Quantum Mechanics for Nuclear Structure, Volume 2. Professor Kris Heyde
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1.17 The Bargmann representation
1.17.1 Representation of operators
1.18 Coherent states for SU(2)
1.19 Properties of SU(2) from coherent states
2 Addition of angular momenta and spins
2.1 The coupling of two spin-12 particles
2.2 The general coupling of two particles with spin or angular momentum
2.4 Vector spherical harmonics
2.5 Clebsch–Gordan coefficients and rotation matrices
2.6 The coupling of many spins and angular momenta and their recoupling
3 Vector and tensor operators
3.3 Matrix elements of spherical tensor operators and the Wigner–Eckart theorem
4 Identical particles
4.2 The occupation number representation for bosons
4.3 The occupation number representation for fermions
4.4 Hamiltonians and other operators in the occupation number representation
4.5 Condensed states (superconductors and superfluids)
4.5.1 Two fermions in a degenerate set of levels with a pairing force
4.5.2 Many fermions in a degenerate set of levels with a pairing force: the quasispin formalism
5 Group theory and quantum mechanics
5.2.3 Space–time transformation
5.3 Transformation on physical systems
5.4 Quantum mechanics: a synoptic view
5.5 Symmetry transformations in quantum mechanics
5.5.2 Consequences of symmetry in quantum mechanics
5.6 Models with symmetry in quantum mechanics
5.8 Dynamical or spectrum generating algebras
5.9.2 Continuous matrix groups
5.9.3 Compact and non-compact groups
5.9.4 Polynomial representation of groups
5.10 Generators of continuous groups and Lie algebras
5.10.1 The matrix group SO(3) and its generators