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Volumn 82, Issue 9, 2010, Pages

Nonequilibrium effects in the thermal switching of underdamped Josephson junctions

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EID: 77957596645     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.82.094505     Document Type: Article
Times cited : (12)

References (33)
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    • -1 and A (y) is the interpolation function given by Mel'nikov and Meshkov (Ref.): A (y) =exp [ 1 π 0 dxln { 1-exp [-y ( x2 + 1 4 ) ] } / ( x2 + 1 4 ) ]
    • - 1 and A (y) is the interpolation function given by Mel'nikov and Meshkov (Ref.): A (y) = exp [1 π 0 d x ln { 1 - exp [- y (x 2 + 1 4)] } / (x 2 + 1 4)].
  • 23
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    • The equations were numerically integrated using the Stochastic Runge Kutta algorithm (3o4s2g) with time step 0.01
    • The equations were numerically integrated using the Stochastic Runge Kutta algorithm (3o4s2g) with time step 0.01.
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    • For the correction factor α introduced in the BHL theory (Ref.), we use the standard value α=1
    • For the correction factor α introduced in the BHL theory (Ref.), we use the standard value α = 1.
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    • -1 =√ m/ V0. Then, the adimensionalized parameters are γ =γ/ω=1.50γ, T = kB T/ V0 =6.45 kB T, and I = I / (ω V0 ) =9.70 I.
    • - 1 = √ m / V 0. Then, the adimensionalized parameters are γ = γ / ω = 1.50 γ, T = k B T / V 0 = 6.45 k B T, and I = I / (ω V 0) = 9.70 I.
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.