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Killing spinor equations in dimension 7 and geometry of integrable G_2-manifolds

Killing spinor equations in dimension 7 and geometry of integrable G_2-manifolds
Killing spinor equations in dimension 7 and geometry of integrable G_2-manifolds

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2201v 1 [m a t h .D G ] 19 D e c 2001KILLING SPINOR EQUATIONS IN DIMENSION 7AND GEOMETRY OF

INTEGRABLE G 2-MANIFOLDS

THOMAS FRIEDRICH AND STEF AN IVANOV Abstract.We compute the scalar curvature of 7-dimensional G 2-manifolds admitting a connection with totally skew-symmetric torsion.We prove the formula for the general so-lution of the Killing spinor equation and express the Riemannian scalar curvature of the solution in terms of the dilation function and the NS 3-form ?eld.In dimension n =7the dilation function involved in the second fermionic string equation has an interpretation as a conformal change of the underlying integrable G 2-structure into a cocalibrated one of pure type W 3.Contents 1.Introduction 12.General properties of G 2-structures 33.Conformal transformations of G 2-structures 44.Connections with torsion,parallel spinors and Riemannian scalar curvature 55.Solutions to the Killing spinor equations in dimension 77References 81.Introduction Riemannian manifolds admitting parallel spinors with respect to a metric connection with totally skew-symmetric torsion became a subject of interest in theoretical and mathematical physics recently.One of the main reasons is that the number of preserved supersymmetries in string theory depends essentially on the number of parallel spinors.In 10-dimensional string theory,the Killing spinor equations with non-constant dilation Φand the 3-form ?eld strength H can be written in the following way [39],(see [25,24,16])(?)?Ψ=0,(d Φ?1

Received by the editors 1st February 2008.

Key words and phrases.G 2-structures,string equations.

Supported by the SFB 288”Di?erential geometry and quantum physics”of the DFG and the European Human Potential Program EDGE,Research Training Network HPRN-CT-2000-00101.S.Ivanov thanks ICTP for the support and excellent environment.

1

2THOMAS FRIEDRICH AND STEFAN IV ANOV

problems in string theory[32,37,21].One possible generalization of Calabi-Yau manifolds, hyper-K¨a hler manifolds,parallel G2-manifolds and parallel Spin(7)-manifolds are manifolds equipped with linear metric connections having skew-symmetric torsion and holonomy con-tained in SU(n),Sp(n),G2,Spin(7).One remarkable fact is that the existence(in small dimen-sions)of a parallel spinor with respect to a metric connection?with skew-symmetric torsion determines the connection in a unique way if its holonomy group is a subgroup of SU,Sp,G2, provided that some additional di?erential conditions on the structure are ful?lled[39,16],and always in dimension8for a subgroup of the group Spin(7)[23].The case of16-dimensional Riemannian manifolds with Spin(9)-structure was investigated in[13],homogeneous models are discussed in[2].The existence of?-parallel spinors in the dimensions4,5,6,7,8is studied in [39,10,24,16,17,23].In dimension7,the?rst consequence is that the manifold should be a G2-manifold with an integrable G2-structure[16],i.e.,the structure group could be reduced to the group G2and the corresponding3-formω3should obey d?ω3=θ∧?ω3for some special 1-formθ.In this paper we study solutions to the Killing spinor equations(?)in dimension 7and the geometry of integrable G2-manifolds.We?nd a formula for the Riemannian scalar curvature in terms of the fundamental3-form.Our?rst main result is the following Theorem1.1.Let(M,g,ω3)be an integrable G2-manifold with the fundamental3-formω3. The Riemannian scalar curvature Scal g is given in terms of the fundamental3-formω3by

Scal g=1

12

||T||2+3δθ,

(1.1)

whereθand T are the Lee form and the torsion of the unique G2-connection given by

(1.2)T=??dω3+1

3

?(?dω3∧ω3)=

1

12

·||T||2?6·△Φ,

where△Φ=δdΦis the Laplacian.The solution has constant dilation if and only if the G2-structure is cocalibrated of pure type W3.

Our proof relies on the existence theorem for a G2-connection with torsion,the Schr¨o dinger-Lichnerowicz formula for the connection with torsion(both established in[16])and the special properties of the Cli?ord action on the special parallel spinor.

