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Volumn 79, Issue 17, 2009, Pages

Dynamical sticking of a solid H4 e film with superfluid overlayer

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EID: 67449103174     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.172503     Document Type: Article
Times cited : (17)

References (28)
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    • The temperature dependence at high temperatures is slightly different between Figs. 2 3, which is caused by thermal cycling of the sample.
    • The temperature dependence at high temperatures is slightly different between Figs. 2 3, which is caused by thermal cycling of the sample.
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    • Experimental data of P are not available but can be estimated on the basis that P is on the order of the adsorption pressure.
    • Experimental data of P are not available but can be estimated on the basis that P is on the order of the adsorption pressure.
  • 21
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    • In the present experiments, we found 1-χ=0.04.
    • In the present experiments, we found 1-χ=0.04.
  • 27
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    • The kinetic energy of the whole system consists of that of 2ALS and of the superfluid overlayer as K= n m 2 n2 + 1 2 m ρs dx vs2. By substituting Eq. 3 into the second term, we obtain K= m 2λ (λ 2π) 2 0□ dx I 2 + m 2 ρs (λ 2πd) 2 0□ dx I 2. Thus, the effective mass of I becomes 1+λ/ (d2 ρs) times larger due to the presence of the superfluid overlayer.
    • The kinetic energy of the whole system consists of that of 2ALS and of the superfluid overlayer as K= n m 2 n2 + 1 2 m ρs dx vs2. By substituting Eq. 3 into the second term, we obtain K= m 2λ (λ 2π) 2 0□ dx I 2 + m 2 ρs (λ 2πd) 2 0□ dx I 2. Thus, the effective mass of I becomes 1+λ/ (d2 ρs) times larger due to the presence of the superfluid overlayer.


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