Material Specification for Bi:2223; [Bi(Pb)-Sr-Ca-Cu-O]
Process: Solid State Reaction
Notes: The authors cite W. Schnelle et al., Physica C, Vol. 161, 123 (1989) and T. Zetterer et al., Phys. Rev. B, Vol. 41, 9499 (1990), and summarize the procedures as follows. "The measurements have been carried out on one Bi-2223 polycrystal and on two Tl-2223 polycrystals."
Formula: Bi1.76Pb0.24Sr2Ca2Cu3Ox
Informal Name: Bi:2223
Chemical Family: Bi(Pb)-Sr-Ca-Cu-O
Chemical Class: Oxide
Structure Type: Polycrystalline
Manufacturer: In House
Commercial Name: In House
Production Date:
Lot Number:
Production Form:
Resistivity (normal state) for Bi:2223; [Bi(Pb)-Sr-Ca-Cu-O]
Angle(j,B) (degrees) |
Temperature (K) |
Magnetic Field (T) |
Resistivity (normal state) (mΩ·cm) |
90 |
80 |
0.4 |
0.0 |
90 |
80 |
1.0 |
0.0008 |
90 |
80 |
2.0 |
0.0015 |
90 |
80 |
3.0 |
0.0018 |
90 |
80 |
4.0 |
0.0020 |
90 |
80 |
5.0 |
0.0021 |
90 |
91 |
0.1 |
0.0 |
90 |
91 |
0.5 |
0.0011 |
90 |
91 |
1.0 |
0.0017 |
90 |
91 |
2.0 |
0.0022 |
90 |
91 |
3.0 |
0.0026 |
90 |
91 |
4.0 |
0.0029 |
90 |
91 |
5.0 |
0.0031 |
90 |
101 |
0.0 |
0.0003 |
90 |
101 |
0.2 |
0.0018 |
90 |
101 |
1.0 |
0.0025 |
90 |
101 |
2.0 |
0.0033 |
90 |
101 |
3.0 |
0.0037 |
90 |
101 |
4.0 |
0.0041 |
90 |
101 |
5.0 |
0.0043 |
90 |
106 |
0.0 |
0.0011 |
90 |
106 |
0.3 |
0.0024 |
90 |
106 |
1.0 |
0.0033 |
90 |
106 |
2.0 |
0.0041 |
90 |
106 |
3.0 |
0.0048 |
90 |
106 |
4.0 |
0.0051 |
90 |
106 |
5.0 |
0.0054 |
90 |
108 |
0.0 |
0.0012 |
90 |
108 |
0.2 |
0.0029 |
90 |
108 |
1.0 |
0.0040 |
90 |
108 |
2.0 |
0.0050 |
90 |
108 |
3.0 |
0.0056 |
90 |
108 |
4.0 |
0.0060 |
90 |
108 |
5.0 |
0.0063 |
90 |
111 |
0.0 |
0.0034 |
90 |
111 |
0.3 |
0.0052 |
90 |
111 |
1.0 |
0.0059 |
90 |
111 |
2.0 |
0.0065 |
90 |
111 |
3.0 |
0.0070 |
90 |
111 |
4.0 |
0.0074 |
90 |
111 |
5.0 |
0.0076 |
90 |
112 |
0.0 |
0.0073 |
90 |
112 |
1.0 |
0.0079 |
90 |
112 |
2.0 |
0.0082 |
90 |
112 |
3.0 |
0.0084 |
90 |
112 |
4.0 |
0.0086 |
90 |
112 |
5.0 |
0.0088 |
0 |
93 |
0.1 |
0.0 |
0 |
93 |
0.5 |
0.0012 |
0 |
93 |
1.0 |
0.0017 |
0 |
93 |
2.0 |
0.0021 |
0 |
93 |
3.0 |
0.0024 |
0 |
93 |
4.0 |
0.0025 |
0 |
93 |
5.0 |
0.0027 |
0 |
103 |
0.0 |
0.0006 |
0 |
103 |
0.4 |
0.0022 |
0 |
103 |
1.0 |
0.0027 |
0 |
103 |
2.0 |
0.0032 |
0 |
103 |
3.0 |
0.0034 |
0 |
103 |
4.0 |
0.0037 |
0 |
103 |
5.0 |
0.0039 |
0 |
108 |
0.0 |
0.0014 |
0 |
108 |
0.5 |
0.0030 |
0 |
108 |
1.0 |
0.0035 |
0 |
108 |
2.0 |
0.0042 |
0 |
108 |
3.0 |
0.0047 |
0 |
108 |
4.0 |
0.0049 |
0 |
108 |
5.0 |
0.0053 |
0 |
110 |
0.0 |
0.0022 |
0 |
110 |
0.3 |
0.0039 |
0 |
110 |
1.0 |
0.0046 |
0 |
110 |
2.0 |
0.0052 |
0 |
110 |
3.0 |
0.0057 |
0 |
110 |
4.0 |
0.0060 |
0 |
110 |
5.0 |
0.0063 |
0 |
112 |
0.0 |
0.0060 |
0 |
112 |
1.0 |
0.0067 |
0 |
112 |
2.0 |
0.0071 |
0 |
112 |
3.0 |
0.0073 |
0 |
112 |
4.0 |
0.0075 |
0 |
112 |
5.0 |
0.0077 |
Measurement Method: Unknown resistivity method
Cautions: Unevaluated Data
No measurement details were noted.
