Lie conformal algebras and the variational complex
|
|
- Wilfrid Carpenter
- 5 years ago
- Views:
Transcription
1 Le conformal algebras and the varatonal complex UMN Math Physcs Semnar February 10, 2014
2 Outlne Varatonal complex: a quck remnder Le conformal algebras and ther cohomology The varatonal complex as a LCA cohomology complex. References: 1 Alberto De Sole, Vctor Kac, Le conformal algebra cohomology and the varatonal complex 2 AS, VK, Alaa Barakat, Posson vertex algebras n the theory of Hamltonan equatons 3 AS, VK, The varatonal Posson cohomology 4 Bojko Bakalov, VK, Alexander Voronov, Cohomology of conformal algebras UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
3 Varatonal complex Recall: f u(x) = (u 1 (x), u 2 (x),..., u k (x)) s an extremum of a varatonal functonal L[u] = I f(x, u, u, u,... ) dx, then δf δu := n ( ) n f δf δu := = 0, = d dx δf δu 1... δf δu k s the Euler-Lagrange varatonal dervatve of f. ( = 1, 2,..., k) UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
4 Varatonal complex Recall: f u(x) = (u 1 (x), u 2 (x),..., u k (x)) s an extremum of a varatonal functonal L[u] = I f(x, u, u, u,... ) dx, then δf δu := n ( ) n f δf δu := = 0, = d dx δf δu 1... δf δu k s the Euler-Lagrange varatonal dervatve of f. ( = 1, 2,..., k) UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
5 Varatonal complex One easly checks that [ and, n partcular,, ] = δ (f) = 0. δu u (n 1) Example Takng f(u) = u2 2, ( δ δu (uu ) = u ) u +... (uu ) = u + (u) = 0 UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
6 Varatonal complex One easly checks that [ and, n partcular,, ] = δ (f) = 0. δu u (n 1) Example Takng f(u) = u2 2, ( δ δu (uu ) = u ) u +... (uu ) = u + (u) = 0 UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
7 Varatonal complex Q: Gven that δ δu (g) = 0, s g = f for some f? A: Yes, n some cases (for example, f f, g are polynomals n u, u, u,... ). δ Problem I: Descrbe the kernel of δu : V Vk for a more general space of functons V. δ Problem II: Descrbe the mage of δu n Vk. F 1 Theorem (Helmholtz): If F =... Im ( δ δu), then F k D F () = DF (), where the Frechet dervatve D F : V k V k s defned by (D F ()) j = n F u j n UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
8 Varatonal complex Q: Gven that δ δu (g) = 0, s g = f for some f? A: Yes, n some cases (for example, f f, g are polynomals n u, u, u,... ). δ Problem I: Descrbe the kernel of δu : V Vk for a more general space of functons V. δ Problem II: Descrbe the mage of δu n Vk. F 1 Theorem (Helmholtz): If F =... Im ( δ δu), then F k D F () = DF (), where the Frechet dervatve D F : V k V k s defned by (D F ()) j = n F u j n UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
9 Varatonal complex Q: Gven that δ δu (g) = 0, s g = f for some f? A: Yes, n some cases (for example, f f, g are polynomals n u, u, u,... ). δ Problem I: Descrbe the kernel of δu : V Vk for a more general space of functons V. δ Problem II: Descrbe the mage of δu n Vk. F 1 Theorem (Helmholtz): If F =... Im ( δ δu), then F k D F () = DF (), where the Frechet dervatve D F : V k V k s defned by (D F ()) j = n F u j n UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
10 Varatonal complex Puttng all that together, we obtan an exact sequence V/V u V k D() D () { Skew-symmetrc k-by-k dfferental matrces } These are the frst few terms of a larger varatonal complex. A geometrc approach (I.Anderson, W.Tulczyjew, A.Vnogradov,... ): thnk of the derham complex on the nfnte jet space of a bundle. A more algebrac approach (I.Gelfand, L.Dckey, I.Dorfman,... ): explot varous algebrac structures on the formal derham complex assocated wth V. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
11 Varatonal complex Puttng all that together, we obtan an exact sequence V/V u V k D() D () { Skew-symmetrc k-by-k dfferental matrces } These are the frst few terms of a larger varatonal complex. A geometrc approach (I.Anderson, W.Tulczyjew, A.Vnogradov,... ): thnk of the derham complex on the nfnte jet space of a bundle. A more algebrac approach (I.Gelfand, L.Dckey, I.Dorfman,... ): explot varous algebrac structures on the formal derham complex assocated wth V. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
12 Varatonal complex Puttng all that together, we obtan an exact sequence V/V u V k D() D () { Skew-symmetrc k-by-k dfferental matrces } These are the frst few terms of a larger varatonal complex. A geometrc approach (I.Anderson, W.Tulczyjew, A.Vnogradov,... ): thnk of the derham complex on the nfnte jet space of a bundle. A more algebrac approach (I.Gelfand, L.Dckey, I.Dorfman,... ): explot varous algebrac structures on the formal derham complex assocated wth V. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
13 Varatonal complex Defnton An algebra of dfferental functons V n the varables u 1,..., u k s a untal, commutatve, assocatve algebra equpped wth a dervaton : V V mutually commutng dervatons [ ] such that, and many s and n s. Example = u (n 1) f : V V, n Z + = 0 for all but fntely The polynomal algebra R k = C[u (n) ] =1,2,...,k;n Z+ wth := u (n+1) and usual dervatons. R k [x] wth (x) := 1 R k [log u, u 1 ] =1,2,...,k UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
14 Varatonal complex Defnton An algebra of dfferental functons V n the varables u 1,..., u k s a untal, commutatve, assocatve algebra equpped wth a dervaton : V V mutually commutng dervatons [ ] such that, and many s and n s. Example = u (n 1) f : V V, n Z + = 0 for all but fntely The polynomal algebra R k = C[u (n) ] =1,2,...,k;n Z+ wth := u (n+1) and usual dervatons. R k [x] wth (x) := 1 R k [log u, u 1 ] =1,2,...,k UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
15 Varatonal complex Defnton An algebra of dfferental functons V n the varables u 1,..., u k s a untal, commutatve, assocatve algebra equpped wth a dervaton : V V mutually commutng dervatons [ ] such that, and many s and n s. Example = u (n 1) f : V V, n Z + = 0 for all but fntely The polynomal algebra R k = C[u (n) ] =1,2,...,k;n Z+ wth := u (n+1) and usual dervatons. R k [x] wth (x) := 1 R k [log u, u 1 ] =1,2,...,k UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
