1977
DOI: 10.1143/ptp.58.1377
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Monte Carlo Simulation of Quantum Spin Systems. I

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Cited by 274 publications
(168 citation statements)
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“…The factor N −2 corrects for the trivial free walk behavior that is present even in the absence of barriers. We now quantize the problem by introducing a standard Trotter-Suzuki time discretization [16]. We choose a regular temporal lattice with N τ = 128 or 256 time slices, a finite step size τ = 1 in the τ direction, and periodic boundary conditions in Trotter time.…”
Section: Results Of Simulationmentioning
confidence: 99%
“…The factor N −2 corrects for the trivial free walk behavior that is present even in the absence of barriers. We now quantize the problem by introducing a standard Trotter-Suzuki time discretization [16]. We choose a regular temporal lattice with N τ = 128 or 256 time slices, a finite step size τ = 1 in the τ direction, and periodic boundary conditions in Trotter time.…”
Section: Results Of Simulationmentioning
confidence: 99%
“…Note that τ needs to be chosen small enough with respect to the energy scales and the other relevant time scales of H (t) such that the exact mathematical solution of the TDSE is obtained up to some fixed numerical precision. Subsequently, the exponential of H (t + τ/2) is decomposed using the Lie-Trotter-Suzuki product formula [54]. This is done by partitioning the tridiagonal matrices into even and odd sums of 2 × 2 block-diagonal matrices such that each matrix exponential can be evaluated analytically (cf.…”
Section: Appendix A: Description Of the Algorithmmentioning
confidence: 99%
“…In early world-line Monte Carlo algorithms, updates of a configuration were done in many steps, 1,22,23) each being a local update that modifies only a small part of the system. Before the loop algorithm, the unit of the local update was a square whose spatial dimension equals the lattice spacing and the temporal dimension the discretization unit of time.…”
Section: Path Integral and Quantum Monte Carlomentioning
confidence: 99%