Quantizations of Kac-Moody algebras

Size: px
Start display at page:

Download "Quantizations of Kac-Moody algebras"

Transcription

1 FES-C UNAM MEXICO 1 4 of July 2013 Noncommutatve Rngs and ther Applcatons LENS, France

2 Quantzatons Quantzed envelopng algebras: Drnfel d (1985), Jmbo (1985).

3 Quantzatons Quantzed envelopng algebras: Drnfel d (1985), Jmbo (1985). Multparameter verson: N. Reshetkhn (1990); P. Cotta-Ramusno, M. Rnald (1991); C. De Concn, V.G. Kac, C. Proces (1992); M. Constantn, M. Varagnolo (1994).

4 Quantzatons Quantzed envelopng algebras: Drnfel d (1985), Jmbo (1985). Multparameter verson: N. Reshetkhn (1990); P. Cotta-Ramusno, M. Rnald (1991); C. De Concn, V.G. Kac, C. Proces (1992); M. Constantn, M. Varagnolo (1994). Deformatons of Hall algebras: C. M. Rngel (1996).

5 Quantzatons Quantzed envelopng algebras: Drnfel d (1985), Jmbo (1985). Multparameter verson: N. Reshetkhn (1990); P. Cotta-Ramusno, M. Rnald (1991); C. De Concn, V.G. Kac, C. Proces (1992); M. Constantn, M. Varagnolo (1994). Deformatons of Hall algebras: C. M. Rngel (1996). Two-parameter quantum groups: G. Benkart, S. Wtherspoon (2004); N. Bergeron, Y. Gao, N. Hu (2005).

6 Hopf algebras Algebras and coalgebras: m : H H H : H H H product; coproduct;

7 Hopf algebras Algebras and coalgebras: m : H H H product; Examples: : H H H coproduct; k[g], (g) = g g, g G; U(L), (l) = l l, l L.

8 Hopf algebras Algebras and coalgebras: m : H H H product; : H H H coproduct; Examples: k[g], (g) = g g, g G; U(L), (l) = l l, l L. Both are cocommutatve: (a) = a (1) a (2) = a (2) a (1).

9 Hopf algebras Algebras and coalgebras: m : H H H product; Examples: : H H H Both are cocommutatve: coproduct; k[g], (g) = g g, g G; U(L), (l) = l l, l L. (a) = a (1) a (2) = a (2) a (1). Thm. (Carter Kostant). Every cocommutatve Hopf algebra (over C) has the form C[G]#U(L).

10 Hopf algebras Algebras and coalgebras: m : H H H product; Examples: : H H H Both are cocommutatve: coproduct; k[g], (g) = g g, g G; U(L), (l) = l l, l L. (a) = a (1) a (2) = a (2) a (1). Thm. (Carter Kostant). Every cocommutatve Hopf algebra (over C) has the form C[G]#U(L). A quantum group = a Hopf algebra whch s nether commutatve nor cocommutatve, but t s close to.

11 Quantzatons In what extend a quantum unversal envelopng algebra of a Kac-Moody algebra g s defned by mult-degrees of ts defnng relatons?

12 Quantzatons In what extend a quantum unversal envelopng algebra of a Kac-Moody algebra g s defned by mult-degrees of ts defnng relatons? R g s a class of character Hopf algebras defned by the same number of defnng relatons of the same degrees as g s.

13 Gabber-Kac representaton Cartan matrx A = a j : an ntegral n n matrx a = 2, a j 0 for j, a j = 0 mples a j = 0.

14 Gabber-Kac representaton Cartan matrx A = a j : an ntegral n n matrx a = 2, a j 0 for j, a j = 0 mples a j = 0. Generators: e, f, h, 1 n.

15 Gabber-Kac representaton Cartan matrx A = a j : an ntegral n n matrx a = 2, a j 0 for j, a j = 0 mples a j = 0. Generators: e, f, h, 1 n. Relatons: [h, h j ] = 0, [h, e j ] = a j e j, [h, f j ] = a j f j ; [e, f j ] = 0 f j, [e, f ] = h ; (ad e ) 1 a j e j = 0, (ad f ) 1 a j f j = 0 f j, (ad a) m b = [... [[b, a], a],..., a]. }{{} m

16 Quantfcaton of Cartan subalgebra h exp(h) = 1 + h + h2 2 + h3 3! + h4 4! + (h) = 1 h + h 1; (exp(h)) = exp(h) exp(h).

17 Quantfcaton of Cartan subalgebra h exp(h) = 1 + h + h2 2 + h3 3! + h4 4! + (h) = 1 h + h 1; (exp(h)) = exp(h) exp(h). [h, h j ] = 0 G = exp(h) s a commutatve group; [h, e j ] = a j e j, G acts on x j = q(e j ) by a character χ j ; [h, f j ] = a j f j, G acts on x j = q(f j ) by a character χ j.

