Effects of magnetic vortices upon Josephson Plasma Wave propagation in Bi<sub>2</sub>Sr<sub>2</sub>CaCu<sub>2</sub>O<sub>8</sub> crystals
ORAL
Abstract
Extremely anisotropic cuprate superconductors contain 'intrinsic' Josephson junctions, stacked along the crystalline c-axis. Consequently, these compounds can support the propagation of Josephson plasmons at frequencies of hundreds of GHz or more. These plasmons primarily transport energy along the CuO2 planes via oscillating Josephson tunneling currents. In Bi2Sr2CaCu2O8, it is predicted that Josephson plasmons could propagate over distances of centimeters, due to the highly underdamped nature of the Josephson oscillations in this material. This phenomenon could have technological applications, such as in highly efficient mixers and detectors for terahertz frequencies.
We observe the propagation of Josephson plasma waves at 0.45 THz through an optimally-doped Bi2Sr2CaCu2O8 slab with diameter 5 mm and thickness 0.21 mm, cut from a TSFZ growth rod and consisting of multiple single crystals. Our zero-field results imply a plasmon decay length that is 0.4 mm at 85 Kelvin (slightly below Tc) and peaks at 0.9 mm at 25 Kelvin. We also find that the plasmon decay length can be either strongly enhanced or suppressed by applied magnetic fields of the order of a few tens of Gauss, depending upon the magnitude of the field. Applying a field of 25 G increases the decay length to approximately 1 cm or more at 4.4 K. We provisionally attribute this behavior to transmission of THz energy via pinned vortex lattices in the crystals of our sample.
We observe the propagation of Josephson plasma waves at 0.45 THz through an optimally-doped Bi2Sr2CaCu2O8 slab with diameter 5 mm and thickness 0.21 mm, cut from a TSFZ growth rod and consisting of multiple single crystals. Our zero-field results imply a plasmon decay length that is 0.4 mm at 85 Kelvin (slightly below Tc) and peaks at 0.9 mm at 25 Kelvin. We also find that the plasmon decay length can be either strongly enhanced or suppressed by applied magnetic fields of the order of a few tens of Gauss, depending upon the magnitude of the field. Applying a field of 25 G increases the decay length to approximately 1 cm or more at 4.4 K. We provisionally attribute this behavior to transmission of THz energy via pinned vortex lattices in the crystals of our sample.
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Presenters
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Timothy M Benseman
Queens College, City University of New York
Authors
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Timothy M Benseman
Queens College, City University of New York
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Sarah Elghazoly
Queens College, City University of New York
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Ulrich Welp
Argonne National Laboratory
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Wai-Kwong Kwok
Argonne National Laboratory
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Alexei E Koshelev
University of Notre Dame
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Geetha Balakrishnan
University of Warwick
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John R Cooper
University of Cambridge