• Title/Summary/Keyword: $Bi_2$$Sr_2$Ca$Cu_2$$O_{8+$\delta$}$polaronic quasiparticle injection

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Tunneling Spectra in Organic Cu-Pc/$Bi_2Sr_2CaCu_2O_{8+\delta}$ Tunnel Junctions

  • Kim, Sunmi;E, Jungyoon;Lee, Kiejin;Ishbas, Takayuki;Lee, Yang-San
    • Progress in Superconductivity
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    • v.3 no.1
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    • pp.41-44
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    • 2001
  • We report the current transport properties of a normal metal/organic conductor/ superconductor tunnel junction as a novel high- $T_{c}$ superconducting three terminal device. The organic copper (II) phthalocyanine (Cu-Pc) layer was used far a polaronic quasiparticle (QP) injector. The injection of polaronic QP from the Cu-Pc interlayer into a superconductor $Bi_2$$Sr_2$$CaCu_2$ $O_{8+}$ $\delta$/(BSCCO) thin film generated a substantially larger nonequilibrium effect as compared to the normal QP injection current. The tunneling spectroscopy of an Au/cu-PC/BSCCO junction exhibited a zero bias conductance peak which may be due to Andreev reflection at a Cu-Pc/d-wave superconductor junction.n..

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Tunneling effect due to UV irradiation in organic Cu-Pc/$Bi_2$$Sr_2$Ca$Cu_2$$O_{8+$\delta$}$ tunnel junction

  • Kim, Sunmi;Lee, Kiejin;Deokjoon Cha;Takayuki Ishibashi
    • Progress in Superconductivity
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    • v.4 no.2
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    • pp.99-103
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    • 2003
  • We studied the nonequilibrium superconductivity due to tunnel injection of polaronic quasiparticle (QP) from organic photoconductor. The transport properties of an organic copper (II) phthalocyanine (Cu -Pc)/d-wave superconductor were investigated in dark and under ultraviolet (UV) radiation for performance of a novel $high -T_{c}$ superconducting three terminal device. We observed that the injection of polaronic QP from the organic Cu -Pc film into the $Bi_2$S $r_2$$CaCuO_{8+{\delta}}$ film generated a substantially larger nonequilibrium effect as compared to the normal QP injection current. We could increase the current gain by UV excitation of the organic photoconductor injector. The tunneling spectroscopy of a Cu -Pc/BSCCO junction exhibited a small enhancement of the zero bias conductance peak under the W excitation. The above phenomena are of importance in developing optically controlled three terminal superconducting device.e.

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