71

?0.77

44.17+0.08

?0.11

19.42±0.120.10<2.50 1.4NVSS 1.52+0.06

?0.05

<0.2622.48+0.19

?0.37

3.01+1.19

?0.97

RXJ033402.54-390048.77.22+0.99

?0.87-0.06+0.30

?0.23

42.05+0.06

?0.06

16.03±0.300.101567.10±52.60 1.4NVSS 1.84+0.07

?0.07

0.51+0.03

?0.03

20.74+0.29

?0.22

3.97+0.69

?0.58

RXJ034119.02-441033.3 2.60+0.41

?0.400.06+0.34

?0.34

43.37+0.06

?0.07

21.55±0.110.10<45.00 5.0PMN 1.19+0.04

?0.04

<0.7221.10+0.38

?0.31

1.48+0.34

?0.25

RXJ043420.48-082136.711.51+2.69

?1.82-1.17+1.21

?0.95

42.97+0.09

?0.07

18.68±0.130.42 3.70±0.60 1.4NVSS 1.32+0.05

?0.05

0.24+0.02

?0.02

21.95+0.11

?0.22

14.67+5.80

?4.18

RXJ045558.99-753229.190.78+4.93

?3.88-2.43+0.26

?0.26

42.08+0.02

?0.02

16.05±0.070.59<20.00 5.0PMN 1.34+0.02

?0.02

<0.2721.89+0.04

?0.04

135.47+13.96

?12.08

RXJ082640.20+263112.3 3.81+0.83

?0.87-1.27+0.93

?1.06

42.61+0.09

?0.11

20.34±0.140.25<0.91 1.4FIRST 1.27+0.06

?0.05

<0.2521.93+0.15

?0.22

4.57+2.06

?1.38

RXJ085340.52+134924.912.00+0.98

?1.16-0.19+0.23

?0.34

43.22+0.03

?0.04

19.21±0.090.2523.20±1.50 1.4NVSS 1.26+0.03

?0.03

0.42+0.01

?0.01

21.38+0.15

?0.25

7.80+1.52

?1.22

RXJ085851.49+141150.7 4.05+0.81

?0.65-1.32+0.82

?0.84

43.26+0.08

?0.08

20.82±0.300.29<2.50 1.4NVSS 1.20+0.08

?0.08

<0.3922.11+0.13

?0.18

4.81+1.51

?1.37

RXJ090518.27+335006.07.58+2.29

?1.33-2.43+1.80

?1.09

43.32+0.11

?0.08

20.45±0.090.16<0.97 1.4FIRST 1.17+0.05

?0.06

<0.2522.41+0.08

?0.18

15.65+6.87

?4.00

RXJ090923.64+423629.27.40+0.97

?0.870.22+0.20

?0.22

42.98+0.05

?0.05

18.25±0.090.11<2.50 1.4NVSS 1.50+0.04

?0.03

<0.1620.69+0.17

?0.18

3.86+0.51

?0.50

RXJ091908.27+745305.6 4.73+1.01

?0.92-0.35+0.54

?0.82

42.01+0.08

?0.09

17.82±0.090.14<2.50 1.4NVSS 1.63+0.05

?0.05

<0.1321.57+0.27

?0.42

4.01+2.69

?1.61

RXJ094144.51+385434.8 2.11+0.51

?0.53-0.12+0.57

?0.58

44.17+0.09

?0.13

21.11±0.140.10<1.01 1.4FIRST 1.35+0.07

?0.06

<0.3221.92+0.46

?0.43

1.34+0.41

?0.37

RXJ095340.67+074426.1 4.32+1.25

?1.09-0.38+0.52

?0.94

43.81+0.11

?0.13

20.01±0.090.19<2.50 1.4NVSS 1.35+0.06

?0.06

<0.3121.77+0.34

?0.45

3.06+1.44

?0.95

RXJ101112.05+554451.3 6.95+0.90

?0.88-0.43+0.29

?0.29

44.32+0.05

?0.06

22.02±1.000.05161.50±0.15 1.4FIRST 1.00+0.18

?0.17

0.78+0.07

?0.07

21.62+0.43

?0.17

4.01+0.91

?0.57

