Violation of CP symmetry. Charles Dunkl (University of Virginia)
|
|
- Benjamin Day
- 6 years ago
- Views:
Transcription
1 Violation of CP symmetry form a point of view of a mathematician Karol Życzkowski in collaboration with Charles Dunkl (University of Virginia) J. Math. Phys. 50, (2009). ZFCz IF UJ, Kraków January 24, 2012 KŻ (UJ) CP violation & unistochastic matrices / 18
2 Discussion with a mathematician: A communication issue: How to explain a mathematician a) What is the CKM Matrix? b) What the term violation of CP symmetry actually means? c) Is it related with the fact that the CKM Matrix is of size 3 (and not 2)? KŻ (UJ) CP violation & unistochastic matrices / 18
3 A mathematical perspective for CP violation I 1) In high energy physics two kinds of interactions are important. They are called strong and weak interactions. 2) Both interactions can be described by Hamiltonians represented by Hermitian matrices H s and H w. 3) Elementary particles consists of quarks, which can be divided into classes, called generations. Initially one used N = 2 generations of quarks, but new particles discovered in sixties forced us to include the third generation. Several later attempts to discover the fourth generation failed, so N = 3 (right now). 4) Both Hamiltonians are represented by generic Hermitian matrices of order N, so they do not commute, [H s, H w ] 0. KŻ (UJ) CP violation & unistochastic matrices / 18
4 A mathematical perspective for CP violation II 5) Representing Hermitian matrices by their eigendecompositions H w = N i=1 w i ψ i ψ i and H s = N j=1 s j φ j φ j one introduces a unitary matrix V U(N) which transforms one eigenbasis into another one: V ij := (ψ i,φ j ) = ψ i φ j. V CKM U(3) CKM matrix (Cabbibo-Kobayashi-Maskawa 1973) 6) Physicists are interested in this very matrix, but they can only measure transition probabilities, B ij = V ij 2, for i, j = 1,...,N. 7) The matrix B is bistochastic: has positive elements B ij 0, sum in each column (each row) equal to unity, i B ij = j B ij = 1. 8) A natural mathematical question arises: Given a bistochastic matrix B find out if there exists a corresponding unitary matrix V such that V ij 2 = B ij and check, whether such a unitary V is orthogonal. KŻ (UJ) CP violation & unistochastic matrices / 18
5 Set B N of bistochastic matrices of size N The Birkhoff polytope A square matrix B is called bistochastic (doubly stochastic) if it has positive elements B ij 0, the sum in each column and each row is equal to unity, i B ij = j B ij = 1. Birkhoff theorem. Every bistochastic matrix can be written as a convex combination of permutation matrices P k, B = k q kp k. Thus the set B N is called the Birkhoff polytope In general a matrix B B N is described by (N 1) 2 parameters, so the Birkhoff polytope B N Ê (N 1)2. Bistochastic matrices for N = 2 [ ] a 1 a B 2 = (a) = = a½ + (1 a)p 1 a a 12, for a [0, 1]. Thus N = 2 Birkhoff polytope is equivalent to unit interval, B 2 = [0, 1]. KŻ (UJ) CP violation & unistochastic matrices / 18
6 Set B N of bistochastic matrices of size N Bistochastic matrices for N = 3, for which B 3 Ê 4 b 1 b 2 1 b 1 b 2 B 3 (b 1, b 2, b 3, b 4 ) := b 3 b 4 1 b 3 b 4 B 3 1 b 1 b 3 1 b 2 b 4 4 i=1 b i 1 The set B 3 is the convex hull of 3! = 6 permutation matrices, {½, P = P 123, P 2 = P 132, P 12, P 13, P 23 }. W denotes the flat bistochastic matrix, W = 1 3 [1, 1, 1; 1, 1, 1; 1, 1, 1], located at the center of the Birkhoff polytope B 3. KŻ (UJ) CP violation & unistochastic matrices / 18
7 Unistochastic and orthostochastic matrices Definitions A bistochastic matrix B B N is called unistochastic if there exists a unitary U U(N) such that B ij = U ij 2, written B = f (U). A bistochastic matrix B B N is called orthostochastic if there exists an orthogonal O O(N) such that B ij = O ij 2, written B = f (O). Let U N and O N denote the sets of unistochastic and orthostochastic matrices of size N, respectively. By definition the following inclusion relation hold O N U N B N. KŻ (UJ) CP violation & unistochastic matrices / 18
8 Uni- and ortho-stochastic matrices for N = 2 Proposition For N = 2 all three sets coincide, O 2 = U 2 = B 2 = [0, 1]. [ Proof. Take any a [0, 1] and set B = a 1 a 1 a a The corresponding[ orthogonal matrix ] reads cos ϑ sinϑ O =, where a = cos sinϑ cos ϑ 2 ϑ. ]. In other words every N = 2 bistochastic matrix is orthostochastic (and thus also unistochastic). KŻ (UJ) CP violation & unistochastic matrices / 18
9 Uni- and ortho-stochastic matrices for N = 3 Proposition. For N = 3 both inclusion relations O 3 U 3 B 3 are proper. a) b) Proof by demonstration a) Fourier matrix F 3 = ω ω 2 with ω = e 2πi/3 is unitary and 1 ω 2 ω corresponds to the flat bistochastic matrix W = f (F 3 ), as W ij = 1/3. Thus W is unistochastic but not orthostochastic, since for N = 3 there are no Hadamard matrices. b) Example of Schur: the bistochastic matrix B S, B S = P+P2 2 = is bistochastic but not unistochastic KŻ (UJ) CP violation & unistochastic matrices / 18