KILLING SPINOR EQUATIONS IN DIMENSION7AND GEOMETRY OF INTEGRABLE G2-MANIFOLDS3

2.General properties of G2-structures

Let us consider R7endowed with an orientation and its standard inner product.Denote an oriented orthonormal basis by e1,...,e7.We shall use the same notation for the dual basis. We denote the monomial e i∧e j∧e k by e ijk.Consider the3-formω3on R7given by

(2.6)

ω3=e127+e135?e146?e236?e245+e347+e567.

The subgroup of SO(7)that?xesω3is the exceptional Lie group G2.It is a compact,simply-connected,simple Lie group of dimension14[34].The3-formω3corresponds to a real spinor and,therefore,G2is the isotropy group of a non-trivial real spinor.A G2-structure on a7-manifold M7is a reduction of the structure group of the tangent bundle to the exceptional group G2.This can be described geometrically by a nowhere vanishing di?erential3-formω3 on M7,which can be locally written as(2.6).The3-formω3is called the fundamental form of the G2-manifold M7(see[3])and it determines the metric completely.The action of G2on the tangent space gives an action of G2on k-forms and we obtain the following splitting[11,6]:Λ1(M7)=Λ17,Λ2(M7)=Λ27⊕Λ214,Λ3(M7)=Λ31⊕Λ37⊕Λ327,

where

Λ27={α∈Λ2(M7)|?(α∧ω3)=2α},Λ214={α∈Λ2(M7) ?(α∧ω3)=?α},Λ37={?(β∧ω3)|β∈Λ1(M7)},Λ327={γ∈Λ3(M7)|γ∧ω3=0,γ∧?ω3=0}. Following[8]we consider the1-formθde?ned by

(2.7)3θ=??(?dω3∧ω3)=?(δω3∧?ω3).

We shall call this1-form the Lee form associated with a given G2-structure.If the Lee form vanishes,then we shall call the G2-structure balanced.The classi?cation of the di?erent types of G2-structures was worked out by Fernandez-Gray[11],and Cabrera used the Lee form to characterize each of the16classes.An integrable G2-structure(or a structure of type W1⊕W3⊕W4)is characterized by the di?erential equation

d?ω3=θ∧?ω3,

and a cocalibrated G2-structure is de?ned by the condition

d?ω3=0.

A cocalibrated G2-structure of pure type W3is characterized by the two condtions d?ω3= 0,dω3∧ω3=0.Then the following proposition follows immediately.

Proposition2.1.If the Lee1-form is closed,then the G2-structure is locally conformal to a balanced G2-structure.

We shall call locally conformally parallel G2-manifolds that are not globally conformally parallel strict locally conformally parallel.

Example2.1.Any7-dimensional oriented spin Riemannian manifold admits a certain G2-structure,in general a non-parallel one(see for example[29]).The?rst known examples of complete parallel G2-manifold were constructed by Bryant and Salamon[7],the?rst compact examples by Joyce[26,27,28].There are many known examples of compact nearly parallel G2-manifolds:S7[11],SO(5)/SO(3)[7,35],the Alo?-Wallach spaces N(g,l)=SU(3)/U(1)g,l [9],any Einstein-Sasakian and any3-Sasakian space in dimension7[14,15].There are also some non-regular3-Sasakian manifolds(see[4,5]).Moreover,compact nearly parallel G2-manifolds with large symmetry group are classi?ed in[15].Compact integrable nilmanifolds are constructed and studied in[12].Any minimal hypersurface N in R8admits a cocalibrated G2-structure[11].Moreover,the structure is parallel,nearly parallel,cocalibrated of pure type if and only if the hypersurface N is totally geodesic,totally umbilic or minimal,respectively.

4THOMAS FRIEDRICH AND STEFAN IV ANOV

3.Conformal transformations of G2-structures

We study the conformal transformation of G2-structures(see[11]).

Proposition3.1.Letˉg=e2f·g,ˉω3=e3f·ω3be a conformal change of a G2-structure(g,ω3) and denote byˉθ,θthe corresponding Lee forms,respectively.Then

(3.8)ˉθ=θ+4d f.

Proof.We have the relations

volˉg=e7f·vol g,dˉω3=e3f·(3d f∧ω3+dω3).