16 Varatonal complex Defnton An algebra of dfferental functons V n the varables u 1,..., u k s a untal, commutatve, assocatve algebra equpped wth a dervaton : V V mutually commutng dervatons [ ] such that, and many s and n s. Example = u (n 1) f : V V, n Z + = 0 for all but fntely The polynomal algebra R k = C[u (n) ] =1,2,...,k;n Z+ wth := u (n+1) and usual dervatons. R k [x] wth (x) := 1 R k [log u, u 1 ] =1,2,...,k UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
17 Varatonal complex Defnton An algebra of dfferental functons V n the varables u 1,..., u k s a untal, commutatve, assocatve algebra equpped wth a dervaton : V V mutually commutng dervatons [ ] such that, and many s and n s. Example = u (n 1) f : V V, n Z + = 0 for all but fntely The polynomal algebra R k = C[u (n) ] =1,2,...,k;n Z+ wth := u (n+1) and usual dervatons. R k [x] wth (x) := 1 R k [log u, u 1 ] =1,2,...,k UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
18 Varatonal complex Defnton An algebra of dfferental functons V n the varables u 1,..., u k s a untal, commutatve, assocatve algebra equpped wth a dervaton : V V mutually commutng dervatons [ ] such that, and many s and n s. Example = u (n 1) f : V V, n Z + = 0 for all but fntely The polynomal algebra R k = C[u (n) ] =1,2,...,k;n Z+ wth := u (n+1) and usual dervatons. R k [x] wth (x) := 1 R k [log u, u 1 ] =1,2,...,k UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
19 Varatonal complex Defnton An algebra of dfferental functons V n the varables u 1,..., u k s a untal, commutatve, assocatve algebra equpped wth a dervaton : V V mutually commutng dervatons [ ] such that, and many s and n s. Example = u (n 1) f : V V, n Z + = 0 for all but fntely The polynomal algebra R k = C[u (n) ] =1,2,...,k;n Z+ wth := u (n+1) and usual dervatons. R k [x] wth (x) := 1 R k [log u, u 1 ] =1,2,...,k UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
20 Varatonal complex For an algebra of dfferental functons V n varables u 1,..., u k, we defne the varatonal dervatve δ δu : V Vk by δ δu (f) := n ( ) n f The derham complex over V s the free untal graded-commutatve assocatve algebra Ω (V) wth generators δu (n) of degree 1 ( = 1, 2,..., k, n Z + ). The dfferental δ on Ω (V) s defned by takng δ(f) := =1,2,...,k;n Z + f. δu (n) on f V and extendng further by the (graded) Lebnz rule. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
21 Varatonal complex For an algebra of dfferental functons V n varables u 1,..., u k, we defne the varatonal dervatve δ δu : V Vk by δ δu (f) := n ( ) n f The derham complex over V s the free untal graded-commutatve assocatve algebra Ω (V) wth generators δu (n) of degree 1 ( = 1, 2,..., k, n Z + ). The dfferental δ on Ω (V) s defned by takng δ(f) := =1,2,...,k;n Z + f. δu (n) on f V and extendng further by the (graded) Lebnz rule. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
22 Varatonal complex For an algebra of dfferental functons V n varables u 1,..., u k, we defne the varatonal dervatve δ δu : V Vk by δ δu (f) := n ( ) n f The derham complex over V s the free untal graded-commutatve assocatve algebra Ω (V) wth generators δu (n) of degree 1 ( = 1, 2,..., k, n Z + ). The dfferental δ on Ω (V) s defned by takng δ(f) := =1,2,...,k;n Z + f. δu (n) on f V and extendng further by the (graded) Lebnz rule. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
23 Varatonal complex Ω 0 (V)= V δ Ω 1 (V)=,n Vδu (n)... The C[]-acton on V = Ω 0 (V) can be extended to the entre complex Ω as an even dervaton and va (δu (n) ) = δu (n+1). Lemma commutes wth the dfferental δ. Defnton The varatonal complex over V s the quotent complex Ω (V) = Ω (V)/ Ω (V). UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
24 Varatonal complex Ω 0 (V)= V δ Ω 1 (V)=,n Vδu (n)... The C[]-acton on V = Ω 0 (V) can be extended to the entre complex Ω as an even dervaton and va (δu (n) ) = δu (n+1). Lemma commutes wth the dfferental δ. Defnton The varatonal complex over V s the quotent complex Ω (V) = Ω (V)/ Ω (V). UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
25 Varatonal complex Ω 0 (V)= V δ Ω 1 (V)=,n Vδu (n)... The C[]-acton on V = Ω 0 (V) can be extended to the entre complex Ω as an even dervaton and va (δu (n) ) = δu (n+1). Lemma commutes wth the dfferental δ. Defnton The varatonal complex over V s the quotent complex Ω (V) = Ω (V)/ Ω (V). UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
26 Varatonal complex Ω 0 (V)= V/V δ Ω 1 (V)= V k... 1 What s the cohomology of Ω (V)? 2 Do cochans and the dfferental operators of Ω (V) have a tangble nterpretaton? An algebra of dfferental functons V admts a fltraton by V n, = {f V f u (m) j = 0 for all(m, j) > (n, )} Theorem An algebra V s sad to be normal f If V s normal, then Ω (V) s exact. V n, = V n,. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
27 Varatonal complex Ω 0 (V)= V/V δ Ω 1 (V)= V k... 1 What s the cohomology of Ω (V)? 2 Do cochans and the dfferental operators of Ω (V) have a tangble nterpretaton? An algebra of dfferental functons V admts a fltraton by V n, = {f V f u (m) j = 0 for all(m, j) > (n, )} Theorem An algebra V s sad to be normal f If V s normal, then Ω (V) s exact. V n, = V n,. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
28 Varatonal complex Ω 0 (V)= V/V δ Ω 1 (V)= V k... 1 What s the cohomology of Ω (V)? 2 Do cochans and the dfferental operators of Ω (V) have a tangble nterpretaton? An algebra of dfferental functons V admts a fltraton by V n, = {f V f u (m) j = 0 for all(m, j) > (n, )} Theorem An algebra V s sad to be normal f If V s normal, then Ω (V) s exact. V n, = V n,. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
