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256:. The basic idea of the HS transformation is to reformulate a system of particles interacting through two-body potentials into a system of independent particles interacting with a fluctuating field. The procedure is widely used in
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276:. A major difficulty arising in the simulation with such field theories is their highly oscillatory nature in case of strong interactions, which leads to the well-known
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220:{\displaystyle \exp \left\{-{\frac {a}{2}}x^{2}\right\}={\sqrt {\frac {1}{2\pi a}}}\;\int _{-\infty }^{\infty }\exp \left\,dy,}
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The resulting field theories are well-suited for the application of effective approximation techniques, like the
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Stratonovich, R.L. (1958). "On a Method of
Calculating Quantum Distribution Functions".
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Hubbard, J. (1959). "Calculation of
Partition Functions".
299:Об одном методе вычисления квантовых функций распределения
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39:and popularized by British physicist
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35:invented by Russian physicist
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297:Стратонович, Р. Л. (1957).
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43:. It is used to convert a
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274:mean field approximation
230:where the real constant
345:Physical Review Letters
311:Translation available:
456:Condensed matter stubs
446:Functions and mappings
395:-related article is a
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278:numerical sign problem
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249:{\displaystyle a>0}
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61:auxiliary scalar field
37:Ruslan L. Stratonovich
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352:(2): 77.
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