We calculate

ˉ?dˉω3=e4f(?dω3+3?(d f∧ω3)),ˉ?dˉω3∧ˉω3=e7f(?dω3∧ω3?12?d f),

where we used the general identity?(ω3∧γ)∧ω3=4?γ,which is valid for any1-formγ. Consequently,we obtainˉθ=?1

3 ?(?dω3∧ω3)?12?2d f =θ+4d f. Proposition3.1allows us to?nd a distinguished G2-structure on a compact7-dimensional G2-manifold.

Theorem3.1.Let(M7,g,ω3)be a compact7-dimensional G2-manifold.Then there exists a unique(up to homothety)conformal G2-structure g0=e2f·g,ω30=e3f·ω3such that the corresponding Lee form is coclosed,δ0θ0=0.

Proof.We shall use the Gauduchon Theorem for the existence of a distinguished metric on a compact,hermitian or Weyl manifold[19,20].We shall use the expression of this theorem in terms of a Weyl structure(see[40],Appendix1).We consider the Weyl manifold(M7,g,θ,?W) with the Weyl1-formθ,where?W is a torsion-free linear connection on M7determined by the condition?W g=θ?g.Applying the Gauduchon Theorem we can?nd,in a unique way, a conformal metric g0such that the corresponding Weyl1-form is coclosed with respect to g0. The key point is that,by Proposition3.1,the Lee form transforms under conformal rescaling according to(3.8),which is exactly the transformation of the Weyl1-form under conformal rescaling of the metricˉg=e4f·g.Thus,there exists(up to homothety)a unique conformal G2-structure(g0,ω30)with coclosed Lee form. We shall call the G2-structure with coclosed Lee form the Gauduchon G2-structure. Corollary3.1.Let(M7,g,Φ)be a compact G2-manifold and(g,Φ)be the Gauduchon struc-ture.Then the following formula holds:

? dδω3∧?ω3 =||δω3||2.

In particular,if the structure is integrable,then

? dδω3∧?ω3 =24||θ||2.

https://www.doczj.com/doc/301603879.html,ing(2.7),we calculate that

0=3·δθ=?d(δω3∧?ω3)=? dδω3∧?ω3??d?ω3∧d?ω3 =? dδω3∧?ω3?||δω3||2·vol . If the structure is integrable,then||δω3||2=24||θ||2. Corollary3.2.On a compact G2-manifold with closed Lee form whose Gauduchon G2-structure is not balanced,the?rst Betti number satis?es b1(M)≥1.

For integrable G2-manifolds one can de?ne a suitable elliptic complex as well as cohomolgy groups?H i(M7)(see[12]).The?rst cohomolgy group is given by

?H1(M7)={α∈Λ1(M7):dα∧?ω3=0,d?α=0}.

KILLING SPINOR EQUATIONS IN DIMENSION7AND GEOMETRY OF INTEGRABLE G2-MANIFOLDS5 Corollary3.3.On a compact integrable manifold which is not globally conformally balanced, one has?b1≥1.

Proof.By the condition of the theorem the Gauduchon structure has a non-identically zero Lee form.Then0=δω3=?(dθ∧?ω3),since the structure is integrable.Adding the condition δθ=0,we obtain?b1≥1.

4.Connections with torsion,parallel spinors and Riemannian scalar curvature The Ricci tensor of an integrable G2-manifold was expressed in principle by the structure form ω3in the paper[16].Here we intend to?nd an explicit formula for the Riemannian scalar https://www.doczj.com/doc/301603879.html,ing the unique connection with skew-symmetric torsion preserving the given integrable G2-structure found in[16],we apply the Schr¨o dinger-Lichnerowicz formula for the Dirac operator of a metric connection with totally skew-symmetric torsion(see[16])in order to derive the formula for the scalar curvature.First,let us summarize the mentioned results from[16].

Theorem4.1.(see[16])Let(M7,g,ω3)be a G2-manifold.Then the following conditions are equivalent:

(1)The G2-structure is integrable,i.e.,d?ω3=θ∧?ω3;

(2)There exists a unique linear connection?preserving the G2-structure with totally skew-

symmetric torsion T given by

(4.9)T=??dω3+

1

7·(dω3,?ω3)?ω3,π47(dω3)=

3

6·λ·Ψ0?θ·Ψ0,λ=?

1

4

||T||2.