Digitized data were obtained from Figure 5(I) of the paper.
Angle(j,B) is the angle between the direction of the applied field (B) and the direction of the current flow (j).
Hall Coefficient for Bi:2223; [Bi(Pb)-Sr-Ca-Cu-O]
Magnetic Field (T) |
Temperature (K) |
Hall Coefficient (mm3 /C) |
5 |
74 |
0.3 |
5 |
84 |
2.0 |
5 |
94 |
3.7 |
5 |
99 |
3.7 |
5 |
105 |
3.2 |
5 |
111 |
5.0 |
5 |
114 |
7.0 |
5 |
117 |
7.7 |
2.5 |
74 |
0.1 |
2.5 |
84 |
0.8 |
2.5 |
94 |
2.4 |
2.5 |
102 |
1.7 |
2.5 |
107 |
0.0 |
2.5 |
112 |
3.4 |
2.5 |
117 |
7.4 |
1 |
74 |
- 0.1 |
1 |
84 |
0.0 |
1 |
89 |
0.5 |
1 |
94 |
1.0 |
1 |
99 |
0.9 |
1 |
107 |
- 4.4 |
1 |
110 |
- 4.5 |
1 |
113 |
1.4 |
1 |
115 |
6.0 |
1 |
117 |
7.2 |
0.5 |
74 |
0.1 |
0.5 |
84 |
0.0 |
0.5 |
94 |
0.5 |
0.5 |
99 |
0.2 |
0.5 |
106 |
- 4.7 |
0.5 |
109 |
- 7.8 |
0.5 |
110 |
- 8.8 |
0.5 |
112 |
- 4.2 |
0.5 |
113 |
- 0.1 |
0.5 |
114 |
3.3 |
0.5 |
115 |
5.8 |
0.5 |
117 |
7.0 |
0.05 |
89 |
- 0.4 |
0.05 |
94 |
- 0.2 |
0.05 |
99 |
- 0.5 |
0.05 |
105 |
- 4.9 |
0.05 |
107 |
- 9.6 |
0.05 |
110 |
-12.8 |
0.05 |
111 |
-14.2 |
0.05 |
112 |
- 9.1 |
0.05 |
113 |
- 2.5 |
0.05 |
115 |
3.3 |
0.05 |
116 |
5.8 |
0.05 |
117 |
7.0 |
Measurement Method: Hall method
The authors cite M. Galffy et al., Solid State Commun., Vol. 68, 929 (1988), and summarize the procedure as follows. "Measurements of the Hall effect... as a function of temperature and magnetic field have been carried out using standard experimental techniques... The current density in these measurements was of the order of 0.5 A/cm
2."
Cautions: Evaluated Data
Digitized data were obtained from Figure 10(I) of the paper.
