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Journal articles on the topic 'BSCCO-2212'

Author: Grafiati

Published: 23 September 2022

Last updated: 28 January 2023

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1

Rahmah, Karlina, Suprihatin Suprihatin, and Pulung Karo Karo. "Pengaruh Variasi Waktu Sintering Terhadap Pertumbuhan Fase Bahan Superkonduktor BSCCO-2212 dengan Kadar Ca=1,10 Menggunakan Metode Pencampuran Basah." Journal of Energy, Material, and Instrumentation Technology 1, no. 1 (May 31, 2020): 7–11. http://dx.doi.org/10.23960/jemit.v1i1.5.

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This research was conducted to determine the effect of sintering time on the formation of the superconducting phase BSCCO-2212 by calculating the level of purity of the phases formed and looking at the microstructure. The variation of sintering time was 10, 20, 30 and 40 hours using the wet mixing method. The sample was calcinated with 800 °C for 10 hours and sintered with 830 °C. The XRD’s characterization result shows a decrease in phase purity with increasing the sintering time. The relative high volume fraction of the BSCCO-2212/ts10 sample is 90,48% while, the lowest volume fraction of BSCCO-2212/tc40 is 50,74%. The relative high orientation degree of BSCCO-2212/ts20 is 18,47% and the lowest orientation degree of BSCCO-2212/ts10 is 8,4%. The SEM’s characterization result shows of all samples have been oriented and have relatively little space between slabs (voids).

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2

Karo, Pulung Karo, Risky Putra Ramadhan, Suprihatin Suprihatin, and Yanti Yulianti. "Analisis Pertumbuhan Fase Superkonduktor BSCCO-2212 dan BPSCCO-2212 Akibat Variasi Suhu Sintering Menggunakan Metode Pencampuran Basah." Journal of Energy, Material, and Instrumentation Technology 2, no. 4 (November 30, 2021): 86–95. http://dx.doi.org/10.23960/jemit.v2i4.77.

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The research was conducted to determine the effect of sintering temperature on the level of purity of the superconducting phase BSCCO-2212 and BPSCCO-2212 using the wet mixing method. Sintering was carried out for 20 hours with variations in sintering temperature: 825, 830, 835 and 840°C. XRD results showed that the phase purity level increased until it reached the optimum point at 835°C sintering temperature and then decreased at 840°C. The highest volume fraction of the BSCCO-2212 sample was obtained at a sintering temperature of 835°C at 71.09% and the highest degree of orientation was obtained at a sintering temperature of 830°C at 26.44%. In the BPSCCO-2212 sample, the highest volume fraction was obtained at a sintering temperature of 835°C at 52.59% and the highest degree of orientation at a sintering temperature of 830°C at 43.49%. The results of the comparison of BSCCO-2212 and BPSCCO-2212 samples showed that the BPSCCO-2212 sample had a higher level of phase purity than BSCCO-2212.

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3

Feng, Yi, D. C. Larbalestier, S. E. Babcock, and J. B. VanderSande. "Phase composition and local grain alignment at the Ag/superconductor interface in Ag-sheathed Bi-Sr-Ca-Cu-O tapes." Proceedings, annual meeting, Electron Microscopy Society of America 51 (August 1, 1993): 1140–41. http://dx.doi.org/10.1017/s0424820100151532.

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Texturing of the superconductor phase and proximity to a sourse of silver appear to be crucial to the development of high critical current density tapes of the Bi-Sr-Ca-Cu-O (BSCCO) high-temperature superconductors, yet relatively little is understood about the mechanism(s) by which the [001] texture develops and the complex role that the silver sheath material plays. We have studied the phase composition, alignment, and bonding at the Ag/BSCCO interface for silver-sheathed tapes of both the 2212 and 2223 phases that have been processed under fundamentally different conditions. High-resolution TEM imaging revealed details of the interface that give insight into these important questions.Ag-sheathed BSCCO tapes with cation compositions Bi2Sr2CaCu2Ox (2212) and Bi1.8Pb0.4Sr2.0Ca2.2Cu3Ox (2223) were prepared by standard powder-in-tube methods. 2212 sample A was heat-treated at 920°C for 15 minutes to melt the superconductor core, then cooled at 240°C/h from 920°C to 840°C and annealed at 840°C for 70 hours.

