In General
* Idea: Originally, a
function whose gradient gives a physical field; Then extended to the mathematical
notion of a function (or sometimes a higher-rank tensor field) which gives,
by differentiation, a field of interest, possibly a dynamical tensor field.
> Vector potential: see aharonov-bohm, connection, electromagnetism.
In Classical Physics > s.a. scattering.
* Retarded potential: It has to be used for systems with large velocities
(corrections are of order v2/c2), or pairs of systems with large separations
compared to the internal motions (even if slow).
@ References: Kellogg 29; Grant & Rosner AJP(94)apr
[orbits in power law V].
@ Retarded potential: Spruch & Kelsey PRA(78)
[elementary derivation]; > s.a. arrow of time.
> Specific systems:
see classical systems; Coulomb
Potential; electromagnetism; newtonian gravitation.
> Results: see Bertrand's Theorem.
In Quantum Theory > s.a. effective
field theories [effective potential];
quantum field theory;
quantum systems [special types].
* Quasi-integrable: A
spectral problem depending on a parameter, such that a finite set of eigenvalues
can be obtained algebraically for special values
of the parameter.
@ Quantum potential: Dewdney & Hiley FP(82)
[and 1D scattering]; Garbaczewski PLA(92)
[from realistic Brownian particle motions]; Carroll qp/04, qp/04 [survey],
gq/05 [and
quantum fluctuations, Weyl tensor]; Delle Site PhyB(04)qp [many-particle
Bohm quantum potential]; Grössing PhyA(09)-a0808 [thermodynamic
origin]; > s.a. measurement, pilot-wave
interpretation.
@ PT-invariant: Weigert CzJP(04)qp; Ahmed JPA(05)
[classical orbits and quantization].
@ Other complex: Muga et al PRP(04) [scattering, absorption].
Specific Types > s.a. oscillator; Pöschl-Teller;
relativistic quantum mechanics [non-local];
schrödinger equation; Yukawa.
@ Inverse square: Gozzi & Mauro PLA(05)
[scale symmetry, anomaly]; Ávila-Aoki et al PLA(09) [classical and quantum
motion].
@ Exactly solvable: Fernández IJMPA(97)qp/96 [supersymmetric];
Rosas-Ortiz JPA(98)qp, qp/98-in;
de Prunelé JPA(06)
[2D]; Tremblay et al JPA(09) [and integrable, 2D, infinite family]; Odake & Sasaki a0906; > s.a. coherent
states.
@ Conditionally exactly solvable: Roychoudhury et al JMP(01).
@ Quasi-exactly solvable / integrable: Turbiner CMP(88), JPA(89);
Ushveridze
SJPP(89), 94; Lazutkin 93 [nearly integrable,
IV]; Braibant & Brihaye
JMP(93) [applications];
Ushveridze 94; Bender & Dunne JMP(96)ht/95;
Bender & Boettcher
JPA(98)phy [quartic];
Debergh et al qp/02, qp/02 [Darboux
transformations], qp/02;
Geojo et al JPA(03)qp/02 [Hamilton-Jacobi
method]; Atre & Panigrahi PLA(03)
[approach]; Bender & Monou qp/05 [sextic];
Koc & Koca mp/05 [Pöschl-Teller
et alia], mp/05 [Eckart-type
potentials]; Klishevich mp/06-in
[conditions].
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