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The bare substrate used in this work is a sample of exfoliated graphite with a total surface area of 182 m2. 4He has a higher binding energy to the graphite surface than does 3He, arising from its smaller zero-point energy. This preferential adsorption is exploited to preplate the surface. The 4He coverage required for precisely two atomic layers is 21.2 nm-2, as shown by previous work 39
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22
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34548766251
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See supporting material on Science Online.
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See supporting material on Science Online.
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34548743106
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2).
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2).
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24
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34548808285
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-2, when the uniform solid first forms.
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25
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34548803210
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3He monolayer adsorbed on bare graphite.
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3He monolayer adsorbed on bare graphite.
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26
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34548749468
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For a strongly correlated 2D 3He fluid monolayer, previous work (12) has shown that the crossover from Curie-law susceptibility at high temperatures to a Pauli susceptibility in the degenerate regime is well described by χ, C/(T2, T F**2)1/2, with Curie constant C, and an effective degeneracy temperature TF**, TF0(1, F0 a, m*/m, where TF0, 0.505n (K nm2) is the Fermi temperature of the corresponding ideal Fermi gas and F0a is a Fermi liquid Landau parameter. However, in the 3He bilayer system we find that the onset of spin degeneracy is governed by T0 rather than TF**. For example, at 9.0 nm-2, TF**
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0 = 12 mK.
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35
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0035950147
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39
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34548807241
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F. Ziouzia, thesis, Royal Holloway, University of London (2004).
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F. Ziouzia, thesis, Royal Holloway, University of London (2004).
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40
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34548783484
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We thank P. Coleman, D. Edwards, M. Grosche, A. Hewson, C. Pépin, and A. J. Schofield for discussions. Supported by the UK Engineering and Physical Sciences Research Council grant GR/S20567/01
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We thank P. Coleman, D. Edwards, M. Grosche, A. Hewson, C. Pépin, and A. J. Schofield for discussions. Supported by the UK Engineering and Physical Sciences Research Council grant GR/S20567/01.
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