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Volumn 85, Issue 3, 1991, Pages 459-467

Coherent Cooper pair tunneling in systems of Josephson junctions: Effects of quasiparticle tunneling and of the electromagnetic environment

Author keywords

[No Author keywords available]

Indexed keywords

EID: 1642516282 PISSN: 07223277 EISSN: 14346036 Source Type: Journal
DOI: 10.1007/BF01307644 Document Type: Article

Times cited : (51)

References (18)

1
- 0000113067
- Mesoscopic phenomena in solids
- B.L., Altshuler, P.A., Lee, R.A., Webb, North Holland, Amsterdam
- (1991) Modern problems in condensed matter sciences
- Averin, D.V.¹ Likharev, K.K.²

7
- 84931537812
- Quantum Tunnelling in Small-Capacitance Josephson Junctions in a General Electromagnetic Environment
- (1991) Europhysics Letters (EPL) , vol.16 , pp. 109
- Falci, G.¹ Bubanja, V.² Schön, G.³

8
- 0025467387
- Incoherent tunneling of the cooper pairs and magnetic flux quanta in ultrasmall Josephson junctions
- (1990) Physica B: Condensed Matter , vol.165-166 , pp. 945
- Averin, D.V.¹ Nazarov² Odintsov, A.A.³

9
- 84956075185
- Simultaneous Bloch and Josephson Oscillations, and Resistance Quantizations in Small Superconducting Double Junctions
- (1987) Japanese Journal of Applied Physics , vol.26 , pp. 1407
- Likharev, K.K.¹ Zorin, A.B.²

12
- 84935178941
- Bobbert, P., Odintsov, A.A.: Europhys. Lett. (submitted for publication)

15
- 0023450673
- (1987) J. Low Temp. Phys. , vol.69 , pp. 219
- Guinea, F.¹ Schön, G.²

16
- 84935217993
- We have checked that this is consistent with our treatment of quasiparticle tunneling if the ratio Rn/Rqp would be as low as 10⁻¹¹, which is extraordinarily small, but on the other hand much larger than formula (21) predicts for the experimental parameters. Still, our tentative mechanism leaves the e-periodicity of the supercurrent is a puzzle.

17
- 0000591202
- (1989) Phys. Lett. A , vol.140 , pp. 251
- Averin, D.V.¹ Odintsov, A.A.²

18
- 84935156566
- The pronounced ridge in the I–V landscape for V>2e/CΣ and q0=0 is contained in formula (18) as the degenerate case (p=0, q=±4, qi=∓2), and corresponds to the second order resonance involving the states |−2 e, 0> and |2 e, 0>. This transition in itself does not transport any current, but in influences the equilibrium populations in such a way as to have a net effect

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