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Journal articles on the topic 'Conductors; Superconductors'

Author: Grafiati

Published: 4 June 2021

Last updated: 1 February 2022

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1

Marchevsky, Maxim. "Quench Detection and Protection for High-Temperature Superconductor Accelerator Magnets." Instruments 5, no. 3 (2021): 27. http://dx.doi.org/10.3390/instruments5030027.

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High-temperature superconductors (HTS) are being increasingly used for magnet applications. One of the known challenges of practical conductors made with high-temperature superconductor materials is a slow normal zone propagation velocity resulting from a large superconducting temperature margin in combination with a higher heat capacity compared to conventional low-temperature superconductors (LTS). As a result, traditional voltage-based quench detection schemes may be ineffective for detecting normal zone formation in superconducting accelerator magnet windings. A developing hot spot may rea

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2

Jérome, D., and H. J. Schulz. "Organic conductors and superconductors." Advances in Physics 51, no. 1 (2002): 293–479. http://dx.doi.org/10.1080/00018730110116362.

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3

Montambaux, G. "Organic conductors and superconductors." Physica B: Condensed Matter 177, no. 1-4 (1992): 339–47. http://dx.doi.org/10.1016/0921-4526(92)90126-d.

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4

Morrison, Gale. "Superconductors Power Up." Mechanical Engineering 121, no. 01 (1999): 46–50. http://dx.doi.org/10.1115/1.1999-jan-1.

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This article reviews the copper cables in Detroit Edison’s Frisbie Station to be retrofit in mid-2000 with high-temperature superconductor (HTS) cables to support a major urban redevelopment project in downtown Detroit. American Superconductor’s partner, Pirelli, is participating in this project. The three HTS cables, weighing 250 pounds, will carry 100 megawatts of power, a job that nine copper cables, with a total weight of 18,000 pounds, are doing. In Germany, Siemens AG has invested hundreds of millions of dollars into researching HTS, because the capability can bring improvements across t

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5

Inokuchi, Hiroo. "Organic semiconductors, conductors and superconductors." International Reviews in Physical Chemistry 8, no. 2-3 (1989): 95–124. http://dx.doi.org/10.1080/01442358909353225.

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6

AHMEDOV, B. J., and F. J. FATTOYEV. "QUASI-STATIONARY ELECTROMAGNETIC EFFECTS IN CONDUCTORS AND SUPERCONDUCTORS IN SCHWARZSCHILD SPACE–TIME." International Journal of Modern Physics D 14, no. 05 (2005): 817–35. http://dx.doi.org/10.1142/s021827180500678x.

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The general principles needed to compute the effect of a stationary gravitational field on the quasistationary electromagnetic phenomena in normal conductors and superconductors are formulated from general relativistic point of view. Generalization of the skin effect, that is the general relativistic modification of the penetration depth (of the time-dependent magnetic field in the conductor) due to its relativistic coupling to the gravitational field is obtained. The effect of the gravitational field on the penetration and coherence depths in superconductors is also studied. As an illustratio

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7

Dressel, Martin. "Advances in Organic Conductors and Superconductors." Crystals 8, no. 9 (2018): 332. http://dx.doi.org/10.3390/cryst8090332.

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Crystalline conductors and superconductors based on organic molecules are a rapidly progressing field of solid-state science, involving chemists, and experimental and theoretical physicists from all around the world[...]

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8

Itahashi, Yuki M., Toshiya Ideue, Yu Saito, et al. "Nonreciprocal transport in gate-induced polar superconductor SrTiO3." Science Advances 6, no. 13 (2020): eaay9120. http://dx.doi.org/10.1126/sciadv.aay9120.

