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e.g., D. Shoenberg in: Magnetic Oscillations in Metals, Cambridge University Press, Cambridge, 1984.
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39749136104
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We ignore the dependence of energy on wave-vector parallel to the applied field, equivalent to working in a two-dimensional electron system. This saves a considerable amount of complexity, but still leads to the central result, Eq. (7).
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We ignore the dependence of energy on wave-vector parallel to the applied field, equivalent to working in a two-dimensional electron system. This saves a considerable amount of complexity, but still leads to the central result, Eq. (7).
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8
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39749174322
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c is really just a short-hand for this quantisation. So provided that the k-dependence of the self-energy can be ignored this is valid.
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c is really just a short-hand for this quantisation. So provided that the k-dependence of the self-energy can be ignored this is valid.
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9
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39749140261
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k and the dHvA frequency F.
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k and the dHvA frequency F.
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12
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42749107913
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0035494406
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39749176198
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In reality the Dingle factor and other pre-factors (see e.g. Ref. [3]) enter the amplitude, so absolute amplitudes cannot be directly compared on different orbits-the point is that strong non-Fermi-liquid behaviour can suppress oscillations to below the measurement threshold.
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In reality the Dingle factor and other pre-factors (see e.g. Ref. [3]) enter the amplitude, so absolute amplitudes cannot be directly compared on different orbits-the point is that strong non-Fermi-liquid behaviour can suppress oscillations to below the measurement threshold.
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