Particle Dynamics > see classical particles; spinning particles; parametrized systems.
Field Theories [with metric signature (–,+,+,+)]
* Maxwell field:
= –
|g|1/2
gac gbd Fab Fcd
= –|g|1/2 gac gbd
[a Ab]
[c Ad]
.
(Or multiply by 1/4
.) With
matter, add a term c–1 Aa Ja; > s.a.
Proca Theory.
* Weak interactions: For the original theory and the one with vector
bosons,
respectively,
= 2–1/2 G Ja(x)
Ja
(x) ,
=
g Ja(x) Wa(x) + h.c. ,
where Ja = la + ha and 2–1/2 G =
g2/mW2.
* Dirac field: With coupling
to a gauge field (check conventions; could add a non-linear, (![]()
)2 term)
=
(ic
aDa – mc2)
+
YM .
* Spin-1 field: In the massive case, the Proca Lagrangian [@ Proca CRAS(36)]
=
Ba
(x)
[
ab(
+
m2) –
a
b]
Bb(x) .
* Spin-2 field:
=
(
ahbc)
(
a hbc)
– (
a hab)
(
c hcb)
.
@ References: Bracken IJTP(05)
[electromagnetic].
> Other theories:
see dilaton; gravity; klein-gordon
field theory; monopoles; Nambu
Mechanics; scalar-tensor; yang-mills
gauge theory.
Other Theories > s.a. constraints; gauge
theory; graph theory.
@ Field theories: Szczyrba APM(76); Hájícek & Kijowski
PRD(98)gq/97 [with
discontinuities]; Boersma PRD(99)gq/00 [and
boundary terms];
Echeverría-Enríquez et al IJMMS(02)mp/01;
de León et al
mp/02, mp/02;
András
gq/04 [coupled
to general relativity].
@ Other types: Barbero & Villaseñor PRD(02)ht [quadratic,
Diff-invariant]; Scholle PRS(04)
[continuum theories]; Castrillón López et al a0711 [interacting
systems, "concatenating" variational
principles]; Crampin & Mestdag a0801 [invariant
Lagrangians on Lie groups]; Bernard & Contreras AM(08) [generic property of families
of Lagrangian systems].
Generalized Theories > s.a. deformation
quantization; higher-order
lagrangians.
* Non-commutative fielod theory:
For a scalar
3 theory,
if * is
the non-commutative
star-product,
= –
|g|1/2 [gab
a
b
+
(m2
2 +
g
*
*
)]
.
@ Singular Lagrangians: Gràcia & Pons JPA(01)mp/00;
Pugliese & Vinogradov
JGP(00);
Gitman & Tyutin NPB(02)ht [Hamiltonian];
Román-Roy mp/06-in.
@ With fractional derivatives: Dreisigmeyer & Young JPA(03)
[non-conservative]; Baleanu & Trujillo a0708 [including exact solutions].
@ Other systems: Hata PRD(94)ht/93 [theories/actions
as variables]; Marolf PLB(95)gq/94 [partial
system]; Baez & Gilliam LMP(94)
[discrete]; Soroka PAN(96)ht/95 [Grassmann-odd];
Fiziev & Kleinert gq/96 [action
principle in spaces with torsion]; Vankerschaver et al RPMP(05)
[non-holonomic,
geometric].
@ Other backgrounds: Marolf CQG(94)gq/93 [degenerate
metric]; Chamseddine & Connes
CMP(97)ht/96,
PRL(96)ht [nc
space].
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Send feedback and suggestions to bombelli at olemiss.edu – Modified
16 mar 2008