The4-formσT de?ned by the formula

σT=

1

6THOMAS FRIEDRICH AND STEFAN IV ANOV

Theorem 4.2.(see [16])Let Ψbe

a

parallel

spinor with respect to a metric connection ?

with totally

skew-symmetric torsion T on a Riemannian spin manifold M n .Then the following formulas hold

3·dT ·Ψ?2·σT ·Ψ+Scal ·Ψ=0,D(T ·Ψ)=dT ·Ψ+δT ·Ψ?2·σT ·Ψ.

Proof of Theorem 1.1.Let Ψ0be the ?-parallel spinor corresponding to the fundamental 3-form ω3.Then the Riemannian Dirac operator D g and the Levi-Civita connection ?g act on Ψ0by the rule

(4.12)?g X Ψ0=?14·T ·Ψ0=?74

·θ·Ψ0,where we used Theorem 4.1.We are going to apply the well known Schr¨o dinger-Lichnerowicz formula [31,38]

(D g )2=△g +1

8·D g λ·Ψ0 +364·λ2+94·δθ ·Ψ0?74·dθ·Ψ0+3

4

·n i =1 ?e i i e i T )·Ψ0?14·δT ·Ψ0?1

2·||T ||2

·Ψ0.Substituting (4.13)and (4.14)into the SL-formula,multiplying the obtained result by Ψ0and taking the real part,we arrive at (4.15) 4916·||θ||2+3322+18

·(σT ·Ψ0,Ψ0).On the other hand,using (4.10),we obtain

D(T ·Ψ0)=D(7

6·λ·Ψ0?θ·Ψ0)=7

6dλ

·Ψ0?d ?θ·Ψ0?δθ·Ψ0=dT ·Ψ0?2σT ·Ψ0+δT ·Ψ0.Multiplying the latter

equality by Ψ0and taking the real part,we obtain ?δθ·||Ψ0||2=(dT ·Ψ0,Ψ0)?(2σT ·Ψ0,Ψ0).Consequently,Theorem (4.2)and (4.11)imply (4.16) ?3·δθ?112·||dω3||2.

KILLING SPINOR EQUATIONS IN DIMENSION7AND GEOMETRY OF INTEGRABLE G2-MANIFOLDS7 Proof.In the case of a cocalibrated G2-structure of pure type,the torsion3-form T=??dω3. The claim follows from Theorem1.1. Using the results in[11]we derive immediately the following formula,which is essentially the reformulated Gauss equation.

Corollary4.4.Let M7be a hypersurface in R8the with second fundamental form S and mean curvature H.Then the Riemannian scalar curvature on M7is given by the formula

Scal g=49

12

·||S0||2,

(4.17)

where S0is the image of the traceless part of the second fundamental form via the isomorphism S20(R7)→Λ327.In particular,if M is a minimal hypersurface,then

Scal g=?

1

2||θ||2since the structure is locally conformally parallel.Then,Theo-

rem1.1leads to the formula

(4.19)Scal g=

15

6 M||θ||2d vol>0,

since the structure is strictly locally conformally parallel.The second assertion is a consequence of Corollary3.2.

5.Solutions to the Killing spinor equations in dimension7

We consider the Killing spinor equations(?)in dimension7.The existence of a?-parallel spinor is equivalent to the existence of a?-parallel integrable G2-structure and the3-form?eld strength H=T is given by(4.9).We now investigate the second Killing spinor equation(?). Proof of Theorem1.2.LetΨbe an arbitrary?-parallel such that(dΦ?T)·Ψ=0.The spinor ?eldΨde?nes a second G2-structureω30such thatΨ=Ψ0is the canonical spinor?eld.Since the connection preserves the spinor?eldΨ,it preserves the G2-structureω30,too.On the other hand,the connection preservingω30is unique.Consequently,the torsion T0coincides with the torsion form T and for the G2-structureω30we have

?Ψ0=0,(dΦ?T0)·Ψ0=0.

The Cli?ord action T0·Ψ0depends only on the(Λ31⊕Λ37)-part of https://www.doczj.com/doc/301603879.html,ing(4.9)and the algebraic formulas

?(γ∧ω30)·Ψ0=?γ(?ω30)·Ψ0=?4·γ·Ψ0,ω30·Ψ0=?7·Ψ0

we calculate

(5.20)T0·Ψ0=?θ·Ψ0?