29 Varatonal complex Ω 0 (V)= V/V δ Ω 1 (V)= V k... 1 What s the cohomology of Ω (V)? 2 Do cochans and the dfferental operators of Ω (V) have a tangble nterpretaton? An algebra of dfferental functons V admts a fltraton by V n, = {f V f u (m) j = 0 for all(m, j) > (n, )} Theorem An algebra V s sad to be normal f If V s normal, then Ω (V) s exact. V n, = V n,. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
30 Varatonal complex Theorem Let V be an algebra of dfferental functons on k varables u 1,..., u k. Then for p 2, Ω r (V) = { r V k V/V}. The dfferental δ acts on S Ω r (V) va r+1 δs(p 1,..., P r+1 ) = ( 1) j+1 (X P js)(p 1,..., ˆP j,..., P r+1 ) j=0 where X P s a dervaton (an evolutonary vector feld ) defned as X P := ( n P ).,n UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
31 Varatonal complex As a corollary, f an algebra V s normal, then δf δu = 0 ff f = g + const F Im ( δ δu) ff DF () DF () = 0. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
32 Posson vertex and Le conformal algebras Let V be a C[]-module, where acts as a dervaton. A λ-bracket on V s a C-lnear map V V C[λ] V denoted by f g {f λ g} subject to sesqulnearty: {f λ g} = λ{f λ g}, {f λ g} = ( + λ)λ{f λ g}; left and rght Lebnz rules (f V has a structure of a untal assocatve algebra); Jacob dentty: {{f λ g} µ h} + {g µ {f λ h}} = {{f λ g} µ+λ h} Defnton A Posson vertex algebra W s a dfferental algebra wth a skew-symmetrc λ-bracket. A Le conformal algebra V s a C[]-module wth a wth a skew-symmetrc λ-bracket. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
33 Posson vertex and Le conformal algebras Let V be a C[]-module, where acts as a dervaton. A λ-bracket on V s a C-lnear map V V C[λ] V denoted by f g {f λ g} subject to sesqulnearty: {f λ g} = λ{f λ g}, {f λ g} = ( + λ)λ{f λ g}; left and rght Lebnz rules (f V has a structure of a untal assocatve algebra); Jacob dentty: {{f λ g} µ h} + {g µ {f λ h}} = {{f λ g} µ+λ h} Defnton A Posson vertex algebra W s a dfferental algebra wth a skew-symmetrc λ-bracket. A Le conformal algebra V s a C[]-module wth a wth a skew-symmetrc λ-bracket. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
34 Posson vertex and Le conformal algebras Let V be a C[]-module, where acts as a dervaton. A λ-bracket on V s a C-lnear map V V C[λ] V denoted by f g {f λ g} subject to sesqulnearty: {f λ g} = λ{f λ g}, {f λ g} = ( + λ)λ{f λ g}; left and rght Lebnz rules (f V has a structure of a untal assocatve algebra); Jacob dentty: {{f λ g} µ h} + {g µ {f λ h}} = {{f λ g} µ+λ h} Defnton A Posson vertex algebra W s a dfferental algebra wth a skew-symmetrc λ-bracket. A Le conformal algebra V s a C[]-module wth a wth a skew-symmetrc λ-bracket. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
35 Posson vertex and Le conformal algebras Let V be a C[]-module, where acts as a dervaton. A λ-bracket on V s a C-lnear map V V C[λ] V denoted by f g {f λ g} subject to sesqulnearty: {f λ g} = λ{f λ g}, {f λ g} = ( + λ)λ{f λ g}; left and rght Lebnz rules (f V has a structure of a untal assocatve algebra); Jacob dentty: {{f λ g} µ h} + {g µ {f λ h}} = {{f λ g} µ+λ h} Defnton A Posson vertex algebra W s a dfferental algebra wth a skew-symmetrc λ-bracket. A Le conformal algebra V s a C[]-module wth a wth a skew-symmetrc λ-bracket. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
36 Cohomology of Le conformal algebras Let V be a Le conformal algebra and M be an V-module. The space of k-cochans of V wth coeffcents n M s the space Γ(V, M) of C-lnear maps such that γ : A k C[λ 1,..., λ k ] M γ(a 1,..., a,..., a k ) = λ γ(a 1,..., a,..., a k ) γ s skew-symmetrc w.r.t. smultaneous permutatons of a s and λ s. The dfferental Γk (V, M) Γ k+1 (V, M) s defned by k+1 δ γ(a 1,..., a k+1 ) = ( 1) +1 (... ) + }{{} =1 Exercse k+1,j=1 <j ( 1) k++j+1 (... ) }{{} Exercse UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
37 Cohomology of Le conformal algebras Let V be a Le conformal algebra and M be an V-module. The space of k-cochans of V wth coeffcents n M s the space Γ(V, M) of C-lnear maps such that γ : A k C[λ 1,..., λ k ] M γ(a 1,..., a,..., a k ) = λ γ(a 1,..., a,..., a k ) γ s skew-symmetrc w.r.t. smultaneous permutatons of a s and λ s. The dfferental Γk (V, M) Γ k+1 (V, M) s defned by k+1 δ γ(a 1,..., a k+1 ) = ( 1) +1 (... ) + }{{} =1 Exercse k+1,j=1 <j ( 1) k++j+1 (... ) }{{} Exercse UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
38 Cohomology of Le conformal algebras Let V be a Le conformal algebra and M be an V-module. The space of k-cochans of V wth coeffcents n M s the space Γ(V, M) of C-lnear maps such that γ : A k C[λ 1,..., λ k ] M γ(a 1,..., a,..., a k ) = λ γ(a 1,..., a,..., a k ) γ s skew-symmetrc w.r.t. smultaneous permutatons of a s and λ s. The dfferental Γk (V, M) Γ k+1 (V, M) s defned by k+1 δ γ(a 1,..., a k+1 ) = ( 1) +1 (... ) + }{{} =1 Exercse k+1,j=1 <j ( 1) k++j+1 (... ) }{{} Exercse UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
39 Cohomology of Le conformal algebras The complex Γ(V, M) can be gven a C[]-acton va ( γ)(a 1,..., a k ) = ( M + λ λ k )( γ(a 1,..., a k )) Lemma and δ on Γ(V, M) commute. Hence, the reduced cohomology complex Γ(V, M) := Γ(V, M)/ Γ(V, M) s well-defned. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
40 Cohomology of Le conformal algebras The complex Γ(V, M) can be gven a C[]-acton va ( γ)(a 1,..., a k ) = ( M + λ λ k )( γ(a 1,..., a k )) Lemma and δ on Γ(V, M) commute. Hence, the reduced cohomology complex Γ(V, M) := Γ(V, M)/ Γ(V, M) s well-defned. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
41 Cohomology of Le conformal algebras Lemma Let V be an algebra of dfferental functons n varables (u ). Consder the Le conformal algebra A = C[]u wth the zero bracket. Then V s a module over A wth the acton gven by u λ f := n λ n f. Theorem The varatonal complex Ω (V) s somorphc to the reduced cohomology complex Γ (A, V). The cochans of Γ (A, V) can be descrbed rather explctly n terms of the poly-λ-brackets. Ths descrpton passed to Ω (V) gves us the structure theorem for Ω (V) dscussed above. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