RXJ101123.17+524912.4 3.34+0.96

?0.87-1.41+0.93

?1.22

43.58+0.11

?0.13

20.86±0.090.05<0.96 1.4FIRST 1.29+0.06

?0.06

<0.2822.51+0.16

?0.28

3.91+1.96

?1.21

RXJ101147.48+505002.2 4.56+1.01

?0.82-0.09+0.44

?0.47

42.07+0.09

?0.09

16.74±0.220.06<0.96 1.4FIRST 1.82+0.07

?0.07

<-0.0220.65+0.73

?0.28

2.75+0.95

?0.55

RXJ104723.37+540412.6 1.71+0.70

?0.61-0.56+0.90

?1.09

43.78+0.15

?0.19

20.09±0.110.06<0.96 1.4FIRST 1.54+0.09

?0.07

<0.2322.22+0.42

?0.61

1.31+0.78

?0.45

RXJ110742.05+723236.08.11+1.22

?1.100.12+0.37

?0.45

44.97+0.06

?0.06

19.07±0.080.21370.60±11.10 1.4NVSS 1.43+0.04

?0.04

0.64+0.01

?0.01

21.58+0.82

?0.38

4.75+1.11

?0.75

RXJ111750.51+075712.816.55+1.57

?1.40-0.15+0.23

?0.29

44.38+0.04

?0.04

20.67±0.090.24<2.50 1.4NVSS 1.01+0.03

?0.03

<0.3621.57+0.18

?0.20

9.94+1.60

?1.26

RXJ111942.16+211518.1 3.44+0.62

?0.480.13+0.30

?0.30

44.24+0.07

?0.07

19.91±0.090.09<0.93 1.4FIRST 1.44+0.04

?0.04

<0.2121.42+0.36

?0.28

1.89+0.37

?0.30

RXJ121017.25+391822.6 4.62+0.68

?0.67-0.02+0.35

?0.49

40.98+0.06

?0.07

17.18±0.500.14<0.98 1.4FIRST 1.73+0.10

?0.10

<0.0421.10+0.22

?0.49

2.88+0.78

?0.51

RXJ121803.82+470854.6 1.51+0.44

?0.42-0.52+0.60

?1.07

43.82+0.11

?0.14

21.04±0.090.08<0.98 1.4FIRST 1.42+0.07

?0.06

<0.3122.30+0.34

?0.69

1.07+0.53

?0.30

RXJ124913.86-055906.2 2.38+0.47

?0.36-0.09+0.57

?0.55

44.36+0.08

?0.07

17.26±0.300.15<2.50 1.4NVSS 1.92+0.07

?0.08

<0.1222.23+0.36

?0.57

1.53+0.39

?0.38

RXJ131635.62+285942.713.74+0.98

?1.000.35+0.10

?0.08

43.64+0.03

?0.03

20.32±0.300.08<0.93 1.4FIRST 1.10+0.06

?0.06

<0.2520.53+0.07

?0.07

6.55+0.50

?0.47

RXJ133152.51+111643.556.99+4.09

?3.88-1.72+0.27

?0.33

43.22+0.03

?0.03

18.16±0.100.138.00±1.00 1.4NVSS 1.17+0.03

?0.03

0.24+0.02

?0.02

21.80+0.06

?0.06

64.44+9.09

?7.69

RXJ135105.69+601538.5 3.83+0.44

?0.45-0.12+0.33

?0.27

43.07+0.05

?0.05

20.53±0.090.12<2.50 1.4NVSS 1.27+0.03

?0.03

<0.3321.17+0.23

?0.25

2.22+0.42

?0.31

RXJ135529.59+182413.6 3.63+0.86

?0.89-0.41+0.84

?0.94

44.02+0.09

?0.12

20.61±0.090.14<2.50 1.4NVSS 1.31+0.06

?0.05

<0.3522.25+0.25

?0.50

2.82+1.29

?0.78

RXJ140134.94+542029.2 2.94+0.58

?0.57-0.13+0.46

?0.59

41.76+0.08

?0.09

18.42±0.090.08<1.00 1.4FIRST 1.63+0.05

?0.04

<0.1021.02+0.39

?0.46

1.89+0.64

?0.39