10 Unistochasticity and chain link condition for N = 3 Unitarity condition UU = ½ can be written as u µ u ν = δ µ,ν Diagonal elements u µ u µ = 1, impose bistochasticity, i B iµ = 1 while orthogonality relation u µ u ν = 0 imposes further constraints for elements of B = f (U)! What constraints for unistochasticity? As the sum u 1 u 2 = 3 j=1 U j1uj2 = L 1e iχ 1 + L 2 e iχ 2 + L 3 e iχ 3 of three complex numbers should vanish, their (ordered) moduli L 1 L 2 L 3 satisfy the following chain link condition (triangle inequality) L 1 L 2 + L 3 with L k := B 1k B 2k. a) unistochastic matrix with a positive area of the unitarity triangle, A 2 > 0, b) limiting case: an orthostochastic matrix with A 2 = 0, c) bistochastic matrix B not included into U 3 for which A 2 < 0. KŻ (UJ) CP violation & unistochastic matrices / 18
11 Unitarity triangle formed by links L 1, L 2, L 3 The length of the links of the unitarity triangle read L 1 = b 1 b 2, L 2 = b 3 b 4, L 3 = (1 b 1 b 2 )(1 b 3 b 4 ), (1) Let p = (L 1 + L 2 + L 3 )/2 denotes its semiperimeter. Making use of the Heron s formula for the area of the triangle A = p(p L 1 )(p L 2 )(p L 3 ), (2) we arrive with a compact expression for the squared area A 2, A 2 = [4b 1 b 2 b 3 b 4 (b 1 + b 2 + b 3 + b 4 1 b 1 b 4 b 2 b 3 ) 2 ]/16. (3) The chain links conditions are equivalent to a single condition for unistochasticity: A 2 (B) 0 (if a triangle exists its area is real and positive!) KŻ (UJ) CP violation & unistochastic matrices / 18
12 The set U 3 of unistochastic matrices of size N = 3 cross-sections of U 3 (implied by A 2 (B) 0 ) Nonconvex 3-Hypocycloid obtained by the cross-section of U 3 along the plane spanned by the equilateral triangle (P, P 2,½), b) a similar cross-section along totally orthogonal plane, c) a view from above. The set O 3 of orthostochastic matrices Proposition. For N = 3 the set O 3 of orthostochastic matrices forms the boundary of the 4D set U 3 of unistochastic matrices. KŻ (UJ) CP violation & unistochastic matrices / 18
13 Unistochastic matrices are useful for quantizing classical dynamical systems (which lead to bistochastic transition matrices). Prot Pakoński, Ph.D. Thesis 2002, Pakoński, Życzkowski, Kuś, 2001, The set U 3 of N = 3 unistochastic matrices was investigated in Bentgsson, Ericsson, Kuś, Tadej, Życzkowski, Commun. Math. Phys. (2005). The set U 3 of unistochastic matrices of size N = 3 occupies (with respect to the Lebesgue measure) more than 3/4 of the corresponding Birkhoff polytope B 3, Dunkl, Życzkowski, 2009 vol(u 3 ) vol(b 3 ) = 8π2 = (4) 105 KŻ (UJ) CP violation & unistochastic matrices / 18
14 Unitarity triangle and Jarlskog invariant (for N = 3) Jarlskog invariant For any unitary U U(3) define the number J(U) := Im(U 11 U 22 U 12U 21) called Jarlskog invariant. Equivalent unitary matrices Two unitary matrices U and U are called equivalent if there exist two diagonal unitary matrices, D A and D B, and two permutations P A and P B such that U U = D A P A UP B D B (5) The following relation holds: if U U then J(U) = J(U ), Jarlskog 1985 Simple calculation shows that the Jarlskog invariant is related to the area of the unitarity triangle, J 2 (U) = 4A 2 (B), where B = f (U). KŻ (UJ) CP violation & unistochastic matrices / 18
15 Jarlskog invariant: extreme values Squared Jarlskog invariant, J 2 = 4A 2, computed for bistochastic matrices takes values between J 2 min = J2 (B s ) = 1/64 for the Schur bistochastic matrix (not unistochastic) to J 2 max = J 2 (W) = 1/108 for the flat bistochastic matrix W = f (F 3 ). If J 2 (B) = 0 the matrix B is orthostochastic. Jarlskog invariant: probability distribution a) J=2A Ι b) 2 2 J =4A Ι * P P 2 P P 2 Distributions a) P( J ) and b) P(J 2 ) at the cross-section of U 3 along the plane formed by two permutation matrices and the identity. KŻ (UJ) CP violation & unistochastic matrices / 18
16 Jarlskog invariant: probability distribution analytical formulae for moments and probability distribution P( J ) given explicitly as an integral of a hypergeometric function 2 F 1, Distributions P( J ) for random unistochastic matrices with respect to a) flat measure (dashed line); b) Haar measure (solid line). KŻ (UJ) CP violation & unistochastic matrices / 18
17 Jarlskog invariant for CKM matrix Experimental data for the CKM matrix V CKM give J obs (V CKM ) = 3.08 [+0.16, 0.18] 10 5 This implies the following probability that a random unitary matrix U U(3) distributed according to Haar measure yields a smaller value of the Jarlskog invariant P { J J obs } = 7.74 [+0.41, 0.45] Such a statement improves the estimation made in the 2009 paper of Gibbons, Gielen, Pope and Turok. Hence CKM matrix V CKM should not be considered as a generic unitary matrix drawn at random with respect to the Haar measure on U(3). KŻ (UJ) CP violation & unistochastic matrices / 18