42 Cohomology of Le conformal algebras Lemma Let V be an algebra of dfferental functons n varables (u ). Consder the Le conformal algebra A = C[]u wth the zero bracket. Then V s a module over A wth the acton gven by u λ f := n λ n f. Theorem The varatonal complex Ω (V) s somorphc to the reduced cohomology complex Γ (A, V). The cochans of Γ (A, V) can be descrbed rather explctly n terms of the poly-λ-brackets. Ths descrpton passed to Ω (V) gves us the structure theorem for Ω (V) dscussed above. UMN Math Physcs Semnar Le conformal algebras and the varatonal complex
9 Characteristic classes
THEODORE VORONOV DIFFERENTIAL GEOMETRY. Sprng 2009 [under constructon] 9 Characterstc classes 9.1 The frst Chern class of a lne bundle Consder a complex vector bundle E B of rank p. We shall construct
More informationPHYS 705: Classical Mechanics. Calculus of Variations II
1 PHYS 705: Classcal Mechancs Calculus of Varatons II 2 Calculus of Varatons: Generalzaton (no constrant yet) Suppose now that F depends on several dependent varables : We need to fnd such that has a statonary
More informationPolynomials. 1 More properties of polynomials
Polynomals 1 More propertes of polynomals Recall that, for R a commutatve rng wth unty (as wth all rngs n ths course unless otherwse noted), we defne R[x] to be the set of expressons n =0 a x, where a
More informationBernoulli Numbers and Polynomials
Bernoull Numbers and Polynomals T. Muthukumar tmk@tk.ac.n 17 Jun 2014 The sum of frst n natural numbers 1, 2, 3,..., n s n n(n + 1 S 1 (n := m = = n2 2 2 + n 2. Ths formula can be derved by notng that
More informationCanonical transformations
Canoncal transformatons November 23, 2014 Recall that we have defned a symplectc transformaton to be any lnear transformaton M A B leavng the symplectc form nvarant, Ω AB M A CM B DΩ CD Coordnate transformatons,
More informationRepresentation theory and quantum mechanics tutorial Representation theory and quantum conservation laws
Representaton theory and quantum mechancs tutoral Representaton theory and quantum conservaton laws Justn Campbell August 1, 2017 1 Generaltes on representaton theory 1.1 Let G GL m (R) be a real algebrac
More informationR n α. . The funny symbol indicates DISJOINT union. Define an equivalence relation on this disjoint union by declaring v α R n α, and v β R n β
Readng. Ch. 3 of Lee. Warner. M s an abstract manfold. We have defned the tangent space to M va curves. We are gong to gve two other defntons. All three are used n the subject and one freely swtches back
More informationarxiv: v2 [math-ph] 23 May 2015
DOUBLE POISSON VERTEX ALGEBRAS AND NON-COMMUTATIVE HAMILTONIAN EQUATIONS ALBERTO DE SOLE, VICTOR G. KAC, DANIELE VALERI arxv:1410.3325v2 [math-ph] 23 May 2015 Abstract. We develop the formalsm of double
More informationOn functors between module categories for associative algebras and for N-graded vertex algebras
On functors between module categores for assocatve algebras and for N-graded vertex algebras Y-Zh Huang and Jnwe Yang Abstract We prove that the weak assocatvty for modules for vertex algebras are equvalent
More informationDIFFERENTIAL FORMS BRIAN OSSERMAN
DIFFERENTIAL FORMS BRIAN OSSERMAN Dfferentals are an mportant topc n algebrac geometry, allowng the use of some classcal geometrc arguments n the context of varetes over any feld. We wll use them to defne
More information8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS
SECTION 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS 493 8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS All the vector spaces you have studed thus far n the text are real vector spaces because the scalars
More informationRestricted Lie Algebras. Jared Warner
Restrcted Le Algebras Jared Warner 1. Defntons and Examples Defnton 1.1. Let k be a feld of characterstc p. A restrcted Le algebra (g, ( ) [p] ) s a Le algebra g over k and a map ( ) [p] : g g called
More informationAn Introduction to Morita Theory
An Introducton to Morta Theory Matt Booth October 2015 Nov. 2017: made a few revsons. Thanks to Nng Shan for catchng a typo. My man reference for these notes was Chapter II of Bass s book Algebrac K-Theory
More informationAPPENDIX A Some Linear Algebra
APPENDIX A Some Lnear Algebra The collecton of m, n matrces A.1 Matrces a 1,1,..., a 1,n A = a m,1,..., a m,n wth real elements a,j s denoted by R m,n. If n = 1 then A s called a column vector. Smlarly,
More informationDISCRIMINANTS AND RAMIFIED PRIMES. 1. Introduction A prime number p is said to be ramified in a number field K if the prime ideal factorization
DISCRIMINANTS AND RAMIFIED PRIMES KEITH CONRAD 1. Introducton A prme number p s sad to be ramfed n a number feld K f the prme deal factorzaton (1.1) (p) = po K = p e 1 1 peg g has some e greater than 1.
More informationwhere a is any ideal of R. Lemma 5.4. Let R be a ring. Then X = Spec R is a topological space Moreover the open sets
5. Schemes To defne schemes, just as wth algebrac varetes, the dea s to frst defne what an affne scheme s, and then realse an arbtrary scheme, as somethng whch s locally an affne scheme. The defnton of
More informationMath 101 Fall 2013 Homework #7 Due Friday, November 15, 2013
Math 101 Fall 2013 Homework #7 Due Frday, November 15, 2013 1. Let R be a untal subrng of E. Show that E R R s somorphc to E. ANS: The map (s,r) sr s a R-balanced map of E R to E. Hence there s a group
More informationThe Degrees of Nilpotency of Nilpotent Derivations on the Ring of Matrices
Internatonal Mathematcal Forum, Vol. 6, 2011, no. 15, 713-721 The Degrees of Nlpotency of Nlpotent Dervatons on the Rng of Matrces Homera Pajoohesh Department of of Mathematcs Medgar Evers College of CUNY
More informationON MECHANICS WITH VARIABLE NONCOMMUTATIVITY
ON MECHANICS WITH VARIABLE NONCOMMUTATIVITY CIPRIAN ACATRINEI Natonal Insttute of Nuclear Physcs and Engneerng P.O. Box MG-6, 07725-Bucharest, Romana E-mal: acatrne@theory.npne.ro. Receved March 6, 2008
More informationProblem Do any of the following determine homomorphisms from GL n (C) to GL n (C)?