RXJ140416.61+541618.2 2.79+0.62

?0.48-0.08+0.34

?0.56

44.14+0.09

?0.08

21.16±0.200.08<0.99 1.4FIRST 1.28+0.06

?0.06

<0.3221.69+0.40

?0.38

1.70+0.45

?0.35

RXJ142754.71+330007.0 3.00+0.51

?0.460.21+0.27

?0.39

43.31+0.07

?0.07

19.66±0.080.07<0.83 1.4FIRST 1.46+0.04

?0.04

<0.1820.81+0.38

?0.35

1.57+0.29

?0.27

RXJ163054.25+781105.18.96+0.74

?0.87-0.01+0.37

?0.29

43.62+0.03

?0.04

20.54±0.140.28<2.50 1.4NVSS 1.11+0.04

?0.04

<0.3521.52+0.17

?0.31

5.81+1.22

?1.06

RXJ163308.57+570258.7 1.89+0.32

?0.33-0.11+0.42

?0.69

44.40+0.07

?0.08

20.06±0.120.1317.20±0.15 1.4FIRST 1.55+0.05

?0.04

0.47+0.01

?0.01

22.48+0.31

?0.54

1.20+0.33

?0.26

RXJ204640.48-363147.5 6.29+0.68

?0.71-0.14+0.45

?0.36

44.31+0.04

?0.05

18.76±0.070.2823.70±0.90 1.4NVSS 1.48+0.03

?0.03

0.40+0.01

?0.01

21.89+0.17

?0.22

3.92+0.65

?0.57

RXJ204716.74-364715.19.13+0.86

?0.91-0.64+0.35

?0.53

41.97+0.04

?0.05

17.57±0.080.28 4.60±0.50 1.4NVSS 1.54+0.03

?0.03

0.16+0.01

?0.01

21.53+0.12

?0.15

7.88+1.65

?1.37

RXJ213807.61-423614.316.71+5.05

?3.62-1.10+0.92

?1.06

41.40+0.11

?0.11

16.15±0.070.18<47.00 5.0PMN 1.67+0.05

?0.05

<0.3221.74+0.17

?0.27

19.00+9.30

?6.98

RXJ235113.89+201347.330.31+3.16

?3.06-0.55+0.29

?0.44

42.37+0.04

?0.05

16.94±0.130.30 5.90±0.50 1.4NVSS 1.43+0.04

?0.04

0.14+0.02

?0.02

21.44+0.12

?0.18

23.84+5.35

?4.08

a Units of erg cm?2s?1

b See Section3.3

c Units of erg cm?2s?1keV?1

(see paper1)will have larger columns at higher redshift (and hence at higher luminosity).

3.6Notes on individual sources

RXJ004651.98-204329.0The hard ROSAT spectrum of this active galaxy was the subject of Elvis et al.(1997) who proposed that absorption in material associated with NGC247may be responsible.

RXJ005801.64-275308.6A second,slightly fainter NELG at J2000position00h58m1.69s?27o53′16.80′′has the same redshift(z=0.086)as,and is within10arcsec-onds of,the NELG identi?ed as the X–ray source.

RXJ013707.63-183846.4The star has an unremarkable G type spectrum,and the X–ray source is coincident with a bright radio source(MRC0134-188)and hence the star is unlikely to be the correct optical counterpart.The real optical counterpart is too faint to be seen on POSS.

RXJ031456.58-552006.8This radio galaxy has ex-tended double lobe structure;see Gruppioni,Mignoli& Zamorani(1999).