18 Quantfcaton of Cartan subalgebra h exp(h) = 1 + h + h2 2 + h3 3! + h4 4! + (h) = 1 h + h 1; (exp(h)) = exp(h) exp(h). [h, h j ] = 0 G = exp(h) s a commutatve group; [h, e j ] = a j e j, G acts on x j = q(e j ) by a character χ j ; [h, f j ] = a j f j, G acts on x j = q(f j ) by a character χ j. g 1 y j g = χ j (g)y j, χ j = (χj ) 1. g 1 y j g = χ j (g)y j,

19 Hopf algebra structure Group-lke element: (g) = g g, ε(g) = 1. The grouplkes span a Hopf subalgebra =k [G].

20 Hopf algebra structure Group-lke element: (g) = g g, ε(g) = 1. The grouplkes span a Hopf subalgebra =k [G]. A skew-prmtve element: (a) = a h + f a, wth f, h G.

21 Hopf algebra structure Group-lke element: (g) = g g, ε(g) = 1. The grouplkes span a Hopf subalgebra =k [G]. A skew-prmtve element: (a) = a h + f a, wth f, h G. Coproduct: (y ± ) = y ± h ± + f ± y ±, h ±, f ± G.

22 Hopf algebra structure Group-lke element: (g) = g g, ε(g) = 1. The grouplkes span a Hopf subalgebra =k [G]. A skew-prmtve element: (a) = a h + f a, wth f, h G. Coproduct: (y ± ) = y ± h ± + f ± y ±, h ±, f ± G. g 1 y ± j g = χ j ± (g)y j, χ j = (χj ) 1, g G.

23 Second and thrd groups of relatons [e, f j ] = 0 f j, [e, f ] = h ; df R j = α j y y j + β j y j y = 0, R (y, y ) = df α y y + β y y k µ k g k = 0, g k G.

24 Second and thrd groups of relatons [e, f j ] = 0 f j, [e, f ] = h ; df R j = α j y y j + β j y j y = 0, R (y, y ) = df α y y + β y y k µ k g k = 0, g k G. (ad e ) 1 a j e j = 0, (ad f ) 1 a j f j = 0 f j : S j (y 1 a j S j (y, y j ) = df 1 a j, y j ) = df k=0 k=0 γ jk y k y j y 1 a j k = 0, j; δ jk (y ) k y j (y ) 1 a j k = 0, j.

25 Second and thrd groups of relatons H = G y, y R j = 0, S ± j = 0, 2n 3 + 3n 2 parameters α j, β j, µ k, γ jk, δ jk.

26 Second and thrd groups of relatons H = G y, y R j = 0, S ± j = 0, 2n 3 + 3n 2 parameters α j, β j, µ k, γ jk, δ jk. Theorem 1. The only way to keep the Hopf algebra structure on H s to replace the Le operaton n Gabber-Kac relatons wth a skew commutator: [u, v] = χ v (h u )uv χ u (f v )vu.

27 Second and thrd groups of relatons H = G y, y R j = 0, S ± j = 0, 2n 3 + 3n 2 parameters α j, β j, µ k, γ jk, δ jk. Theorem 1. The only way to keep the Hopf algebra structure on H s to replace the Le operaton n Gabber-Kac relatons wth a skew commutator: [u, v] = χ v (h u )uv χ u (f v )vu. Remans just n 2 parameters, p j = χ (h j )χ (f j ), of 2n 3 + 3n 2.

28 Indecomposable Cartan matrces A = a j. Defnton. A quantfcaton H s regular f p j p j = p a j.

29 Indecomposable Cartan matrces A = a j. Defnton. A quantfcaton H s regular f p j p j = p a j. All known quantzatons are regular.

30 Indecomposable Cartan matrces A = a j. Defnton. A quantfcaton H s regular f p j p j = p a j. All known quantzatons are regular. Theorem 2. There exsts just a fnte number of algebra structures for exceptonal quantzatons of a gven Kac-Moody algebra.

31 Indecomposable Cartan matrces A = a j. Defnton. A quantfcaton H s regular f p j p j = p a j. All known quantzatons are regular. Theorem 2. There exsts just a fnte number of algebra structures for exceptonal quantzatons of a gven Kac-Moody algebra. Theorem 3. If one of the parameters p j p j, 1, j n s not a root of 1 then the quantfcaton H s regular.

32 Indecomposable Cartan matrces A = a j. Defnton. A matrx A s symmetrzable f there exsts natural d 1, d 2,..., d n such that, d a j = d j a j, 1, j n. An n-tuple (m 1, m 2,..., m n ) s a modular symmetrzaton f m a j m j a j (mod N), 0 m, m j < N, 1, j n.

33 Indecomposable Cartan matrces A = a j. Defnton. A matrx A s symmetrzable f there exsts natural d 1, d 2,..., d n such that, d a j = d j a j, 1, j n. An n-tuple (m 1, m 2,..., m n ) s a modular symmetrzaton f m a j m j a j (mod N), 0 m, m j < N, 1, j n. Theorem 4. The algebrac structure of a regular quantfcaton s defned by two ndependent parameters q k and m M so that p = q d ξ m, m = (m 1, m 2,..., m n ), where ξ s a fxed Nth prmtve root of 1.