Homework 8 solutons. Problem 16.1. Whch of the followng defne homomomorphsms from C\{0} to C\{0}? Answer. a) f 1 : z z Yes, f 1 s a homomorphsm. We have that z s the complex conjugate of z. If z 1,z 2
More information12 MATH 101A: ALGEBRA I, PART C: MULTILINEAR ALGEBRA. 4. Tensor product
12 MATH 101A: ALGEBRA I, PART C: MULTILINEAR ALGEBRA Here s an outlne of what I dd: (1) categorcal defnton (2) constructon (3) lst of basc propertes (4) dstrbutve property (5) rght exactness (6) localzaton
More informationDifferential Polynomials
JASS 07 - Polynomals: Ther Power and How to Use Them Dfferental Polynomals Stephan Rtscher March 18, 2007 Abstract Ths artcle gves an bref ntroducton nto dfferental polynomals, deals and manfolds and ther
More informationLectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix
Lectures - Week 4 Matrx norms, Condtonng, Vector Spaces, Lnear Independence, Spannng sets and Bass, Null space and Range of a Matrx Matrx Norms Now we turn to assocatng a number to each matrx. We could
More informationALGEBRA SCHEMES AND THEIR REPRESENTATIONS
ALGEBRA SCHEMES AND THEIR REPRESENTATIONS AMELIA ÁLVAREZ, CARLOS SANCHO, AND PEDRO SANCHO Introducton The equvalence (Carter dualty) between the category of topologcally flat formal k-groups and the category
More informationwhere a is any ideal of R. Lemma Let R be a ring. Then X = Spec R is a topological space. Moreover the open sets
11. Schemes To defne schemes, just as wth algebrac varetes, the dea s to frst defne what an affne scheme s, and then realse an arbtrary scheme, as somethng whch s locally an affne scheme. The defnton of
More informationModelli Clamfim Equazioni differenziali 7 ottobre 2013
CLAMFIM Bologna Modell 1 @ Clamfm Equazon dfferenzal 7 ottobre 2013 professor Danele Rtell danele.rtell@unbo.t 1/18? Ordnary Dfferental Equatons A dfferental equaton s an equaton that defnes a relatonshp
More informationNOTES FOR QUANTUM GROUPS, CRYSTAL BASES AND REALIZATION OF ŝl(n)-modules
NOTES FOR QUANTUM GROUPS, CRYSTAL BASES AND REALIZATION OF ŝl(n)-modules EVAN WILSON Quantum groups Consder the Le algebra sl(n), whch s the Le algebra over C of n n trace matrces together wth the commutator
More informationModelli Clamfim Equazione del Calore Lezione ottobre 2014
CLAMFIM Bologna Modell 1 @ Clamfm Equazone del Calore Lezone 17 15 ottobre 2014 professor Danele Rtell danele.rtell@unbo.t 1/24? Convoluton The convoluton of two functons g(t) and f(t) s the functon (g
More informationThe Pseudoblocks of Endomorphism Algebras
Internatonal Mathematcal Forum, 4, 009, no. 48, 363-368 The Pseudoblocks of Endomorphsm Algebras Ahmed A. Khammash Department of Mathematcal Scences, Umm Al-Qura Unversty P.O.Box 796, Makkah, Saud Araba
More informationInner Product. Euclidean Space. Orthonormal Basis. Orthogonal
Inner Product Defnton 1 () A Eucldean space s a fnte-dmensonal vector space over the reals R, wth an nner product,. Defnton 2 (Inner Product) An nner product, on a real vector space X s a symmetrc, blnear,
More information2 More examples with details
Physcs 129b Lecture 3 Caltech, 01/15/19 2 More examples wth detals 2.3 The permutaton group n = 4 S 4 contans 4! = 24 elements. One s the dentty e. Sx of them are exchange of two objects (, j) ( to j and
More informationFixed points of IA-endomorphisms of a free metabelian Lie algebra
Proc. Indan Acad. Sc. (Math. Sc.) Vol. 121, No. 4, November 2011, pp. 405 416. c Indan Academy of Scences Fxed ponts of IA-endomorphsms of a free metabelan Le algebra NAIME EKICI 1 and DEMET PARLAK SÖNMEZ
More informationAffine and Riemannian Connections
Affne and Remannan Connectons Semnar Remannan Geometry Summer Term 2015 Prof Dr Anna Wenhard and Dr Gye-Seon Lee Jakob Ullmann Notaton: X(M) space of smooth vector felds on M D(M) space of smooth functons
More informationALGEBRA SCHEMES AND THEIR REPRESENTATIONS
ALGEBRA SCHEMES AND THEIR REPRESENTATIONS AMELIA ÁLVAREZ, CARLOS SANCHO, AND PEDRO SANCHO Introducton The equvalence (Carter dualty) between the category of topologcally flat formal k-groups and the category
More informationIntegrals and Invariants of Euler-Lagrange Equations
Lecture 16 Integrals and Invarants of Euler-Lagrange Equatons ME 256 at the Indan Insttute of Scence, Bengaluru Varatonal Methods and Structural Optmzaton G. K. Ananthasuresh Professor, Mechancal Engneerng,
More informationSUPER PRINCIPAL FIBER BUNDLE WITH SUPER ACTION
talan journal of pure appled mathematcs n. 33 2014 (63 70) 63 SUPER PRINCIPAL FIBER BUNDLE WITH SUPER ACTION M.R. Farhangdoost Department of Mathematcs College of Scences Shraz Unversty Shraz, 71457-44776
More informationELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM
ELASTIC WAVE PROPAGATION IN A CONTINUOUS MEDIUM An elastc wave s a deformaton of the body that travels throughout the body n all drectons. We can examne the deformaton over a perod of tme by fxng our look
More informationHomework 1 Lie Algebras
Homework 1 Le Algebras Joshua Ruter February 9, 018 Proposton 0.1 Problem 1.7a). Let A be a K-algebra, wth char K. Then A s alternatve f and only f the folowng two lnear) denttes hold for all a, b, y A.