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Polar conductors/superconductors with Rashba-type spin-orbit interaction are potential material platforms for quantum transport and spintronic functionalities. One of their inherent properties is the nonreciprocal transport, where the rightward and leftward currents become inequivalent, reflecting spatial inversion/time-reversal symmetry breaking. Such a rectification effect originating from the polar symmetry has been recently observed at interfaces or bulk Rashba semiconductors, while its mechanism in a polar superconductor remains elusive. Here, we report the nonreciprocal transport in gate

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9

OGASAWARA, Takeshi. "Conductor design issues for oxide superconductors. II. Exemplification of stable conductors." TEION KOGAKU (Journal of Cryogenics and Superconductivity Society of Japan) 23, no. 4 (1988): 221–24. http://dx.doi.org/10.2221/jcsj.23.221.

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10

Schöllhorn, R. "From electronic/ionic conductors to superconductors." Solid State Ionics 26, no. 2 (1988): 145. http://dx.doi.org/10.1016/0167-2738(88)90038-0.

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11

SCHOLLHORN, R. "From electronic/ionic conductors to superconductors." Solid State Ionics 32-33 (February 1989): 23–39. http://dx.doi.org/10.1016/0167-2738(89)90199-9.

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12

Larbalestier, David C., and Martin P. Maley. "Conductors from Superconductors: Conventional Low-Temperature and New High-Temperature Superconducting Conductors." MRS Bulletin 18, no. 8 (1993): 50–56. http://dx.doi.org/10.1557/s0883769400037775.

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A useful superconducting conductor must have several properties. Some of the key properties among these are illustrated by the cross section of a Nb-47wt%Ti/Cu composite (Figure 1) which was manufactured for the dipole magnets of the Superconducting Super Collider (SSC). It represents the state of the art for conventional conductor fabrication and is thus an excellent place to start in considering what is needed for any new conductor. First among the essential properties is a high critical current density (Jc); the lower limit of useful Jc is ~104 A/cm2, but really useful values lie between 10

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13

Ogasawara, T. "Conductor design issues for oxide superconductors Part 2: exemplification of stable conductors." Cryogenics 29, no. 1 (1989): 6–9. http://dx.doi.org/10.1016/0011-2275(89)90003-9.

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14

Jérome, Denis. "The development of organic conductors: Organic superconductors." Solid State Sciences 10, no. 12 (2008): 1692–700. http://dx.doi.org/10.1016/j.solidstatesciences.2008.02.001.

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15

Gorshunov, B. P., A. A. Volkov, A. S. Prokhorov, et al. "Terahertz BWO spectroscopy of conductors and superconductors." Quantum Electronics 37, no. 10 (2007): 916–23. http://dx.doi.org/10.1070/qe2007v037n10abeh013614.

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16

Pouget, J. P., S. Ravy, and R. Moret. "Organic conductors and superconductors: A comparative survey." Phase Transitions 14, no. 1-4 (1989): 261–74. http://dx.doi.org/10.1080/01411598908208103.

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17

Kobayashi, Keiji, Carl Th Pedersen, and Jan Becher. "Sulfur Heterocycles for Organic Conductors and Superconductors." Phosphorus, Sulfur, and Silicon and the Related Elements 43, no. 1-2 (1989): 187–208. http://dx.doi.org/10.1080/10426508908040285.

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18

Jerome, D. "Collective modes in organic conductors and superconductors." Synthetic Metals 19, no. 1-3 (1987): 259–64. http://dx.doi.org/10.1016/0379-6779(87)90364-x.

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19

Chaikin, P. M., W. Kang, S. Hannahs, and R. C. Yu. "Organic conductors and superconductors at high field." Physica B: Condensed Matter 177, no. 1-4 (1992): 353–60. http://dx.doi.org/10.1016/0921-4526(92)90128-f.

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20

Selvamanickam, V., Y. Xie, J. Reeves, and Y. Chen. "MOCVD-Based YBCO-Coated Conductors." MRS Bulletin 29, no. 8 (2004): 579–82. http://dx.doi.org/10.1557/mrs2004.164.