34 Indecomposable Cartan matrces A = a j. Defnton. A matrx A s symmetrzable f there exsts natural d 1, d 2,..., d n such that, d a j = d j a j, 1, j n. An n-tuple (m 1, m 2,..., m n ) s a modular symmetrzaton f m a j m j a j (mod N), 0 m, m j < N, 1, j n. Theorem 4. The algebrac structure of a regular quantfcaton s defned by two ndependent parameters q k and m M so that p = q d ξ m, m = (m 1, m 2,..., m n ), where ξ s a fxed Nth prmtve root of 1. In all known quantzatons, m = (0, 0,..., 0).

35 The number of exceptonal quantzatons Here ϕ, 0 s the Fbonacc sequence 1, 1, 2, 3, 5, 8, 13, 21,.... A n ϕ 2n 2 G 2 12 E (1) B n 2ϕ 2n 2 A (1) 1 6 E (1) C n 2ϕ 2n A (1) l ϕ 2n + ϕ 2n 2 2 A (2) 2 24 E C (1) l 4ϕ 2n A (2) 2l 4ϕ 2n E G (1) 2 38 D (2) l+1 4ϕ 2n + 2 E F (1) 4 91 E (2) 6 80 F 4 40 E (1) D (3) 4 19 D n ϕ 2n + ϕ 2n 7 2 D (1) l 15 ϕ 2n ϕ 2n 8 2 A (2) 2l 1 2ϕ 2n 2 + 2ϕ 2n B (1) l ϕ 2n+1 + 5ϕ 2n 5 2

36 THE END THANK YOU

HOPF ALGEBRAS WITH TRACE AND CLEBSCH-GORDAN COEFFICIENTS. 1. Recollections and the problem

HOPF 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 information

Categorification of quantum groups

Categorification of quantum groups Categorfcaton of quantum groups Aaron Lauda Jont wth Mkhal Khovanov Columba Unversty June 29th, 2009 Avalable at http://www.math.columba.edu/ lauda/talks/ Aaron Lauda Jont wth Mkhal Khovanov (Columba Categorfcaton

More information

NOTES FOR QUANTUM GROUPS, CRYSTAL BASES AND REALIZATION OF ŝl(n)-modules

NOTES 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 information

Quantum groups and quantized q-difference birational Weyl group actions

Quantum 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 information

12 MATH 101A: ALGEBRA I, PART C: MULTILINEAR ALGEBRA. 4. Tensor product

12 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 information

An Introduction to Morita Theory

An 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 information

Lecture 14 - Isomorphism Theorem of Harish-Chandra

Lecture 14 - Isomorphism Theorem of Harish-Chandra Lecture 14 - Isomorphsm Theorem of Harsh-Chandra March 11, 2013 Ths lectures shall be focused on central characters and what they can tell us about the unversal envelopng algebra of a semsmple Le algebra.

More information

Restricted Lie Algebras. Jared Warner

Restricted 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 information

An application of non-associative Composition-Diamond lemma

An 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 information

A Duality Theorem for L-R Crossed Product

A Duality Theorem for L-R Crossed Product Flomat 30:5 (2016), 1305 1313 DOI 10.2298/FIL1605305C Publshed by Faculty of Scences and Mathematcs, Unversty of Nš, Serba Avalable at: http://www.pmf.n.ac.rs/flomat A Dualty Theorem for L-R Crossed Product

More information

Quantum Groups and Quantizations of Isomonodromic Systems

Quantum Groups and Quantizations of Isomonodromic Systems Quantum Groups and Quantzatons of Isomonodromc Systems Gen KUROKI (Tohoku Unversty, Japan) 5 March 2007 Exploraton of New Structures and Natural Constructons n Mathematcal Physcs Graduate School of Mathematcs

More information

8.4 COMPLEX VECTOR SPACES AND INNER PRODUCTS

8.4 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 information

Lecture 7: Gluing prevarieties; products

Lecture 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 information

Modulo Magic Labeling in Digraphs

Modulo Magic Labeling in Digraphs Gen. Math. Notes, Vol. 7, No., August, 03, pp. 5- ISSN 9-784; Copyrght ICSRS Publcaton, 03 www.-csrs.org Avalable free onlne at http://www.geman.n Modulo Magc Labelng n Dgraphs L. Shobana and J. Baskar

More information

Degree of Parabolic Quantum Groups

Degree of Parabolic Quantum Groups Unverstà degl stud Roma Tre Dottorato d rcerca n Matematca XVI cclo Tes d Dottorato Degree of Parabolc Quantum Groups Dottorando Rccardo Pulcn Drettore d tes Corrado De Concn September 26, 2005 Coordnatrce

More information

Crystal monoids. Robert Gray (joint work with A. J. Cain and A. Malheiro) AAA90: 90th Workshop on General Algebra Novi Sad, 5th June 2015

Crystal monoids. Robert Gray (joint work with A. J. Cain and A. Malheiro) AAA90: 90th Workshop on General Algebra Novi Sad, 5th June 2015 Crystal monods Robert Gray (jont work wth A. J. Can and A. Malhero) AAA90: 90th Workshop on General Algebra Nov Sad, 5th June 05 Plactc monod va Knuth relatons Defnton Let A n be the fnte ordered alphabet