18 Concluding Remarks A bistochastic matrix B corresponds to a unitary matrix if it is unistochastic, B = f (U) so that B ij = U ij 2. The set U N of unistochastic matrices is characterized for N = 3 as B U 3 A 2 (B) 0. For N 4 the unistochasticity problem for remains open. for N = 2 every bistochastic matrix is orthostochastic. For N = 3 a generic unistochastic matrix is not orthostochastic, so the underlying unitary is not real. Thus the symmetry with respect to complex conjugation is violated. For N = 3 we computed the volume of the set U 3 and the average value of the Jarlskog invariant J for a random Haar unitary matrix U U(3). Cumulative probability P { J J obs } is small, what (according to Gibbons et al.) may provide an argument that the CKM matrix V CKM is not a generic random unitary of order N = 3. KŻ (UJ) CP violation & unistochastic matrices / 18
Structured Hadamard matrices and quantum information
Structured Hadamard matrices and quantum information Karol Życzkowski in collaboration with Adam G asiorowski, Grzegorz Rajchel (Warsaw) Dardo Goyeneche (Concepcion/ Cracow/ Gdansk) Daniel Alsina, José
More informationQuantum Stochastic Maps and Frobenius Perron Theorem
Quantum Stochastic Maps and Frobenius Perron Theorem Karol Życzkowski in collaboration with W. Bruzda, V. Cappellini, H.-J. Sommers, M. Smaczyński Institute of Physics, Jagiellonian University, Cracow,
More informationNumerical range and random matrices
Numerical range and random matrices Karol Życzkowski in collaboration with P. Gawron, J. Miszczak, Z. Pucha la (Gliwice), C. Dunkl (Virginia), J. Holbrook (Guelph), B. Collins (Ottawa) and A. Litvak (Edmonton)
More informationQuantum Chaos and Nonunitary Dynamics
Quantum Chaos and Nonunitary Dynamics Karol Życzkowski in collaboration with W. Bruzda, V. Cappellini, H.-J. Sommers, M. Smaczyński Phys. Lett. A 373, 320 (2009) Institute of Physics, Jagiellonian University,
More informationComplex Hadamard matrices and some of their applications
Complex Hadamard matrices and some of their applications Karol Życzkowski in collaboration with W. Bruzda and W. S lomczyński (Cracow) W. Tadej (Warsaw) and I. Bengtsson (Stockholm) Institute of Physics,
More informationANOTHER METHOD FOR A GLOBAL FIT OF THE CABIBBO-KOBAYASHI-MASKAWA MATRIX
ANOTHER METHOD FOR A GLOBAL FIT OF THE CABIBBO-KOBAYASHI-MASKAWA MATRIX PETRE DIÞÃ Institute of Physics and Nuclear Engineering, P.O. Box MG6, Bucharest, Romania Received February 1, 005 Recently we proposed
More informationarxiv: v2 [math-ph] 7 Feb 2017
Equiangular tight frames and unistochastic matrices Dardo Goyeneche Institute of Physics, Jagiellonian University, Kraków, Poland Faculty of Applied Physics and Mathematics, Technical University of Gdańsk,
More informationGROUP THEORY PRIMER. New terms: so(2n), so(2n+1), symplectic algebra sp(2n)
GROUP THEORY PRIMER New terms: so(2n), so(2n+1), symplectic algebra sp(2n) 1. Some examples of semi-simple Lie algebras In the previous chapter, we developed the idea of understanding semi-simple Lie algebras
More informationPonownie o zasadach nieoznaczoności:
.. Ponownie o zasadach nieoznaczoności: Specjalne seminarium okolicznościowe CFT, 19 czerwca 2013 KŻ (CFT/UJ) Entropic uncertainty relations June 19, 2013 1 / 20 Majorization Entropic Uncertainty Relations
More informationDiagonalization by a unitary similarity transformation
Physics 116A Winter 2011 Diagonalization by a unitary similarity transformation In these notes, we will always assume that the vector space V is a complex n-dimensional space 1 Introduction A semi-simple
More informationarxiv: v1 [math-ph] 28 Jun 2016
The Birkhoff theorem for unitary matrices of arbitrary dimensions arxiv:1606.08642v1 [math-ph] 28 Jun 2016 Stijn De Baerdemacker a,b, Alexis De Vos c, Lin Chen d,e, Li Yu f a Ghent University, Center for
More informationA Concise Guide to Complex Hadamard Matrices
Open Sys. & Information Dyn. 2006 13: 133 177 DOI: 10.1007/s11080-006-8220-2 In a 1867 paper on simultaneous sign-successions, tessellated pavements in two or more colors, and ornamental tile-work Sylvester
More informationarxiv:quant-ph/ v2 25 May 2006
A concise guide to complex Hadamard matrices arxiv:quant-ph/0512154v2 25 May 2006 Wojciech Tadej 1 and Karol Życzkowski2,3 1 Faculty of Mathematics and Natural Sciences, College of Sciences, Cardinal Stefan
More informationRestricted Numerical Range and some its applications
Restricted Numerical Range and some its applications Karol Życzkowski in collaboration with P. Gawron, J. Miszczak, Z. Pucha la (Gliwice), L. Skowronek (Kraków), M.D. Choi (Toronto), C. Dunkl (Virginia)