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AbstractMetalorganic chemical vapor deposition (MOCVD) is a well-developed deposition process that shows great promise for scaling up the production of high-temperature superconductors (HTSs) to quickly fabricate useful lengths of superconducting tapes and wires.The primary advantage of MOCVD is its potential for high tape throughput, a key factor in determining the cost of second-generation HTS tapes.This article details progress in long-length HTS tape fabrication, high-throughput processing, and techniques to improve critical current levels in high magnetic fields.

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21

Gor'kov, L. P. "Organic Conductors and Superconductors in High Magnetic Fields." Japanese Journal of Applied Physics 26, S3-3 (1987): 1983. http://dx.doi.org/10.7567/jjaps.26s3.1983.

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22

Greaves, C. "Chapter 9. Electronic conductors, including high temperature superconductors." Annual Reports Section "A" (Inorganic Chemistry) 87 (1990): 167. http://dx.doi.org/10.1039/ic9908700167.

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23

Greaves, C. "Chapter 21. Electronic conductors, including high temperature superconductors." Annual Reports Section "A" (Inorganic Chemistry) 88 (1991): 419. http://dx.doi.org/10.1039/ic9918800419.

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24

Greaves, C. "Chapter 21. Electronic conductors, including high temperature superconductors." Annual Reports Section "A" (Inorganic Chemistry) 89 (1992): 393. http://dx.doi.org/10.1039/ic9928900393.

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25

Zimmerman, George, and J. Speickennan. "New Solders for Superconductors, Semiconductors, and Conventional Conductors." Materials and Processing Report 5, no. 12 (1991): 3. http://dx.doi.org/10.1080/08871949.1991.11752416.

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26

Saito, Gunzi, and Yukihiro Yoshida. "ChemInform Abstract: Frontiers of Organic Conductors and Superconductors." ChemInform 44, no. 42 (2013): no. http://dx.doi.org/10.1002/chin.201342269.

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27

Schläfer, Dietrich, Klaus Fischer, Margitta Schubert, and Brigitte Schlobach. "Texture Investigations on High Temperature Superconductors." Textures and Microstructures 24, no. 1-3 (1995): 93–103. http://dx.doi.org/10.1155/tsm.24.93.

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The formation of a structure with strong crystallographic texture is an important requirement for high critical current densities at 77 K in high temperature superconductive materials (HTSC). In this work several methods for texture investigation in the superconductive phase of BiPbSrCaCuO/Ag- and YBaCuO/AgPd-composite conductors prepared according to the “powder in tube”-method as well as in YBaCuO-thick layers are presented. For the characterisation of the texture development in dependence on technological steps at the preparation of HTSC-composite conductors the determination of the halfwid

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28

Auban-Senzier, P., and D. Jérome. "(TM)2X organic superconductors: prototypes of one-dimensional conductors." Synthetic Metals 133-134 (March 2003): 1–5. http://dx.doi.org/10.1016/s0379-6779(02)00241-2.

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29

Grioni, M., I. Vobornik, F. Zwick, and G. Margaritondo. "High-resolution photoemission in low-dimensional conductors and superconductors." Journal of Electron Spectroscopy and Related Phenomena 100, no. 1-3 (1999): 313–29. http://dx.doi.org/10.1016/s0368-2048(99)00053-5.

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30

DELHAES, P., and L. DUCASSE. "ChemInform Abstract: Magnetic Properties of Organic Conductors and Superconductors." ChemInform 28, no. 6 (2010): no. http://dx.doi.org/10.1002/chin.199706320.

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31

Ravy, S., R. Moret, J. P. Pouget, and R. Comes. "Competition between structural instabilities in organic conductors and superconductors." Physica B+C 143, no. 1-3 (1986): 542–46. http://dx.doi.org/10.1016/0378-4363(86)90191-9.

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32

Tixador, Pascal. "Concepts for HTS and MgB₂ in Transformers." Advances in Science and Technology 47 (October 2006): 195–203. http://dx.doi.org/10.4028/www.scientific.net/ast.47.195.

