Find link

language:

jump to random article

Find link is a tool written by Edward Betts.

Longer titles found: History of Lorentz transformations (view), Derivations of the Lorentz transformations (view)

searching for Lorentz transformation 30 found (296 total)

alternate case: lorentz transformation

Fock–Lorentz symmetry (441 words) [view diff] exact match in snippet view article find links to article

new invariance, known as Fock–Lorentz symmetry or the projective Lorentz transformation. The general study of such theories began with Fock, who was motivated
Spacetime wave packets (299 words) [view diff] exact match in snippet view article find links to article
beam is shown to be transformed into spacetime wave packets under Lorentz transformation, thus any monochromatic Gaussian beam observed in a reference frame
Four-force (1,190 words) [view diff] exact match in snippet view article find links to article
expression of force. In special relativity the transformation will be a Lorentz transformation between coordinate systems moving with a relative constant velocity
Invariant decomposition (2,082 words) [view diff] exact match in snippet view article find links to article
algebra SO ( 3 , 1 ) {\textstyle {\text{SO}}(3,1)} , where any Lorentz transformation can be decomposed into a commuting rotation and boost. Any bivector
Enrique Loedel Palumbo (919 words) [view diff] case mismatch in snippet view article find links to article
theoretician." Amar, Henri (1955). "New Geometric Representation of the Lorentz Transformation". American Journal of Physics. 23 (8): 487–489. Bibcode:1955AmJPh
Doubly special relativity (1,766 words) [view diff] exact match in snippet view article find links to article
motivation has been criticized, on the grounds that the result of a Lorentz transformation does not itself constitute an observable phenomenon. DSR also suffers
James Clerk Maxwell Foundation (1,831 words) [view diff] exact match in snippet view article find links to article
Einstein showed that Maxwell's equations were invariant under a Lorentz transformation (as opposed to a Galilean transformation) and, inter alia, used
Dirac algebra (2,342 words) [view diff] exact match in snippet view article find links to article
} This corresponds to an infinitesimal Lorentz transformation on a spinor. Then a finite Lorentz transformation, parametrized by the components ω μ ν {\displaystyle
Paradox of radiation of charged particles in a gravitational field (2,255 words) [view diff] exact match in snippet view article find links to article
the frame of the supported observer. This manipulation is not a Lorentz transformation, because the two frames have a relative acceleration. Instead, the
Relativistic mechanics (5,028 words) [view diff] exact match in snippet view article find links to article
which its proper time is measured. This quantity is invariant under Lorentz transformation, so to check to see what an observer in a different reference frame
Electric charge (4,970 words) [view diff] case mismatch in snippet view article find links to article
Retrieved 11 April 2018. "How can we prove charge invariance under Lorentz Transformation?". physics.stackexchange.com. Retrieved 2018-03-27. Singal, A.K
Faraday's law of induction (4,699 words) [view diff] exact match in snippet view article find links to article
the circuit in the comoving reference frame K’ as a result of the Lorentz transformation of the magnetic field B {\displaystyle \mathbf {B} } , present in
Raising and lowering indices (3,706 words) [view diff] exact match in snippet view article find links to article
{\displaystyle \delta ^{\mu }{}_{\nu }} , which is the identity map, or a Lorentz transformation Λ μ ν . {\displaystyle \Lambda ^{\mu }{}_{\nu }.} For a (0,2) tensor
Pauli–Lubanski pseudovector (2,044 words) [view diff] exact match in snippet view article find links to article
acted on by 5×5 matrices with the upper left 4×4 block an ordinary Lorentz transformation, the last column reserved for translations and the action effected
De Sitter invariant special relativity (3,598 words) [view diff] exact match in snippet view article find links to article
