2009
DOI: 10.1093/bjps/axp015
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Time Reversal in Classical Electromagnetism

Abstract: Richard Feynman has claimed that anti-particles are nothing but particles 'propagating backwards in time'; that time reversing a particle state always turns it into the corresponding anti-particle state.

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Cited by 60 publications
(33 citation statements)
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“…' Greaves ([2010], p. 28) also poses the question 'How can there be such an intimate relationship between spatiotemporal symmetries (Lorentz invariance, parity reversal, time reversal) on the one hand, and charge conjugation, not obviously a spatiotemporal notion at all, on the other?' This is echoed in (Arntzenius [2011], p. 634), and (Arntzensius and Greaves [2009], p. 584). 24…”
Section: Greenberg On Relativity and Cpt Invariancementioning
confidence: 89%
See 1 more Smart Citation
“…' Greaves ([2010], p. 28) also poses the question 'How can there be such an intimate relationship between spatiotemporal symmetries (Lorentz invariance, parity reversal, time reversal) on the one hand, and charge conjugation, not obviously a spatiotemporal notion at all, on the other?' This is echoed in (Arntzenius [2011], p. 634), and (Arntzensius and Greaves [2009], p. 584). 24…”
Section: Greenberg On Relativity and Cpt Invariancementioning
confidence: 89%
“…It has been influential in both the physics and philosophy of physics literature, since it suggests a test for violations of Lorentz invariance via experiments that measure CPT violation (Kostelecky [2011]; Hagar [2009], p. 261). Moreover, in apparently linking Lorentz invariance with CPT invariance, it suggests the latter is somehow mysterious; in particular, some philosophers have wondered how the charge conjugation transformation C can arise from a purely spatiotemporal symmetry (Arntzenius [2011]; Greaves [2010]; Arntzenius and Greaves [2009]).…”
Section: Introductionmentioning
confidence: 99%
“…In mathematical terms, if ℎ is the unique history with ℎ( ) = , then the unique history ℎ ′ with ℎ ′ ( + Δ ) = is given by ℎ ′ ( + Δ ) = ℎ( ). Time reversal symmetry is a little harder to define (see Albert (2000, ch.1) for a careful but very accessible discussion; see also discussion by Arntzenius and Greaves (2009), Malament (2004), and Earman (2002) but roughly speaking, it requires that the dynamical system has qualitatively the same structure in the past as in the future. Normally this is imposed by stipulating some appropriate time reversal map of state space to itself, so that if ℎ is the history through some state , the history ℎ ′ through is given by ℎ ′ ( ) = ℎ(− ).…”
Section: Classical Mechanicsmentioning
confidence: 99%
“…1), Earman (2002, Malament (2004) and Arntzenius and Greaves (2009) for an illuminating recent discussion of the time reversal operation only in the context of classical electromagnetic theory.…”
Section: The Relevance Of Time Reversal Invariancementioning
confidence: 99%