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: Metallurgy, HRTEM, Magnetic Properties and Specific Heat of Tl2Ba2Cu1O6+δ 90K-Superconductors Obtained by a New Process
Author(s): C.Opagiste, M.Couach, A.Khoder, T.Graf, A.Junod, G.Triscone, J.Muller, T.K.Jondo, J.L.Jorda, R.Abraham, et al.
Publication: Physica C Volume: 205 Issue: Not Available Year: 1993 Page(s): 247-258
Editor(s): Not Available
Publisher: Elsevier Science Publishers B.V.
Language: English
Notes: et al.=M.Th.Cohen-Adad, L.A.Bursill, O.Leckel,M.G.Blanchin
Keywords: Material Specification, Crystallography, Critical Temperature, Magnetic Susceptibility, Specific Heat, Irreversibility Field

Materials and Properties

Tl:221; [Tl-Ba-Cu-O]
Material Specification for Tl:221; [Tl-Ba-Cu-O] Process: Solid State Reaction
Notes: "We used Tl2Ba2O5 and CuO (Cerac, 99.9%) powder either directly (batch B) or after annealing for 3 days at 750 °C under (0.1 MPa =1 bar) O2 (batch A). After pressing the stoichiometric mixture under(0.5 GPa = 5 kbar), the pellets were given appropriate heat treatments, i.e. (1) reaction at 900-930 °C under (10 MPa = 100 bar) of oxygen during 30 min to obtain the orthorhombic, non-superconducting phase. The weight loss is somewhat below 0.8%. (2) reaction at 850 °C under (10 MPa = 100 bar) of argon or helium during 12 min, followed by regrinding and repeating the procedure twice, to form the tetragonal superconducting 2201 phase. A more significant weight loss of 1.5% is observed in this case."
Formula: Tl2Ba2CuO6+x
Informal Name: Tl:221
Chemical Family: Tl-Ba-Cu-O
Chemical Class: Oxide
Structure Type: Polycrystalline
Manufacturer: In House
Commercial Name: In House
Production Date:
Lot Number:
Production Form:

Crystallography for Tl:221; [Tl-Ba-Cu-O]
Crystal System:
Formula Units per Cell:
Space Group:
Cell Parameters
Batch Number () Gas Preparation () Temp K a Å b Å c Å
B helium 296 3.8694(4) -- 23.221(4)
B helium 296 3.8674(3) -- 23.218(3)
B argon 296 3.8717(5) -- 23.225(4)
A argon 296 3.8706(4) -- 23.224(3)
A argon 296 3.8685(3) -- 23.223(3)
A argon 296 3.8700(3) -- 23.226(2)
A argon 296 3.8693(4) -- 23.230(3)
A oxygen 296 5.4467(8) 5.4911(7) 23.144(2)
A oxygen 296 5.4470(6) 5.4974(5) 23.141(2)
Measurement Method: X-ray diffraction
"The crystal structure was studied at ambient temperature by X-ray diffraction using a Guinier camera with CuKα radiation. Silicon was added to the powdered samples as an internal standard (a=5.4308 σ). The lattice parameters of the...orthorhombic and tetragonal phases were determined from least-squares fits using more than 20 lines (10° < 4θ < 160°). The lines were indexed according to the space group I4/mmm for the tetragonal phase and Ccc2 (A2aa) for the orthorhombic phase."

Cautions: Evaluated Data
Critical Temperature for Tl:221; [Tl-Ba-Cu-O]
Batch Number () Gas Preparation () Critical Temperature (K)
B helium 90.8
B helium 91.8
B argon 91.1
A argon 92.1
A argon 90.5
A argon 92.0
A argon 87.4
Measurement Method: Ac susceptibility
"The superconducting transitions were detected by means of a mutual inductance bridge operating between 80 and 800 Mz. The AC field amplitude was set in a first run to a low value of typically (4 A/m = 0.05 Oe) rms. The earth field is compensated by a screen of µ-metal." No additional measurement details were noted.

Cautions: Evaluated Data
Magnetic Susceptibility for Tl:221; [Tl-Ba-Cu-O]
Magnetic Field (T) Temperature (K) Magnetic Susceptibility (arbitrary)
0 6 -0.78
0 22 -0.77
0 46 -0.75
0 67 -0.71
0 89 -0.49
0 99 0.00
0 100 0.00
0.05 34 -0.66
0.05 46 -0.61
0.05 57 -0.35
0.05 61 -0.18
0.05 67 -0.05
0.05 77 0.00
0.05 100 0.00
0.1 34 -0.63
0.1 46 -0.53
0.1 51 -0.32
0.1 58 -0.09
0.1 67 -0.01
0.1 89 0.00
0.1 100 0.00
0.2 28 -0.64
0.2 43 -0.43
0.2 46 -0.35
0.2 52 -0.13
0.2 62 -0.01
0.2 67 0.00
0.2 100 0.00
0.5 25 -0.63
0.5 34 -0.51
0.5 41 -0.22
0.5 45 -0.09
0.5 53 0.00
0.5 100 0.00
1 23 -0.60
1 32 -0.35
1 35 -0.15
1 41 -0.04
1 45 0.00
1 100 0.00
1.8 6 -0.72
1.8 16 -0.65
1.8 23 -0.50
1.8 28 -0.24
1.8 35 -0.07
1.8 39 0.00
1.8 100 0.00
Measurement Method: Ac susceptibility
"The superconducting transitions were detected by means of a mutual inductance bridge operating between 80 and 800 Mz. The AC field amplitude was set in a first run to a low value of typically (4 A/m = 0.05 Oe) rms. The earth field is compensated by a screen of µ-metal." No additional measurement details were noted.

Cautions: Evaluated Data
Digitized data were obtained from Figure 6 of the paper.
Specific Heat for Tl:221; [Tl-Ba-Cu-O]
Temperature (K) Specific Heat (J kg-1 K-1)
65 10.2
67 10.6
71 11.2
75 12.0
80 12.8
88 13.9
92 14.5
96 15.1
100 15.4
104 15.9
105 16.1
107 16.2
Measurement Method: Adiabatic calorimeter
"The calorimeter used for this study is of the adiabatic, continuous heating type; the sample is in vacuo. Years of operation have confirmed an accuracy better than 1% using 0.5 g samples, whereas the scatter may be as low as 0.1% to 0.2%." No additional measurement details were noted.

Cautions: Evaluated Data
Digitized data were obtained from Figure 12 of the paper.
Irreversibility Field for Tl:221; [Tl-Ba-Cu-O]
Temperature (K) Irreversibility Field (T)
50 1.8
55 1.0
61 0.5
67 0.2
73 0.09
77 0.05
Measurement Method: Ac susceptibility
"The superconducting transitions were detected by means of a mutual inductance bridge operating between 80 and 800 Mz. The AC field amplitude was set in a first run to a low value of typically (4 A/m = 0.05 Oe) rms. The earth field is compensated by a screen of µ-metal." No additional measurement details were noted.

Cautions: Evaluated Data
Digitized data were obtained from Figure 7 of the paper.