More informationON ONE PARAMETRIZATION OF KOBAYASHI-MASKAWA MATRIX
ELEMENTARY PARTICLE PHYSICS ON ONE PARAMETRIZATION OF KOBAYASHI-MASKAWA MATRIX P. DITA Horia Hulubei National Institute for Nuclear Physics and Engineering, P.O.Box MG-6, RO-077125 Bucharest-Magurele,
More informationFilterbank Optimization with Convex Objectives and the Optimality of Principal Component Forms
100 IEEE TRANSACTIONS ON SIGNAL PROCESSING, VOL. 49, NO. 1, JANUARY 2001 Filterbank Optimization with Convex Objectives and the Optimality of Principal Component Forms Sony Akkarakaran, Student Member,
More informationLECTURE 10: THE ATIYAH-GUILLEMIN-STERNBERG CONVEXITY THEOREM
LECTURE 10: THE ATIYAH-GUILLEMIN-STERNBERG CONVEXITY THEOREM Contents 1. The Atiyah-Guillemin-Sternberg Convexity Theorem 1 2. Proof of the Atiyah-Guillemin-Sternberg Convexity theorem 3 3. Morse theory
More informationPhysics 4022 Notes on Density Matrices
Physics 40 Notes on Density Matrices Definition: For a system in a definite normalized state ψ > the density matrix ρ is ρ = ψ >< ψ 1) From Eq 1 it is obvious that in the basis defined by ψ > and other
More informationNotes on SU(3) and the Quark Model
Notes on SU() and the Quark Model Contents. SU() and the Quark Model. Raising and Lowering Operators: The Weight Diagram 4.. Triangular Weight Diagrams (I) 6.. Triangular Weight Diagrams (II) 8.. Hexagonal
More informationQuark flavour physics
Quark flavour physics Michal Kreps Physics Department Plan Kaon physics and SM construction (bit of history) Establishing SM experimentally Looking for breakdown of SM Hard to cover everything in details
More informationOptimisation Problems for the Determinant of a Sum of 3 3 Matrices
Irish Math. Soc. Bulletin 62 (2008), 31 36 31 Optimisation Problems for the Determinant of a Sum of 3 3 Matrices FINBARR HOLLAND Abstract. Given a pair of positive definite 3 3 matrices A, B, the maximum
More informationParity violation. no left-handed ν$ are produced
Parity violation Wu experiment: b decay of polarized nuclei of Cobalt: Co (spin 5) decays to Ni (spin 4), electron and anti-neutrino (spin ½) Parity changes the helicity (H). Ø P-conservation assumes a
More informationValerio Cappellini. References
CETER FOR THEORETICAL PHYSICS OF THE POLISH ACADEMY OF SCIECES WARSAW, POLAD RADOM DESITY MATRICES AD THEIR DETERMIATS 4 30 SEPTEMBER 5 TH SFB TR 1 MEETIG OF 006 I PRZEGORZAłY KRAKÓW Valerio Cappellini
More informationIGA Lecture I: Introduction to G-valued moment maps
IGA Lecture I: Introduction to G-valued moment maps Adelaide, September 5, 2011 Review: Hamiltonian G-spaces Let G a Lie group, g = Lie(G), g with co-adjoint G-action denoted Ad. Definition A Hamiltonian
More informationSYMMETRY BEHIND FLAVOR PHYSICS: THE STRUCTURE OF MIXING MATRIX. Min-Seok Seo (Seoul National University)
SYMMETRY BEHIND FLAVOR PHYSICS: THE STRUCTURE OF MIXING MATRIX Min-Seok Seo (Seoul National University) INTRODUCTION Flavor Issues in Standard Model: 1. Mass hierarchy of quarks and leptons 2. Origin of
More informationNeutrino Masses & Flavor Mixing 邢志忠. Zhi-zhong Xing. (IHEP, Winter School 2010, Styria, Austria. Lecture B
Neutrino Masses & Flavor Mixing Zhi-zhong Xing 邢志忠 (IHEP, Beijing) @Schladming Winter School 2010, Styria, Austria Lecture B Lepton Flavors & Nobel Prize 2 1975 1936 = 1936 1897 = 39 Positron: Predicted
More informationConstructive quantum scaling of unitary matrices
Quantum Inf Process (016) 15:5145 5154 DOI 10.1007/s1118-016-1448-z Constructive quantum scaling of unitary matrices Adam Glos 1, Przemysław Sadowski 1 Received: 4 March 016 / Accepted: 1 September 016
More informationSupplement to Multiresolution analysis on the symmetric group
Supplement to Multiresolution analysis on the symmetric group Risi Kondor and Walter Dempsey Department of Statistics and Department of Computer Science The University of Chicago risiwdempsey@uchicago.edu
More informationLecture 3: QR-Factorization
Lecture 3: QR-Factorization This lecture introduces the Gram Schmidt orthonormalization process and the associated QR-factorization of matrices It also outlines some applications of this factorization
More information1. Groups Definitions
1. Groups Definitions 1 1. Groups Definitions A group is a set S of elements between which there is defined a binary operation, usually called multiplication. For the moment, the operation will be denoted
More informationA LITTLE TASTE OF SYMPLECTIC GEOMETRY: THE SCHUR-HORN THEOREM CONTENTS
A LITTLE TASTE OF SYMPLECTIC GEOMETRY: THE SCHUR-HORN THEOREM TIMOTHY E. GOLDBERG ABSTRACT. This is a handout for a talk given at Bard College on Tuesday, 1 May 2007 by the author. It gives careful versions
More informationMATH 423 Linear Algebra II Lecture 33: Diagonalization of normal operators.