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4

Barzi, E., V. Lombardo, D. Turrioni, F. J. Baca, and T. G. Holesinger. "BSCCO-2212 Wire and Cable Studies." IEEE Transactions on Applied Superconductivity 21, no. 3 (June 2011): 2335–39. http://dx.doi.org/10.1109/tasc.2011.2106106.

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5

Timofeev, V. N., and I. G. Gorlova. "Superstructure defects in BSCCO (2212) whiskers." Physica C: Superconductivity 282-287 (August 1997): 875–76. http://dx.doi.org/10.1016/s0921-4534(97)00527-3.

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6

Gorlova, I. G., S. G. Zybtsev, V. Ya Pokrovskii, and V. N. Timofeev. "Fluctuation conductivity of BSCCO (2212) whiskers." Physica C: Superconductivity 282-287 (August 1997): 1533–34. http://dx.doi.org/10.1016/s0921-4534(97)00871-x.

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7

Dhalle, M., M. N. Cuthbert, J. Thomas, G. K. Perkins, A. D. Caplin, M. Yang, and M. Gorringe. "Dissipation in BSCCO/Ag 2212 ribbons." IEEE Transactions on Appiled Superconductivity 5, no. 2 (June 1995): 1317–20. http://dx.doi.org/10.1109/77.402805.

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8

Wang, Jyh-Lih, I.-Fei Tsu, X. Y. Cai, R. J. Kelley, M. D. Vaudin, S. E. Babcock, and D. C. Larbalestier. "Electromagnetic and microstructural investigations of a naturally grown 8° [001] tilt bicrystal of Bi2Sr2CaCu208 + x." Journal of Materials Research 11, no. 4 (April 1996): 868–77. http://dx.doi.org/10.1557/jmr.1996.0108.

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Electromagnetic characterization and high resolution transmission electron microscopy have been conducted on the same 8° [001] symmetrical (010) tilt boundary in a naturally grown, bulk-scale bicrystal of Bi2Sr2CaCu2O8 + x (BSCCO-2212). The resistive transition showed excess resistance above and below Tc, suggesting some weak coupling at the boundary, but the inter- and intragranular voltage-current characteristics, irreversibility fields, and critical current density (Jc) values were very similar and characteristic of strongly coupled grains and grain boundary. The misorientation was accommodated by a set of partial dislocations with the Frank spacing of 1.9 nm. The dislocation cores appeared to be separated by relatively undistorted regions of crystal. The Jc, values at 25 K exceeded 103 A/cm2 in fields of several tesla, more than two orders of magnitude larger than that found earlier in [001] twist boundaries of BSCCO-2212. This result is consistent with the view that low angle [001] till boundaries play an important role for current transport in polycrystalline BSCCO tapes.

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9

POP, M., GH BORODI, I. Gr DEAC, and S. SIMON. "Gd SUBSTITUTION EFFECT ON THE FORMATION OF Bi-BASED SUPERCONDUCTING GLASS CERAMICS." Modern Physics Letters B 14, no. 02 (January 20, 2000): 59–63. http://dx.doi.org/10.1142/s0217984900000100.

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The effect of calcium substitution by gadolinium on the superconducting phases formation in BSCCO-type compounds is studied by X-ray diffraction and ac susceptibility measurements on the undoped and Gd-doped Bi1.8Pb0.2Sr2CaCu2Oz and Bi1.8Pb0.2Sr2Ca2Cu3Oz systems. The addition of gadolinium to the samples favors the 2212 phase formation in both 2212 and 2223 starting compositions. It is suggested that a correlation exists between the stabilization effect of gadolinium on the 2212 phase formation and the Gd3+ coordination in oxide compounds.