More information

A categorification of quantum sl n

A categorification of quantum sl n A categorfcaton of quantum sl n Aaron Lauda Jont wth Mkhal Khovanov Columba Unversty January 20th, 2009 Avalable at http://www.math.columba.edu/ lauda/talks/kyoto Aaron Lauda Jont wth Mkhal Khovanov (Columba

More information

Representation theory of symplectic singularities

Representation theory of symplectic singularities Quantzatons Hggs and Coulomb branches Category O and the algebra T Representaton theory of symplectc sngulartes Unversty of Vrgna December 9, 2016 Representaton theory of symplectc sngulartes Quantzatons

More information

Symmetry, Integrability and Geometry: Methods and Applications

Symmetry, Integrability and Geometry: Methods and Applications Symmetry, Integrablty and Geometry: Methods and Applcatons Zero Acton on Perfect Crystals for U q G 1) 2 Kalash C. MISRA, Mahathr MOHAMAD and Masato OKADO Department of Mathematcs, North Carolna State

More information

Representation theory and quantum mechanics tutorial Representation theory and quantum conservation laws

Representation 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 information

SMARANDACHE-GALOIS FIELDS

SMARANDACHE-GALOIS FIELDS SMARANDACHE-GALOIS FIELDS W. B. Vasantha Kandasamy Deartment of Mathematcs Indan Insttute of Technology, Madras Chenna - 600 036, Inda. E-mal: vasantak@md3.vsnl.net.n Abstract: In ths aer we study the

More information

Homework Notes Week 7

Homework 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 information

A how to guide to second quantization method.

A 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 information

Quantum Painlevé tau-functions

Quantum Painlevé tau-functions Quantum Panlevé tau-functons Gen Kurok Tohoku Unversty December 11, 2018 Conformal feld theory, somonodromy tau-functons and Panlevé equatons, 2018 December 10-12, 2018 Room B301, Graduate School of Scence,

More information

APPENDIX A Some Linear Algebra

APPENDIX 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 information

Fixed points of IA-endomorphisms of a free metabelian Lie algebra

Fixed 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 information

Weyl group. Chapter locally finite and nilpotent elements

Weyl group. Chapter locally finite and nilpotent elements Chapter 4 Weyl group In ths chapter, we defne and study the Weyl group of a Kac-Moody Le algebra and descrbe the smlartes and dfferences wth the classcal stuaton Here because the Le algebra g(a) s not

More information

GELFAND-TSETLIN BASIS FOR THE REPRESENTATIONS OF gl n

GELFAND-TSETLIN BASIS FOR THE REPRESENTATIONS OF gl n GELFAND-TSETLIN BASIS FOR THE REPRESENTATIONS OF gl n KANG LU FINITE DIMENSIONAL REPRESENTATIONS OF gl n Let e j,, j =,, n denote the standard bass of the general lnear Le algebra gl n over the feld of

More information

The Pseudoblocks of Endomorphism Algebras

The 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 information

SUPER PRINCIPAL FIBER BUNDLE WITH SUPER ACTION

SUPER 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 information

763622S ADVANCED QUANTUM MECHANICS Solution Set 1 Spring c n a n. c n 2 = 1.

763622S ADVANCED QUANTUM MECHANICS Solution Set 1 Spring c n a n. c n 2 = 1. 7636S ADVANCED QUANTUM MECHANICS Soluton Set 1 Sprng 013 1 Warm-up Show that the egenvalues of a Hermtan operator  are real and that the egenkets correspondng to dfferent egenvalues are orthogonal (b)

More information

Subset Topological Spaces and Kakutani s Theorem

Subset Topological Spaces and Kakutani s Theorem MOD Natural Neutrosophc Subset Topologcal Spaces and Kakutan s Theorem W. B. Vasantha Kandasamy lanthenral K Florentn Smarandache 1 Copyrght 1 by EuropaNova ASBL and the Authors Ths book can be ordered

More information

2.3 Nilpotent endomorphisms

2.3 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 information

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur

Module 3 LOSSY IMAGE COMPRESSION SYSTEMS. Version 2 ECE IIT, Kharagpur Module 3 LOSSY IMAGE COMPRESSION SYSTEMS Verson ECE IIT, Kharagpur Lesson 6 Theory of Quantzaton Verson ECE IIT, Kharagpur Instructonal Objectves At the end of ths lesson, the students should be able to:

More information

Pacific Journal of Mathematics

Pacific Journal of Mathematics Pacfc Journal of Mathematcs IRREDUCIBLE REPRESENTATIONS FOR THE ABELIAN EXTENSION OF THE LIE ALGEBRA OF DIFFEOMORPHISMS OF TORI IN DIMENSIONS GREATER THAN CUIPO JIANG AND QIFEN JIANG Volume 23 No. May

