NIST High Temp. Superconducting Materials (HTS) Database:

NIST Standard Reference Database 62

Last Update to Data Content: 1996

DOI: https://doi.org/10.18434/T4KP8J


Bibliographic Information

Title: Tunneling Spectroscopic Measurements on Boride Carbide Superconductors
Author(s): T. Hasegawa, M. Ogino, A. Takagi, E. Watanabe, M. Nantoh, H. Takagi, S. Uchida, R.J. Cava, and K. Kitazawa
Publication: Physica C Volume: 235 Issue: Not Available Year: 1994 Page(s): 1859-1860
Editor(s): Not Available
Publisher: Elsevier Science Publishers B.V.
Language: English
Notes: Vol. 235-240, multivolume issue
Keywords: Material Specification, Critical Temperature, Energy Gap(2 delta)

Materials and Properties

[Lu-Ni-B-C]
Material Specification for ; [Lu-Ni-B-C] Process: Melt Processed
Notes: "Polycrystalline samples of single phase LuNi2B2C were prepared by arc melting and annealing." No additional processing details were noted.
Formula: LuNi2B2C
Informal Name:
Chemical Family: Lu-Ni-B-C
Chemical Class: Carbide
Structure Type: Polycrystalline
Manufacturer: In House
Commercial Name: In House
Production Date:
Lot Number:
Production Form:

Critical Temperature for ; [Lu-Ni-B-C]
Transition Width (K) Critical Temperature (K)
0.5 16.6
Measurement Method: Electrical resistance
No measurement details were noted.

Cautions: Unevaluated Data
Energy Gap(2 delta) for ; [Lu-Ni-B-C]
Temperature (K) Energy Gap (2Δ) (meV)
4.7 4.6 ± 0.4
Measurement Method: Tunneling microscopy
"...we report the tunneling spectroscopic measurements... using cryogenic temperature scanning tunneling microscoppy (CT-STM). ... The CT-STM instrument employed in this experiment was laboratory-constructed. The STM unit was sustained in the dual concentric stainless steel tubes which were directly immersed into liquid He. Specimens were cooled down to 4.2 K through He exchange gas. Surface of the samples were polished by an Al2O3 sheet in air just prior to the tunneling measurements. The observed spectra had rather complex background conductance dependent on temperature. In order to determine the gap value quantitatively, the experimental conductance curves was divided by an appropriate background assumed at each temperature independently. ... By fitting the Dynes' function to the background corrected conductance curves, we have deduced the energy gap Δ."

Cautions: Unevaluated Data