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: Dependence of the Superconducting Transition Temperature of HgBa2CuO4+δ on Hydrostatic Pressure
Author(s): A.K. Klehe, A.K. Gangopadhyay, J. Diederichs, and J.S. Schilling
Publication: Physica C Volume: 213 Issue: Not Available Year: 1992 Page(s): 266-270
Editor(s): Not Available
Publisher: Elsevier Science Publishers B.V.
Language: English
Notes: Not Available
Keywords: Material Specification, Density (mass), Crystallography, Critical Temperature, Magnetic Susceptibility

Materials and Properties

Hg:121; [Hg-Ba-Cu-O]
Material Specification for Hg:121; [Hg-Ba-Cu-O] Process: Solid State Reaction
Notes: "The superconducting sample... was prepared from the solid state reaction of HgO (99.998% pure, Johnson Matthey) with a Ba2CuO3 precursor. To synthesize this precursor, stoichiometric amounts of Ba(NO3)2 (99.999% pure, Johnson Matthey) and CuO (99.999% pure, Johnson Matthey) were mixed together in a sapphire mortar and reacted at 930 °C for 48 h in flowing O2 with one intermediate grinding. Since Ba2CuO3 reacts with moisture, all subsequent handling of the material was done in a glove box utilizing nitrogen gas. A mixture of HgO and Ba2CuO3 was then pelletized under (about) 0.8 GPa pressure and sealed in a thick-walled quartz tube (7 mm I.D., 10 mm O.D.) under (about 0.1 mPa = 10-6 torr) vacuum. The quartz tube was enclosed in a stainless steel container and welded shut as an additional protection against a possible rupture of the quartz tube... Superconducting samples were obtained either by rapid heating (10-15 K/min) to 800 °C or by inserting the sample into a preheated furnace; slow heating (10 h to 800 °C) resulted in a severe reaction of the sample with the quartz tube and yielded non-superconducting samples. Reaction at either 800 °C or 845 °C for 5-8 h followed by an oven cool to ambient temperature resulted in superconducting samples. The sample used in the present high pressure study was then annealed at 200 °C for 12 h in flowing O2."
Formula: HgBa2CuO4+x
Informal Name: Hg:121
Chemical Family: Hg-Ba-Cu-O
Chemical Class: Oxide
Structure Type: Polycrystalline
Manufacturer: In House
Commercial Name: In House
Production Date:
Lot Number:
Production Form:

Density (mass) for Hg:121; [Hg-Ba-Cu-O]
Density (g cm-3)
7.0
Measurement Method: X-ray diffraction
"The X-ray powder diffraction pattern (CuKα radiation) for the present sample is consistent with a tetragonal unit cell..." No additional measurement details were noted.

Cautions: Unevaluated Data
Crystallography for Hg:121; [Hg-Ba-Cu-O]
Crystal System: Tetragonal
Formula Units per Cell:
Space Group: P4/mmm
Cell Parameters
Temp K a Å b Å c Å
296 3.875(1) -- 9.516(1)
Measurement Method: X-ray diffraction
"The X-ray powder diffraction pattern (CuKα radiation) for the present sample is consistent with a tetragonal unit cell..." No additional measurement details were noted.

Cautions: Unevaluated Data
Critical Temperature for Hg:121; [Hg-Ba-Cu-O]
Pressure (GPa) Tc(upper) (K) Critical Temperature (K)
0.0 98.1 95.0
0.2 98.3 95.2
0.4 98.8 95.7
0.5 99.0 95.9
0.6 99.1 96.1
0.7 99.3 96.3
0.8 99.5 96.5
0.9 99.6 96.6
Measurement Method: Ac susceptibility
"The He-gas three-stage compressor system used in the present experiments was acquired from Harwood Engineering (Walpole, Massachussetts) and connected via a CuBe capillary tube to a cylindrical (28 mm O.D. x 7 mm I.D.) CuBe pressure cell from Unipress (Warsaw, Poland). The pressure vessel was inserted into a cryostat with a full liquid nitrogen shield and cooled indirectly by exchange gas. All changes in pressure were carried out at a temperature above the melting curve of He (56 K at 0.9 GPa). A nonmagnetically wound wire heater on the pressure cell allowed one to vary the temperature. The AC susceptibility was measured using a standard primary/secondary coil system with a 2.0 mm I.D. cylindrical sample space. An EG&G Model 5210 two-phase lock-in amplifier set at 500 Hz was used to simultaneously measure the in-phase... and out-of-phase... components." The susceptibility is reported for zero pressure in a field of 7.9 A/m = 0.1 Oe.

Cautions: Evaluated Data
"Upon cooling (the susceptibility) shows a slight but sharp break from the horizontal at a temperature Tc (upper)....This initial decrease...clearly marks a superconducting onset, perhaps arising from a small region (about 3%) of the sample which is nearly optimally doped. The primary transition to superconductivity for the bulk of the sample appears to occur below Tc(lower) where (the susceptibility) begins to fall rapidly and trace out a characteristic S-shaped curve." Digitized data were obtained from Figure 3 of the paper.
Magnetic Susceptibility for Hg:121; [Hg-Ba-Cu-O]
Temperature (K) Magnetic Susceptibility (arbitrary)
80 -13.6
90 -12.0
92 - 8.0
93 - 4.0
95 - 0.4
96 - 0.3
98 - 0.2
99 0.0
Measurement Method: Ac susceptibility
"The He-gas three-stage compressor system used in the present experiments was acquired from Harwood Engineering (Walpole, Massachussetts) and connected via a CuBe capillary tube to a cylindrical (28 mm O.D. x 7 mm I.D.) CuBe pressure cell from Unipress (Warsaw, Poland). The pressure vessel was inserted into a cryostat with a full liquid nitrogen shield and cooled indirectly by exchange gas. All changes in pressure were carried out at a temperature above the melting curve of He (56 K at 0.9 GPa). A nonmagnetically wound wire heater on the pressure cell allowed one to vary the temperature. The AC susceptibility was measured using a standard primary/secondary coil system with a 2.0 mm I.D. cylindrical sample space. An EG&G Model 5210 two-phase lock-in amplifier set at 500 Hz was used to simultaneously measure the in-phase... and out-of-phase... components." The susceptibility is reported for zero pressure in a field of 7.9 A/m = 0.1 Oe.

Cautions: Evaluated Data
"Upon cooling (the susceptibility) shows a slight but sharp break from the horizontal at a temperature Tc(upper)... This initial decrease...clearly marks a superconducting onset, perhaps arising from a small region ( (about) 3%) of the sample which is nearly optimally doped. ... The primary transition to superconductivity for the bulk of the sample appears to occur below Tc(lower) where (the susceptibility) begins to fall rapidly and trace out a characteristic S-shaped curve." Digitized data were obtained from Figure 1 and Figure 1 (inset) of the paper.