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After the emergence of AC NbTi strands, superconducting transformers were successfully built. But the very high cost of 4 K cryogenics made these transformers economically not attractive. The high Tc superconductors (HTS), operating at much higher temperatures, change these conclusions with low cost HTS conductors. The high cost of PIT tapes and the relatively large AC losses remain issues. The second generation HTS wires, the REBCO coated conductors, are under development and achieved substantial progress recently. They operate at higher temperatures and intrinsically show lower AC losses esp

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33

Brooks, J. S. "Organic Conductors and Superconductors: New Directions in the Solid State." MRS Bulletin 18, no. 8 (1993): 29–37. http://dx.doi.org/10.1557/s088376940003774x.

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In single-crystal organic salts, we find a keen competition between superconducting, magnetic, insulating, and metallic states. The physics of these materials is further enriched by the sensitivity of these states to pressure, temperature, chemical formulation, and magnetic field. A growing international community of scientists have turned their attention to these materials, and are applying the techniques and theories of metal and semiconductor physics to probe these new systems. In this article we will explore these materials. We will discover that these materials have given us many new thin

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34

Beenakker, C. W. J. "Random-matrix theory of mesoscopic fluctuations in conductors and superconductors." Physical Review B 47, no. 23 (1993): 15763–75. http://dx.doi.org/10.1103/physrevb.47.15763.

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35

Abdallah Ahmed Elfaki, Amel. "The Effect of Temperature on Conductivity of Conductors and Superconductors." American Journal of Physics and Applications 5, no. 1 (2017): 1. http://dx.doi.org/10.11648/j.ajpa.20170501.11.

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36

Larsson, Sven. "Electronic and vibrational structure of one-dimensional conductors and superconductors." Faraday Discuss. 131 (2006): 69–77. http://dx.doi.org/10.1039/b506642p.

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37

Jérome, D., F. Creuzet, and C. Bourbonnais. "A survey of the physics of organic conductors and superconductors." Physica Scripta T27 (January 1, 1989): 130–35. http://dx.doi.org/10.1088/0031-8949/1989/t27/023.

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38

Gervais, Francois, RicardoP S. M. Lobo, Marina Licheron, and Francisco J. Gotor. "Temperature dependence of reflectivity spectra of oxide conductors and superconductors." Ferroelectrics 177, no. 1 (1996): 107–22. http://dx.doi.org/10.1080/00150199608216957.

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39

Schöllhorn, Robert. "From Electronic/Ionic Conductors to Superconductors: Control of Materials Properties." Angewandte Chemie 100, no. 10 (1988): 1446–54. http://dx.doi.org/10.1002/ange.19881001047.

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40

Schöllhorn, Robert. "From Electronic/Ionic Conductors to Superconductors: Control of Materials Properties." Angewandte Chemie International Edition in English 27, no. 10 (1988): 1392–400. http://dx.doi.org/10.1002/anie.198813921.

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41

Chang, Nolanne A, Jacob J Richardson, Paul G Clem, and Julia W P. Hsu. "Additive Patterning of Conductors and Superconductors by Solution Stamping Nanolithography." Small 2, no. 1 (2006): 75–79. http://dx.doi.org/10.1002/smll.200500264.

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42

Wallis, John D., Andreas Karrer, and Jack D. Dunitz. "Chiral metals? A chiral substrate for organic conductors and superconductors." Helvetica Chimica Acta 69, no. 1 (1986): 69–70. http://dx.doi.org/10.1002/hlca.19860690110.

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43

Golovnya, A. V., V. Ya Pokrovskii, S. G. Zybtsev, and I. G. Gorlova. "Thermal expansion measurements of whiskers of superconductors and Peierls conductors." Journal de Physique IV (Proceedings) 131 (December 2005): 341. http://dx.doi.org/10.1051/jp4:2005131086.

