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Review of topics in group theory

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1 Review of topics in group theory
PHY 745 Group Theory 11-11:50 AM MWF Olin 102 Plan for Lecture 19: Review of topics in group theory Chapters 1-10 in DDJ General concepts and definitions in group theory Representations of groups; great orthogonality theorem Point groups; space groups 2/24/2017 PHY 745 Spring Lecture 19

2 2/24/2017 PHY 745 Spring Lecture 19

3 An abstract algebraic construction in mathematics
Group theory An abstract algebraic construction in mathematics Definition of a group: 2/24/2017 PHY 745 Spring Lecture 19

4 Class members of a group generated by the conjugate construction
Some definitions: Order of the group  number of elements (members) in the group (positive integer for finite group, ∞ for infinite group) Subgroup  collection of elements within a group which by themselves form a group Coset  Given a subgroup gi of a group a right coset can be formed by multiply an element of g with each element of gi Class members of a group generated by the conjugate construction 2/24/2017 PHY 745 Spring Lecture 19

5 Example of a 6-member group E,A,B,C,D,F,G
2/24/2017 PHY 745 Spring Lecture 19

6 For our example: 2/24/2017 PHY 745 Spring Lecture 19

7 Representations of a group
2/24/2017 PHY 745 Spring Lecture 19

8 Example: 2/24/2017 PHY 745 Spring Lecture 19

9 The great orthogonality theorem on unitary irreducible representations
2/24/2017 PHY 745 Spring Lecture 19

10 Great orthogonality theorem for characters
2/24/2017 PHY 745 Spring Lecture 19

11 Character table for P(3):
1 c2 -1 c3 2 2/24/2017 PHY 745 Spring Lecture 19

12 The number of characters=the number of classes
The characters ci behave as a vector space with the dimension equal to the number of classes. The number of characters=the number of classes 2/24/2017 PHY 745 Spring Lecture 19

13 “Standard” notation for representations of C2v
Example of H2O sv sv’ “Standard” notation for representations of C2v 2/24/2017 PHY 745 Spring Lecture 19

14 Symmetry analysis Dy1 Dy2 Dy3 Dx1 Dy1 Dz1 Dx2 R Dy2 Dz2 Dx3 Dy3 Dz3
C2 sv sv’ 2/24/2017 PHY 745 Spring Lecture 19

15 Dx Dx1 Dy Dy1 Dz Dz1 Dx Dx2 E Dy2 = Dy2 Dz Dz2 Dx Dx3 Dy Dy3 Dz Dz3 c(E)=9 2/24/2017 PHY 745 Spring Lecture 19

16 Dx Dx1 Dy Dy1 Dz Dz1 Dx Dx2 C2 Dy2 = Dy2 Dz Dz2 Dx Dx3 Dy Dy3 Dz Dz3 c(C2)=-1 Similarly: c(sv)=3 c(sv’)=1 2/24/2017 PHY 745 Spring Lecture 19

17 2/24/2017 PHY 745 Spring Lecture 19

18 2/24/2017 PHY 745 Spring Lecture 19

19 Some properties of continuous group SO(3)
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20 2/24/2017 PHY 745 Spring Lecture 19

21 Irreducible representations in terms of angular momentum eigenfunctions
2/24/2017 PHY 745 Spring Lecture 19

22 Group of all unitary matrices of dimension 2 – SU(2)
2/24/2017 PHY 745 Spring Lecture 19

23 Group of all unitary matrices of dimension 2 – SU(2) --continued
2/24/2017 PHY 745 Spring Lecture 19


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