1

8THOMAS FRIEDRICH AND STEFAN IV ANOV

Comparing with the second Killing spinor equation(?)we?nd2·dΦ=?β,(dω30,?ω30)=0 which completes the proof. As a corollary we obtain the result from[21],which states that any solution to both equations (?)has necessarily the NS three form H=T given by(1.4).A more precise analysis using Proposition3.1and Theorem1.1of the explicit solutions constructed in[21]shows that these solutions are conformally equivalent to a cocalibrated structure of pure type.In other words, the multiplication of the G2-structures(g±,ω3±)by(eΦ·g±,e(3/2)Φ·ω3±)is a new example of a cocalibrated G2-structure of pure type W3,and it is a solution to the Killing spinor equations with constant dilation.The same conclusions are valid for the solutions constructed in[1,37,32]. Theorem1.2allows us to construct a lot of compact solutions to the Killing spinor equations.If the dilation is a globally de?ned function,then any solution is globally conformally equivalent to a cocalibrated G2-structure of pure type.For example,any conformal transformation of a compact7-dimensional manifold with a Riemannian holonomy group G2constructed by Joyce [26,27]is a solution with non-constant dilation.Another source of solutions are conformal transformations of the cocalibrated G2-structures of pure type W3induced on any minimal hypersurface in R8.Summarizing,we obtain:

Corollary5.1.Any solution(M7,g,ω3)to the Killing spinor equations(?)in dimension7with non-constant globally de?ned dilation functionΦcomes from a solution with constant dilation by a conformal transformation(g=eΦ·g0,ω3=e(3/2)Φ·ω30),where(g0,ω30)is a cocalibrated G2-structure of pure type W3.

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Thomas Friedrich

Institut f¨u r Reine Mathematik

Humboldt-Universit¨a t zu Berlin

Sitz:WBC Adlershof

D-10099Berlin,Germany

friedric@mathematik.hu-berlin.de

Stefan Ivanov

F aculty of Mathematics and Informatics

University of Sofia“St.Kl.Ohridski”

blvd.James Bourchier5

1164Sofia,Bulgaria

ivanovsp@fmi.uni-sofia.bg

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JOIN IN 学生用书1 Word List Starter Unit 1.Good afternoon 下午好 2.Good evening 晚上好 3.Good morning 早上好 4.Good night 晚安 5.Stand 站立 Unit 1 6.count [kaunt] (依次)点数 7.javascript:;eight [eit] 八 8.eleven [i'levn] 十一 9.four [f?:] 四 10.five [faiv] 五 11.flag [fl?g] 旗 12.guess [ges] 猜 13.jump [d??mp] 跳 14.nine [nain] 九 15.number ['n?mb?] 数字 16.one [w?n] 一 17.seven ['sevn] 七 18.six [siks] 六 19.ten [ten] 十 20.three [θri:] 三 21.twelve [twelv] 十二 22.two [tu:] 二 23.your [ju?] 你的 24.zero ['zi?r?u] 零、你们的 Unit 2 25.black [bl?k] 黑色26.blue [blu:] 蓝色 27.car [kɑ:] 小汽车 28.colour ['k?l?] 颜色 29.door [d?:] 门 30.favourite [feiv?rit]javascript:; 特别喜爱的 31.green [gri:n] 绿色 32.jeep [d?i:p] 吉普车 33.orange ['?:rind?] 橙黄色 34.pin k [pi?k] 粉红色 35.please [pli:z] 请 36.purple ['p?:pl] 紫色 37.red [red] 红色 38.white [wait] 白色 39.yellow ['jel?u] 黄色 Unit 3 40.blackboard ['bl?kb?:d] 黑板 41.book [buk] 书 42.chair [t???] 椅子 43.desk [desk] 桌子 44.pen [pen] 钢笔 45.pencil ['pensl] 铅笔 46.pencil case [keis] 笔盒 47.ruler ['ru:l?] 尺、直尺 48.schoolbag [sku:l] 书包 49.tree [tri:] 树 50.window ['wind?u] 窗、窗口 Unit 4 51.brown [braun] 棕色 52.cat [k?t] 猫