MATH 423 Linear Algebra II Lecture 33: Diagonalization of normal operators. Adjoint operator and adjoint matrix Given a linear operator L on an inner product space V, the adjoint of L is a transformation
More informationHamiltonian Toric Manifolds
Hamiltonian Toric Manifolds JWR (following Guillemin) August 26, 2001 1 Notation Throughout T is a torus, T C is its complexification, V = L(T ) is its Lie algebra, and Λ V is the kernel of the exponential
More informationAppendix: SU(2) spin angular momentum and single spin dynamics
Phys 7 Topics in Particles & Fields Spring 03 Lecture v0 Appendix: SU spin angular momentum and single spin dynamics Jeffrey Yepez Department of Physics and Astronomy University of Hawai i at Manoa Watanabe
More informationTrades in complex Hadamard matrices
Trades in complex Hadamard matrices Padraig Ó Catháin Ian M. Wanless School of Mathematical Sciences, Monash University, VIC 3800, Australia. February 9, 2015 Abstract A trade in a complex Hadamard matrix
More informationRESEARCH ARTICLE. An extension of the polytope of doubly stochastic matrices
Linear and Multilinear Algebra Vol. 00, No. 00, Month 200x, 1 15 RESEARCH ARTICLE An extension of the polytope of doubly stochastic matrices Richard A. Brualdi a and Geir Dahl b a Department of Mathematics,
More informationSymmetries for fun and profit
Symmetries for fun and profit Sourendu Gupta TIFR Graduate School Quantum Mechanics 1 August 28, 2008 Sourendu Gupta (TIFR Graduate School) Symmetries for fun and profit QM I 1 / 20 Outline 1 The isotropic
More informationMeasurement of CP Violation in B s J/ΨΦ Decay at CDF
Measurement of CP Violation in B s J/ΨΦ Decay at CDF Gavril Giurgiu Johns Hopkins University University of Virginia Seminar April 4, 2012 Introduction - CP violation means that the laws of nature are not
More informationSpectral Theorem for Self-adjoint Linear Operators
Notes for the undergraduate lecture by David Adams. (These are the notes I would write if I was teaching a course on this topic. I have included more material than I will cover in the 45 minute lecture;
More informationSYMPLECTIC GEOMETRY: LECTURE 5
SYMPLECTIC GEOMETRY: LECTURE 5 LIAT KESSLER Let (M, ω) be a connected compact symplectic manifold, T a torus, T M M a Hamiltonian action of T on M, and Φ: M t the assoaciated moment map. Theorem 0.1 (The
More informationINNER PRODUCT SPACE. Definition 1
INNER PRODUCT SPACE Definition 1 Suppose u, v and w are all vectors in vector space V and c is any scalar. An inner product space on the vectors space V is a function that associates with each pair of
More informationQuarks and Leptons. Subhaditya Bhattacharya, Ernest Ma, Alexander Natale, and Daniel Wegman
UCRHEP-T54 October 01 Heptagonic Symmetry for arxiv:110.6936v1 [hep-ph] 5 Oct 01 Quarks and Leptons Subhaditya Bhattacharya, Ernest Ma, Alexander Natale, and Daniel Wegman Department of Physics and Astronomy,
More informationNumerical Range of non-hermitian random Ginibre matrices and the Dvoretzky theorem
Numerical Range of non-hermitian random Ginibre matrices and the Dvoretzky theorem Karol Życzkowski Institute of Physics, Jagiellonian University, Cracow and Center for Theoretical Physics, PAS, Warsaw
More informationCompound matrices and some classical inequalities
Compound matrices and some classical inequalities Tin-Yau Tam Mathematics & Statistics Auburn University Dec. 3, 04 We discuss some elegant proofs of several classical inequalities of matrices by using
More informationON CONSTRUCTION OF HADAMARD MATRICES
International Journal of Science, Environment and Technology, Vol. 5, No 2, 2016, 389 394 ISSN 2278-3687 (O) 2277-663X (P) ON CONSTRUCTION OF HADAMARD MATRICES Abdul Moiz Mohammed 1 & Mohammed Abdul Azeem
More informationSubadditivity of entropy for stochastic matrices
Subadditivity of entropy for stochastic matrices Wojciech S lomczyński 1 PREPRIT 2001/16 Abstract The entropy of irreducible stochastic matrix measures its mixing properties. We show that this quantity
More informationOn the algebraic structure of Dyson s Circular Ensembles. Jonathan D.H. SMITH. January 29, 2012
Scientiae Mathematicae Japonicae 101 On the algebraic structure of Dyson s Circular Ensembles Jonathan D.H. SMITH January 29, 2012 Abstract. Dyson s Circular Orthogonal, Unitary, and Symplectic Ensembles
More informationEigenvalues and Eigenvectors
/88 Chia-Ping Chen Department of Computer Science and Engineering National Sun Yat-sen University Linear Algebra Eigenvalue Problem /88 Eigenvalue Equation By definition, the eigenvalue equation for matrix
More informationAssignment 1: From the Definition of Convexity to Helley Theorem
Assignment 1: From the Definition of Convexity to Helley Theorem Exercise 1 Mark in the following list the sets which are convex: 1. {x R 2 : x 1 + i 2 x 2 1, i = 1,..., 10} 2. {x R 2 : x 2 1 + 2ix 1x