More information

Lecture Notes Introduction to Cluster Algebra

Lecture 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 information

CHAPTER-5 INFORMATION MEASURE OF FUZZY MATRIX AND FUZZY BINARY RELATION

CHAPTER-5 INFORMATION MEASURE OF FUZZY MATRIX AND FUZZY BINARY RELATION CAPTER- INFORMATION MEASURE OF FUZZY MATRI AN FUZZY BINARY RELATION Introducton The basc concept of the fuzz matr theor s ver smple and can be appled to socal and natural stuatons A branch of fuzz matr

More information

Inner Product. Euclidean Space. Orthonormal Basis. Orthogonal

Inner 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 information

MATH 241B FUNCTIONAL ANALYSIS - NOTES EXAMPLES OF C ALGEBRAS

MATH 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 information

Math 101 Fall 2013 Homework #7 Due Friday, November 15, 2013

Math 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 information

The Order Relation and Trace Inequalities for. Hermitian Operators

The Order Relation and Trace Inequalities for. Hermitian Operators Internatonal Mathematcal Forum, Vol 3, 08, no, 507-57 HIKARI Ltd, wwwm-hkarcom https://doorg/0988/mf088055 The Order Relaton and Trace Inequaltes for Hermtan Operators Y Huang School of Informaton Scence

More information

2 More examples with details

2 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 information

Lectures - Week 4 Matrix norms, Conditioning, Vector Spaces, Linear Independence, Spanning sets and Basis, Null space and Range of a Matrix

Lectures - 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 information

Poisson brackets and canonical transformations

Poisson brackets and canonical transformations rof O B Wrght Mechancs Notes osson brackets and canoncal transformatons osson Brackets Consder an arbtrary functon f f ( qp t) df f f f q p q p t But q p p where ( qp ) pq q df f f f p q q p t In order

More information

Continuous Time Markov Chain

Continuous Time Markov Chain Contnuous Tme Markov Chan Hu Jn Department of Electroncs and Communcaton Engneerng Hanyang Unversty ERICA Campus Contents Contnuous tme Markov Chan (CTMC) Propertes of sojourn tme Relatons Transton probablty

More information

COMPLEX NUMBERS AND QUADRATIC EQUATIONS

COMPLEX NUMBERS AND QUADRATIC EQUATIONS COMPLEX NUMBERS AND QUADRATIC EQUATIONS INTRODUCTION We know that x 0 for all x R e the square of a real number (whether postve, negatve or ero) s non-negatve Hence the equatons x, x, x + 7 0 etc are not

More information

hal , version 2-3 Dec 2009

hal , version 2-3 Dec 2009 SKEW GROUP ALGEBRAS OF PATH ALGEBRAS AND PREPROJECTIVE ALGEBRAS LAURENT DEMONET Abstract. We compute explctly up to Morta-equvalence the skew group algebra of a fnte group actng on the path algebra of

More information

Universal K-matrices via quantum symmetric pairs

Universal K-matrices via quantum symmetric pairs Universal K-matrices via quantum symmetric pairs Martina Balagović (joint work with Stefan Kolb) School of Mathematics and Statistics Newcastle University Leicester, September 215 1. Introduction - Universal

More information

DISCRIMINANTS 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. 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 information

COMPLEX SEMISIMPLE QUANTUM GROUPS AND REPRESENTATION THEORY

COMPLEX SEMISIMPLE QUANTUM GROUPS AND REPRESENTATION THEORY COMPLEX SEMISIMPLE QUANTUM GROUPS AND REPRESENTATION THEORY CHRISTIAN VOIGT AND ROBERT YUNCKEN 2010 Mathematcs Subject Classfcaton. 16T05, 17B37, 46L65, 81R50. The frst author would lke to thank the Isaac

More information

Errata to Invariant Theory with Applications January 28, 2017

Errata to Invariant Theory with Applications January 28, 2017 Invarant Theory wth Applcatons Jan Drasma and Don Gjswjt http: //www.wn.tue.nl/~jdrasma/teachng/nvtheory0910/lecturenotes12.pdf verson of 7 December 2009 Errata and addenda by Darj Grnberg The followng

More information

UNIQUENESS OF REPRESENTATION THEORETIC HYPERBOLIC KAC MOODY GROUPS OVER Z. 1. Introduction

UNIQUENESS OF REPRESENTATION THEORETIC HYPERBOLIC KAC MOODY GROUPS OVER Z. 1. Introduction UNIQUENESS OF REPRESENTATION THEORETIC HYPERBOLIC KAC MOODY GROUPS OVER Z LISA CARBONE AND FRANK WAGNER Abstract For a smply laced and hyperbolc Kac Moody group G = G(R) over a commutatve rng R wth 1,

More information

9 Characteristic classes

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 information

Week 2. This week, we covered operations on sets and cardinality.