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10

Thomas, P. J., J. C. Fenton, G. Yang, and C. E. Gough. "Intrinsic c-axis transport in 2212-BSCCO." Physica C: Superconductivity 341-348 (November 2000): 1547–50. http://dx.doi.org/10.1016/s0921-4534(00)01330-7.

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11

Dhallé, M., J. Thomas, M. N. Cuthbert, M. Yang, M. J. Goringe, and A. D. Caplin. "Critical currents in BSCCO/Ag 2212 ribbons." Physica C: Superconductivity 235-240 (December 1994): 3031–32. http://dx.doi.org/10.1016/0921-4534(94)91042-1.

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12

Yang, Ming, R. Jenkins, H. Jones, MJ Goringe, and CRM Grovenor. "Prototype BSCCO 2212 coils: Processing and properties." Physica C: Superconductivity 235-240 (December 1994): 3435–36. http://dx.doi.org/10.1016/0921-4534(94)91244-0.

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13

Briant, C. L., E. L. Hall, K. W. Lay, and I. E. Tkaczyk. "Microstructural evolution of the BSCCO-2223 during powder-in-tube processing." Journal of Materials Research 9, no. 11 (November 1994): 2789–808. http://dx.doi.org/10.1557/jmr.1994.2789.

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This paper reports a study of the microstructural changes that occur when BSCCO powder is processed by the powder-in-tube method. In this study the initial powder consisted of the 2212 phase plus second phases containing Ca, Cu, Sr, and Pb. When the material was drawn, there was no alignment of the 2212 phase and the second phase particles remained large and blocky. Rolling induced a small amount of alignment into the 2212 phase so that its c-axis was perpendicular to the rolling direction. Rolling also caused the second phase particles to become flatter. When these rolled samples were annealed at 828 °C, the core sintered into a platelet structure, and there was an increase in the amount of aligned material, particularly after annealing treatments of 16 and 32 h. After 8 h at 828 °C, the 2212 variant of the superconducting phase began to transform to the 2223 variant. Pressing this structure improved the alignment, and annealing after pressing allowed further conversion of the 2212 phase to the 2223 phase and apparently removed the strains produced by the pressing. Repeated pressing improved the alignment and repeated annealing allowed more conversion of 2212 to 2223. Both the improved alignment, produced by pressing, and the transformation of 2212 to 2223, produced by the anneals, caused the superconducting properties of the material to improve.

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14

Kasuga, Toshihiro, Masayasu Ono, Kenji Tsuji, Yoshihiro Abe, Koichi Nakamura, and Eikichi Inukai. "Formation of Bi-2212 superconducting whiskers from melt-quenched BSCCO containing alumina." Journal of Materials Research 9, no. 5 (May 1994): 1098–103. http://dx.doi.org/10.1557/jmr.1994.1098.

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Bi–Sr–Ca–Cu–O (BSCCO) superconducting whiskers (2212 phase) were prepared by heating in air the compacted specimens of the mixtures of melt-quenched Bi2SryCa2Cu4Al1Ox powders and alumina powders. Formation of the whiskers depends on the composition and the applied pressure of the compacts. The optimum composition of the melt-quenched products for preparing the long whiskers is Bi2Sr2Ca2Cu4Al1Ox. Superconducting whiskers <1 mm in length (2212 phase) containing an excess amount of copper were grown numerously from the specimen compacted at 20 MPa; long whiskers (2212 phase) of 1–5 mm in length were obtained from that compacted at 180 MPa. These whiskers showed diamagnetic signals below Tc ≃ 80 K.

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15

Sekkina, Morsy M. A., M. El-Hofy, Khaled M. Elsabawy, and M. Bediwy. "BSCCO 2212 Defective Tellurium Ions on Bi-Site." Defect and Diffusion Forum 319-320 (October 2011): 161–66. http://dx.doi.org/10.4028/www.scientific.net/ddf.319-320.161.

