2010
DOI: 10.1103/physrevb.81.224518
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Counterintuitive consequence of heating in strongly-driven intrinsic junctions ofBi2Sr2CaCu2O8+δ

Abstract: Anomalously high and sharp peaks in the conductance of intrinsic Josephson junctions in Bi 2 Sr 2 CaCu 2 O 8+␦ ͑Bi2212͒ mesas have been commonly interpreted as superconducting energy gaps but here we show they are a result of strong self-heating. This conclusion follows directly from a comparison to the equilibrium gap measured by tunneling in single break junctions on equivalent crystals. As the number of junctions in the mesa, N, and thus heating increase, the peak voltages decrease and the peak width abrupt… Show more

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Cited by 45 publications
(51 citation statements)
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References 51 publications
(161 reference statements)
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“…In figure 5, the contact resistance can be seen in our data below T c due to our three-point measurements: it is usually < 5 except for one sample (w = 40 μm). A recent study on 10×10 μm 2 mesas show the contact resistance to be a superconductor-insulator-normal-metal junction that can be expected to be weakly temperature-dependent above T c and diverge at low temperatures [29]. Values range from 0.00015 to 0.0005 cm 2 .…”
Section: Resultsmentioning
confidence: 99%
“…In figure 5, the contact resistance can be seen in our data below T c due to our three-point measurements: it is usually < 5 except for one sample (w = 40 μm). A recent study on 10×10 μm 2 mesas show the contact resistance to be a superconductor-insulator-normal-metal junction that can be expected to be weakly temperature-dependent above T c and diverge at low temperatures [29]. Values range from 0.00015 to 0.0005 cm 2 .…”
Section: Resultsmentioning
confidence: 99%
“…2). As can be seen in the plot, the IV-characteristics are strongly influenced by self-heating, to the extent that it is S-shaped, which is typical for mesas of this size [12,15]. For the mesas on this chip, THz emission occurs where dI/dV is very large, or even negative, and it has been suggested [16] that this may be essential for some modes of THz emission in these devices.…”
mentioning
confidence: 89%
“…We take advantage of a number of studies [19][20][21] that show clearly that the normal state conductance is a smoothly varying function which merges with the superconducting conductance for voltages just beyond that of the hump in the dip or hump spectral feature. Published SIS tunneling conductances [16] have been normalized by generating a normal state conductance which smoothly interpolates between the positive and negative high bias superconducting data just beyond the hump voltage.…”
mentioning
confidence: 99%