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Resonant Cavity Modes in Bi2Sr2CaCu2O8+x Intrinsic Josephson Junction

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dc.contributor.author Zhang, HL
dc.contributor.author Wieland, R
dc.contributor.author Chen, W
dc.contributor.author Kizilaslan, O
dc.contributor.author Ishida, S
dc.contributor.author Han, C
dc.contributor.author Tian, WH
dc.contributor.author Xu, ZY
dc.contributor.author Qi, ZD
dc.contributor.author Qing, T
dc.contributor.author Lv, YY
dc.contributor.author Zhou, XJ
dc.contributor.author Kinev, N
dc.contributor.author Ermakov, AB
dc.contributor.author Dorsch, E
dc.contributor.author Ziegele, M
dc.contributor.author Koelle, D
dc.contributor.author Eisaki, H
dc.contributor.author Yoshida, Y
dc.contributor.author Koshelets, VP
dc.contributor.author Kleiner, R
dc.contributor.author Wang, HB
dc.contributor.author Wu, PH
dc.date.accessioned 2022-10-11T13:33:19Z
dc.date.available 2022-10-11T13:33:19Z
dc.date.issued 2019
dc.identifier.uri http://hdl.handle.net/11616/76335
dc.description.abstract We report on a detailed investigation of terahertz-emission properties related to resonant cavity modes. We discuss data for an underdoped and an optimally doped Bi2Sr2CaCu2O8+x (BSCCO) intrinsic junction stack having the same geometry. At high bias, in the presence of a hot spot, the emission frequency seems to be continuously tunable by changing the bias current and the bath temperature. By contrast, at low bias the emission frequencies f(e) are remarkably discrete and temperature independent for both stacks. The values of f(e) point to the formation of (0, m) cavity modes with m = 3 to 6. The total voltage V across the stack varies much stronger than f(e), and there seems to be an excess voltage indicating groups of junctions that are unlocked. For the case of the underdoped stack we perform intensive numerical simulations based on coupled sine Gordon equations combined with heat-diffusion equations. Many overall features can be reproduced well and point to an unexpected large value of the in-plane resistivity. However, unlike in experiment, in simulations the different resonant modes strongly overlap. The reason for this discrepancy is presently unclear.
dc.source PHYSICAL REVIEW APPLIED
dc.title Resonant Cavity Modes in Bi2Sr2CaCu2O8+x Intrinsic Josephson Junction
dc.title Stacks


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