Negative Differential Resistance due to Nonlinearities in Single and Stacked Josephson Junctions

Josephson junction systems with a negative differential resistance (NDR) play an essential role for applications. As a well-known example, long Josephson junctions of the BSCCO type have been considered as a source of terahertz radiation in recent experiments. Numerical results for the dynamics of the fluxon system have demonstrated that a cavity induced NDR plays a crucial role for the emission of electromagnetic radiation. We consider the case of an NDR region in the McCumber curve itself of a single junction and found that it has an effect on the emission of electromagnetic radiation. Two different shapes of NDR region are considered, and we found that it is essential to distinguish between current bias and voltage bias.

[1]  V. Pierro,et al.  Negative differential resistance in Josephson junctions coupled to a cavity , 2014 .

[2]  W. Kwok,et al.  Tunable terahertz emission from Bi_{2}Sr_{2}CaCu_{2}O_{8+δ} mesa devices , 2014 .

[3]  R. Kleiner,et al.  Superconducting emitters of THz radiation , 2013, Nature Photonics.

[4]  D. Koelle,et al.  Modeling the linewidth dependence of coherent terahertz emission from intrinsic Josephson junction stacks in the hot-spot regime , 2013, 1307.3391.

[5]  D. Koelle,et al.  Linewidth dependence of coherent terahertz emission from Bi2Sr2CaCu2O8 intrinsic Josephson junction stacks in the hot-spot regime , 2012, 1206.2125.

[6]  A. Yurgens Temperature distribution in a large Bi2Sr2CaCu2O8+δ mesa , 2011 .

[7]  W. Kwok,et al.  Tunable terahertz emission from Bi2Sr2CaCu2O8+δ mesa devices , 2011, 1108.0143.

[8]  T. Koike,et al.  High Temperature Superconductor Terahertz Emitters: Fundamental Physics and Its Applications , 2011 .

[9]  D. Koelle,et al.  Coherent THz emission of Bi_2Sr_2CaCu_2O_8 intrinsic Josephson junction stacks in the hot spot regime , 2010, 1005.0081.

[10]  Hidetoshi Minami,et al.  Geometrical resonance conditions for THz radiation from the intrinsic Josephson junctions in Bi(2)Sr(2)CaCu(2)O(8+δ). , 2010, Physical review letters.

[11]  D. Koelle,et al.  Coherent THz emission of Bi_2Sr_2CaCu_2O_8 intrinsic Josephson junction stacks in the hot spot regime , 2010, 1005.0081.

[12]  T. Koyama,et al.  Mechanism of terahertz electromagnetic wave emission from intrinsic Josephson junctions. , 2008, Physical review letters.

[13]  W. Kwok,et al.  Direct observation of tetrahertz electromagnetic waves emitted from intrinsic Josephson junctions in single crystalline Bi2Sr2CaCu2O8+δ , 2008 .

[14]  N. Pedersen,et al.  Repulsive fluxons in a stack of Josephson junctions perturbed by a cavity , 2008 .

[15]  P. Reimann,et al.  Observation of negative absolute resistance in a Josephson junction. , 2008, Physical review letters.

[16]  W. Kwok,et al.  Emission of Coherent THz Radiation from Superconductors , 2007, Science.

[17]  D. Gokhfeld Description of hysteretic current-voltage characteristics of SNS junctions , 2006, cond-mat/0609541.

[18]  D. Gokhfeld Description of hysteretic current–voltage characteristics of superconductor–normal metal–superconductor junctions , 2006 .

[19]  G. Filatrella,et al.  Synchronization of underdamped Josephson-junction arrays , 2003 .

[20]  N. Pedersen,et al.  Stacked Josephson Junctions , 2010 .

[21]  S. Shitov,et al.  Integrated superconducting receivers , 2000 .

[22]  A. B. Cawthorne,et al.  STIMULATED EMISSION AND AMPLIFICATION IN JOSEPHSON JUNCTION ARRAYS , 1999 .

[23]  Niels Grønbech-Jensen,et al.  Fiske modes and Eck steps in long Josephson junctions: Theory and experiments , 1998 .

[24]  N. Pedersen,et al.  Fluxons in thin-film superconductor-insulator superlattices , 1993 .

[25]  K. Likharev,et al.  Dynamics of Josephson Junctions and Circuits , 1986 .

[26]  N. Pedersen,et al.  Half-harmonic parametric oscillations in Josephson junctions , 1980 .

[27]  N. Pedersen,et al.  Parametric amplification on rf‐induced steps in a Josephson tunnel junction , 1979 .

[28]  T. Claeson,et al.  Parametric amplification in arrays of Josephson tunnel junctions , 1977 .

[29]  N. Pedersen Zero‐voltage nondegenerate parametric mode in Josephson tunnel junctions , 1976 .

[30]  Niels Falsig Pedersen,et al.  Parametric excitation of plasma oscillations in Josephson Junctions , 1973 .