RXJ033402.54-390048.7This source is a wide angle

c 0000RAS,MNRAS000,000–000

8Page,Mittaz &

Carrera

Figure 5.αOX and αOR for the hard sources

tail radio source in the galaxy cluster Abell 3135.A mag-nitude V ~16Galactic star is also close to the X-ray source position but is unlikely to be related.

RXJ043420.48-082136.7The identi?cation spectrum of this object was taken on the WHT as part of RIXOS,but the source was not part of the ?nal RIXOS sample and is not included in the ?nal catalogue (Mason et al.2000).

RXJ085340.52+134924.9This RIXOS identi?cation is uncertain because there is another optical counterpart closer to the centre of the X–ray error circle that was not observed.Note also that the position of the optical counterpart is incorrect in

Mason et al.(2000),which should be the same as that in Table 1,i.e.08h 53m 41.01s +13o 49′19.7′′(J2000).

RXJ095340.67+074426.1The RIXOS identi?cation and redshift of this source are based on a relatively poor optical spectrum and therefore may be incorrect.

RXJ101112.05+554451.3This source was identi?ed as an obscured radio loud AGN by Barcons et al.(1998).It has strong narrow emission lines but Mg II λ2798is broad,and hence we have classi?ed it as a BLAGN.

RXJ101147.48+505002.2This X–ray source was iden-ti?ed with a NELG with z =0.067by Carballo et al.(1995),but we identify the source with a BLAGN with z =0.079,which is brighter and closer to the X–ray source.Notably,the z =0.079BLAGN showed only narrow lines in the optical spectrum of Carballo et al.(1995);the H αline pro?le appears genuinely to have changed between 1994and 1998.

Figure 6.Fitted columns and unabsorbed 0.5-2keV luminosi-ties for the di?erent types of hard sources.

RXJ111926.34+210646.1This galaxy cluster and the target of the PSPC observation (PG 1116+215)in which it was found have very similar redshifts (0.0176and 0.1765respectively)and therefore this source is not strictly serendipitous.

RXJ112056.87+132726.2The X–ray source is coin-cident with the symmetric double radio source 87GB 111822.7+134349,and hence the star is unlikely to be the correct identi?cation for the X–ray source.

RXJ120403.79+280711.2This galaxy cluster and the target of the PSPC observation (PG 1202+281)in which it was found have similar redshifts (0.0167and 0.1653re-spectively)and therefore this source may not be strictly serendipitous.

RXJ124913.86-055906.2This broad absorption line (BAL)QSO was the only bona-?de BALQSO in sample of Green &Mathur (1996)to be detected as a PSPC source.RXJ133146.37+111420.4This X–ray source is coinci-dent with the radio source 87GB 132918.1+112918,and hence the star is unlikely to be the correct optical coun-terpart.

RXJ142754.71+330007.0The RIXOS identi?cation and redshift of this source are based on a relatively poor optical spectrum and therefore may be incorrect.

4DISCUSSION

Excluding the clusters,which are unlikely to be an impor-tant part of the faint,hard X–ray source population (see

c

0000RAS,MNRAS 000,000–000

A Survey of hard spectrum ROSAT sources2:optical identi?cation of hard sources9

Section3.1),we have identi?ed3types of extragalactic hard source:BLAGN,NELGs and galaxies.At?rst sight the identi?cation content of the sample appears similar to that of other PSPC surveys with similar?ux limits but without any spectral selection,eg BLAGN being the most numerous source.However,in two respects the identi?ca-tion content of this survey is signi?cantly di?erent.

The?rst di?erence is that there is a higher proportion of radio loud objects(15+7?5%)in this survey(see Section 3.4).There are two possible reasons why this should be so.One is that the intrinsic X–ray emission of radio loud sources may be harder than that of radio quiet sources (Reeves et al.1997)because the radio loud sources have an additional,hard spectrum X–ray emission component from the inner parts of radio jets.The other possibility is that our radio loud sources are absorbed,and because they are intrinsically more X–ray luminous than radio quiet sources they are relatively numerous in a relatively bright survey of hard spectrum sources.This would be analo-gous to the high proportion of(presumably unabsorbed) radio loud sources present in bright soft X–ray surveys(eg 11±2%in the EMSS,Della Ceca et al.1994)compared to fainter soft X–ray surveys(eg2.5+3.3

?1.6

%in the CRSS, Ciliegi et al.1995).