More informationHomework Notes Week 7
Homework Notes Week 7 Math 4 Sprng 4 #4 (a Complete the proof n example 5 that s an nner product (the Frobenus nner product on M n n (F In the example propertes (a and (d have already been verfed so we
More informationLecture 7: Gluing prevarieties; products
Lecture 7: Glung prevaretes; products 1 The category of algebrac prevaretes Proposton 1. Let (f,ϕ) : (X,O X ) (Y,O Y ) be a morphsm of algebrac prevaretes. If U X and V Y are affne open subvaretes wth
More informationLecture 20: Noether s Theorem
Lecture 20: Noether s Theorem In our revew of Newtonan Mechancs, we were remnded that some quanttes (energy, lnear momentum, and angular momentum) are conserved That s, they are constant f no external
More informationRandić Energy and Randić Estrada Index of a Graph
EUROPEAN JOURNAL OF PURE AND APPLIED MATHEMATICS Vol. 5, No., 202, 88-96 ISSN 307-5543 www.ejpam.com SPECIAL ISSUE FOR THE INTERNATIONAL CONFERENCE ON APPLIED ANALYSIS AND ALGEBRA 29 JUNE -02JULY 20, ISTANBUL
More informationNUMERICAL DIFFERENTIATION
NUMERICAL DIFFERENTIATION 1 Introducton Dfferentaton s a method to compute the rate at whch a dependent output y changes wth respect to the change n the ndependent nput x. Ths rate of change s called the
More informationarxiv: v2 [math-ph] 6 Feb 2013
THE VARIATIONAL POISSON COHOMOLOGY ALBERTO DE SOLE 1 AND VICTOR G. KAC 2 arxv:1106.0082v2 [math-ph] 6 Feb 2013 To the memory of Bors Kupershmdt 11/27/1946 12/12/2010 Abstract. It s well nown that the valdty
More informationFACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP
C O L L O Q U I U M M A T H E M A T I C U M VOL. 80 1999 NO. 1 FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP BY FLORIAN K A I N R A T H (GRAZ) Abstract. Let H be a Krull monod wth nfnte class
More informationCALCULUS CLASSROOM CAPSULES
CALCULUS CLASSROOM CAPSULES SESSION S86 Dr. Sham Alfred Rartan Valley Communty College salfred@rartanval.edu 38th AMATYC Annual Conference Jacksonvlle, Florda November 8-, 202 2 Calculus Classroom Capsules
More information10. Canonical Transformations Michael Fowler
10. Canoncal Transformatons Mchael Fowler Pont Transformatons It s clear that Lagrange s equatons are correct for any reasonable choce of parameters labelng the system confguraton. Let s call our frst
More informationPHYS 705: Classical Mechanics. Canonical Transformation II
1 PHYS 705: Classcal Mechancs Canoncal Transformaton II Example: Harmonc Oscllator f ( x) x m 0 x U( x) x mx x LT U m Defne or L p p mx x x m mx x H px L px p m p x m m H p 1 x m p m 1 m H x p m x m m
More informationModule 3: Element Properties Lecture 1: Natural Coordinates
Module 3: Element Propertes Lecture : Natural Coordnates Natural coordnate system s bascally a local coordnate system whch allows the specfcaton of a pont wthn the element by a set of dmensonless numbers
More informationMATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS
MATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS These are nformal notes whch cover some of the materal whch s not n the course book. The man purpose s to gve a number of nontrval examples
More informationGroup Analysis of Ordinary Differential Equations of the Order n>2
Symmetry n Nonlnear Mathematcal Physcs 997, V., 64 7. Group Analyss of Ordnary Dfferental Equatons of the Order n> L.M. BERKOVICH and S.Y. POPOV Samara State Unversty, 4430, Samara, Russa E-mal: berk@nfo.ssu.samara.ru
More informationDeterminants Containing Powers of Generalized Fibonacci Numbers
1 2 3 47 6 23 11 Journal of Integer Sequences, Vol 19 (2016), Artcle 1671 Determnants Contanng Powers of Generalzed Fbonacc Numbers Aram Tangboonduangjt and Thotsaporn Thanatpanonda Mahdol Unversty Internatonal
More informationSL n (F ) Equals its Own Derived Group
Internatonal Journal of Algebra, Vol. 2, 2008, no. 12, 585-594 SL n (F ) Equals ts Own Derved Group Jorge Macel BMCC-The Cty Unversty of New York, CUNY 199 Chambers street, New York, NY 10007, USA macel@cms.nyu.edu
More informationHOPF ALGEBRAS WITH TRACE AND CLEBSCH-GORDAN COEFFICIENTS. 1. Recollections and the problem
HOPF ALGEBRAS WITH TRACE AND CLEBSCH-GORDAN COEFFICIENTS CORRADO DE CONCINI Abstract. In ths lecture I shall report on some jont work wth Proces, Reshetkhn and Rosso [1]. 1. Recollectons and the problem
More informationLecture Notes Introduction to Cluster Algebra
Lecture Notes Introducton to Cluster Algebra Ivan C.H. Ip Updated: Ma 7, 2017 3 Defnton and Examples of Cluster algebra 3.1 Quvers We frst revst the noton of a quver. Defnton 3.1. A quver s a fnte orented
More informationn α j x j = 0 j=1 has a nontrivial solution. Here A is the n k matrix whose jth column is the vector for all t j=0
MODULE 2 Topcs: Lnear ndependence, bass and dmenson We have seen that f n a set of vectors one vector s a lnear combnaton of the remanng vectors n the set then the span of the set s unchanged f that vector
More informationSOME RESULTS ON TRANSFORMATIONS GROUPS OF N-LINEAR CONNECTIONS IN THE 2-TANGENT BUNDLE
STUDIA UNIV. BABEŞ BOLYAI MATHEMATICA Volume LIII Number March 008 SOME RESULTS ON TRANSFORMATIONS GROUPS OF N-LINEAR CONNECTIONS IN THE -TANGENT BUNDLE GHEORGHE ATANASIU AND MONICA PURCARU Abstract. In
More informationSOME MULTILINEAR ALGEBRA OVER FIELDS WHICH I UNDERSTAND
SOME MULTILINEAR ALGEBRA OER FIELDS WHICH I UNDERSTAND Most of what s dscussed n ths handout extends verbatm to all felds wth the excepton of the descrpton of the Exteror and Symmetrc Algebras, whch requres
More informationPHYS 705: Classical Mechanics. Newtonian Mechanics
1 PHYS 705: Classcal Mechancs Newtonan Mechancs Quck Revew of Newtonan Mechancs Basc Descrpton: -An dealzed pont partcle or a system of pont partcles n an nertal reference frame [Rgd bodes (ch. 5 later)]