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BSCCO 2212 superconducting samples, doped Tellurium, with the chemical formula Bi2-xTexSr2CaCu2O8, were prepared by the conventional solid state reaction technique. The prepared samples were studied utilizing XRD, DC-electrical conductivity and SEM. XRD spectra indicated that 2212 with tetragonal structure is the major phase, whereas Bi-2201 and CaTeO4 are minor phases. At higher Te-additions x, traces from some other semi conducting phases were detected. The critical transition temperature Tcoffset was found to decrease non-linearly with x, which attributed to the hole filling caused by the liberated electrons of Te4+ ions. For x–values in the range 0.1 ≤ x ≤ 0.4, the steepness of (ρ vs T) relationship increases abruptly around 150 K; this was attributed to change in the oxygen vacancy feature (phase-like transition). SEM photographs revealed that as Te-content increases the compactness of the surface and the connectivity of the grains decreases, while pores and voids increase as a result of decreasing the amount of Bi and presence of multiple-phases in the sample.

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16

Marken, K. R., W. Dai, L. Cowey, S. Ting, and S. Hong. "Progress in BSCCO-2212/silver composite tape conductors." IEEE Transactions on Appiled Superconductivity 7, no. 2 (June 1997): 2211–14. http://dx.doi.org/10.1109/77.621033.

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17

Iavarone, M., Y. De Wilde, P. Guptasarma, D. G. Hinks, G. W. Crabtree, and P. C. Canfield. "STM investigation of BSCCO 2212 and borocarbide materials." Journal of Physics and Chemistry of Solids 59, no. 10-12 (October 1998): 2030–33. http://dx.doi.org/10.1016/s0022-3697(98)00171-1.

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18

Timofeev, V. N., and I. G. Gorlova. "Growth defects in BSCCO (2212) single crystal whiskers." Physica C: Superconductivity 309, no. 1-2 (December 1998): 113–19. http://dx.doi.org/10.1016/s0921-4534(98)00562-0.

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19

Cabral, Leonardo R. E., Clécio C. de Souza Silva, Ernst Helmut Brandt, and J. Albino Aguiar. "Magnetization curves and geometric barrier in BSCCO-2212." Physica C: Superconductivity 369, no. 1-4 (March 2002): 196–99. http://dx.doi.org/10.1016/s0921-4534(01)01241-2.

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20

Tonomura, Akira. "Vortex dynamics in BSCCO(2212) with Lorentz Microscopy." Physica C: Superconductivity 235-240 (December 1994): 33–36. http://dx.doi.org/10.1016/0921-4534(94)91307-2.

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21

Elschner, S., J. Bock, G. Brommer, and P. F. Herrmann. "High currents in MCP BSCCO 2212 bulk material." IEEE Transactions on Magnetics 32, no. 4 (July 1996): 2724–27. http://dx.doi.org/10.1109/20.511437.

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22

Lim, H. J., J. G. Byrne, M. S. Chae, and M. B. Maple. "Processing of BSCCO 2212 and 2223 Superconductor Compounds." Materials and Manufacturing Processes 12, no. 2 (March 1997): 261–74. http://dx.doi.org/10.1080/10426919708935140.

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23

Yavuz, M., K. K. Uprety, G. Subramanian, and P. Paliwal. "Preparation and characterization of BSCCO 2212 thin films." IEEE Transactions on Appiled Superconductivity 13, no. 2 (June 2003): 3295–97. http://dx.doi.org/10.1109/tasc.2003.812293.

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24

Marken, K. R., H. Miao, M. Meinesz, B. Czabaj, and S. Hong. "BSCCO-2212 conductor development at oxford superconducting technology." IEEE Transactions on Appiled Superconductivity 13, no. 2 (June 2003): 3335–38. http://dx.doi.org/10.1109/tasc.2003.812307.

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25

Badica, P., and K. Togano. "Growth of superconducting and non-superconducting whiskers in the Bi-Sr-Ca-Cu-O (BSCCO) system." Journal of Materials Research 20, no. 12 (December 1, 2005): 3358–67. http://dx.doi.org/10.1557/jmr.2005.0413.