joinin剑桥小学英语

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Join In剑桥小学英语.doc

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2011-2012 学年度上学期六年级复习题(Unit2-Unit3 ) 一、听力部分 1、听录音排序 ( ) () ()() () 2、听录音,找出与你所听到的单词属同一类的单词 () 1. A. spaceman B. pond C . tiger () 2. A.mascots B. potato C . jeans () 3. A. door B. behind C . golden () 4. A. sometimes B. shop C . prince () 5. A. chair B. who C . sell 3、听录音,将下面人物与他的梦连线 Sarah Tim Juliet Jenny Peter 4、听短文,请在属于Mr. Brown的物品下面打√ ( ) ( ) ( ) ( ) ( ) ( ) ( ) 5、听问句选答句 () 1. A. Yes, I am B. Yes, I have C . Yes, you do () 2. A.Pink B. A friendship band C . Yes. () 3. A. OK B. Bye-bye. C . Thanks, too. () 4. A. Monday. B. Some juice. C . Kitty. () 5. A. I ’ve got a shookbag. B. I ’m a student. C . It has got a round face. 6、听短文,选择正确答案 () 1. Where is Xiaoqing from? She is from . A.Hebei B. Hubei C . Hunan () 2. She goes to school at . A.7:00 B.7:30 C . 7:15 () 3. How many classes in the afternoon? classes. A. four B. three C . two () 4. Where is Xiaoqing at twelve o ’clock? She is . A. at home B. at school C .in the park () 5. What does she do from seven to half past eight? She . A.watches TV B. reads the book C. does homework

三年级下学期英语(Joinin剑桥英语)全册单元知识点归纳整理-

Starter Unit Good to see you again知识总结 一. 短语 1. dance with me 和我一起跳舞 2. sing with me 和我一起唱歌 3. clap your hands 拍拍你的手 4. jump up high 高高跳起 5.shake your arms and your legs晃晃你的胳膊和腿 6. bend your knees 弯曲你的膝盖 7. touch your toes 触摸你的脚趾8. stand nose to nose鼻子贴鼻子站 二. 句子 1. ---Good morning. 早上好。 ---Good morning, Mr Li. 早上好,李老师。 2. ---Good afternoon. 下午好。 ---Good afternoon, Mr Brown. 下午好,布朗先生。 3. ---Good evening,Lisa. 晚上好,丽莎。 ---Good evening, Bob. 晚上好,鲍勃。 4. ---Good night. 晚安。 ----Good night. 晚安。 5. ---What’s your name? 你叫什么名字? ---I’m Bob./ My name is Bob. 我叫鲍勃。 6. ---Open the window, please. 请打开窗户。 ---Yes ,Miss. 好的,老师。 7. ---What colour is it? 它是什么颜色? 它是蓝红白混合的。 ---It’s blue, red and white. 皮特的桌子上是什么? 8. ---What’s on Pit’s table? ---A schoolbag, an eraser and two books. 一个书包,一个橡皮和两本书。 9. ---What time is it? 几点钟? 两点钟。 ---It’s two. 10.---What’s this? 这是什么? ---My guitar. 我的吉他。

10 Reaction Equations要点

10. REACTION EQUATIONS Clicking the Reaction Equations button in the main menu shows the Reaction Equations Window, see Fig. 1. With this calculation option you can calculate the heat capacity, enthalpy, entropy and Gibbs energy values of a single species as well as of specified reactions between pure substances. See the reference state definitions, valid notations and abbreviations for the description of the chemical formulae in Chapter 28. Databases, chapter 2. 10.1 One Chemical Substance Fig. 1. Reaction Equations Window of HSC Chemistry.

Fig. 2.Thermodynamic data of A12O3 (alumina) displayed by the Reaction Equation option of HSC Chemistry. By entering a single chemical formula into the Formula box you will get similar tables of thermochemical data as presented in many thermochemical data books. HSC will, however, provide the results faster and exactly at those temperatures which you really want. Please follow these steps: 1.Write a chemical formula into the box, Fig. 1. For example: Fe, Na2SO4, Al2O3, SO4(-a), H(+a) or SO2(g). See the valid notation and syntax of chemical formulae in Chapter 21.2. 2.Select the lower limit, upper limit and temperature step. 3.Select the Temperature and Energy Units, by clicking the corresponding buttons. 4.Select the Format of the results. Normal (Absolute scale): H(species), S(species) and C(species) This format is used for example in the famous I. Barin, O. Knacke, and O. Kubaschewski data compilation1. Delta (Formation functions):