Week 2. This week, we covered operations on sets and cardinality. Week 2 Ths week, we covered operatons on sets and cardnalty. Defnton 0.1 (Correspondence). A correspondence between two sets A and B s a set S contaned n A B = {(a, b) a A, b B}. A correspondence from

More information

FACTORIZATION IN KRULL MONOIDS WITH INFINITE CLASS GROUP

FACTORIZATION 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 information

Module 3: Element Properties Lecture 1: Natural Coordinates

Module 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 information

Fall 2012 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede

Fall 2012 Analysis of Experimental Measurements B. Eisenstein/rev. S. Errede Fall 0 Analyss of Expermental easurements B. Esensten/rev. S. Errede We now reformulate the lnear Least Squares ethod n more general terms, sutable for (eventually extendng to the non-lnear case, and also

More information

A CLASS OF RECURSIVE SETS. Florentin Smarandache University of New Mexico 200 College Road Gallup, NM 87301, USA

A CLASS OF RECURSIVE SETS. Florentin Smarandache University of New Mexico 200 College Road Gallup, NM 87301, USA A CLASS OF RECURSIVE SETS Florentn Smarandache Unversty of New Mexco 200 College Road Gallup, NM 87301, USA E-mal: smarand@unmedu In ths artcle one bulds a class of recursve sets, one establshes propertes

More information

Computing π with Bouncing Balls

Computing π with Bouncing Balls by Let the mass of two balls be M and m, where M = (6 n )m for n N. The larger ball s rolled towards the lghter ball, whch ear a wall and ntally at rest. Fnd the number of collsons between the two balls

More information

R 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

R 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 information

Abelian and non-abelian second cohomologies of quantized enveloping algebras

Abelian and non-abelian second cohomologies of quantized enveloping algebras Journal of Algebra 320 (2008) 1 47 www.elsever.com/locate/jalgebra Abelan and non-abelan second cohomologes of quantzed envelopng algebras Akra Masuoka Insttute of Mathematcs, Unversty of Tsukuba, Tsukuba,

More information

arxiv: v1 [math.qa] 22 Jan 2010

arxiv: v1 [math.qa] 22 Jan 2010 COMPLETE REDUCIBILITY THEOREMS FOR MODULES OVER POINTED HOPF ALGEBRAS arxv:1001.3977v1 [math.qa] 22 Jan 2010 NICOLÁS ANDRUSKIEWITSCH, DAVID RADFORD, AND HANS-JÜRGEN SCHNEIDER Dedcated to Susan Montgomery

More information

h-analogue of Fibonacci Numbers

h-analogue of Fibonacci Numbers h-analogue of Fbonacc Numbers arxv:090.0038v [math-ph 30 Sep 009 H.B. Benaoum Prnce Mohammad Unversty, Al-Khobar 395, Saud Araba Abstract In ths paper, we ntroduce the h-analogue of Fbonacc numbers for

More information

Hash functions : MAC / HMAC

Hash functions : MAC / HMAC Hash functons : MAC / HMAC Outlne Message Authentcaton Codes Keyed hash famly Uncondtonally Secure MACs Ref: D Stnson: Cryprography Theory and Practce (3 rd ed), Chap 4. Unversal hash famly Notatons: X

More information

GEOMETRIC DESCRIPTION OF C-VECTORS AND REAL LÖSUNGEN. 1. Introduction

GEOMETRIC DESCRIPTION OF C-VECTORS AND REAL LÖSUNGEN. 1. Introduction GEOMETRIC DESCRIPTION OF C-VECTORS AND REAL LÖSUNGEN KYU-HWAN LEE AND KYUNGYONG LEE Abstract. We propose a combnatoral/geometrc model and formulate several conectures to descrbe the c-matrces of an arbtrary

More information

ALGEBRA MID-TERM. 1 Suppose I is a principal ideal of the integral domain R. Prove that the R-module I R I has no non-zero torsion elements.

ALGEBRA MID-TERM. 1 Suppose I is a principal ideal of the integral domain R. Prove that the R-module I R I has no non-zero torsion elements. ALGEBRA MID-TERM CLAY SHONKWILER 1 Suppose I s a prncpal deal of the ntegral doman R. Prove that the R-module I R I has no non-zero torson elements. Proof. Note, frst, that f I R I has no non-zero torson

More information

A Quantum Gauss-Bonnet Theorem

A Quantum Gauss-Bonnet Theorem A Quantum Gauss-Bonnet Theorem Tyler Fresen November 13, 2014 Curvature n the plane Let Γ be a smooth curve wth orentaton n R 2, parametrzed by arc length. The curvature k of Γ s ± Γ, where the sgn s postve

More information

SL n (F ) Equals its Own Derived Group

SL 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 information

Affine niltemperley-lieb Algebras and Generalized Weyl Algebras: Combinatorics and Representation Theory

Affine niltemperley-lieb Algebras and Generalized Weyl Algebras: Combinatorics and Representation Theory Affne nltemperley-leb Algebras and Generalzed Weyl Algebras: Combnatorcs and Representaton Theory Dssertaton zur Erlangung des Doktorgrades (Dr. rer. nat.) der Mathematsch-Naturwssenschaftlchen Fakultät

More information

Root Structure of a Special Generalized Kac- Moody Algebra

Root Structure of a Special Generalized Kac- Moody Algebra Mathematcal Computaton September 04, Volume, Issue, PP8-88 Root Structu of a Specal Generalzed Kac- Moody Algebra Xnfang Song, #, Xaox Wang Bass Department, Bejng Informaton Technology College, Bejng,

