Computational Many-Particle Physics
DOI: 10.1007/978-3-540-74686-7_13
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Path Integral Monte Carlo Simulation of Charged Particles in Traps

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Cited by 4 publications
(6 citation statements)
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“…To take advantage of the main benefits from the usual continuous space WA, we will temporarily construct artificial trajectories and sample new beads according to standard PIMC techniques, e.g. [43]. The initial situation for our considerations is illustrated in the left panel of figure 4, where a pre-existing trajectory (pink curve) with four missing beads in the middle is shown in the τ-x-plane.…”
Section: Sampling Schemementioning
confidence: 99%
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“…To take advantage of the main benefits from the usual continuous space WA, we will temporarily construct artificial trajectories and sample new beads according to standard PIMC techniques, e.g. [43]. The initial situation for our considerations is illustrated in the left panel of figure 4, where a pre-existing trajectory (pink curve) with four missing beads in the middle is shown in the τ-x-plane.…”
Section: Sampling Schemementioning
confidence: 99%
“…(i) Deform: this update is similar to standard PIMC techniques, e.g. [43], and deforms a randomly constructed artificial trajectory.…”
Section: Appendix Monte Carlo Updatesmentioning
confidence: 99%
“…To simulate the system using the standard path integral Monte Carlo method, e.g. [3,4], we exploit a group property of the density matrix…”
Section: Standard Pimcmentioning
confidence: 99%
“…However, even simple models used to describe interacting quantum systems in the regime where strong Coulomb correlations and quantum exchange effects are present are computationally very demanding. Therefore, trapped few-particle systems such as electrons in quantum dots [2] ("artificial atoms") serve as a suitable laboratory for the investigation of fundamental many-body interaction phenomena without requiring undesirable (uncontrollable) simplifications of the fundamental physics.Path integral Monte Carlo (PIMC) is a finite temperature simulation technique for an ab-initio description of correlated quantum systems with arbitrarily strong Coulomb and quantum exchange (spin) effects [3,4]. Furthermore, it provides a high flexibility with respect to trap geometry or the inclusion of defects et cetera, and quasi exact simulations with up to N ∼ 10 4 bosons and boltzmannons are feasible [5,6].…”
mentioning
confidence: 99%
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