More informationON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EQUATION
Advanced Mathematcal Models & Applcatons Vol.3, No.3, 2018, pp.215-222 ON A DETERMINATION OF THE INITIAL FUNCTIONS FROM THE OBSERVED VALUES OF THE BOUNDARY FUNCTIONS FOR THE SECOND-ORDER HYPERBOLIC EUATION
More informationSalmon: Lectures on partial differential equations. Consider the general linear, second-order PDE in the form. ,x 2
Salmon: Lectures on partal dfferental equatons 5. Classfcaton of second-order equatons There are general methods for classfyng hgher-order partal dfferental equatons. One s very general (applyng even to
More informationDifferentiating Gaussian Processes
Dfferentatng Gaussan Processes Andrew McHutchon Aprl 17, 013 1 Frst Order Dervatve of the Posteror Mean The posteror mean of a GP s gven by, f = x, X KX, X 1 y x, X α 1 Only the x, X term depends on the
More informationModelli Clamfim Equazioni differenziali 22 settembre 2016
CLAMFIM Bologna Modell 1 @ Clamfm Equazon dfferenzal 22 settembre 2016 professor Danele Rtell danele.rtell@unbo.t 1/22? Ordnary Dfferental Equatons A dfferental equaton s an equaton that defnes a relatonshp
More informationMTH 819 Algebra I S13. Homework 1/ Solutions. 1 if p n b and p n+1 b 0 otherwise ) = 0 if p q or n m. W i = rw i
MTH 819 Algebra I S13 Homework 1/ Solutons Defnton A. Let R be PID and V a untary R-module. Let p be a prme n R and n Z +. Then d p,n (V) = dm R/Rp p n 1 Ann V (p n )/p n Ann V (p n+1 ) Note here that
More information12. The Hamilton-Jacobi Equation Michael Fowler
1. The Hamlton-Jacob Equaton Mchael Fowler Back to Confguraton Space We ve establshed that the acton, regarded as a functon of ts coordnate endponts and tme, satsfes ( ) ( ) S q, t / t+ H qpt,, = 0, and
More informationLagrangian Field Theory
Lagrangan Feld Theory Adam Lott PHY 391 Aprl 6, 017 1 Introducton Ths paper s a summary of Chapter of Mandl and Shaw s Quantum Feld Theory [1]. The frst thng to do s to fx the notaton. For the most part,
More informationU.C. Berkeley CS294: Beyond Worst-Case Analysis Luca Trevisan September 5, 2017
U.C. Berkeley CS94: Beyond Worst-Case Analyss Handout 4s Luca Trevsan September 5, 07 Summary of Lecture 4 In whch we ntroduce semdefnte programmng and apply t to Max Cut. Semdefnte Programmng Recall that
More informationCoordinate-Free Projective Geometry for Computer Vision
MM Research Preprnts,131 165 No. 18, Dec. 1999. Beng 131 Coordnate-Free Proectve Geometry for Computer Vson Hongbo L, Gerald Sommer 1. Introducton How to represent an mage pont algebracally? Gven a Cartesan
More informationA how to guide to second quantization method.
Phys. 67 (Graduate Quantum Mechancs Sprng 2009 Prof. Pu K. Lam. Verson 3 (4/3/2009 A how to gude to second quantzaton method. -> Second quantzaton s a mathematcal notaton desgned to handle dentcal partcle
More informationLECTURE V. 1. More on the Chinese Remainder Theorem We begin by recalling this theorem, proven in the preceeding lecture.
LECTURE V EDWIN SPARK 1. More on the Chnese Remander Theorem We begn by recallng ths theorem, proven n the preceedng lecture. Theorem 1.1 (Chnese Remander Theorem). Let R be a rng wth deals I 1, I 2,...,
More informationAn application of non-associative Composition-Diamond lemma
An applcaton of non-assocatve Composton-Damond lemma arxv:0804.0915v1 [math.ra] 6 Apr 2008 Yuqun Chen and Yu L School of Mathematcal Scences, South Chna Normal Unversty Guangzhou 510631, P. R. Chna Emal:
More informationTHEOREMS OF QUANTUM MECHANICS
THEOREMS OF QUANTUM MECHANICS In order to develop methods to treat many-electron systems (atoms & molecules), many of the theorems of quantum mechancs are useful. Useful Notaton The matrx element A mn
More informationYong Joon Ryang. 1. Introduction Consider the multicommodity transportation problem with convex quadratic cost function. 1 2 (x x0 ) T Q(x x 0 )
Kangweon-Kyungk Math. Jour. 4 1996), No. 1, pp. 7 16 AN ITERATIVE ROW-ACTION METHOD FOR MULTICOMMODITY TRANSPORTATION PROBLEMS Yong Joon Ryang Abstract. The optmzaton problems wth quadratc constrants often
More information17. Coordinate-Free Projective Geometry for Computer Vision
17. Coordnate-Free Projectve Geometry for Computer Vson Hongbo L and Gerald Sommer Insttute of Computer Scence and Appled Mathematcs, Chrstan-Albrechts-Unversty of Kel 17.1 Introducton How to represent
More informationAnalytical classical dynamics
Analytcal classcal ynamcs by Youun Hu Insttute of plasma physcs, Chnese Acaemy of Scences Emal: yhu@pp.cas.cn Abstract These notes were ntally wrtten when I rea tzpatrck s book[] an were later revse to
More informationDeformation quantization and localization of noncommutative algebras and vertex algebras
Deformaton quantzaton and localzaton of noncommutatve algebras and vertex algebras TOSHIRO KUWABARA 1 The present paper s a report for the proceengs of 59th Algebra Symposum held at the Unversty of Tokyo
More informationQuantum Mechanics I Problem set No.1
Quantum Mechancs I Problem set No.1 Septembe0, 2017 1 The Least Acton Prncple The acton reads S = d t L(q, q) (1) accordng to the least (extremal) acton prncple, the varaton of acton s zero 0 = δs = t
More information1 Matrix representations of canonical matrices
1 Matrx representatons of canoncal matrces 2-d rotaton around the orgn: ( ) cos θ sn θ R 0 = sn θ cos θ 3-d rotaton around the x-axs: R x = 1 0 0 0 cos θ sn θ 0 sn θ cos θ 3-d rotaton around the y-axs:
More informationIntegrals and Invariants of
Lecture 16 Integrals and Invarants of Euler Lagrange Equatons NPTEL Course Varatonal Methods and Structural Optmzaton G. K. Ananthasuresh Professor, Mechancal Engneerng, Indan Insttute of Scence, Banagalore
More information= = = (a) Use the MATLAB command rref to solve the system. (b) Let A be the coefficient matrix and B be the right-hand side of the system.
