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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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Improper Lorentz Transformations
Physical Review, 1958The irreducible representations of the extended Lorentz group, including the space- and time-like reflections, are discussed. It is shown that there exist certain representations (up to the sign) which can be used to describe a particle with two states of opposite parity.
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On entanglement and Lorentz transformations.
Quantum Inf. Comput., 2002We study the transformation of maximally entangled states under the action of Lorentz transformations in a fully relativistic setting. By explicit calculation of the Wigner rotation, we describe the relativistic analog of the Bell states as viewed from two inertial frames moving with constant velocity with respect to each other.
Alsing, P. M., Milburn, G. J.
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American Journal of Physics, 1968
A simple-straightforward derivation of the most general form of the homogeneous Lorentz transformation is presented. In the process, the well-known decomposition of a generic element of the group into two pure rotations and a “one-dimensional” Lorentz transformation is obtained in a physically obvious manner.
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A simple-straightforward derivation of the most general form of the homogeneous Lorentz transformation is presented. In the process, the well-known decomposition of a generic element of the group into two pure rotations and a “one-dimensional” Lorentz transformation is obtained in a physically obvious manner.
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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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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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2022
Erwin-Schrödinger-Archiv / Signatur B33-547 Autor*in: Sandgathe, Dr. Empfänger*in: Schrödinger, Erwin Ort: Düsseldorf Datum / Laufzeit: 1956-12-03 Sprache: deutsch Umfang: 2 Blatt, 2 Seiten, 15,3 x 21 cm Original Brief, Typoskript, mit Unterschrift Normdaten (Gemeinsame Normdatei) Brief https://d-nb.info/gnd/4008240-4 Düsseldorf https://d-nb.info/gnd ...
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Erwin-Schrödinger-Archiv / Signatur B33-547 Autor*in: Sandgathe, Dr. Empfänger*in: Schrödinger, Erwin Ort: Düsseldorf Datum / Laufzeit: 1956-12-03 Sprache: deutsch Umfang: 2 Blatt, 2 Seiten, 15,3 x 21 cm Original Brief, Typoskript, mit Unterschrift Normdaten (Gemeinsame Normdatei) Brief https://d-nb.info/gnd/4008240-4 Düsseldorf https://d-nb.info/gnd ...
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On the linearity of the Lorentz transformation
1936The present paper is an attempt to establish the linearity of the transformation from simple arguments ...
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1998
Abstract Constantia enters your room. “What’s all the commotion?” You whisper to Mr. Veil, “Breathe none of this to her.” You turn to Constantia. “Ready for the next lesson?” Around Constantia’s neck is a pearl necklace giving her the vague appearance of a young Jacqueline Kennedy. Her shirt is covered with musical notes.
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Abstract Constantia enters your room. “What’s all the commotion?” You whisper to Mr. Veil, “Breathe none of this to her.” You turn to Constantia. “Ready for the next lesson?” Around Constantia’s neck is a pearl necklace giving her the vague appearance of a young Jacqueline Kennedy. Her shirt is covered with musical notes.
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