The second di?erence is that there are nearly half as many NELGs as BLAGN(see Table1)compared to ratios of~1:13NELGS to AGN in RIXOS(Mason et al.2000) and~1:6in the CCRS(Boyle,Wilkes&Elvis1997). This implies that the fraction of sources with hard spectra is larger in the NELG population than in the BLAGN population.This is consistent with the?ndings that the NELGs in faint X–ray surveys have,on average,harder X–ray spectra than BLAGN(Romero-Colmenero et al.1996, Almaini et al.1996),and with the hypothesis that most X–ray selected NELGs are absorbed AGN(Schmidt et al. 1998,Lehmann et al.2000).

Hence the hypothesis that most of the sources have hard X–ray spectra because they are absorbed could ac-count for both the high radio loud and NELG content of this survey.It is also consistent with the preliminary anal-yses of the optical spectra and optical colours of the hard sources(Mittaz et al.2001and Carrera et al.2001).

Related to the absorption hypothesis,an important ?nding is that the distributions of X–ray spectral slopes and?uxes of the BLAGN,NELGs and galaxies are in-distinguishable within the current sample,but the three groups have di?erent ranges of luminosities.The galax-ies are found at low luminosity while the high luminosity sources are BLAGN(see?gures4and6).The absence of high luminosity,absorbed narrow line AGN has also been noted by Akiyama et al.(2000)in the ASCA Large Sky survey.These results are consistent with all three source types having the same mechanism for their X–ray spec-tra(an absorbed active nucleus)but optical emission line properties which depend on luminosity.For this reason we point out that the high redshift,high luminosity,absorbed QSOs expected to produce a large fraction of the X–ray background are not neccessarily narrow line objects(the proposed“QSO2s”)like Seyfert2s,their low luminosity counterparts.5CONCLUSIONS

We have performed a survey of ROSAT?elds for serendip-itous sources with hard spectra(α<0.5);such sources must be a major contributor to the X–ray background at faint?uxes.In this paper we have presented optical identi?cations for62of these sources.Almost half(28)of these sources are BLAGN,while12are NELGs and5are galaxies without visible emission lines.We have also found 8clusters of galaxies among the hard spectrum sources. However,these are predominantly bright sources and are not particularly hard(their best?t spectral indices all lie in the range0.0<α<0.5),and hence clusters are un-likely to be an important component of the hard,faint population.

The hard spectrum BLAGN have a distribution of X–ray to optical ratios which is similar to that found for AGN from other soft X–ray surveys(1<αOX<2).However,a relatively large proportion(15%)of the BLAGN,NELGs and galaxies are radio loud.This could be because the radio jets in these objects produce intrinsically hard X–ray emission,or if they are absorbed,it could be because radio loud objects are more X–ray luminous than radio quiet objects.

The BLAGN,NELGs and galaxies have indistinguish-able distributions of X–ray?ux and spectra,hence any or all may be important to the hard,faint population required to solve the XRB spectral paradox.The ma-jority of the galaxies are low luminosity sources,while the highest luminosity objects,and all the high redshift (z>1)sources,are BLAGN.Their ROSAT spectra are consistent with their being AGN obscured by columns of 20.5

FJC thanks the DGES for partial?nancial support,un-der project PB95-0122.This research was based on obser-vations collected at the European Southern Observatory, Chile,ESO No.62.O-0659,and on observations made at the William Herschel Telescope which is operated on the island of La Palma by the Isaac Newton Group in the Spanish Observatorio del Roque de los Muchachos of the Instituto de Astro?sica de Canarias.This research has made use of data obtained from the Leicester Database and Archive Service at the Department of Physics and Astronomy,Leicester University,UK.This research has made use of the SIMBAD database,operated at CDS, Strasbourg,France,and of the NASA/IPAC Extragalac-tic Database(NED)which is operated by the Jet Propul-sion Laboratory,California Institute of Technology,under contract with the National Aeronautics and Space Admin-istration.