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Growth of such non-superconducting whiskers [Sr2.24Ca0.4Al2Ox, (Ca0.8–0.85Sr0.15–0.1)2CuO3,CuO, or Bi2.44Sr2Ca1.3–2Cu6.9–9.95Al0.35–0.46Ox (Cu-rich whiskers)] formed during the growth of Bi-2212 superconducting whiskers from powder or glassy substrates, is discussed. These whiskers are likely to grow from the bottom end, and there is a tight relationship with the growth of the Bi-2212 whiskers. A general reaction-path model for the whisker growth in the BSCCO system, independent of the type of the catalytic impurity and substrate, is proposed. When whiskers are grown under magnetic fields, up to 10 T, changes in the whisker size, aspect ratio, and morphology are observed.

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26

Pfuch, A., F. Schmidl, A. Wiese, L. Dörrer, U. Hübner, and P. Seidel. "Several kinds of Josephson junctions based on BSCCO-2212 and TBCCO-2212 thin films." Cryogenics 37, no. 10 (January 1997): 685–89. http://dx.doi.org/10.1016/s0011-2275(97)00061-1.

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27

Li, Ming Ya, Xi Wei Qi, Zhi Yong Yu, and Zheng He Han. "The Stability Range of Lead Oxide Compounds in Bi-System High Temperature Superconducting Materials." Key Engineering Materials 336-338 (April 2007): 719–22. http://dx.doi.org/10.4028/www.scientific.net/kem.336-338.719.

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The stability range of lead oxide compounds Pb3Sr2.5Bi0.5Ca2CuOy (3321) phase in Bi-system high temperature superconducting materials has been investigated. In this study (Bi,Pb)2Sr2Ca2Cu3Ox (BSCCO) powder was heat treated in different oxygen partial pressure and different temperature. The formation and the relative volume fraction of the 3321 phase were determined by X-ray diffraction. The microstructure of the quenched pellets was observed using SEM. Experimental results show that the stability range of the 3321 phase depends on both the temperature and oxygen partial pressure. A three dimensional plot of relative 3321 phase formation was obtained for BSCCO powder in which the main phase is (Bi,Pb)-2212 at different temperature and oxygen partial pressure.

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28

Lehndorff, B., H. Piel, M. Hortig, G. W. Schulz, and R. Theisejans. "Microstructural analysis of BSCCO-2212 wires for magnet application." IEEE Transactions on Appiled Superconductivity 7, no. 2 (June 1997): 1687–90. http://dx.doi.org/10.1109/77.620903.

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29

Zavaritsky, Vladimir N. "Josephson vortex lattice transformations in BSCCO-2212 single crystal." Physica Scripta T66 (January 1, 1996): 230–33. http://dx.doi.org/10.1088/0031-8949/1996/t66/042.

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30

Latyshev, Yu I., P. Monceau, and V. N. Pavlenko. "Intrinsic Josephson effects on BSCCO 2212 single crystal whiskers." Physica C: Superconductivity 282-287 (August 1997): 387–90. http://dx.doi.org/10.1016/s0921-4534(97)00282-7.

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31

Zavaritsky, Vladimir N. "Criterion dependence of the irreversibility field in BSCCO-2212." Physica C: Superconductivity and its Applications 282-287 (August 1997): 2167–68. http://dx.doi.org/10.1016/s0921-4534(97)01213-6.

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32

Zavaritsky, Vladimir N. "Anisotropic mixed state transport in BSCCO-2212 single crystal." Physica C: Superconductivity 235-240 (December 1994): 2715–16. http://dx.doi.org/10.1016/0921-4534(94)92578-x.

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33

Keartland, J. "Transport measurements in BSCCO-2212 in high magnetic fields." Physica B: Condensed Matter 284-288 (July 2000): 883–84. http://dx.doi.org/10.1016/s0921-4526(99)02200-0.

