In General > s.a. torsion.
* Motivation: Torsion
arises in string theory as an antisymmetric field, and would be required by
the modification of general relativity that can accomodate the
existence
of gravitomagnetic monopoles.
* Minimal coupling: Requires
that the trace of the torsion tensor be a gradient, Ta =
a
,
and that the modified volume element
=
exp{
} |g| dx1
...
dxn
be used in the action formulation of a physical model.
@ General references: Hehl & Obukhov a0711 [geometry
and field theory].
@ Dynamics of torsion: Saa GRG(97)gq/96;
Mosna & Saa JMP(05)gq [minimal
coupling]; Poplawski gq/06,
JMP(06).
@ Singularities: García de Andrade FP(90), IJTP(90); Esposito
NCB(90)gq/95, FdP(92)gq/95.
@ Topological defects: Letelier CQG(95)gq; Garcia de Andrade MPLA(97),
JMP(98)gq/98, gq/98 [domain
walls], gq/99/PRD;
Anandan gq/99-in.
@ And electromagnetism: Hammond GRG(88), GRG(91);
Horie ht/95;
de Andrade & Pereira IJMPD(99)gq/97;
Filewood
gq/98; Rubilar
et al CQG(03)
[and birefringence].
@ Angular momentum conservation: Yishi Duan & Ying Jiang GRG(99)gq/98;
Capozziello et al EPL(99)ap [fermion
helicity flip].
@ And topological invariants: Aouane et al CQG(07)
[from integral of Nieh-Yan 4-form]; Nieh IJMPA(07)
[rev].
> Specific theories:
see dirac
fields in curved spacetime; field
theories; particle
models; schwarzschild.
> Related topics: see
lagrangian theories;
lorentz invariance; regge
calculus; sound [acoustic torsion].
And Gravity > s.a. gravitation.
* Couplings and gravity:
In general, torsion couples to the spin current of the Dirac field; In the
teleparallel theory of gravity, curvature and torsion are alternative ways
of describing the gravitational field, and are consequently related to the
same degrees of freedom; More general gravity theories, like Einstein-Cartan
and gauge theories for the Poincaré and the affine groups, consider
curvature and torsion as representing independent degrees of freedom.
@ General references: Hehl et al RMP(76);
Penrose FP(83);
Hehl FP(85);
Hammond GRG(90), GRG(94), GRG(94), CP(95)
[II]; Gangopadhyay & Sengupta ht/97 [symmetries];
Fiziev gq/98-in, gq/98;
Israelit FP(98)-a0712,
in(99)-a0712 [and
electromagnetism]; de Sabbata & Ronchetti FP(99)
[Hamiltonian]; Megged ht/00 [gravity
+ Yang-Mills]; Garecki RGC(04)gq/01 [overview, T not
needed]; Mahato MPLA(02)gq/06 [G in
Riemann-Cartan spacetime]; Watanabe & Hayashi gq/04;
Arcos & Pereira CQG(04), IJMPD(04)gq/05 [rev];
Mahato IJMPA(07)gq/06;
Kim & Pak CQG(08)-gq/06 [quantum
gravity];
Lecian et al gq/07-in;
Aldrovandi & Pereira a0801-AFLB
[rev]; Schücking a0803 [Einstein's
theory is about torsion].
@ Connection formulation:
Montesinos JMP(99)
[and Ashtekar–Barbero connection].
@ Higher-order theories: Hammond JMP(89), JMP(90)
[second-order equations]; Troncoso & Zanelli CQG(00)ht/99;
Kruglov
a0710 [quantum];
Capozziello et al CQG(07)
[metric-affine].
@ Higher-dimensional theories: Mukhopadhyaya et al PRD(02)
[large extra dimensions], PRL(02)
[in Randall-Sundrum scenario].
> Specific types of theories:
see 2D gravity; 3D
gravity; action
for general relativity; einstein-cartan; teleparallel.
Phenomenology > s.a. bianchi
models; brans-dicke;
CPT; tests of
general relativity [precession]; wormholes.
* Particle motion: Notice
that, in a manifold with torsion, geodesics as extremal lines do not coincide
with autoparallels.
* Idea: The question
whether there is torsion in the physical world is
not settled; There is an issue of which notion of geodesics (extremal or autoparallel)
is the appropriate one for test particle geodesics.
* Bounds: The axial torsion K
1.5
× 10–15 m–1 [@ Lämmerzahl
PLA(97)].
@ Particle motion: Kleinert & Pelster GRG(99)gq/96;
Kleinert GRG(00)gq/98,
GRG(00)gq/98;
Shapiro ht/98-in,
PRP(02)ht/01 [rev];
Sivaram & Garcia de Andrade gq/01;
Aprea et al IJMPD(03)gq/04;
Arcos et al IJMPD(04)gq;
> s.a. higher-spin fields, spinning particles.
@ Other hep effects: Alimohammadi & Shariati MPLA(99),
Adak et al CQG(01)gq [
oscillations],
PRD(04)gq/03 [and
non-metricity]; Abel & Owen
NPB(03)
[CP violation, CKM matrix]; Khriplovich & Pomeransky PRD(06)ht/05 [spinning
particles, Immirzi parameter].
@ Gravitation: de Andrade et al gq/04-in
[coupling, and Dirac spinor]; Aros & Contreras PRD(06)gq [black
holes]; Chen a0705.
@ Cosmology: Capozziello et al gq/01-in,
Watanabe & Hayashi gq/04 [acceleration];
Wanas a0705,
IJMPA(07)-a0802 [torsion
energy]; > s.a. acceleration, frw
models.
@ Torsion waves: Hammond GRG(97); Babourova et al CQG(99)gq/98; King & Vassiliev
CQG(01)gq/00 [and
neutrinos].
@ Experimental evidence: Zhang et al GRG(92);
Lämmerzahl PLA(97)gq [Hughes-Drever
experiment]; Garcia de Andrade gq/01 [gravitational
radiation detectors]; Mao et al PRD(07)gq/06,
Flanagan & Rosenthal PRD(07)-a0704 [PPN-like
formalism, and
Gravity Probe B]; Pereira a0704-in
[possible interpretations]; Kostelecky et al PRL(08)-a0712
[bounds
from searches of
Lorentz violation with fermions]; Russell a0803-in [similarities with Lorentz
violation].
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Send feedback and suggestions to bombelli at olemiss.edu – Modified
22 jun 2008