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bT]. The same electric deflection profiles were obtained. For the same reason, diabatic passages (occurring at crossings with very small gaps) are not expected to change the calculated profiles of deflection.
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30
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26844444841
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note
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ψ dθ dφ dψ where δ is the δ-Dirac function. With a change of variables in the integration, it is easy to see that the profile g(x) is the same under the transformation F* = αF, T* = αT (where K∇F is constant).
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