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1
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16244372190
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Di Ventra, M, Evoy, S, Heflin, J. R, Eds, Kluwer Academics: Boston
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Introduction to Nanoscale Science and Technology, Di Ventra, M., Evoy, S., Heflin, J. R., Eds.: Kluwer Academics: Boston, 2004.
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(2004)
Introduction to Nanoscale Science and Technology
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4
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33846366237
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Chen, Y.-C.; Zwolak, M.; Di Ventra, M. Nano Lett. 2003, 3, 1961.
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Nano Lett
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Chen, Y.-C.1
Zwolak, M.2
Di Ventra, M.3
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5
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4644363101
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Chen, Y.-C.; Zwolak, M.; Di Ventra, M. Nano Lett. 2004, 4, 1709.
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(2004)
Nano Lett
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Chen, Y.-C.1
Zwolak, M.2
Di Ventra, M.3
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6
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18244388957
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Chen, Y.-C.; Zwolak, M.; Di Ventra, M. Nano Lett. 2005, 5, 621.
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Nano Lett
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Chen, Y.-C.1
Zwolak, M.2
Di Ventra, M.3
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7
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33745748485
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Huang, Z. F.; Xu, B. Q.; Chen, Y.-C.; Di Ventra, M.; Tao, N. J. Nano Lett. 2006, 6, 1240.
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Nano Lett
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Huang, Z.F.1
Xu, B.Q.2
Chen, Y.-C.3
Di Ventra, M.4
Tao, N.J.5
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9
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33846363488
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The linear relation between thermal conductivity and specific heat in metallic quantum point contacts has been verified experimentally in: Molekamp, L. W, Gravier, T, van Houten, H, Buijk, O. J. A, Mabesoone, M. A. A. Phys. Rev. Lett. 1992, 68, 3765
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The linear relation between thermal conductivity and specific heat in metallic quantum point contacts has been verified experimentally in: Molekamp, L. W.; Gravier, T.; van Houten, H.; Buijk, O. J. A.: Mabesoone, M. A. A. Phys. Rev. Lett. 1992, 68, 3765.
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10
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0026839505
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van Houten, H.; Molenkamp, L. W.; Beenakker, C. W. J.; Foxon, C. T. Semicond. Sci. Technol. 1992, 7, B215.
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Semicond. Sci. Technol
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van Houten, H.1
Molenkamp, L.W.2
Beenakker, C.W.J.3
Foxon, C.T.4
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11
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0004088231
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Springer-Verlag: New York
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Holm, R. Electric Contacts; Springer-Verlag: New York, 1967.
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Electric Contacts
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Holm, R.1
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15
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4143086686
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Vignale, G.; Ullrich, C. A.; Conti, S. Phys. Rev. Lett. 1997, 79, 4878.
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Phys. Rev. Lett
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Vignale, G.1
Ullrich, C.A.2
Conti, S.3
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17
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33846355952
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Equation 5 can also be derived from first principles for the electron liquid applying a similar approach that was used to derive the quantum Navier-Stokes equations 3 see ref 11
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Equation 5 can also be derived from first principles for the electron liquid applying a similar approach that was used to derive the quantum Navier-Stokes equations 3 (see ref 11).
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18
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27144496078
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Sai, N.; Zwolak, M.; Vignale, G.: Di Ventra, M. Phys. Rev. Lett. 2005, 94, 186810.
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Phys. Rev. Lett
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Sai, N.1
Zwolak, M.2
Vignale, G.3
Di Ventra, M.4
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19
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33846383306
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In eq 8 we are assuming that the temperature variations are small so that the density fluctuations due to temperature can be neglected
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In eq 8 we are assuming that the temperature variations are small so that the density fluctuations due to temperature can be neglected.
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20
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33846353452
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We assume that the system is in local thermal equilibrium; thus local thermodynamic quantities such as energy and entropy densities can be defined
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We assume that the system is in local thermal equilibrium; thus local thermodynamic quantities such as energy and entropy densities can be defined.
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21
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33846361310
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It is well-known that for a translationally invariant electron, liquid η(ω=0) diverges for small temperatures as 1/Te2, See: Abrikosov, A. A, Khalatnikov, I. M. Rep. Prog. Phys. 1959, 22, 330, The presence of the nanojunction breaks translational invariance thus putting an effective cut-off to this divergence. We can see this as follows. In an ideal electron liquid the divergence of η can be understood by bearing in mind that η is related via a Kramers-Kronig relation to the value of the shear modulus μ∞. We thus have μ∞, f dωη(ω)/π ∝ η(ω=0)/τ where τ is the quasi-particle lifetime, which in an ideal electron liquid diverges as 1/Te2 However, the constriction introduces another lifetime τc due to the elastic scattering with the junction 8 which cuts-off the divergence of η(ω=0) via the relation
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c.
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23
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30644470693
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Bushong, N.; Sai, N.; Di Ventra, M. Nano Lett. 2005, 5, 2569).
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(2005)
Nano Lett
, vol.5
, pp. 2569
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Bushong, N.1
Sai, N.2
Di Ventra, M.3
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25
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33846381583
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θ(x) - 1 if x > 0, θ(0) = 1/2, and 0 otherwise.
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θ(x) - 1 if x > 0, θ(0) = 1/2, and 0 otherwise.
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26
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33846380868
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In this hydrodynamic picture, the Fermi velocity does not contribute to the fluid velocity, the former being an incoherent part of the electron motion.
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In this hydrodynamic picture, the Fermi velocity does not contribute to the fluid velocity, the former being an "incoherent" part of the electron motion.
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27
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33846336024
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2(x) given in eq 11.
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2(x) given in eq 11.
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28
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0017472840
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Tinkham, M.; Octavio, M.; Skocpol, W. J. J. Appl. Phys. 1977, 48, 1311.
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J. Appl. Phys
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Tinkham, M.1
Octavio, M.2
Skocpol, W.J.3
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