1991
DOI: 10.1007/bf01548563
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The nonlinear effects of quantum electrodynamics at high energies

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Cited by 1 publication
(2 citation statements)
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“…If the stimulating beam is diraction and Fourier limited, and if its optics and pulse length are adapted to the two other colliding beams, F is simply equal to the number of photons in the stimulating beam. For m a = 1eV, g = 1 0 10 GeV -1 , F = 1 0 16 , w e get = 1 0 9 s. Clearly the axion does not decay inside the detector.…”
Section: Upper Limits On the Coupling Constantmentioning
confidence: 92%
See 1 more Smart Citation
“…If the stimulating beam is diraction and Fourier limited, and if its optics and pulse length are adapted to the two other colliding beams, F is simply equal to the number of photons in the stimulating beam. For m a = 1eV, g = 1 0 10 GeV -1 , F = 1 0 16 , w e get = 1 0 9 s. Clearly the axion does not decay inside the detector.…”
Section: Upper Limits On the Coupling Constantmentioning
confidence: 92%
“…Therefore the contribution of the axion never dominates (g. 4). The soft dependance of the axion cross section and of the QED cross section [16] on polarisation and on angle does not provide any help. …”
Section: C2 High Energy Limitmentioning
confidence: 99%