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: Lower Critical Field Measurements in YBa2Cu3O6+x Single Crystals
Author(s): D.L. Kaiser, L.J. Swartzendruber, F.W. Gayle, and L.H. Bennett
Publication: AMSAHTS 90: Adv. in Matls. Sci. and Appl. of HTS Volume: Not Available Issue: Not Available Year: 1991 Page(s): 249-255
Editor(s): L.H. Bennett, Y. Flom, and K. Moorjani
Publisher: National Aeronautics and Space Administration
Language: English
Notes: NASA Conference Publication 3100
Keywords: Material Specification, Critical Field Strength Hc1

Materials and Properties

Y:123; [Y-Ba-Cu-O]
Material Specification for Y:123; [Y-Ba-Cu-O] Process: Melt Processed
Notes: The authors cite D.L. Kaiser, et al., Appl. Phys. Lett., Vol. 51, 1040-1042 (1987), and summarize the procedure as follows. "... crystals... were grown from Y-Ba-Cu-O melts and subsequently annealed in oxygen gas at 420 °C for 80 h... Two crystals were selected for measurement... (AN3-5) exhibited characteristic (110) twin planes and was nearly cubic with dimensions 120 x 135 x 120 µm3 (c-dimension = 120 µm)... (AN9-5) was fully detwinned via a thermo-mechanical process... and had dimensions a x b c = 200 x 250 x 100 µm3."
Formula: YBa2Cu3O6+x
Informal Name: Y:123
Chemical Family: Y-Ba-Cu-O
Chemical Class: Oxide
Structure Type: Single Crystal
Manufacturer: In House
Commercial Name: In House
Production Date:
Lot Number:
Production Form:

Critical Field Strength Hc1 for Y:123; [Y-Ba-Cu-O]
Field Direction () Temperature (K) Crit.Mag.Field Strength Hc1 (kA/m)
H//c 10 56
H//c 77 12
H//c 86 6
H//c 88 4
H//c 90 3
H//c 92 0.5
H//ab 10 14
H//ab 40 11
H//ab 50 8
H//ab 60 7
H//ab 65 5
H//ab 75 3
H//ab 80 2
H//ab 85 1
Measurement Method: SQUID magnetometer
"Magnetic measurements were made using superconducting quantum interference device (SQUID) magnetometer, with the c axis of the crystal aligned either perpendicular or parallel to the applied field H. The crystal was first cooled in zero field to a predetermined temperature and the magnetization was then measured as the applied field was increased to a value in excess of H ."

Cautions: Evaluated Data
Digitized data were obtained from Figure 3a and 3b of the paper.