Thermoelectric Power for Bi:2223; [Bi(Pb)-Sr-Ca-Cu-O]
Angle (ΔT, B) (degrees) |
Magnetic Field (T) |
Temperature (K) |
Thermoelectric Power (µV/K) |
90 |
0 |
81 |
0.0 |
90 |
0 |
44 |
0.0 |
90 |
0 |
32 |
0.0 |
90 |
0 |
110 |
1.3 |
90 |
0 |
112 |
3.8 |
90 |
0 |
114 |
6.4 |
90 |
0 |
115 |
7.4 |
90 |
0.5 |
81 |
0.0 |
90 |
0.5 |
91 |
0.1 |
90 |
0.5 |
101 |
0.7 |
90 |
0.5 |
105 |
0.9 |
90 |
0.5 |
111 |
3.0 |
90 |
0.5 |
112 |
4.5 |
90 |
0.5 |
115 |
7.4 |
90 |
1 |
76 |
0.0 |
90 |
1 |
86 |
0.2 |
90 |
1 |
96 |
0.8 |
90 |
1 |
106 |
1.5 |
90 |
1 |
110 |
3.7 |
90 |
1 |
112 |
5.0 |
90 |
1 |
115 |
7.5 |
90 |
2.5 |
71 |
0.1 |
90 |
2.5 |
76 |
0.2 |
90 |
2.5 |
91 |
1.4 |
90 |
2.5 |
105 |
2.7 |
90 |
2.5 |
111 |
4.9 |
90 |
2.5 |
115 |
7.5 |
90 |
5 |
71 |
0.4 |
90 |
5 |
86 |
1.7 |
90 |
5 |
95 |
2.9 |
90 |
5 |
106 |
4.1 |
90 |
5 |
112 |
6.8 |
90 |
5 |
115 |
7.7 |
0 |
0 |
70 |
0.0 |
0 |
0 |
110 |
0.3 |
0 |
0 |
112 |
3.8 |
0 |
0 |
114 |
6.4 |
0 |
0 |
115 |
7.5 |
0 |
0.5 |
86 |
0.0 |
0 |
0.5 |
98 |
0.2 |
0 |
0.5 |
106 |
0.4 |
0 |
0.5 |
110 |
1.4 |
0 |
0.5 |
111 |
2.8 |
0 |
0.5 |
115 |
7.5 |
0 |
1 |
85 |
0.1 |
0 |
1 |
101 |
0.6 |
0 |
1 |
108 |
1.3 |
0 |
1 |
111 |
4.0 |
0 |
1 |
115 |
7.6 |
0 |
2.5 |
76 |
0.0 |
0 |
2.5 |
93 |
0.7 |
0 |
2.5 |
105 |
1.7 |
0 |
2.5 |
111 |
4.0 |
0 |
2.5 |
115 |
7.5 |
0 |
5 |
71 |
0.0 |
0 |
5 |
85 |
0.8 |
0 |
5 |
103 |
2.2 |
0 |
5 |
110 |
4.0 |
0 |
5 |
115 |
7.6 |
Measurement Method: Thermopower method
Thermopower was "measured as a function of magnetic field (swept at about 0.5 T/min) at fixed temperatures stabilized within about 50 mK with an imposed temperature gradient of about 0.5 K to 1 K... The temperature gradient, built up by a small heater (manganin; dp/dB=0) using a constant heating current, was measured with calibrated Pt-resistors mounted to the ends of the sample... The thermomagnetic voltages were measured using calibrated Cu wires with an accuracy of about 50 nV."
Cautions: Evaluated Data
Digitized data were obtained from Figure 16(I) of the paper.
Material Specification for Tl:2223; [Tl-Ba-Ca-Cu-O]
Process: Solid State Reaction
Notes: The authors cite W. Schnelle et al., Physica C, Vol. 161, 123 (1989) and T. Zetterer et al., Phys. Rev. B, Vol. 41, 9499 (1990), and summarize the procedures as follows. "The measurements have been carried out on one Bi-2223 polycrystal and on two Tl-2223 polycrystals."