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34

Chen, Shu-jan, Sushil Patel, Eiki Narumi, David T. Shaw, Dell St. Julien, and Thomas D. Ketcham. "BSCCO-2212 thick films on a flexible YSZ substrate." Physica C: Superconductivity 218, no. 1-2 (December 1993): 191–96. http://dx.doi.org/10.1016/0921-4534(93)90282-u.

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35

Zavaritsky, Vladimir N., and Wei Yao Liang. "Observation of Josephson vortex lattice transformations in BSCCO-2212." Journal of Low Temperature Physics 105, no. 5-6 (December 1996): 1273–78. http://dx.doi.org/10.1007/bf00753875.

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36

Masterov, V. F., N. M. Shibanova, and K. F. Shtel’makh. "Electron spin resonance in manganese-doped BSCCO (2212) crystals." Technical Physics 42, no. 10 (October 1997): 1234–35. http://dx.doi.org/10.1134/1.1258808.

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37

Suntao Yang, Binjiang Chen, E. E. Hellstrom, E. Stiers, and J. M. Pfotenhauer. "Thermal conductivity and contact conductance of BSCCO-2212 material." IEEE Transactions on Appiled Superconductivity 5, no. 2 (June 1995): 1471–74. http://dx.doi.org/10.1109/77.402844.

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38

Walker, M. S., C. M. Trautwein, L. R. Motowidlo, D. R. Dietderich, and F. A. List. "Practical, coated BSCCO-2212 high T/sub c/ conductors." IEEE Transactions on Appiled Superconductivity 5, no. 2 (June 1995): 1857–59. http://dx.doi.org/10.1109/77.402943.

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39

Wu, K. T., A. K. Fischer, V. A. Maroni, and M. W. Rupich. "Raman microscopy examination of phase evolution in Bi(Pb)–Sr–Ca–Cu–O superconducting ceramics." Journal of Materials Research 12, no. 5 (May 1997): 1195–204. http://dx.doi.org/10.1557/jmr.1997.0168.

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Raman microspectroscopy (RMS) and imaging Raman microscopy (IRM) were used to probe the composition and spatial distribution of chemical phases in Bi(Pb)–Sr–Ca–Cu–O (BSCCO) ceramic superconductor powders and silver-BSCCO composites. The Raman techniques were used to identify various phases, including alkaline earth cuprates, CuO, Bi-2212, Bi-2223, and Pb-containing phases. Changes in the Ca/Sr ratios in (Ca, Sr)2CuO3 phases were distinguished by differences in orientation with respect to polarization of the exciting radiation. Variations were observed in the content and distribution of lead in various phases formed during intermediate stages of the thermal processing of composite conductors. The spatial distribution of the various phases detected in powder and composite conductors was established to a resolution of a few microns by collecting images of the Raman scattering at wavelengths corresponding to the signature peaks of the observed phases. Reference Raman spectra of the major phases observed in the BSCCO system are also reported. The Raman techniques, when combined with complementary techniques, such as x-ray diffraction and electron microscopy, can provide valuable information about the reaction paths and mechanisms of the high temperature BSCCO superconducting ceramics.

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40

Wong-Ng, W., L. P. Cook, F. Jiang, W. Greenwood, U. Balachandran, and M. Lanagan. "Subsolidus phase equilibria of coexisting high-Tc Pb-2223 and 2212 superconductors in the (Bi, Pb)–Sr–Ca–Cu–O system under 7.5% O2." Journal of Materials Research 12, no. 11 (November 1997): 2855–65. http://dx.doi.org/10.1557/jmr.1997.0379.

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The subsolidus phase relationships of the high-Tc 2223 superconductor in the (Bi, Pb)–Sr–Ca–Cu–O (BSCCO) system have been examined at 810–820 °C. All experiments were carried out at ambient pressure in a 7.5% O2 (92.5% Ar) atmosphere. Eleven phases were found to exist in equilibrium with the 2223 phase. These 11 phases include CuO and 10 oxide solid solutions. From among these phases, a total of 48 five-phase combinations including the 2223 and 2212 phases were investigated experimentally, and 16 equilibrium assemblages were found which define a multicomponent compositional space corresponding to the 2223 + 2212 solid-state compatibility region. The subsolidus data form a partial basis for future investigation of the Pb-2223 primary phase field.

