In General
* Idea: Quantum mechanics
or quantum field theory is formulated as an equilibrium state of a statistical
system coupled to
a
thermal
reservoir in Euclidean space (see, e.g., the Fokker-Planck equation); This
can be considered
as an independent approach to quantum theory, or as a tool
to
evaluate (Euclidean) path integrals, with the same physical interpretation;
It is used mostly for gauge field theories.
* Remark: The real time t of
quantum theory cannot be used as the evolution parameter of the stochastic
process, since then one does not get the Schrödinger
equation.
References > s.a. modified quantum
mechanics [stochastic
extension].
@ Proposal: Nelson PR(66); Parisi & Wu SS(81); Altaisky ht/05-in
[multiscale version, wavelet-based].
@ General: Kracklauer PRD(74);
Ali RNC(85); Mielnik & Tengstrand IJTP(80)
[criticism]; Guerra & Marra PRD(83) [and operator algebra]; Damgaard & Hüffel
PRP(87),
ed-88; Klauder in(87); Parisi 88; Haba 99 [r Maassen van den Brink qp/02];
Masujima 00.
@ Related topics: de la Peña-Auerbach & Cetto PRD(71)
[self-interaction], NCB(72)
[diffusion coefficient]; Smolin PLA(86)
[quantum diffusion constant and inertial mass]; Pugnetti NPB(88)
[renormalization group]; Iengo & Pugnetti NPB(88)
[non-markovian regularization], NPB(88)
[critical exponents];
Wang PRA(88)
[role of interference]; Fliess qp/06 [quantum
fluctuations].
@ Quantum mechanics and stochastic mechanics: Carlen & Loffredo PLA(89)
[multiply connected apaces]; Garbaczewski PLA(90), PLA(90);
Schulz AdP(09)-a0807 [and
Bell's inequalities].
@ Quantum mechanics from stochastic metric fluctuations: Bergia et al PLA(89);
Calogero
PLA(97).
Variations
@ References: Beck ht/03-in
[chaotic quantization and standard model]; Kazinski a0704 [deformation
and relativistic diffusion equation]; Hüffel a0710-in [with non-linear Brownian
motion as underlying stochastic process].
For Specific Theories > s.a. boundaries
in field theory; semiclassical general relativity [stochastic].
@ Quantum mechanical systems:
Durran et al JMP(08) [atomic elliptic states].
@ Ising model: Bérard & Grandati IJTP(99).
@ Fermions: Guerra & Marra PRD(84);
Horsley & Schoenmaker PRD(85);
Garbaczewski FdP(90) [neutral spin-1/2].
@ Electrodynamics: Claverie & Diner IJQC(78);
Davidson JMP(81);
Puthoff PRA(89);
Hüffel & Kelnhofer PLB(04)ht/03 [=
path integral].
@ Gauge theory: Hüffel & Kelnhofer AP(98)ht [Yang-Mills];
Masujima 00; Zwanziger PRD(03)ht/02.
@ Quantum gravity: Prugovecki 84; Klauder in(86);
Rumpf in(86); Miller
JMP(99) [1+1];
> s.a. approaches to quantum gravity,
Horava Gravity.
@ Linearized gravity: Davidson JMP(82)qp/01.
@ Scalar fields: Menezes & Svaiter PhyA(07)ht/05 [![]()
4 theory];
Menezes
& Svaiter JPA(07)-a0706 [in
Einstein and Rindler spaces]; de Aguiar et al CQG(09)
[in de Sitter
space]; de Aguiar et al a0908 [at finite temperature].
@ Other theories: Garbaczewski JPA(87)
[Fermi oscillator]; Lim & Muniandy PLA(04)
[non-local fields]; Farajollahi &
Luckock gq/04/IJTGN
[locally
supersymmetric]; Hotta et al ht/04 [Born-Infeld
theory]; Haas IJTP(05)
[t-dependent oscillator]; Bhattacharjee & Gangopadhyay cm/05 [non-equilibrium
sm]; Menezes & Svaiter JMP(06)ht [topological
field theory]; Scarfone JSM(07)cm [interacting
particle systems]; Menezes & Svaiter JMP(08)-a0807 [systems
with complex-valued path
integral weights]; Dijkgraaf et al NPB(09) [relating field theories].
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send feedback and suggestions to bombelli at olemiss.edu – modified 18
oct
2009