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从实践的角度探讨在日语教学中多媒体课件的应用

从实践的角度探讨在日语教学中多媒体课件的应用 在今天中国的许多大学,为适应现代化,信息化的要求,建立了设备完善的适应多媒体教学的教室。许多学科的研究者及现场教员也积极致力于多媒体软件的开发和利用。在大学日语专业的教学工作中,教科书、磁带、粉笔为主流的传统教学方式差不多悄然向先进的教学手段而进展。 一、多媒体课件和精品课程的进展现状 然而,目前在专业日语教学中能够利用的教学软件并不多见。比如在中国大学日语的专业、第二外語用教科书常见的有《新编日语》(上海外语教育出版社)、《中日交流标准日本語》(初级、中级)(人民教育出版社)、《新编基础日语(初級、高級)》(上海译文出版社)、《大学日本语》(四川大学出版社)、《初级日语》《中级日语》(北京大学出版社)、《新世纪大学日语》(外语教学与研究出版社)、《综合日语》(北京大学出版社)、《新编日语教程》(华东理工大学出版社)《新编初级(中级)日本语》(吉林教育出版社)、《新大学日本语》(大连理工大学出版社)、《新大学日语》(高等教育出版社)、《现代日本语》(上海外语教育出版社)、《基础日语》(复旦大学出版社)等等。配套教材以录音磁带、教学参考、习题集为主。只有《中日交流標準日本語(初級上)》、《初級日语》、《新编日语教程》等少数教科书配备了多媒体DVD视听教材。 然而这些试听教材,有的内容为日语普及读物,并不适合专业外语课堂教学。比如《新版中日交流标准日本语(初级上)》,有的尽管DVD视听教材中有丰富的动画画面和语音练习。然而,课堂操作则花费时刻长,不利于教师重点指导,更加适合学生的课余练习。比如北京大学的《初级日语》等。在这种情形下,许多大学的日语专业致力于教材的自主开发。 其中,有些大学的还推出精品课程,取得了专门大成绩。比如天津外国语学院的《新编日语》多媒体精品课程为2007年被评为“国家级精品课”。目前已被南开大学外国语学院、成都理工大学日语系等全国40余所大学推广使用。

新视野大学英语全部课文原文

Unit1 Americans believe no one stands still. If you are not moving ahead, you are falling behind. This attitude results in a nation of people committed to researching, experimenting and exploring. Time is one of the two elements that Americans save carefully, the other being labor. "We are slaves to nothing but the clock,” it has been said. Time is treated as if it were something almost real. We budget it, save it, waste it, steal it, kill it, cut it, account for it; we also charge for it. It is a precious resource. Many people have a rather acute sense of the shortness of each lifetime. Once the sands have run out of a person’s hourglass, they cannot be replaced. We want every minute to count. A foreigner’s first impression of the U.S. is li kely to be that everyone is in a rush -- often under pressure. City people always appear to be hurrying to get where they are going, restlessly seeking attention in a store, or elbowing others as they try to complete their shopping. Racing through daytime meals is part of the pace

日语日常用语100句

こんにちは。(kon ni qi wa) 你好。 こんばんは。(kon ban wa) 晚上好。 おはようございます。(o ha you go za i mas) 早上好。 お休(やす)みなさい。(o ya su mi na sai) 晚安。 お元気(げんき)ですか。(o gen ki de s ka?) 您还好吧,相当于英语的“How are you”,一种打招呼的方式。 いくらですか。(i ku la de s ka?) 多少钱? すみません。(su mi ma sen) 不好意思,麻烦你…。相当于英语的“Excuse me”。用于向别人开口时。 ごめんなさい。(go men na sai) 对不起。 どういうことですか。(dou iu ko to de su ka?) 什么意思呢? 山田さんは中国語(ちゅうごくご)が上手(じょうず)ですね。 (ya ma da san wa jiu go ku ko ga zyou zu de su ne) 山田的中国话说的真好。 まだまだです。(ma da ma da de s) 没什么。没什么。(自谦) どうしたの。(dou si ta no) どうしたんですか。(dou si tan de su ka?) 发生了什么事啊。 なんでもない。(nan de mo nai) 没什么事。