外研社剑桥小学英语Join_in四年级上册整体课时教案

外研社剑桥小学英语Join_in四年级上册整体课时教案Starter Unit Let's begin 第一学时: The pupils learn to understand: How are you today? I’m fine/OK. Goodbye. The pupils learn to use: What’s your name? I’m (Alice). How are you? I’m fine. I’m OK. Activities and skills: Decoding meaning from teacher input. Using phrases for interaction in class. Greeting each other. I Introduce oneself. Asking someone’s mane. Teaching process: Step 1: Warm—up. Sing a song. Hello, what’s your name? Step 2: Presentation. 1. What’s your name? I’m…. (1) The teacher introduces herself, saying: Hello, /Good morning, I’m Miss Sun. (2) Asks a volunteer’s name:

What’s your name? The teacher prompt the pupil by whispering, I’m (Alice). (3) Asks all the pupils the same question and help those who need it by whispering I’m…. 2. How are you today? I’m fine. I’m OK. (1) The teacher explains the meaning of How are you today? (2) Tell the class to ask the question all together and introduce two answers, I’m (not very) fine/I’m Ok. (3) Asks all the pupils the same question and make sure that all the students can reply. Step3: Speak English in class. 1. Tells the pupils to open their books at page3, look at the four photographs, and listen to the tape. 2. Asks the pupils to dramatise the situations depicted in the four photographs. A volunteer will play the part of the parts of the other pupils, answering as a group. 第二学时: The pupils learn to use these new words: Sandwich, hamburger, hot dog, puller, cowboy, jeans, cinema, walkman, snack bar, Taxi, clown, superstar.

剑桥英语JOININ三年级上册知识点(供参考)

Join in三年级上册知识点 1.见面打招呼 Hello! = Hi! 你好 Good morning! 早上好! Good afternoon! 下午好! Good evening! 晚上好! (注意:Good night的意思是“晚安”) 2.询问身体健康状况 How are you? 你好吗? I’m fine. = I’m OK.我很好。 3.临走分别 Goodbye. = Bye bye. 再见。 See you tomorrow. 明天见。 4.Miss小姐Mr先生 5.询问名字 -What’s your name? 你叫什么名字? -I’m Toby. = My name is Toby. = Toby.我叫托比。 6.Let’s+动词原形 如Let’s go! 我们走吧! Let’s begin! 我们开始吧! 7. Are you ready? 你准备好了吗? I’m ready. 我准备好了。 8.十二个动词 look看listen听mime比划着表达speak讲read读write写draw画colour涂sing唱think想guess猜play玩9.询问物体 -What’s this? 这是什么? -It’s my dog. / It’s a dog. / My dog. 这是我的狗。 10.my/your+名词 如my apple我的苹果 your apple你的苹果 11.数字0-10 zero零one一two二three三four四five五six六seven七eight八nine九ten十12.询问电话号码 -What’s your phone number? 你的电话号码是多少? -It’s . / . 13.guess sth 猜东西 如Guess the number. 猜数字 14. What’s in the box? 盒子里有什么? 15.询问数量 -How many? 多少? -Nine. 九个。 16. Here is / are sth. 这是……

代理公司注册登记协议书简易版

It Is Necessary To Clarify The Rights And Obligations Of The Parties, To Restrict Parties, And To Supervise Both Parties To Keep Their Promises And To Restrain The Act Of Reckless Repentance. 编订:XXXXXXXX 20XX年XX月XX日 代理公司注册登记协议书 简易版

代理公司注册登记协议书简易版 温馨提示:本协议文件应用在明确协议各方的权利与义务、并具有约束力和可作为凭证,且对当事人双方或者多方都有约制性,能实现监督双方信守诺言、约束轻率反悔的行为。文档下载完成后可以直接编辑,请根据自己的需求进行套用。 代理公司注册登记协议书 甲方:_________ 地址:_________ 电话:_________ 联系人:_________ 乙方:_________ 地址:_________ 电话:_________ 联系人:_________ 为了充分发挥_________的资源和信息服务优势,甲、乙双方经过友好协商,本着平等互利、友好合作的意愿达成本协议书,并郑重声