More information

ON THE EXTENDED HAAGERUP TENSOR PRODUCT IN OPERATOR SPACES. 1. Introduction

ON THE EXTENDED HAAGERUP TENSOR PRODUCT IN OPERATOR SPACES. 1. Introduction ON THE EXTENDED HAAGERUP TENSOR PRODUCT IN OPERATOR SPACES TAKASHI ITOH AND MASARU NAGISA Abstract We descrbe the Haagerup tensor product l h l and the extended Haagerup tensor product l eh l n terms of

More information

7. Products and matrix elements

7. Products and matrix elements 7. Products and matrx elements 1 7. Products and matrx elements Based on the propertes of group representatons, a number of useful results can be derved. Consder a vector space V wth an nner product ψ

More information

arxiv:math/ v1 [math.qa] 17 Feb 2000

arxiv:math/ v1 [math.qa] 17 Feb 2000 A COMBINATORIAL APPROACH TO QUANTIFICATION OF LIE ALGEBRAS arxiv:math/0002149v1 [math.qa] 17 Feb 2000 V.K. KHARCHENKO Abstract. We propose a notion of a quantum universal enveloping algebra for an arbitrary

More information

MEM 255 Introduction to Control Systems Review: Basics of Linear Algebra

MEM 255 Introduction to Control Systems Review: Basics of Linear Algebra MEM 255 Introducton to Control Systems Revew: Bascs of Lnear Algebra Harry G. Kwatny Department of Mechancal Engneerng & Mechancs Drexel Unversty Outlne Vectors Matrces MATLAB Advanced Topcs Vectors A

More information

Group Analysis of Ordinary Differential Equations of the Order n>2

Group 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 information

2-Verma modules. Grégoire Naisse Joint work with Pedro Vaz. 22 November Université catholique de Louvain

2-Verma modules. Grégoire Naisse Joint work with Pedro Vaz. 22 November Université catholique de Louvain 2-Verma modules Grégore Nasse Jont work wth Pedro Vaz Unversté catholque de Louvan 22 November 2017 Hghest weght representatons g s a (symmetrzable) quantum KacMoody algebra. There are 3 knds of hghest

More information

ON THE DAVENPORT CONSTANT AND GROUP ALGEBRAS

ON THE DAVENPORT CONSTANT AND GROUP ALGEBRAS ON THE DAVENPORT CONSTANT AND GROUP ALGEBRAS DANIEL SMERTNIG Abstract. For a fnte abelan group G and a splttng feld K of G, let d(g, K) denote the largest nteger l N for whch there s a sequence S = g 1...

More information

A Simple Method for Obtaining PBW-Basis for Some Small Quantum Algebras

A Simple Method for Obtaining PBW-Basis for Some Small Quantum Algebras International Journal of Algebra, Vol. 12, 2018, no. 2, 69-81 HIKARI Ltd, www.m-hikari.com https://doi.org/10.12988/ija.2018.827 A Simple Method for Obtaining PBW-Basis for Some Small Quantum Algebras

More information

ALGEBRA SCHEMES AND THEIR REPRESENTATIONS

ALGEBRA 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 information

Convexity preserving interpolation by splines of arbitrary degree

Convexity preserving interpolation by splines of arbitrary degree Computer Scence Journal of Moldova, vol.18, no.1(52), 2010 Convexty preservng nterpolaton by splnes of arbtrary degree Igor Verlan Abstract In the present paper an algorthm of C 2 nterpolaton of dscrete

More information

Character Degrees of Extensions of PSL 2 (q) and SL 2 (q)

Character Degrees of Extensions of PSL 2 (q) and SL 2 (q) Character Degrees of Extensons of PSL (q) and SL (q) Donald L. Whte Department of Mathematcal Scences Kent State Unversty, Kent, Oho 444 E-mal: whte@math.kent.edu July 7, 01 Abstract Denote by S the projectve

More information

ALGEBRA SCHEMES AND THEIR REPRESENTATIONS

ALGEBRA 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 information

Maximum Likelihood Estimation of Binary Dependent Variables Models: Probit and Logit. 1. General Formulation of Binary Dependent Variables Models

Maximum Likelihood Estimation of Binary Dependent Variables Models: Probit and Logit. 1. General Formulation of Binary Dependent Variables Models ECO 452 -- OE 4: Probt and Logt Models ECO 452 -- OE 4 Maxmum Lkelhood Estmaton of Bnary Dependent Varables Models: Probt and Logt hs note demonstrates how to formulate bnary dependent varables models

More information

Linear, affine, and convex sets and hulls In the sequel, unless otherwise specified, X will denote a real vector space.