ちょっと待ってください。(jou to ma te ku da sai,可以简单地表达为:jou to)请稍等一下。 約束(やくそく)します。(ya ku so ko si ma s) 就这么说定了。 これでいいですか。(korede idesuka ?) 这样可以吗? けっこうです。(ke kou de s) もういいです。(mou i i de s) 不用了。 どうして。(dou si de) なぜ(na ze) 为什么啊? いただきます(i ta da ki ma s) 那我开动了。(吃饭动筷子前) ごちそうさまでした。(ko ji sou sa ma de si ta) 我吃饱了。(吃完后) ありがとうございます。(a li ga to go za i ma s) 谢谢。 どういたしまして。(dou i ta si ma si de) 别客气。 本当(ほんとう)ですか。(hon dou de su ka?) 真的? うれしい。(so ne si i) 我好高兴。(女性用语) よし。いくぞ。(yo si。i ku zo) 好!出发(行动)。(男性用语)

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日语常用会话100句

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实用日语100句

?第1课 “对不起” ---------------------------------------------------------------------------------------------------------------------- ~在成田机场①~ ?みか:あのう、すみません。 ?美香:对不起 パスポートが落お ちましたよ (你的)护照掉了。 ?レオ:えっ! ?莱奥:什么? ---------------------------------------------------------------------------------------------------------------------- ?重点语句 #1 「あのう、すみません」 「あのう、すみません」是和陌生人打招呼时的说法。「あのう」可以唤起对方的注意,以便开始对话。「すみません」是“对不起”的意思。 ?第2课 “谢谢” ---------------------------------------------------------------------------------------------------------------------- ~在成田机场②~ ?みか:あのう、すみません。 ?美香:对不起 パスポートが落お ちましたよ (你的)护照掉了。 ?レオ:えっ! ?莱奥:什么? ああ、どうもありがとうございます。 啊,谢谢。 ?みか:どういたしまして。 ?美香:不客气。 ---------------------------------------------------------------------------------------------------------------------- ?重点语句 #2 「どうもありがとうございます」 「どうもありがとうございます」时表示感谢的较为郑重的说法。「ありがとう」是“谢谢”的意思,在它的前面和后面分别加上「どうも」和「ございます」,语气就变得格外郑重了。当有人向你表示感谢时,你可以回答说「どういたしまして」。 ?第3课 “请多关照” ---------------------------------------------------------------------------------------------------------------------- ~在成田机场③~ ?レオ:あのう、ぼくはレオ…。あなたは? ?莱奥:嗯,我叫莱奥…… 你呢? ?みか:私わたしはみか、岡田おかだ みかです。 ?美香:我叫美香,冈田美香。 どうぞよろしく。 请多关照。 ?レオ:こちらこそ、どうぞよろしく。 ?莱奥:也请你多多关照。 ---------------------------------------------------------------------------------------------------------------------- ?重点语句 #3 「どうぞよろしく」 「どうぞよろしく」是和初次见面的人寒暄时使用的比较简略的说法,一般是在说完自己的姓名之后,再说「どうぞよろしく」。 ?第4课 “我第一次来日本” ---------------------------------------------------------------------------------------------------------------------- ~在成田机场④~

