AC susceptibility with superimposed DC magnetic field in a current biased granular high Tc superconductor
We have investigated the effect in AC magnetic susceptibility, κ{script}ac=κ{script}′+jκ{script} ″, of both DC transport current, Jt, and DC magnetic field, Hdc, in polycristalline HTSC. Two regimes are observed: at low DC fields critical state is modified by the current self field; but as Hdc is in...
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| Formato: | Capítulo de libro |
| Lenguaje: | Inglés |
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1994
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| Acceso en línea: | Registro en Scopus DOI Handle Registro en la Biblioteca Digital |
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| LEADER | 03152caa a22004217a 4500 | ||
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| 001 | PAPER-27 | ||
| 003 | AR-BaUEN | ||
| 005 | 20250314092408.0 | ||
| 008 | 190411s1994 xx ||||fo|||| 00| 0 eng|d | ||
| 024 | 7 | |2 scopus |a 2-s2.0-50749132139 | |
| 030 | |a PHYCE | ||
| 040 | |a Scopus |b spa |c AR-BaUEN |d AR-BaUEN | ||
| 100 | 1 | |a Codner, G. | |
| 245 | 1 | 0 | |a AC susceptibility with superimposed DC magnetic field in a current biased granular high Tc superconductor |
| 260 | |c 1994 | ||
| 270 | 1 | 0 | |m Codner, G. |
| 504 | |a Kim, Critical Persistent Currents in Hard Superconductors (1962) Physical Review Letters, 9, p. 306 | ||
| 504 | |a Clem, Granular and superconducting-glass properties of the high-temperature superconductors (1988) Physica C: Superconductivity, 153-155, p. 50 | ||
| 504 | |a Levy, Ferrari, Bekeris, Acha, AC susceptibility and local intergranular magnetic field in high-Tc superconductors (1993) Physica C: Superconductivity, 214, p. 111 | ||
| 504 | |a Polla, Archa, Duran, Baggio, de Benyacar, Chemical incorporation of halogens in high Tc superconductors: I:Chlorine incorporation in La1.8Sr0.2CuO4 (1990) Solid State Communications, 74, p. 487 | ||
| 506 | |2 openaire |e Política editorial | ||
| 520 | 3 | |a We have investigated the effect in AC magnetic susceptibility, κ{script}ac=κ{script}′+jκ{script} ″, of both DC transport current, Jt, and DC magnetic field, Hdc, in polycristalline HTSC. Two regimes are observed: at low DC fields critical state is modified by the current self field; but as Hdc is increased, Jt becomes dissipative (Vdc≠0) and κ{script}ac is determined by the samples's "resistance". © 1994. |l eng | |
| 536 | |a Detalles de la financiación: Consejo Nacional de Investigaciones Científicas y Técnicas, 332400092 | ||
| 536 | |a Detalles de la financiación: *This work was partially supported by CONICET Grant No 332400092 | ||
| 593 | |a Laboratorio de Bajas Temperaturas, FCEN-UBA, Ciudad Universitaria, Pab. I, (1428) Cap. Fed. Argentina, Argentina | ||
| 593 | |a División Física del Sólidi, Comisión Nacional de Energía Atómica, Libertador 8250 (1429) Cap. Fed, Argentina | ||
| 700 | 1 | |a Ferrari, Hernán Javier | |
| 700 | 1 | |a Acha, C. | |
| 700 | 1 | |a Bekeris, V. | |
| 700 | 1 | |a Levy, P. | |
| 773 | 0 | |d 1994 |g v. 235-240 |h pp. 3227-3228 |k n. PART 5 |p Phys C Supercond Appl |x 09214534 |w (AR-BaUEN)CENRE-278 |t Physica C: Superconductivity and its applications | |
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| 856 | 4 | 0 | |u https://doi.org/10.1016/0921-4534(94)91140-1 |x doi |y DOI |
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| 961 | |a paper_09214534_v235-240_nPART5_p3227_Codner |b paper |c PE | ||
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| 963 | |a VARI | ||