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The inverse field width of each window is about 3.6 times larger than the inverse field spacing between the centres of consecutive windows.
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The inverse field width of each window is about 3.6 times larger than the inverse field spacing between the centres of consecutive windows.
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27
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One could also invoke quantum interference oscillations as a source of splitting of dHvA peaks. However, as shown in Ref., these are by nature insensitive to temperature. We can show with high-temperature data (not shown in the paper) that no oscillations remain above 800 mK over the whole field range from 18 to 2 T.
-
One could also invoke quantum interference oscillations as a source of splitting of dHvA peaks. However, as shown in Ref., these are by nature insensitive to temperature. We can show with high-temperature data (not shown in the paper) that no oscillations remain above 800 mK over the whole field range from 18 to 2 T.
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77956320824
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note
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- 1 (300 / 234) = 52 °], an angle covered by our data. The α 1 orbit, if closed near the top of the zone, would show a downturn of the frequency at an angle below 52 °. Oscillations were searched at higher angles than those shown in this paper but none were detected.
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77956318742
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note
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At first sight it may seem that the combination of specific heat and dHvA is incompatible with previous transport data that show a factor of 7 rise in the strength of T 2 scattering at low T as the critical point is approached (Ref.). At zero field and without impurity scattering, the temperature-dependent resistivity contribution from the γ 2 pocket, which comprises a maximum of only one fifth of the Fermi surface, would be shorted out by the other pockets. However, at finite field as well as in the limit of residual scattering dominating the resistivity, a realistic calculation based on the multiband Fermi surface of Sr 3 Ru 2 O 7 shows that the transport could, in principle, be accounted for by a factor of 10 increase in the γ 2 mass.
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33
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77956318537
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(private communication).
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R. A. Borzi (private communication).
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Borzi, R.A.1
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