More informationLie Algebra and Representation of SU(4)
EJTP, No. 8 9 6 Electronic Journal of Theoretical Physics Lie Algebra and Representation of SU() Mahmoud A. A. Sbaih, Moeen KH. Srour, M. S. Hamada and H. M. Fayad Department of Physics, Al Aqsa University,
More informationGROUP THEORY PRIMER. D(g 1 g 2 ) = D(g 1 )D(g 2 ), g 1, g 2 G. and, as a consequence, (2) (3)
GROUP THEORY PRIMER New terms: representation, irreducible representation, completely reducible representation, unitary representation, Mashke s theorem, character, Schur s lemma, orthogonality theorem,
More informationSymmetries, Groups, and Conservation Laws
Chapter Symmetries, Groups, and Conservation Laws The dynamical properties and interactions of a system of particles and fields are derived from the principle of least action, where the action is a 4-dimensional
More informationTheory of CP Violation
Theory of CP Violation IPPP, Durham CP as Natural Symmetry of Gauge Theories P and C alone are not natural symmetries: consider chiral gauge theory: L = 1 4 F µνf µν + ψ L i σdψ L (+ψ R iσ ψ R) p.1 CP
More informationWeak Interactions Cabbibo Angle and Selection Rules
Particle and s Cabbibo Angle and 03/22/2018 My Office Hours: Thursday 1:00-3:00 PM 212 Keen Building Outline 1 2 3 4 Helicity Helicity: Spin quantization along direction of motion. Helicity Helicity: Spin
More informationA group G is a set of discrete elements a, b, x alongwith a group operator 1, which we will denote by, with the following properties:
1 Why Should We Study Group Theory? Group theory can be developed, and was developed, as an abstract mathematical topic. However, we are not mathematicians. We plan to use group theory only as much as
More informationArchive of past papers, solutions and homeworks for. MATH 224, Linear Algebra 2, Spring 2013, Laurence Barker
Archive of past papers, solutions and homeworks for MATH 224, Linear Algebra 2, Spring 213, Laurence Barker version: 4 June 213 Source file: archfall99.tex page 2: Homeworks. page 3: Quizzes. page 4: Midterm
More informationEntropic Uncertainty Relations, Unbiased bases and Quantification of Quantum Entanglement
Entropic Uncertainty Relations, Unbiased bases and Quantification of Quantum Entanglement Karol Życzkowski in collaboration with Lukasz Rudnicki (Warsaw) Pawe l Horodecki (Gdańsk) Phys. Rev. Lett. 107,
More informationFlavour Physics Lecture 1
Flavour Physics Lecture 1 Chris Sachrajda School of Physics and Astronomy University of Southampton Southampton SO17 1BJ UK New Horizons in Lattice Field Theory, Natal, Rio Grande do Norte, Brazil March
More informationAssignment 3. A tutorial on the applications of discrete groups.
Assignment 3 Given January 16, Due January 3, 015. A tutorial on the applications of discrete groups. Consider the group C 3v which is the cyclic group with three elements, C 3, augmented by a reflection
More informationarxiv:quant-ph/ v1 29 Mar 2003
Finite-Dimensional PT -Symmetric Hamiltonians arxiv:quant-ph/0303174v1 29 Mar 2003 Carl M. Bender, Peter N. Meisinger, and Qinghai Wang Department of Physics, Washington University, St. Louis, MO 63130,
More informationClarkson Inequalities With Several Operators
isid/ms/2003/23 August 14, 2003 http://www.isid.ac.in/ statmath/eprints Clarkson Inequalities With Several Operators Rajendra Bhatia Fuad Kittaneh Indian Statistical Institute, Delhi Centre 7, SJSS Marg,
More informationTriangular mass matrices of quarks and Cabibbo-Kobayashi-Maskawa mixing
PHYSICAL REVIEW D VOLUME 57, NUMBER 11 1 JUNE 1998 Triangular mass matrices of quarks and Cabibbo-Kobayashi-Maskawa mixing Rainer Häussling* Institut für Theoretische Physik, Universität Leipzig, D-04109
More informationKähler configurations of points
Kähler configurations of points Simon Salamon Oxford, 22 May 2017 The Hesse configuration 1/24 Let ω = e 2πi/3. Consider the nine points [0, 1, 1] [0, 1, ω] [0, 1, ω 2 ] [1, 0, 1] [1, 0, ω] [1, 0, ω 2
More informationIntroduction to Modern Quantum Field Theory
Department of Mathematics University of Texas at Arlington Arlington, TX USA Febuary, 2016 Recall Einstein s famous equation, E 2 = (Mc 2 ) 2 + (c p) 2, where c is the speed of light, M is the classical
More informationBRST and Dirac Cohomology
BRST and Dirac Cohomology Peter Woit Columbia University Dartmouth Math Dept., October 23, 2008 Peter Woit (Columbia University) BRST and Dirac Cohomology October 2008 1 / 23 Outline 1 Introduction 2 Representation
More informationQuantum Field Theory II
Quantum Field Theory II T. Nguyen PHY 391 Independent Study Term Paper Prof. S.G. Rajeev University of Rochester April 2, 218 1 Introduction The purpose of this independent study is to familiarize ourselves