Formula: Tl2Ba2Ca2Cu3Ox
Informal Name: Tl:2223
Chemical Family: Tl-Ba-Ca-Cu-O
Chemical Class: Oxide
Structure Type: Polycrystalline
Manufacturer: In House
Commercial Name: In House
Production Date:
Lot Number:
Production Form:
Resistivity (normal state) for Tl:2223; [Tl-Ba-Ca-Cu-O]
Angle(j,B) (degrees) |
Temperature (K) |
Magnetic Field (T) |
Resistivity (normal state) (mΩ·cm) |
90 |
80.9 |
1.3 |
0.00 |
90 |
80.9 |
2.0 |
0.0001 |
90 |
80.9 |
3.0 |
0.0002 |
90 |
80.9 |
4.0 |
0.0027 |
90 |
80.9 |
5.0 |
0.0004 |
90 |
90.4 |
0.6 |
0.00 |
90 |
90.4 |
1.0 |
0.0001 |
90 |
90.4 |
2.0 |
0.0003 |
90 |
90.4 |
3.0 |
0.0005 |
90 |
90.4 |
4.0 |
0.0006 |
90 |
90.4 |
5.0 |
0.0006 |
90 |
99.6 |
0.2 |
0.00 |
90 |
99.6 |
1.0 |
0.0004 |
90 |
99.6 |
2.0 |
0.0006 |
90 |
99.6 |
3.1 |
0.0008 |
90 |
99.6 |
4.0 |
0.0009 |
90 |
99.6 |
5.0 |
0.0010 |
90 |
111.4 |
0.2 |
0.0006 |
90 |
111.4 |
1.0 |
0.0011 |
90 |
111.4 |
2.1 |
0.0015 |
90 |
111.4 |
3.1 |
0.0017 |
90 |
111.4 |
4.0 |
0.0020 |
90 |
111.4 |
5.0 |
0.0022 |
90 |
115.9 |
0.0 |
0.0006 |
90 |
115.9 |
0.3 |
0.0012 |
90 |
115.9 |
1.1 |
0.0019 |
90 |
115.9 |
2.0 |
0.0025 |
90 |
115.9 |
3.1 |
0.0028 |
90 |
115.9 |
4.0 |
0.0032 |
90 |
115.9 |
5.0 |
0.0033 |
0 |
92 |
0.5 |
0.00 |
0 |
92 |
1.0 |
0.0001 |
0 |
92 |
2.0 |
0.0003 |
0 |
92 |
3.0 |
0.0005 |
0 |
92 |
4.0 |
0.0006 |
0 |
92 |
5.0 |
0.0006 |
0 |
107.7 |
0.1 |
0.00 |
0 |
107.7 |
0.4 |
0.0006 |
0 |
107.7 |
1.0 |
0.0008 |
0 |
107.7 |
2.0 |
0.0011 |
0 |
107.7 |
3.0 |
0.0013 |
0 |
107.7 |
4.0 |
0.0015 |
0 |
107.7 |
5.0 |
0.0017 |
0 |
113.2 |
0.0 |
0.0001 |
0 |
113.2 |
0.3 |
0.0007 |
0 |
113.2 |
1.0 |
0.0011 |
0 |
113.2 |
2.0 |
0.0015 |
0 |
113.2 |
3.0 |
0.0018 |
0 |
113.2 |
4.0 |
0.0021 |
0 |
113.2 |
5.0 |
0.0023 |
0 |
116 |
0.0 |
0.0003 |
0 |
116 |
0.2 |
0.0010 |
0 |
116 |
1.0 |
0.0019 |
0 |
116 |
2.0 |
0.0023 |
0 |
116 |
3.0 |
0.0027 |
0 |
116 |
4.0 |
0.0031 |
0 |
116 |
5.0 |
0.0033 |
0 |
118.9 |
0.0 |
0.0030 |
0 |
118.9 |
1.0 |
0.0036 |
0 |
118.9 |
2.0 |
0.0040 |
0 |
118.9 |
3.0 |
0.0042 |
0 |
118.9 |
4.0 |
0.0044 |
0 |
118.9 |
5.0 |
0.0046 |
0 |
122.2 |
0.0 |
0.0057 |
0 |
122.2 |
1.0 |
0.0058 |
0 |
122.2 |
2.0 |
0.0058 |
0 |
122.2 |
3.0 |
0.0058 |
0 |
122.2 |
4.0 |
0.0059 |
0 |
122.2 |
5.0 |
0.0059 |
Measurement Method: Unknown resistivity method
Cautions: Unevaluated Data
Angle(j,B) is the angle between the directions of the current flow and the applied magnetic field. Angle(j,B) = 0 means the current flows in a direction parallel to the applied field. For angle(j,B) = 90, the current is perpendicular to the field.
Digitized data were obtained from Figure 5(II) of the paper.
