In General > s.a. equivalence
principle; newtonian gravity.
* Idea: The concept of mass is related to two different physical phenomena,
inertia and gravitation.
* Inertial mass: Defined
by Newton's second law, F = mi a.
* Gravitational mass:
The active and passive gravitational masses are defined by
Fgrav = mp g , g(x) = –G (ma/ r2) (r/r) (for each point source) .
* Relationships: In Newtonian mechanics, the two gravitational ones are proportional as a consequence of the third law, ma = mp = mg – an inequality would imply a violation of momentum conservation; The principle of equivalence states the proportionality of mi and mg (specifically, mp).
The "Origin'' of Mass > s.a. Higgs
Mechanism; mach's
principle; quantum particles.
* Electromagnetic mass:
The quantity me = 4U/3c2 appearing
in
the
Abraham-Lorentz equation (> see radiation); For
an
accelerated charged particle,
the measured mass would be m = m0 + me;
Note that, unless one
uses
a cutoff, for a point particle me =
,
so one needs to renormalize
it.
* Mass generation in quantum
field theory:
For gauge fields the known mechanisms are the
Higgs
mechanism and, in 3D, adding Proca/Pauli-Fierz or Chern-Simons terms.
@ Inertial origin: Haisch et al ThSc(94)nov;
Rueda & Haisch FP(98)phy,
PLA(98)phy;
Haisch
et al AdP(01)gq/00;
Rueda
& Haisch AdP(05)gq [passive mg];
Milgrom PRD(06)gq [in
acoustic
spacetime]; > s.a.
inertia [fluctuations], vacuum.
@ Mass generation in quantum
field theory: Drechsler & Tann FP(99)
[broken Weyl symmetry];
Deser & Tekin CQG(02)ht,
[in 2+1 dimensions]; Jaramillo & Aldaya MPLA(02)ht [diff-invariant
theories]; Dvali et al PRL(06)ht/05 [topological,
4D]; Wilczek MPLA(06);
Sevostyanov ht/06, ht/06 [gauge
theory];
Nesbet a0711 [fermions,
from self-interaction]; Sevostyanov IJMPA(08) [comparing mechanisms].
@ Electromagnetic: in Rohrlich 65 [renormalization]; Haeffner phy/00 [??];
Ray Apeiron(07)phy/04 [Lorentz's
conjecture]; Wanas IJGMP(07)gq;
Bhadra a0710-PhD
[overview]; > s.a. inertia.
In Special Relativity and Quantum Theory > s.a. [special
relativity]; particles [unstable, mass
uncertainty].
* Predictions: Mass-energy, m =
m0, E = mc2.
* Remark: Misleading
to say that m converts to E (could
I substitute
"inertia" for
"mass" here? mass is energy).
@ Mass and E = mc2:
Poincaré
AN(1900)
[precursor]; Einstein AdP(05), BAMS(35),
reprinted BAMS(00)
[elementary]; Feigenbaum & Mermin AJP(88)jan;
Okun PT(89)jun;
Sandin AJP(91)nov;
Kim qp/00-in;
Bodanis 00; Luetzelschwab AJP(03)sep
[apparatus to measure]; Thomas EJP(05);
Rainville et al Nat(05)dec
+ sr(05)dec
+ pn(06)jan
[direct
measurements]; Baierlein AJP(07)apr;
Pandya a0705 [history
and response to criticism]; Okun PU(08)-a0808,
AJP(09)may;
Hecht AJP(09)sep [Einstein on mass and energy].
@ Derivations: Rohrlich
AJP(90)apr [simple];
Gould ap/05/ApJ
[without special relativity]; Ohanian SHPMP(09)-a0805 [Einstein's
attempts].
@ Other topics: Horwitz & Belenkiy FP(02)
[Schopenhauer & Hegel]; Cushman
& van der Kallen DG&A(06)mp/05 [group
theoretic interpretation]; Zenczykowski qp/05 [for
quarks]; Benghi Pinto EJP(07)
[bare vs effective].
And Gravitation > s.a. equivalence
principle; gravitational energy; test-particle
motion.
* Newtonian theory: The
total (gravitational, active) mass inside a
surface S can be defined, using the gravitational potential
,
by
M =
S
, j dS j
.
* General relativity:
Several definitions have been given, some of
which are equivalent in general relativity but not in
other theories.
* Kaluza-Klein: In the
4D reduction of the theory, the effective mass of a
particle can vary along its worldline.
@ References: Rosen & Cooperstock CQG(92);
Toussaint GRG(00)gq/99 [m as
translation charge]; Petkov gq/01 [distance
dependence of ma?]; Ehlers et al PRD(05)
[and pressure]; Widom gq/06 [inertial
and gravitational]; Bel & Martin-Martin a0906 [proper
mass]; > s.a. black holes; cosmological
constant [minimum mass].
Negative mass > s.a. bimetric
theory; schwarzschild
spacetime.
* Properties: While a
positive gravitational mass attracts everything, a negative one repels everything;
A positive and a negative mass
will
chase each other (conserving momentum); To avoid runaway motion, negative
mass
systems can not coexist with positive mass ones, and will have negative
temperatures.
@ References: NS(90)mar17, p54-56; Price AJP(93)mar;
Pollard & Dunning-Davies NCB(95); Cavalleri & Tonni
NCB(97) [self-acceleration].
References > s.a. Center
of Mass; particle types; photon; renormalization; stars.
@ I: Nambu ThSc(92)may
[symmetry breaking].
@ General: Jammer 61; Pietschmann pr(86);
Okun PT(89)jun;
Jammer 00; Roche EJP(05);
Okun 09; > s.a. physical theories.
@ Measurement: Poncharal et al Sci(99)mar
+ pn(00)mar
[10–12 g,
nanotubes]; Ilic et al JAP(04)
+ pw(04)feb
+ pn(04)feb
[10–18 g,
nanoelectromechanical device]; news pn(05)apr [zeptogram
(10–21 g)
sensitivity]; news pw(07)feb
[nanocantilevers].
@ In field theory: Faraoni & Cooperstock EJP(98)phy; Frasca
a0807 [massive
solutions of massless theories]; > s.a. Yang-Mills
gauge theories.
@ In quantum mechanics: Jaekel & Reynaud EPL(97)qp/96 [as
observable]; Bohm & Harshman NPB(00)hp [resonances,
and Gamow vectors].
@ And geometry: Tolksdorf mp/02, mp/02 [mass as curvature].
@ Related topics: Donoghue & Holstein EJP(87)
[T dependence?];
Mannheim GRG(93)
[dynamical]; Wesson MPLA(04)
[quantized?]; McCulloch a0712 [cosmology
and variations of inertial mass]; >
s.a. inertia.
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nov 2009