More informationElectric Dipole Moment and Neutrino Mixing due to Planck Scale Effects
EJTP 7, No. 23 (2010) 35 40 Electronic Journal of Theoretical Physics Electric Dipole Moment and Neutrino Mixing due to Planck Scale Effects Bipin Singh Koranga Kirori Mal College (University of Delhi,)
More informationPart 1a: Inner product, Orthogonality, Vector/Matrix norm
Part 1a: Inner product, Orthogonality, Vector/Matrix norm September 19, 2018 Numerical Linear Algebra Part 1a September 19, 2018 1 / 16 1. Inner product on a linear space V over the number field F A map,
More informationGLOBAL, GEOMETRICAL COORDINATES ON FALBEL S CROSS-RATIO VARIETY
GLOBAL GEOMETRICAL COORDINATES ON FALBEL S CROSS-RATIO VARIETY JOHN R. PARKER & IOANNIS D. PLATIS Abstract. Falbel has shown that four pairwise distinct points on the boundary of complex hyperbolic -space
More informationThe C-Numerical Range in Infinite Dimensions
The C-Numerical Range in Infinite Dimensions Frederik vom Ende Technical University of Munich June 17, 2018 WONRA 2018 Joint work with Gunther Dirr (University of Würzburg) Frederik vom Ende (TUM) C-Numerical
More informationOptimal Realizations of Controlled Unitary Gates
Optimal Realizations of Controlled nitary Gates Guang Song and Andreas Klappenecker Department of Computer Science Texas A&M niversity College Station, TX 77843-3112 {gsong,klappi}@cs.tamu.edu Abstract
More informationRotational motion of a rigid body spinning around a rotational axis ˆn;
Physics 106a, Caltech 15 November, 2018 Lecture 14: Rotations The motion of solid bodies So far, we have been studying the motion of point particles, which are essentially just translational. Bodies with
More informationCKM Matrix and CP Violation in Standard Model
CKM Matrix and CP Violation in Standard Model CP&Viola,on&in&Standard&Model&& Lecture&15& Shahram&Rahatlou& Fisica&delle&Par,celle&Elementari,&Anno&Accademico&2014815& http://www.roma1.infn.it/people/rahatlou/particelle/
More informationarxiv: v1 [quant-ph] 4 Jul 2013
GEOMETRY FOR SEPARABLE STATES AND CONSTRUCTION OF ENTANGLED STATES WITH POSITIVE PARTIAL TRANSPOSES KIL-CHAN HA AND SEUNG-HYEOK KYE arxiv:1307.1362v1 [quant-ph] 4 Jul 2013 Abstract. We construct faces
More informationWavelets and Linear Algebra
Wavelets and Linear Algebra 4(1) (2017) 43-51 Wavelets and Linear Algebra Vali-e-Asr University of Rafsanan http://walavruacir Some results on the block numerical range Mostafa Zangiabadi a,, Hamid Reza
More informationLinear Algebra and Dirac Notation, Pt. 1
Linear Algebra and Dirac Notation, Pt. 1 PHYS 500 - Southern Illinois University February 1, 2017 PHYS 500 - Southern Illinois University Linear Algebra and Dirac Notation, Pt. 1 February 1, 2017 1 / 13
More informationGENERALIZED NUMERICAL RANGES AND QUANTUM ERROR CORRECTION
J. OPERATOR THEORY 00:0(0000, 101 110 Copyright by THETA, 0000 GENERALIZED NUMERICAL RANGES AND QUANTUM ERROR CORRECTION CHI-KWONG LI and YIU-TUNG POON Communicated by Editor ABSTRACT. For a noisy quantum
More informationGroup Theory and the Quark Model
Version 1 Group Theory and the Quark Model Milind V Purohit (U of South Carolina) Abstract Contents 1 Introduction Symmetries and Conservation Laws Introduction Finite Groups 4 1 Subgroups, Cosets, Classes
More informationLecture 11. Weak interactions
Lecture 11 Weak interactions 1962-66: Formula/on of a Unified Electroweak Theory (Glashow, Salam, Weinberg) 4 intermediate spin 1 interaction carriers ( bosons ): the photon (γ) responsible for all electromagnetic
More informationSymmetry Groups conservation law quantum numbers Gauge symmetries local bosons mediate the interaction Group Abelian Product of Groups simple
Symmetry Groups Symmetry plays an essential role in particle theory. If a theory is invariant under transformations by a symmetry group one obtains a conservation law and quantum numbers. For example,
More information3 Quantization of the Dirac equation
3 Quantization of the Dirac equation 3.1 Identical particles As is well known, quantum mechanics implies that no measurement can be performed to distinguish particles in the same quantum state. Elementary
More informationTOPICS IN HARMONIC ANALYSIS WITH APPLICATIONS TO RADAR AND SONAR. Willard Miller
TOPICS IN HARMONIC ANALYSIS WITH APPLICATIONS TO RADAR AND SONAR Willard Miller October 23 2002 These notes are an introduction to basic concepts and tools in group representation theory both commutative
More informationHamilton Cycles in Digraphs of Unitary Matrices
Hamilton Cycles in Digraphs of Unitary Matrices G. Gutin A. Rafiey S. Severini A. Yeo Abstract A set S V is called an q + -set (q -set, respectively) if S has at least two vertices and, for every u S,
More informationFactorizable completely positive maps and quantum information theory. Magdalena Musat. Sym Lecture Copenhagen, May 9, 2012