2020年1月广东省自学考试各专业开考课程考试时间安排表

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ちょっと待ってください。(jou to ma te ku da sai,可以简单地表达为:jou to) 请稍等一下。 約束(やくそく)します。(ya ku so ko si ma s) 就这么说定了。 これでいいですか。(ko na de i i de su ka?) 这样可以吗? けっこうです。(ke kou de s) もういいです。(mou i i de s) 不用了。 どうして。(dou si de) なぜ(na ze) 为什么啊? いただきます(i ta da ki ma s) 那我开动了。(吃饭动筷子前) ごちそうさまでした。(ko ji sou sa ma de si ta) 我吃饱了。(吃完后) ありがとうございます。(a li ga to go za i ma s) 谢谢。 どういたしまして。(dou i ta si ma si de) 别客气。 本当(ほんとう)ですか。(hon dou de su ka?) 真的? うれしい。(so ne si i) 我好高兴。(女性用语) よし。いくぞ。(yo si。i ku zo) 好!出发(行动)。(男性用语) いってきます。(i te ki ma s) 我走了。(离开某地对别人说的话) いってらしゃい。(i te la si yai) 您好走。(对要离开的人说的话)

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新视野大学英语2课文翻译(Unit1-Unit7) Unit 1 Section A 时间观念强的美国人 Para. 1 美国人认为没有人能停止不前。如果你不求进取,你就会落伍。这种态度造就了一个投身于研究、实验和探索的民族。时间是美国人注意节约的两个要素之一,另一个是劳力。 Para. 2 人们一直说:“只有时间才能支配我们。”人们似乎是把时间当作一个差不多是实实在在的东西来对待的。我们安排时间、节约时间、浪费时间、挤抢时间、消磨时间、缩减时间、对时间的利用作出解释;我们还要因付出时间而收取费用。时间是一种宝贵的资源,许多人都深感人生的短暂。时光一去不复返。我们应当让每一分钟都过得有意义。 Para. 3 外国人对美国的第一印象很可能是:每个人都匆匆忙忙——常常处于压力之下。城里人看上去总是在匆匆地赶往他们要去的地方,在商店里他们焦躁不安地指望店员能马上来为他们服务,或者为了赶快买完东西,用肘来推搡他人。白天吃饭时人们也都匆匆忙忙,这部分地反映出这个国家的生活节奏。工作时间被认为是宝贵的。Para. 3b 在公共用餐场所,人们都等着别人吃完后用餐,以便按时赶回去工作。你还会发现司机开车很鲁莽,人们推搡着在你身边过去。你会怀念微笑、简短的交谈以及与陌生人的随意闲聊。不要觉得这是针对你个人的,这是因为人们非常珍惜时间,而且也不喜欢他人“浪费”时间到不恰当的地步。 Para. 4 许多刚到美国的人会怀念诸如商务拜访等场合开始时的寒暄。他们也会怀念那种一边喝茶或咖啡一边进行的礼节性交流,这也许是他们自己国家的一种习俗。他们也许还会怀念在饭店或咖啡馆里谈生意时的那种轻松悠闲的交谈。一般说来,美国人是不会在如此轻松的环境里通过长时间的闲聊来评价他们的客人的,更不用说会在增进相互间信任的过程中带他们出去吃饭,或带他们去打高尔夫球。既然我们通常是通过工作而不是社交来评估和了解他人,我们就开门见山地谈正事。因此,时间老是在我们心中的耳朵里滴滴答答地响着。 Para. 5 因此,我们千方百计地节约时间。我们发明了一系列节省劳力的装置;我们通过发传真、打电话或发电子邮件与他人迅速地进行交流,而不是通过直接接触。虽然面对面接触令人愉快,但却要花更多的时间, 尤其是在马路上交通拥挤的时候。因此,我们把大多数个人拜访安排在下班以后的时间里或周末的社交聚会上。 Para. 6 就我们而言,电子交流的缺乏人情味与我们手头上事情的重要性之间很少有或完全没有关系。在有些国家, 如果没有目光接触,就做不成大生意,这需要面对面的交谈。在美国,最后协议通常也需要本人签字。然而现在人们越来越多地在电视屏幕上见面,开远程会议不仅能解决本国的问题,而且还能通过卫星解决国际问题。

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