Chapter Matlab Exercses Chapter Matlab Exercses. Consder the lnear system of Example n Secton.. x x x y z y y z (a) Use the MATLAB command rref to solve the system. (b) Let A be the coeffcent matrx and
More information2.3 Nilpotent endomorphisms
s a block dagonal matrx, wth A Mat dm U (C) In fact, we can assume that B = B 1 B k, wth B an ordered bass of U, and that A = [f U ] B, where f U : U U s the restrcton of f to U 40 23 Nlpotent endomorphsms
More informationAdvanced Quantum Mechanics
Advanced Quantum Mechancs Rajdeep Sensarma! sensarma@theory.tfr.res.n ecture #9 QM of Relatvstc Partcles Recap of ast Class Scalar Felds and orentz nvarant actons Complex Scalar Feld and Charge conjugaton
More informationChapter 5. Solution of System of Linear Equations. Module No. 6. Solution of Inconsistent and Ill Conditioned Systems
Numercal Analyss by Dr. Anta Pal Assstant Professor Department of Mathematcs Natonal Insttute of Technology Durgapur Durgapur-713209 emal: anta.bue@gmal.com 1 . Chapter 5 Soluton of System of Lnear Equatons
More informationMASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.265/15.070J Fall 2013 Lecture 12 10/21/2013. Martingale Concentration Inequalities and Applications
MASSACHUSETTS INSTITUTE OF TECHNOLOGY 6.65/15.070J Fall 013 Lecture 1 10/1/013 Martngale Concentraton Inequaltes and Applcatons Content. 1. Exponental concentraton for martngales wth bounded ncrements.
More informationThe non-negativity of probabilities and the collapse of state
The non-negatvty of probabltes and the collapse of state Slobodan Prvanovć Insttute of Physcs, P.O. Box 57, 11080 Belgrade, Serba Abstract The dynamcal equaton, beng the combnaton of Schrödnger and Louvlle
More informationA CHARACTERIZATION OF ADDITIVE DERIVATIONS ON VON NEUMANN ALGEBRAS
Journal of Mathematcal Scences: Advances and Applcatons Volume 25, 2014, Pages 1-12 A CHARACTERIZATION OF ADDITIVE DERIVATIONS ON VON NEUMANN ALGEBRAS JIA JI, WEN ZHANG and XIAOFEI QI Department of Mathematcs
More informationD.K.M COLLEGE FOR WOMEN (AUTONOMOUS), VELLORE DEPARTMENT OF MATHEMATICS
D.K.M COLLEGE FOR WOMEN (AUTONOMOUS), VELLORE DEPARTMENT OF MATHEMATICS SUB: ALGEBRA SUB CODE: 5CPMAA SECTION- A UNIT-. Defne conjugate of a n G and prove that conjugacy s an equvalence relaton on G. Defne
More informationINTERVAL SEMIGROUPS. W. B. Vasantha Kandasamy Florentin Smarandache
Interval Semgroups - Cover.pdf:Layout 1 1/20/2011 10:04 AM Page 1 INTERVAL SEMIGROUPS W. B. Vasantha Kandasamy Florentn Smarandache KAPPA & OMEGA Glendale 2011 Ths book can be ordered n a paper bound reprnt
More informationcoordinates. Then, the position vectors are described by
Revewng, what we have dscussed so far: Generalzed coordnates Any number of varables (say, n) suffcent to specfy the confguraton of the system at each nstant to tme (need not be the mnmum number). In general,
More informationREDUCTION MODULO p. We will prove the reduction modulo p theorem in the general form as given by exercise 4.12, p. 143, of [1].
REDUCTION MODULO p. IAN KIMING We wll prove the reducton modulo p theorem n the general form as gven by exercse 4.12, p. 143, of [1]. We consder an ellptc curve E defned over Q and gven by a Weerstraß
More informationRandom Walks on Digraphs
Random Walks on Dgraphs J. J. P. Veerman October 23, 27 Introducton Let V = {, n} be a vertex set and S a non-negatve row-stochastc matrx (.e. rows sum to ). V and S defne a dgraph G = G(V, S) and a drected
More informationw ). Then use the Cauchy-Schwartz inequality ( v w v w ).] = in R 4. Can you find a vector u 4 in R 4 such that the
Math S-b Summer 8 Homework #5 Problems due Wed, July 8: Secton 5: Gve an algebrac proof for the trangle nequalty v+ w v + w Draw a sketch [Hnt: Expand v+ w ( v+ w) ( v+ w ) hen use the Cauchy-Schwartz
More informationPoisson vertex algebras in the theory of Hamiltonian equations
Japan. J. Math. 4, 141 252 (2009 DOI: 10.1007/s11537-009-0932-y Posson vertex algebras n the theory of Hamltonan eqatons Alaa Barakat Alberto De Sole Vctor G. Kac Receved: 7 Jly 2009 / Revsed: 18 November
More informationPfaffian Formulae and Their Applications to Symmetric Function Identities. Soichi OKADA (Nagoya University)
Pfaffan Formulae and Ther Applcatons to Symmetrc Functon Identtes Soch OKADA Nagoya Unversty 73rd Sémnare Lotharngen de Combnatore Strobl, September 9, 2014 Schur-type Pfaffans Pfaffan Let A = a j 1, j
More information10.40 Appendix Connection to Thermodynamics and Derivation of Boltzmann Distribution
10.40 Appendx Connecton to Thermodynamcs Dervaton of Boltzmann Dstrbuton Bernhardt L. Trout Outlne Cannoncal ensemble Maxmumtermmethod Most probable dstrbuton Ensembles contnued: Canoncal, Mcrocanoncal,
More informationNOTES ON SIMPLIFICATION OF MATRICES
NOTES ON SIMPLIFICATION OF MATRICES JONATHAN LUK These notes dscuss how to smplfy an (n n) matrx In partcular, we expand on some of the materal from the textbook (wth some repetton) Part of the exposton
More informationLecture 3: Probability Distributions
Lecture 3: Probablty Dstrbutons Random Varables Let us begn by defnng a sample space as a set of outcomes from an experment. We denote ths by S. A random varable s a functon whch maps outcomes nto the
More informationKernel Methods and SVMs Extension
Kernel Methods and SVMs Extenson The purpose of ths document s to revew materal covered n Machne Learnng 1 Supervsed Learnng regardng support vector machnes (SVMs). Ths document also provdes a general
More informationQuantum groups and quantized q-difference birational Weyl group actions
q Weyl Quantum groups and quantzed q-dfference bratonal Weyl group actons ( ) Gen KUROKI (Tohoku Unversty, Japan) 24 September 2010 2010 2010 9 22 25 (24 September 2010, Verson 1.7) Quantum bratonal Weyl
More informationPerron Vectors of an Irreducible Nonnegative Interval Matrix
Perron Vectors of an Irreducble Nonnegatve Interval Matrx Jr Rohn August 4 2005 Abstract As s well known an rreducble nonnegatve matrx possesses a unquely determned Perron vector. As the man result of
More information