Factorizable completely positive maps and quantum information theory Magdalena Musat Sym Lecture Copenhagen, May 9, 2012 Joint work with Uffe Haagerup based on: U. Haagerup, M. Musat: Factorization and
More informationStatus of the Cabibbo-Kobayashi-Maskawa Quark Mixing Matrix
Status of the Cabibbo-Kobayashi-Maskawa Quark Mixing Matrix Johannes-Gutenberg Universität, Mainz, Germany Electronic address: Burkhard.Renk@uni-mainz.de Summary. This review, prepared for the 2002 Review
More informationThe S 3. symmetry: Flavour and texture zeroes. Journal of Physics: Conference Series. Related content. Recent citations
Journal of Physics: Conference Series The S symmetry: Flavour and texture zeroes To cite this article: F González Canales and A Mondragón 2011 J. Phys.: Conf. Ser. 287 012015 View the article online for
More informationdeterminantal conjecture, Marcus-de Oliveira, determinants, normal matrices,
1 3 4 5 6 7 8 BOUNDARY MATRICES AND THE MARCUS-DE OLIVEIRA DETERMINANTAL CONJECTURE AMEET SHARMA Abstract. We present notes on the Marcus-de Oliveira conjecture. The conjecture concerns the region in the
More informationImplications of Time-Reversal Symmetry in Quantum Mechanics
Physics 215 Winter 2018 Implications of Time-Reversal Symmetry in Quantum Mechanics 1. The time reversal operator is antiunitary In quantum mechanics, the time reversal operator Θ acting on a state produces
More informationMathematical contributions to the theory of Dirac matrices
Contributions mathématiques à la théorie des matrices de Dirac nn. de l Inst. Henri Poincaré 6 (936) 09-36. Mathematical contributions to the theory of Dirac matrices By W. PULI Zurich Translated by D
More informationWeak Interactions and Mixing (adapted)
Observations and Implications Weak Interactions and Mixing (adapted) Heavy particles that are produced very readily in nuclear collisions but which decay very slowly despite their heavy mass are said to
More informationLecture 2: Vector-Vector Operations
Lecture 2: Vector-Vector Operations Vector-Vector Operations Addition of two vectors Geometric representation of addition and subtraction of vectors Vectors and points Dot product of two vectors Geometric
More informationA little taste of symplectic geometry
A little taste of symplectic geometry Timothy Goldberg Thursday, October 4, 2007 Olivetti Club Talk Cornell University 1 2 What is symplectic geometry? Symplectic geometry is the study of the geometry
More informationOn a non-cp-violating electric dipole moment of elementary. particles. J. Giesen, Institut fur Theoretische Physik, Bunsenstrae 9, D Gottingen
On a non-cp-violating electric dipole moment of elementary particles J. Giesen, Institut fur Theoretische Physik, Bunsenstrae 9, D-3773 Gottingen (e-mail: giesentheo-phys.gwdg.de) bstract description of
More informationMath 407: Linear Optimization
Math 407: Linear Optimization Lecture 16: The Linear Least Squares Problem II Math Dept, University of Washington February 28, 2018 Lecture 16: The Linear Least Squares Problem II (Math Dept, University
More informationRepresentation theory and quantum mechanics tutorial Spin and the hydrogen atom
Representation theory and quantum mechanics tutorial Spin and the hydrogen atom Justin Campbell August 3, 2017 1 Representations of SU 2 and SO 3 (R) 1.1 The following observation is long overdue. Proposition
More informationIoP Masterclass B PHYSICS. Tim Gershon University of Warwick March 18 th 2009
IoP Masterclass B PHYSICS Tim Gershon University of Warwick March 18 th 2009 The Standard Model 2 Some Questions What is antimatter? Why are there three colours of quarks? Why are there so many bosons?
More informationMath 350 Fall 2011 Notes about inner product spaces. In this notes we state and prove some important properties of inner product spaces.
Math 350 Fall 2011 Notes about inner product spaces In this notes we state and prove some important properties of inner product spaces. First, recall the dot product on R n : if x, y R n, say x = (x 1,...,
More information11. Representations of compact Lie groups
11. Representations of compact Lie groups 11.1. Integration on compact groups. In the simplest examples like R n and the torus T n we have the classical Lebesgue measure which defines a translation invariant
More informationLie Theory in Particle Physics
Lie Theory in Particle Physics Tim Roethlisberger May 5, 8 Abstract In this report we look at the representation theory of the Lie algebra of SU(). We construct the general finite dimensional irreducible
More information2-Dimensional Density Matrices
A Transformational Property of -Dimensional Density Matrices Nicholas Wheeler January 03 Introduction. This note derives from recent work related to decoherence models described by Zurek and Albrecht.
More information