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Generalization of the Lorentz Transformation
Nature, 1970ALWAY1 has proposed a transformation which should be a generalization of the well known Lorentz transformation in special relativity. The new transformation was derived without the usual supposition of space homogeneity. Here I discuss briefly some consequences of the proposed transformation, quoting experiments which support the Lorentz transformation.
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Degree of freedom in the Lorentz transformation
, 2013Lorentz pointed out in 1899 that a relativistic space-time transformation that leaves Maxwell’s equations invariant could only be defined to within a common factor on the basis of then-existing experimental data.
R. Buenker
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The Lorentz Transformation [PDF]
Nature, 1953 ON the basis of rather less restrictive postulates concerning the behaviour of light than are customary in special relativity theory, Capildeo has recently1 given the transformation equations connecting two frames of reference S and S′ (with suitably oriented axes) in uniform ...
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The Mathematical Gazette, 1925
The methods usually adopted for demonstrating the Lorentz Transformation are algebraic. Algebra is a powerful means of arriving at results, but does not in itself explain those results. In the present matter, the average reader is left with a sense of puzzledom, baffled by the paradoxes evolved by the algebra ; the results are demonstrated, but he is ...
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The methods usually adopted for demonstrating the Lorentz Transformation are algebraic. Algebra is a powerful means of arriving at results, but does not in itself explain those results. In the present matter, the average reader is left with a sense of puzzledom, baffled by the paradoxes evolved by the algebra ; the results are demonstrated, but he is ...
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Entanglement properties of a system of two spin-1 particles under a Lorentz transformation
, 2012We analize the entanglement change, under a Lorentz transformation, of a system consisting of two spin-one particles, considering different partitions of the Hilbert space, which has spin and momentum degrees of freedom.
Esteban Castro-Ruiz, E. Nahmad-Achar
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2020
We consider an observer in the reference system \(\Sigma '\) moving with respect to our reference system \(\Sigma _o\) with the velocity v.
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We consider an observer in the reference system \(\Sigma '\) moving with respect to our reference system \(\Sigma _o\) with the velocity v.
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1984
We started the last chapter by formally deriving the Galilean transformation in an attempt to try and identify any wrong assumptions in the argument. We came to the conclusion that the only part of the argument that we could throw away was that time was the same in all frames of reference.
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We started the last chapter by formally deriving the Galilean transformation in an attempt to try and identify any wrong assumptions in the argument. We came to the conclusion that the only part of the argument that we could throw away was that time was the same in all frames of reference.
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Generalized Lorentz transformation for an accelerated, rotating frame of reference
, 1987An exact, explicit coordinate transformation between an inertial frame of reference and a frame of reference having an arbitrary time‐dependent, nongravitational acceleration and an arbitrary time‐dependent angular velocity is given.
R. Nelson
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1993
We shall derive the Lorentz transformation by physical arguments. Let us pretend for a short while that we do not know about Minkowski space-time and Minkowski coordinates. Instead, we are aware of space and time and inertial frames of reference. An inertial observer, an idealized point observer subject to no forces, is assumed to follow a straight ...
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We shall derive the Lorentz transformation by physical arguments. Let us pretend for a short while that we do not know about Minkowski space-time and Minkowski coordinates. Instead, we are aware of space and time and inertial frames of reference. An inertial observer, an idealized point observer subject to no forces, is assumed to follow a straight ...
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Lorentz Transformation and the Thomas Precession
, 1955The various kinematic effects of special relativity are here treated by considering iterations of the infinitesimal Lorentz transformation. There is only one relativistic effect that appears as a difference between an infinitesimal Lorentz transformation
W. H. Furry
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