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Volumn 7, Issue 6, 2007, Pages 1789-1792

Electron turbulence at nanoscale junctions

Author keywords

[No Author keywords available]

Indexed keywords

ELECTRON LIQUIDS; NANOSCALE JUNCTIONS; NANOSCALE SYSTEMS; NONLINEAR DYNAMICAL EFFECTS;

EID: 34547352658     PISSN: 15306984     EISSN: None     Source Type: Journal    
DOI: 10.1021/nl070935e     Document Type: Article
Times cited : (17)

References (41)
  • 16
    • 0004185784 scopus 로고
    • Cambridge University Press: Cambridge
    • Frisch, U. Turbulence; Cambridge University Press: Cambridge, 1995.
    • (1995) Turbulence
    • Frisch, U.1
  • 37
    • 84858085037 scopus 로고    scopus 로고
    • Each electrode is 51.8 Å wide in the x direction, and 22.4 Å long in the z direction of current flow (see Figure I). The width of the rectangular bridge is 2.8 Å, and the gap between the electrodes is 9.8 Å.
    • Each electrode is 51.8 Å wide in the x direction, and 22.4 Å long in the z direction of current flow (see Figure I). The width of the rectangular bridge is 2.8 Å, and the gap between the electrodes is 9.8 Å.
  • 38
    • 34547249705 scopus 로고    scopus 로고
    • We have used the adiabatic local density approximation to the scalar exchange-correlation potential,29-31 as derived by Ceperley and Alder32 and parametrized by Perdew and Zunger.33
    • 33
  • 39
    • 84858085038 scopus 로고    scopus 로고
    • The grid spacing of the jellium system is 0.7 Å, and the timestep used to propagate the system is 2.5 × 10-3 fs. We used the Chebyshev method34 for constructing the time-evolution operator
    • 34 for constructing the time-evolution operator.
  • 40
    • 34547255885 scopus 로고    scopus 로고
    • For the simulation of the Navier-Stokes equations, we use Dirchlet boundary conditions for the velocity at the inlet, and Neumann boundary conditions at the outlet
    • For the simulation of the Navier-Stokes equations, we use Dirchlet boundary conditions for the velocity at the inlet, and Neumann boundary conditions at the outlet.
  • 41
    • 34547301120 scopus 로고    scopus 로고
    • The issue of compressibility is also related to the treatment of the fluid at the boundaries of the confining structure. In general, wavefunctions tend to exhibit exponentially decreasing density at the edges of a confining potential, while incompressible classical fluids are described with hard walls and no-slip boundary conditions. The assumption in the Naiver-Stokes equations that the electron liquid is incompressible also neglects the formation of surface charges; for a discussion of dynamical charging effects near nanoscopic junctions, see ref 20
    • The issue of compressibility is also related to the treatment of the fluid at the boundaries of the confining structure. In general, wavefunctions tend to exhibit exponentially decreasing density at the edges of a confining potential, while incompressible classical fluids are described with hard walls and "no-slip" boundary conditions. The assumption in the Naiver-Stokes equations that the electron liquid is incompressible also neglects the formation of surface charges; for a discussion of dynamical charging effects near nanoscopic junctions, see ref 20.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.