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Coherent Control and Switching: 1st

Jeremy J. Baumberg

Published Jan 1, 1999• 0 citations
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The macroscopic quantum tunneling (MQT) in the current-biased intrinsic Josephson junctions (IJJs) of high- T c cuprates has attracted much attention for decades. Although the MQT for the phase switches from the zero to the first voltage state (1st SW) in the multiple-branched I-V curves is well explained by the conventional theory, the occurrence of MQT for the higher order switches such as the switch from the 1st to 2nd voltage state (2nd SW) has been still debated. Here, we present an experimental study on the phase switches of small IJJs fabricated from underdoped Bi 2 Sr 2 (Ca,Y)Cu 2 O y . We observed the single photon transition between quantized energy levels in the 3rd phase switches at 59.15 GHz and 2 K. The comparison with the previous studies on the nearly optimal-doped Bi 2 Sr 2 CaCu 2 O y clearly suggests a possibility that the MQT rate for the higher-order phase switches is commonly enhanced by the effective suppression of the energy barrier for the higher-order phase escape due to the phase-running state after the 1st SW, in spite of the large difference in a critical current density and T c .

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“Coherent Control?” Is not a Question

W. S. Warren

Springer series in chemical physics•Jan 1, 1994•0 citations
The macroscopic quantum tunneling (MQT) in the current-biased intrinsic Josephson junctions (IJJs) of high- T c cuprates has attracted much attention for decades. Although the MQT for the phase switches from the zero to the first voltage state (1st SW) in the multiple-branched I-V curves is well explained by the conventional theory, the occurrence of MQT for the higher order switches such as the switch from the 1st to 2nd voltage state (2nd SW) has been still debated. Here, we present an experimental study on the phase switches of small IJJs fabricated from underdoped Bi 2 Sr 2 (Ca,Y)Cu 2 O y . We observed the single photon transition between quantized energy levels in the 3rd phase switches at 59.15 GHz and 2 K. The comparison with the previous studies on the nearly optimal-doped Bi 2 Sr 2 CaCu 2 O y clearly suggests a possibility that the MQT rate for the higher-order phase switches is commonly enhanced by the effective suppression of the energy barrier for the higher-order phase escape due to the phase-running state after the 1st SW, in spite of the large difference in a critical current density and T c .
We present a study of the first and second switches (SWs) with nearly identical switching current ISWI_{\rm SW}ISW​ in Bi2_22​Sr2_22​Ca0.85_{0.85}0.85​Y0.15_{0.15}0.15​Cu2_22​Oy_yy​ intrinsic Josephson junctions (IJJs). In contrast to early studies where a large difference between ISW1stI_{\rm SW}^{\rm 1st}ISW1st​ and ISW2ndI_{\rm SW}^{\rm 2nd}ISW2nd​ was observed, a crossover temperature TcrT_{\rm cr}Tcr​ to the quantum phase escapes for the 2nd SW is strongly reduced $(\sim$2.8~K) and agrees with that for the 1st SW. This confirms that the anomalous enhancement of Tcr2ndT_{\rm cr}^{\rm 2nd}Tcr2nd​, commonly observed in the IJJs with ISW1st<ISW2ndI_{\rm SW}^{\rm 1st} < I_{\rm SW}^{\rm 2nd}ISW1st​<ISW2nd​, originates from the phase running state after the 1st SW. Detailed analysis of the microwave-induced escapes strongly suggests that nonlinear bifurcated phenomena possibly occurs in IJJs.