PHY 745 Group Theory 11 11 50 AM

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PHY 745 Group Theory 11 -11: 50 AM MWF Olin 102 Plan for Lecture

PHY 745 Group Theory 11 -11: 50 AM MWF Olin 102 Plan for Lecture 4: The “great” orthogonality theorem Reading: Chapter 2 in DDJ 1. Schur’s lemmas 2. Prove the “Great Orthgonality Theorem” 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 1

1/20/2017 PHY 745 Spring 2017 -- Lecture 4 2

1/20/2017 PHY 745 Spring 2017 -- Lecture 4 2

The great orthogonality theorem on unitary irreducible representations 1/20/2017 PHY 745 Spring 2017 --

The great orthogonality theorem on unitary irreducible representations 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 3

Proof of the great orthogonality theorem • Prove that all representations can be unitary

Proof of the great orthogonality theorem • Prove that all representations can be unitary matrices • Prove Schur’s lemma part 1 – any matrix which commutes with all matrices of an irreducible representation must be a constant matrix • Prove Schur’s lemma part 2 • Put all parts together 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 4

Proof of the great orthogonality theorem • Prove that all representations can be unitary

Proof of the great orthogonality theorem • Prove that all representations can be unitary matrices • Prove Schur’s lemma part 1 – any matrix which commutes with all matrices of an irreducible representation must be a constant matrix • Prove Schur’s lemma part 2 • Put all parts together Schur’s lemma part 1: A matrix M which commutes with all of the matrices of an irreducible representation must be a constant matrix: M=s. I where s is a scalar constant and I is the identity matrix. 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 5

Schur’s lemmas part 1: A matrix M which commutes with all of the matrices

Schur’s lemmas part 1: A matrix M which commutes with all of the matrices of an irreducible representation must be a constant matrix: M=s. I where s is a scalar constant and I is the identity matrix. 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 6

Example irreducible representation: In these terms, the premise is: 1/20/2017 PHY 745 Spring 2017

Example irreducible representation: In these terms, the premise is: 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 7

Hermitian matrices can be diagonalized by a unitary transformation U 1/20/2017 PHY 745 Spring

Hermitian matrices can be diagonalized by a unitary transformation U 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 8

Proof of the great orthogonality theorem • Prove that all representations can be unitary

Proof of the great orthogonality theorem • Prove that all representations can be unitary matrices • Prove Schur’s lemma part 1 – any matrix which commutes with all matrices of an irreducible representation must be a constant matrix • Prove Schur’s lemma part 2 • Put all parts together 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 9

1/20/2017 PHY 745 Spring 2017 -- Lecture 4 10

1/20/2017 PHY 745 Spring 2017 -- Lecture 4 10

Schur’s lemma part 2 -- continued 1/20/2017 PHY 745 Spring 2017 -- Lecture 4

Schur’s lemma part 2 -- continued 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 11

Schur’s lemma part 2 -- continued 1/20/2017 PHY 745 Spring 2017 -- Lecture 4

Schur’s lemma part 2 -- continued 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 12

Proof of the great orthogonality theorem • Prove that all representations can be unitary

Proof of the great orthogonality theorem • Prove that all representations can be unitary matrices • Prove Schur’s lemma part 1 – any matrix which commutes with all matrices of an irreducible representation must be a constant matrix • Prove Schur’s lemma part 2 • Put all parts together 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 13

1/20/2017 PHY 745 Spring 2017 -- Lecture 4 14

1/20/2017 PHY 745 Spring 2017 -- Lecture 4 14

Proof continued: 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 15

Proof continued: 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 15

Proof continued: 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 16

Proof continued: 1/20/2017 PHY 745 Spring 2017 -- Lecture 4 16