Linear, affine, and convex sets and hulls In the sequel, unless otherwise specified, X will denote a real vector space. Lnear, affne, and convex sets and hulls In the sequel, unless otherwse specfed, X wll denote a real vector space. Lnes and segments. Gven two ponts x, y X, we defne xy = {x + t(y x) : t R} = {(1 t)x +

More information

Lorentz Group. Ling Fong Li. 1 Lorentz group Generators Simple representations... 3

Lorentz Group. Ling Fong Li. 1 Lorentz group Generators Simple representations... 3 Lorentz Group Lng Fong L ontents Lorentz group. Generators............................................. Smple representatons..................................... 3 Lorentz group In the dervaton of Drac

More information

Piecewise Linear Parametrization of Canonical Bases

Piecewise Linear Parametrization of Canonical Bases Pecewse Lnear Parametrzaton of Canoncal Bases The MIT Faculty has made ths artcle openly avalle. Please share how ths access benefts you. Your story matters. Ctaton As Publshed Publsher Lusztg, G. Pecewse

More information

A combinatorial proof of multiple angle formulas involving Fibonacci and Lucas numbers

A combinatorial proof of multiple angle formulas involving Fibonacci and Lucas numbers Notes on Number Theory and Dscrete Mathematcs ISSN 1310 5132 Vol. 20, 2014, No. 5, 35 39 A combnatoral proof of multple angle formulas nvolvng Fbonacc and Lucas numbers Fernando Córes 1 and Dego Marques

More information

Representation theory through the lens of categorical actions: part II

Representation theory through the lens of categorical actions: part II Representaton theory through the lens of categorcal actons: part II Unversty of Vrgna June 10, 2015 Remnder from last tme Last tme, we dscussed what t meant to have sl 2 act on a category. Defnton An sl

More information

Dedicated to Claus Michael Ringel on the occasion of his 60th birthday

Dedicated to Claus Michael Ringel on the occasion of his 60th birthday GENERIC EXTENSIONS AND CANONICAL BASES FOR CYCLIC QUIVERS BANGMING DENG, JIE DU AND JIE XIAO Abstract. We use the monomal bass theory developed n [4] to present an elementary algebrac constructon of the

More information

Knot invariants via quantizations of Hecke modifications

Knot invariants via quantizations of Hecke modifications Knot nvarants va quantzatons of Hecke modfcatons Unversty of Vrgna Unversty of Waterloo Permeter Insttute for Mathematcal Physcs Aprl 29, 2017 Two approaches to Jones polynomal (1984) Jones defnes the

More information

Lie Algebras of Finite and Affine Type

Lie Algebras of Finite and Affine Type Lie Algebras of Finite and Affine Type R. W. CARTER Mathematics Institute University of Warwick CAMBRIDGE UNIVERSITY PRESS Preface page xiii Basic concepts 1 1.1 Elementary properties of Lie algebras 1

More information

where 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

where 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 information

Lecture 12: Discrete Laplacian

Lecture 12: Discrete Laplacian Lecture 12: Dscrete Laplacan Scrbe: Tanye Lu Our goal s to come up wth a dscrete verson of Laplacan operator for trangulated surfaces, so that we can use t n practce to solve related problems We are mostly

More information

arxiv:hep-th/ v2 11 Feb 1992

arxiv:hep-th/ v2 11 Feb 1992 CERN-TH.6324/91 New fuson rules and R-matrces for SL(N) q at roots of unty arxv:hep-th/9112022v2 11 Feb 1992 Danel Arnaudon * Theory Dvson, CERN CH-1211 Genève 23, Swtzerland Abstract We derve fuson rules

More information

Lagrangian Field Theory

Lagrangian 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 information

THE SUMMATION NOTATION Ʃ

THE SUMMATION NOTATION Ʃ Sngle Subscrpt otaton THE SUMMATIO OTATIO Ʃ Most of the calculatons we perform n statstcs are repettve operatons on lsts of numbers. For example, we compute the sum of a set of numbers, or the sum of the

More information

Dynamic Programming. Preview. Dynamic Programming. Dynamic Programming. Dynamic Programming (Example: Fibonacci Sequence)

Dynamic Programming. Preview. Dynamic Programming. Dynamic Programming. Dynamic Programming (Example: Fibonacci Sequence) /24/27 Prevew Fbonacc Sequence Longest Common Subsequence Dynamc programmng s a method for solvng complex problems by breakng them down nto smpler sub-problems. It s applcable to problems exhbtng the propertes

More information

Section 8.3 Polar Form of Complex Numbers

Section 8.3 Polar Form of Complex Numbers 80 Chapter 8 Secton 8 Polar Form of Complex Numbers From prevous classes, you may have encountered magnary numbers the square roots of negatve numbers and, more generally, complex numbers whch are the

More information

From Biot-Savart Law to Divergence of B (1)

From Biot-Savart Law to Divergence of B (1) From Bot-Savart Law to Dvergence of B (1) Let s prove that Bot-Savart gves us B (r ) = 0 for an arbtrary current densty. Frst take the dvergence of both sdes of Bot-Savart. The dervatve s wth respect to

More information

Singular Value Decomposition: Theory and Applications

Singular Value Decomposition: Theory and Applications Sngular Value Decomposton: Theory and Applcatons Danel Khashab Sprng 2015 Last Update: March 2, 2015 1 Introducton A = UDV where columns of U and V are orthonormal and matrx D s dagonal wth postve real

More information