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A f77 program can be obtained from the authors upon request
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A f77 program can be obtained from the authors upon request.
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54
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85037188076
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Recall that for a monochromatic field (Formula presented) we have (Formula presented) and (Formula presented). For bichromatic fields this condition holds for odd n, but not for even n. The different periodicity is already observed for (Formula presented) two orders of magnitude smaller than (Formula presented) This is not explained by the classical model, which does not hold when one of the two fields is too weak
-
Recall that for a monochromatic field (Formula presented) we have (Formula presented) and (Formula presented). For bichromatic fields this condition holds for odd n, but not for even n. The different periodicity is already observed for (Formula presented) two orders of magnitude smaller than (Formula presented) This is not explained by the classical model, which does not hold when one of the two fields is too weak.
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0003048242
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85037189890
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The emission rate for an electronic wave packet in the tunneling regime (Formula presented) is proportional to (Formula presented)
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The emission rate for an electronic wave packet in the tunneling regime (Formula presented) is proportional to (Formula presented) 29, where the constant C depends on the potential barrier in question. This appears to hold in our case already for (Formula presented).
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