• Journal of Infrared and Millimeter Waves
  • Vol. 40, Issue 3, 321 (2021)
Zhi-Yong SONG1、2、4, Li-Yan SHANG1、*, Jun-Hao CHU2, Ping-Ping CHEN1、2, [in Chinese]3, and Ting-Ting KANG2、4、**
Author Affiliations
  • 1East China Normal University, Shanghai 200062, China
  • 2State Key Laboratory of Infrared Physics, Shanghai Institute of Technical Physics, Chinese Academy of Sciences, Shanghai 200083, China
  • 3University of Fukui, Fukui, 910-8507, Japan
  • 4Key Laboratory of Nanodevices and Applications, Suzhou Institute of Nano-Tech and Nano-Bionics, Chinese Academy of Sciences, Suzhou 215123, China
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    DOI: 10.11972/j.issn.1001-9014.2021.03.007 Cite this Article
    Zhi-Yong SONG, Li-Yan SHANG, Jun-Hao CHU, Ping-Ping CHEN, [in Chinese], Ting-Ting KANG. Flux pinning properties of InN[J]. Journal of Infrared and Millimeter Waves, 2021, 40(3): 321 Copy Citation Text show less
    X-ray diffraction pattern of the InN film.
    Fig. 1. X-ray diffraction pattern of the InN film.
    (a) R-T transitions,(b) R-B2 transitions as a function of temperature,(c) The upper critical field Bc2 as a function of temperature. In(a–c), the resistance is measured with a current of 1 μA
    Fig. 2. (a) R-T transitions,(b) R-B2 transitions as a function of temperature,(c) The upper critical field Bc2 as a function of temperature. In(a–c), the resistance is measured with a current of 1 μA
    (a) I-V curves at various temperatures from 120 mK to 3 K for self-field,(b) VG scaling of the I-V curves in(a).(c) The temperature dependence of I-V exponent in(a)
    Fig. 3. (a) I-V curves at various temperatures from 120 mK to 3 K for self-field,(b) VG scaling of the I-V curves in(a).(c) The temperature dependence of I-V exponent in(a)
    Vortex phase diagram of InN superconductor.
    Fig. 4. Vortex phase diagram of InN superconductor.
    (a) log(R) vs 1/T in various fields and the fitting results of TAFF model.(b) Field dependence of U0 (B). the solid lines are power-law fits using U0(B)~ B-α.
    Fig. 5. (a) log(R) vs 1/T in various fields and the fitting results of TAFF model.(b) Field dependence of U0 (B). the solid lines are power-law fits using U0(B)~ B.
    (a) The dots are experimental data of temperature dependence of Ic at zero field. The blue, green, and red lines are fitting results using δTc, δL, and the combined δL+δTcmodel, respectively,(b) Temperature dependence of Ic in various fields and the fitting results of δL+δTc model.
    Fig. 6. (a) The dots are experimental data of temperature dependence of Ic at zero field. The blue, green, and red lines are fitting results using δTc, δL, and the combined δL+δTcmodel, respectively,(b) Temperature dependence of Ic in various fields and the fitting results of δL+δTc model.
    (a) Magnetic field dependence of critical current Ic and the fitting results of exponential-law,(b) Reduced field dependence of normalized flux pinning force fp(h) at various temperatures. Solid line is the fitting curve using Eq.(6)
    Fig. 7. (a) Magnetic field dependence of critical current Ic and the fitting results of exponential-law,(b) Reduced field dependence of normalized flux pinning force fp(h) at various temperatures. Solid line is the fitting curve using Eq.(6)
    Zhi-Yong SONG, Li-Yan SHANG, Jun-Hao CHU, Ping-Ping CHEN, [in Chinese], Ting-Ting KANG. Flux pinning properties of InN[J]. Journal of Infrared and Millimeter Waves, 2021, 40(3): 321
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