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44

Helberg, H. W. "Network of the intermolecular contacts in organic conductors and superconductors." Synthetic Metals 19, no. 1-3 (1987): 251–56. http://dx.doi.org/10.1016/0379-6779(87)90363-8.

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45

TAKAHASHI, S., A. E. KOVALEV, S. HILL, et al. "FERMI SURFACE STUDIES OF QUASI-1D and QUASI-2D ORGANIC SUPERCONDUCTORS USING PERIODIC ORBIT RESONANCE IN HIGH MAGNETIC FIELDS." International Journal of Modern Physics B 18, no. 27n29 (2004): 3499–504. http://dx.doi.org/10.1142/s0217979204026895.

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We have studied periodic orbit resonances (PORs) in order to probe the topology of the Fermi surface (FS) of the quasi-1D organic conductor ( TMTSF )2 ClO 4 and the quasi-2D organic conductors κ-( ET )2 Cu ( NCS )2 and κ-( ET )2 I 3. The FS of ( TMTSF )2 ClO 4 consists of a pair of weakly corrugated open sheets, while κ-( ET )2 Cu ( NCS )2 and κ-( ET )2 I 3 additionally possess warped cylindrical FS sections. In this paper, we review the POR technique for the straightforward case of ( TMTSF )2 ClO 4. We then report on a detailed study of the FS topology for κ-( ET )2 Cu ( NCS )2.

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46

Patel, Dipak, Akiyoshi Matsumoto, Hiroaki Kumakura, et al. "MgB2 for MRI applications: dual sintering induced performance variations in in situ and IMD processed MgB2 conductors." Journal of Materials Chemistry C 8, no. 7 (2020): 2507–16. http://dx.doi.org/10.1039/c9tc06114b.

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47

Zhang, Hongye, Zezhao Wen, Francesco Grilli, Konstantinos Gyftakis, and Markus Mueller. "Alternating Current Loss of Superconductors Applied to Superconducting Electrical Machines." Energies 14, no. 8 (2021): 2234. http://dx.doi.org/10.3390/en14082234.

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Superconductor technology has recently attracted increasing attention in power-generation- and electrical-propulsion-related domains, as it provides a solution to the limited power density seen by the core component, electrical machines. Superconducting machines, characterized by both high power density and high efficiency, can effectively reduce the size and mass compared to conventional machine designs. This opens the way to large-scale purely electrical applications, e.g., all-electrical aircrafts. The alternating current (AC) loss of superconductors caused by time-varying transport current

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48

Nakazawa, Y., and S. Kruchinin. "Experimental and theoretical aspects of thermodynamic properties of quasi-1D and quasi-2D organic conductors and superconductors." International Journal of Modern Physics B 32, no. 17 (2018): 1840036. http://dx.doi.org/10.1142/s0217979218400362.

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We deal with thermodynamic features of organic conductors and superconductors where itinerant [Formula: see text]-electrons/holes released from organic molecules are playing essential roles for electronic properties. Since they are low-dimensional electronic systems with relatively soft lattice framework, they show variety of phenomena related to electron correlations and electron–lattice coupling. The drastic changes of conductive and magnetic properties owing to quantum features of [Formula: see text]-electrons can be induced by external perturbations such as magnetic/electric field, pressur

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49

Shiohara, Yuh, Masateru Yoshizumi, Yuji Takagi, and Teruo Izumi. "Future prospects of high Tc superconductors-coated conductors and their applications." Physica C: Superconductivity 484 (January 2013): 1–5. http://dx.doi.org/10.1016/j.physc.2012.03.058.

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50

Dyachenko, D. A., S. V. Konovalikhin, V. V. Gritsenko, R. N. Lyubovskaya, and R. B. Lyubovskii. "Structural design of organic conductors and superconductors with mercury-containing anions." Acta Crystallographica Section A Foundations of Crystallography 49, s1 (1993): c297—c298. http://dx.doi.org/10.1107/s0108767378091709.

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