Shell model for large systems and quantum monte carlo diagonalization method

Author(s):  
Takaharu Otsuka ◽  
Michio Honma ◽  
Takahiro Mizusaki
1996 ◽  
Vol 77 (16) ◽  
pp. 3315-3318 ◽  
Author(s):  
Michio Honma ◽  
Takahiro Mizusaki ◽  
Takaharu Otsuka

1999 ◽  
Vol 10 (08) ◽  
pp. 1399-1407 ◽  
Author(s):  
S. TODO ◽  
K. KATO ◽  
H. TAKAYAMA ◽  
K. HARADA ◽  
N. KAWASHIMA ◽  
...  

Ground-state phase transition of site-diluted Heisenberg antiferromagnets on a square lattice is studied. By using the continuous-time loop algorithm, we perform large-scale quantum Monte Carlo simulation on large systems at quite low temperatures. It is found that the critical concentration of magnetic sites is independent of the spin size S, and equal to the classical percolation threshold. However, the existence of quantum fluctuations makes the critical exponents deviate from those of the classical percolation transition. It is found that the transition is not universal, i.e., the critical exponents depend on the spin size S.


2001 ◽  
Vol 15 (10n11) ◽  
pp. 1463-1473
Author(s):  
T. OTSUKA ◽  
T. MIZUSAKI ◽  
Y. UTSUNO ◽  
N. SHIMIZU ◽  
M. HONMA

The formulation and recent applications of the Quantum Monte Carlo diagonalization (QMCD) method are reported. The QMCD has been proposed for solving the quantum many-body inteacting systems, providing us with energy eigenvalues, transition matrix elements and wave functions. Its application to the nuclear shell model is referred to as the Monte Carlo Shell Model. By the Monte Carlo Shell Model calculations, the level structure of low-lying states can be studied with realistic interactions, providing a useful tool for nuclear spectroscopy. The Monte Carlo Shell Model has been applied to the study of a variety of nuclei, and can be characterized as the importance truncation scheme to the full diagonalization which is infeasible in many cases due to extremely large dimensions.


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