Hall Coefficient for Tl:2223; [Tl-Ba-Ca-Cu-O]
Magnetic Field (T) |
Temperature (K) |
Hall Coefficient (mm3 /C) |
5 |
70 |
0.1 |
5 |
82 |
0.1 |
5 |
98 |
0.7 |
5 |
103 |
1.1 |
5 |
108 |
0.9 |
5 |
112 |
0.1 |
5 |
117 |
1.5 |
5 |
121 |
2.6 |
5 |
130 |
3.9 |
3 |
71 |
0.1 |
3 |
82 |
0.0 |
3 |
88 |
0.1 |
3 |
98 |
0.4 |
3 |
109 |
0.0 |
3 |
113 |
-0.5 |
3 |
119 |
0.9 |
3 |
122 |
2.2 |
3 |
130 |
3.9 |
2 |
71 |
0.0 |
2 |
83 |
0.0 |
2 |
94 |
0.1 |
2 |
99 |
0.2 |
2 |
104 |
0.1 |
2 |
110 |
-0.6 |
2 |
115 |
-1.1 |
2 |
118 |
-0.2 |
2 |
121 |
1.9 |
2 |
130 |
3.9 |
1 |
71 |
0.1 |
1 |
88 |
0.0 |
1 |
97 |
0.1 |
1 |
109 |
-1.2 |
1 |
115 |
-2.5 |
1 |
117 |
-1.8 |
1 |
120 |
-0.3 |
1 |
121 |
1.4 |
1 |
130 |
3.9 |
0.5 |
70 |
0.0 |
0.5 |
88 |
-0.2 |
0.5 |
98 |
0.0 |
0.5 |
107 |
-1.0 |
0.5 |
111 |
-2.2 |
0.5 |
116 |
-3.6 |
0.5 |
119 |
-2.1 |
0.5 |
121 |
0.9 |
0.5 |
130 |
3.9 |
Measurement Method: Hall method
The authors cite M. Galffy et al., Solid State Commun., Vol. 68, 929 (1988), and summarize the procedure as follows. "Measurements of the Hall effect... as a function of temperature and magnetic field have been carried out using standard experimental techniques... The current density in these measurements was of the order of 0.5 A/cm
2."
Cautions: Evaluated Data
Digitized data were obtained from Figure 10(II) of the paper.
Thermoelectric Power for Tl:2223; [Tl-Ba-Ca-Cu-O]
Angle (ΔT, B) (degrees) |
Magnetic Field (T) |
Temperature (K) |
Thermoelectric Power (µV/K) |
90 |
5 |
84 |
1.3 |
90 |
5 |
109 |
4.1 |
90 |
5 |
120 |
6.5 |
90 |
3 |
91 |
1.1 |
90 |
3 |
120 |
6.2 |
90 |
1 |
82 |
0.3 |
90 |
1 |
106 |
1.8 |
90 |
1 |
111 |
3.8 |
90 |
1 |
120 |
6.2 |
90 |
0.2 |
91 |
0.0 |
90 |
0.2 |
105 |
1.4 |
90 |
0.2 |
120 |
6.1 |
90 |
0 |
91 |
0.0 |
90 |
0 |
105 |
0.0 |
90 |
0 |
112 |
3.8 |
90 |
0 |
122 |
6.2 |
0 |
5 |
93 |
0.4 |
0 |
5 |
108 |
1.4 |
0 |
5 |
113 |
1.7 |
0 |
5 |
119 |
4.3 |
0 |
5 |
122 |
6.0 |
0 |
4 |
92 |
0.3 |
0 |
4 |
100 |
0.6 |
0 |
4 |
113 |
1.1 |
0 |
4 |
119 |
4.0 |
0 |
4 |
122 |
5.9 |
0 |
3 |
92 |
0.2 |
0 |
3 |
100 |
0.5 |
0 |
3 |
113 |
1.0 |
0 |
3 |
119 |
3.7 |
0 |
3 |
122 |
5.8 |
0 |
2 |
93 |
0.2 |
0 |
2 |
108 |
0.4 |
0 |
2 |
113 |
0.6 |
0 |
2 |
119 |
3.7 |
0 |
2 |
122 |
5.4 |
0 |
2 |
123 |
5.9 |
0 |
1 |
92 |
0.0 |
0 |
1 |
108 |
0.3 |
0 |
1 |
113 |
0.4 |
0 |
1 |
119 |
3.3 |
0 |
1 |
122 |
5.3 |
0 |
0 |
92 |
0.0 |
0 |
0 |
94 |
0.0 |
0 |
0 |
119 |
2.9 |
0 |
0 |
122 |
5.4 |
Measurement Method: Thermopower method
Thermopower was "measured as a function of magnetic field (swept at about 0.5 T/min) at fixed temperatures stabilized within about 50 mK with an imposed temperature gradient of about 0.5 K to 1 K... The temperature gradient, built up by a small heater (manganin; dp/dB=0) using a constant heating current, was measured with calibrated Pt-resistors mounted to the ends of the sample... The thermomagnetic voltages were measured using calibrated Cu wires with an accuracy of about 50 nV."
Cautions: Evaluated Data
Angle(ΔT,B) is the angle between the directions of the temperature gradient ΔT and the applied field B. Angle(ΔT,B) = 0 means the direction of the gradient is parallel to the applied field. For angle(ΔT,B) = 90°, the gradient is perpendicular to the field.
Digitized data were obtained from Figure 16(II) of the paper.