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Computational Problem Lipkin Model

Understand the Lipkin Model through the commutation relation of angular momenta with SU(2), conservation laws, and Hamiltonian matrix calculation. Study quasi-spin properties and ground state characteristics.

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Computational Problem Lipkin Model

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  1. Computational Problem Lipkin Model m=1 m=2 m= e/2 s=1 Fermi level -e/2 s=-1 H. Lipkin, N. Meshkov & A.J. Glick, Nucl. Phys. 6, 188 (1965) Ring & Schuck, The Nuclear Many-Body Problem, Sec. 5.4 A.P. Severyukhin, M. Bender and P.-H. Heenen, Phys. Rev. C 74, 024311 (2006) quasi-spin operators: Commutation relation of angular momenta: SU(2) Remember:

  2. The LM Hamiltonian can be written as: As the Hamiltonian is written explicitly in terms of SU(2) generators, it commutes with the total quasi-spin operator eigenstates of the LM Hamiltonian conserve total quasi-spin The LM Hamiltonian conserves the total number of particles The third component of quasi-spin measures half of the difference between the number of particles in the upper and the lower levels.

  3. even number of particles signature operator odd number of particles Signature operation rotates by 180o around the third axis eigenstates of the LM Hamiltonian conserve signature q.n.

  4. Task: calculate Hamiltonian matrix! basis state Size of the basis (representation) is 2K+1 The single-particle term is diagonal in K0 The interaction term changes K0 by two Hamiltonian conserves quasi-spin and signature but mixes K0. For a given K, the size of the Hamiltonian matrix is 2K+1. It splits into two blocks with dimensions K and K+1 having different signature.

  5. m=1 m=2 m= e/2 s=1 Fermi level -e/2 s=-1 What is quasi-spin of the ground state? Consider If interaction is weak, the lowest energy of the system corresponds to occupying the lower level by N particles. What is K? • Homework: • set up the Hamiltonian matrix • diagonalize it for =1, V=0.1, =10, N=10

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