(2001). "An extension of the concept of inertial frame and of Lorentz transformation". Proc. Natl. Acad. Sci. USA. 73 (5): 1418–21. Bibcode:1976PNAS
Aubrey William Ingleton (762 words) [view diff] exact match in snippet view article find links to article
fields’. Proc. Cambridge Philos. Soc. 48 (1) (1952) 41–45. ‘The Lorentz transformation’. Nature 171 (1953) 618. ‘The rank f circulant matrices’. J. London
Dirac equation in curved spacetime (2,309 words) [view diff] exact match in snippet view article find links to article
forming this representation at the group level. We can write a finite Lorentz transformation on R 1 , 3 {\displaystyle \mathbb {R} ^{1,3}} as Λ σ ρ = exp ⁡ (
Intrabeam scattering (1,542 words) [view diff] exact match in snippet view article find links to article
_{y'}} which the factor of γ {\displaystyle \gamma } coming from the Lorentz transformation. From this equation, we see that due to the factor of γ {\displaystyle
Bivector (complex) (926 words) [view diff] case mismatch in snippet view article
Shaw, Ronald; Bowtell, Graham (1969). "The Bivector Logarithm of a Lorentz Transformation". Quarterly Journal of Mathematics. 20 (1): 497–503. doi:10.1093/qmath/20
Trouton–Noble experiment (3,771 words) [view diff] exact match in snippet view article find links to article
molecular forces. However, there is no known mechanism for how a Lorentz transformation could produce such molecular forces. In addition, if two point charges
Conformal field theory (6,808 words) [view diff] exact match in snippet view article find links to article
R_{\nu }^{\mu }(x)} is a rotation (i.e. an orthogonal matrix) or Lorentz transformation. The conformal group is locally isomorphic to S O ( 1 , d + 1 )
Frame fields in general relativity (4,996 words) [view diff] exact match in snippet view article find links to article
{\partial x'^{\mu }}{\partial x^{\nu }}}T^{\nu a}} whilst under a local Lorentz transformation we have: T ′ μ a = Λ ( x )   b a T μ b . {\displaystyle T'^{\mu
Clifford algebra (9,161 words) [view diff] exact match in snippet view article find links to article
transformation that takes the bilinear form to the canonical form is not a Lorentz transformation of the underlying spacetime. The Clifford algebra of spacetime used
Wave function (13,534 words) [view diff] exact match in snippet view article find links to article
requirement of Lorentz invariance. Their solutions must transform under Lorentz transformation in a prescribed way, i.e. under a particular representation of the
Lie sphere geometry (3,959 words) [view diff] exact match in snippet view article find links to article
between the Möbius group and the Lorentz group (see Möbius group#Lorentz transformation). The Lie quadric of the plane is defined as follows. Let R3,2 denote
Conformal geometric algebra (3,304 words) [view diff] exact match in snippet view article find links to article
null-cone, which directions are hyperbolically orthogonal? (cf Lorentz transformation pix) in 2+1 D, if S is (1,a,b), (using co-ords e-, {e+, ei}), the
List of topics characterized as pseudoscience (38,829 words) [view diff] exact match in snippet view article find links to article
physics theory proposed in the 1940s that claims the equations of the Lorentz transformation are incorrectly formulated to describe relativistic effects, which
Four-gradient (8,619 words) [view diff] exact match in snippet view article find links to article
{\displaystyle \delta _{\mu }^{\nu }} is the 4D Kronecker delta. The Lorentz transformation is written in tensor form as: 69  X μ ′ = Λ ν   μ ′ X ν {\displaystyle
Lie algebra extension (17,636 words) [view diff] exact match in snippet view article find links to article
Poincaré group, (0, Λ)(a, I)(0, Λ−1) = (Λ a, I) ∈ T ⊂ P. Thus every Lorentz transformation Λ corresponds to an automorphism ΦΛ of T with inverse ΦΛ−1 and Φ
Light-front computational methods (11,024 words) [view diff] exact match in snippet view article find links to article
for extending the cutoff as required when one wishes to make the Lorentz transformation that yields momenta which exceed the cutoff. Both concepts of the