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41

Kim, Kyu-Tae, Eui-Cheol Park, Seok-Hern Jang, Jun-Hyung Lim, Jin-Ho Joo, Chan-Joong Kim, Hye-Rim Kim, and Ok-Bae Hyun. "A Study on the Casting Process Variables and Optimum SrSO4Content of the BSCCO(2212) Bulk Superconductor." Journal of the Korean Institute of Electrical and Electronic Material Engineers 19, no. 6 (June 1, 2006): 579–85. http://dx.doi.org/10.4313/jkem.2006.19.6.579.

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42

Ting, S. M., K. R. Marken, L. Cowey, W. Dai, S. Hong, and S. Nelson. "Development of current leads using dip coated BSCCO-2212 tape." IEEE Transactions on Appiled Superconductivity 7, no. 2 (June 1997): 700–702. http://dx.doi.org/10.1109/77.614600.

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43

Gannon, J. J., and K. H. Sandhage. "Solid-state high-oxygen-fugacity processing of BSCCO-2212 superconductors." IEEE Transactions on Appiled Superconductivity 7, no. 2 (June 1997): 1533–36. http://dx.doi.org/10.1109/77.620865.

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44

Le Bars, J., T. Dechambre, P. Regnier, and K. Gagnant. "Development of current leads using electrolytically deposited BSCCO 2212 tapes." IEEE Transactions on Appiled Superconductivity 9, no. 2 (June 1999): 503–6. http://dx.doi.org/10.1109/77.783345.

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45

Ozyuzer, L., N. Miyakawa, J. F. Zasadzinski, Z. Yusof, P. Romano, C. Kendziora, P. Guptasarma, D. G. Hinks, and K. E. Gray. "Simultaneous quasiparticle and Josephson tunneling in BSCCO-2212 break junctions." IEEE Transactions on Appiled Superconductivity 9, no. 2 (June 1999): 2898–901. http://dx.doi.org/10.1109/77.783635.

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46

Moriya, M., T. Sudoh, Y. Koike, K. Usami, T. Kobayashi, and T. Goto. "Anisotropic properties of BSCCO (2212) films deposited on tilted substrates." IEEE Transactions on Appiled Superconductivity 11, no. 1 (March 2001): 2700–2702. http://dx.doi.org/10.1109/77.919619.

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Elschner, S., F. Breuer, A. Wolf, M. Noe, L. Cowey, and J. Bock. "Characterization of BSCCO 2212 bulk material for resistive current limiters." IEEE Transactions on Appiled Superconductivity 11, no. 1 (March 2001): 2507–10. http://dx.doi.org/10.1109/77.920375.

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Barzi, E., V. Lombardo, A. Tollestrup, and D. Turrioni. "Study of Effects of Transverse Deformation in BSCCO-2212 Wires." IEEE Transactions on Applied Superconductivity 21, no. 3 (June 2011): 2808–11. http://dx.doi.org/10.1109/tasc.2011.2106105.

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Gough, C. E., P. J. Thomas, J. C. Fenton, and G. Yang. "Quasiparticle tunnelling and field-dependent critical current in 2212-BSCCO." Physica C: Superconductivity 341-348 (November 2000): 1539–42. http://dx.doi.org/10.1016/s0921-4534(00)01327-7.

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Balestrino, G., A. Crisan, D. V. Livanov, S. I. Manokhin, and E. Milani. "Fluctuation magnetoconductivity of BSCCO-2212 films in parallel magnetic field." Physica C: Superconductivity 355, no. 1-2 (June 2001): 135–39. http://dx.doi.org/10.1016/s0921-4534(00)01771-8.

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