明共同遵守: 一、甲方同意按照本协议的规定,授权乙方为其代办公司注册手续。 二、乙方提供的代办咨询服务范围仅限如下: 1.为甲方代办工商营业执照、组织机构代码证、税务证、三章(法人章、公章、财务章); 2.约定的其他服务: _________。 三、甲方的责任: 1.甲方应指定专人配合乙方完成新企业工商登记注册等事务,并提供齐全的证件和规范的法律文件资料。 2.甲方对提供的证件和法律文件资料的真实性、正确性、合法性承担全部责任。

【精品】joinin英语剑桥版五年级(上)单词表

beautiful美丽的,美好的 clean(把。。。)弄干净 hard费劲地;费力地 learn学习;学会 New South Wales新南威尔士州 soon不久,很快 summer holiday暑假 take拍摄 take photos拍照 time一段时间;某段日子 the UK英国 umbrella雨伞 whose谁的 work工作,劳动 both两者,两个都 change转变;转换 come in 进来 come on快点 cook煮,烧;厨师 cousin堂(表)兄弟;表姐妹doctor医师,大夫 driver司机、驾驶员 family家庭 fantastic太好了;极好的 famer农民 grandfather祖父;外祖父 grandmother祖母;外祖母 grandparent祖父;外祖父;祖母;外祖母granny奶奶;外婆 introduce介绍,引见 Little Red Riding Hood小红帽 member成员 nurse护士 phone电话 police警察 problem问题,难题 role角色 run away逃跑 scene一场 taxi出租车 these这些 walk off离开 woods小树林,林地 word字、单词 worker工人 always总是,每次都 band圈,箍,带 because因为

bell铃 bring带来 cool冷静的,沉着的darling亲爱的,宝贝儿dollar美元 easy不担心的,不紧张的everywhere处处 friendship友谊 hurt弄伤; luck好运;幸运 mascot吉祥物 necklace项链 Olympic奥运会的 popular受欢迎的 Puma Ranch美洲狮大牧场 ring戒指 shell贝壳 silver银制的;银色的soft toy毛绒玩具 test测验 watch out小心 answer答案 athlete运动员 collect收集采集 cyclist骑自行车者 end结束;停止 go开始(做某事)kilometre千米,公里 opera house歌剧院 quarter一刻钟,十五分钟say说 special特殊的,特别的spot圆点,斑点 stamp邮票 tell告诉 time次,回 top最佳的,最好的train火车,列车 Yours您真挚的autograph亲笔签名 comic连环画 email电子邮件 for为了要;为了得到gone走了;不见了 hat帽子 postcard明信片 sticker贴纸 take接受

Part1OrdinaryDifferentialEquations(常微分方程式微分变数只有一个)

Chapter 1 First-Order ODEs C C h h a a p p t t e e r r 22 S S e e c c o o n n d d --O O r r d d e e r r L L i i n n e e a a r r O O D D E E s s ((二二階階線線性性常常微微分分方方程程式式)) Chapter 3 Higher-Order Linear ODEs Chapter 5 Series Solutions of ODEs Chapter 6 Laplace Transforms ? Ordinary differential equations may be divided into two large classes, linear (線性) and nonlinear (非線性) ODEs. Where nonlinear ODEs are difficult to solve, linear ODEs are much simpler because there are standard methods for solving many of these equations. 22..11 H H o o m m o o g g e e n n e e o o u u s s L L i i n n e e a a r r O O D D E E s s o o f f S S e e c c o o n n d d O O r r d d e e r r ((二二階階線線性性齊齊性性微微分分方方程程式式)) ? A second-order ODE is called linear (線性的) if it can be written as ()()()y p x y q x y r x '''++=. (1) ? 線性:方程式的每一項都不得出現()y x 和其導數(y ', y '',…)的乘積或自乘 In case ()0r x =, the equation is called homogeneous (齊性的). In case ()0r x ≠, the equation is called nonhomogeneous (非齊性的). The functions ()p x and ()q x are called the coefficients of the ODEs. ? Theorem 1 Superposition Principle for the Homogeneous Linear ODE (適用於線性 齊性常微分方程式的疊加原理) If both 1()y x and 2()y x are solutions of the homogeneous linear ODE ()()0y p x y q x y '''++=, (2) then a linear combination (線性組合) of 1y and 2y , say 1122()()c y x c y x +, is also a solution of the differential equation. Proof –

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