Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films

Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constit...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Paredes, O. [verfasserIn] Baca, E. [verfasserIn] Morán, O. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2012

Schlagwörter:	Composites Superconducting ceramics Manganites

Übergeordnetes Werk:	Enthalten in: Journal of superconductivity - Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988, 26(2012), 6 vom: 09. Feb., Seite 2323-2327
Übergeordnetes Werk:	volume:26 ; year:2012 ; number:6 ; day:09 ; month:02 ; pages:2323-2327

Links:	Volltext

DOI / URN:	10.1007/s10948-012-1455-y

Katalog-ID:	SPR014884089

Internformat


LEADER	01000caa a22002652 4500
001	SPR014884089
003	DE-627
005	20220111012855.0
007	cr uuu---uuuuu
008	201006s2012 xx \|\|\|\|\|o 00\| \|\|eng c
024	7		\|a 10.1007/s10948-012-1455-y \|2 doi
035			\|a (DE-627)SPR014884089
035			\|a (SPR)s10948-012-1455-y-e
040			\|a DE-627 \|b ger \|c DE-627 \|e rakwb
041			\|a eng
082	0	4	\|a 530 \|q ASE
084			\|a 33.74 \|2 bkl
100	1		\|a Paredes, O. \|e verfasserin \|4 aut
245	1	0	\|a Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films
264		1	\|c 2012
336			\|a Text \|b txt \|2 rdacontent
337			\|a Computermedien \|b c \|2 rdamedia
338			\|a Online-Ressource \|b cr \|2 rdacarrier
520			\|a Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase.
650		4	\|a Composites \|7 (dpeaa)DE-He213
650		4	\|a Superconducting ceramics \|7 (dpeaa)DE-He213
650		4	\|a Manganites \|7 (dpeaa)DE-He213
700	1		\|a Baca, E. \|e verfasserin \|4 aut
700	1		\|a Morán, O. \|e verfasserin \|4 aut
773	0	8	\|i Enthalten in \|t Journal of superconductivity \|d Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 \|g 26(2012), 6 vom: 09. Feb., Seite 2323-2327 \|w (DE-627)313651175 \|w (DE-600)2000540-4 \|x 1572-9605 \|7 nnns
773	1	8	\|g volume:26 \|g year:2012 \|g number:6 \|g day:09 \|g month:02 \|g pages:2323-2327
856	4	0	\|u https://dx.doi.org/10.1007/s10948-012-1455-y \|z lizenzpflichtig \|3 Volltext
912			\|a GBV_USEFLAG_A
912			\|a SYSFLAG_A
912			\|a GBV_SPRINGER
912			\|a GBV_ILN_20
912			\|a GBV_ILN_22
912			\|a GBV_ILN_23
912			\|a GBV_ILN_24
912			\|a GBV_ILN_31
912			\|a GBV_ILN_32
912			\|a GBV_ILN_39
912			\|a GBV_ILN_40
912			\|a GBV_ILN_60
912			\|a GBV_ILN_62
912			\|a GBV_ILN_69
912			\|a GBV_ILN_70
912			\|a GBV_ILN_73
912			\|a GBV_ILN_74
912			\|a GBV_ILN_90
912			\|a GBV_ILN_95
912			\|a GBV_ILN_100
912			\|a GBV_ILN_101
912			\|a GBV_ILN_105
912			\|a GBV_ILN_110
912			\|a GBV_ILN_120
912			\|a GBV_ILN_138
912			\|a GBV_ILN_152
912			\|a GBV_ILN_161
912			\|a GBV_ILN_171
912			\|a GBV_ILN_187
912			\|a GBV_ILN_224
912			\|a GBV_ILN_250
912			\|a GBV_ILN_281
912			\|a GBV_ILN_285
912			\|a GBV_ILN_293
912			\|a GBV_ILN_370
912			\|a GBV_ILN_602
912			\|a GBV_ILN_702
936	b	k	\|a 33.74 \|q ASE
951			\|a AR
952			\|d 26 \|j 2012 \|e 6 \|b 09 \|c 02 \|h 2323-2327

Indexfelder

author_variant	o p op e b eb o m om
matchkey_str	article:15729605:2012----::nepabtenimgeiadermgeipaeni23ys
hierarchy_sort_str	2012
bklnumber	33.74
publishDate	2012
allfields	10.1007/s10948-012-1455-y doi (DE-627)SPR014884089 (SPR)s10948-012-1455-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Paredes, O. verfasserin aut Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase. Composites (dpeaa)DE-He213 Superconducting ceramics (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 Baca, E. verfasserin aut Morán, O. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 26(2012), 6 vom: 09. Feb., Seite 2323-2327 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:26 year:2012 number:6 day:09 month:02 pages:2323-2327 https://dx.doi.org/10.1007/s10948-012-1455-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 26 2012 6 09 02 2323-2327
spelling	10.1007/s10948-012-1455-y doi (DE-627)SPR014884089 (SPR)s10948-012-1455-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Paredes, O. verfasserin aut Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase. Composites (dpeaa)DE-He213 Superconducting ceramics (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 Baca, E. verfasserin aut Morán, O. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 26(2012), 6 vom: 09. Feb., Seite 2323-2327 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:26 year:2012 number:6 day:09 month:02 pages:2323-2327 https://dx.doi.org/10.1007/s10948-012-1455-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 26 2012 6 09 02 2323-2327
allfields_unstemmed	10.1007/s10948-012-1455-y doi (DE-627)SPR014884089 (SPR)s10948-012-1455-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Paredes, O. verfasserin aut Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase. Composites (dpeaa)DE-He213 Superconducting ceramics (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 Baca, E. verfasserin aut Morán, O. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 26(2012), 6 vom: 09. Feb., Seite 2323-2327 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:26 year:2012 number:6 day:09 month:02 pages:2323-2327 https://dx.doi.org/10.1007/s10948-012-1455-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 26 2012 6 09 02 2323-2327
allfieldsGer	10.1007/s10948-012-1455-y doi (DE-627)SPR014884089 (SPR)s10948-012-1455-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Paredes, O. verfasserin aut Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase. Composites (dpeaa)DE-He213 Superconducting ceramics (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 Baca, E. verfasserin aut Morán, O. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 26(2012), 6 vom: 09. Feb., Seite 2323-2327 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:26 year:2012 number:6 day:09 month:02 pages:2323-2327 https://dx.doi.org/10.1007/s10948-012-1455-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 26 2012 6 09 02 2323-2327
allfieldsSound	10.1007/s10948-012-1455-y doi (DE-627)SPR014884089 (SPR)s10948-012-1455-y-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Paredes, O. verfasserin aut Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase. Composites (dpeaa)DE-He213 Superconducting ceramics (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 Baca, E. verfasserin aut Morán, O. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 26(2012), 6 vom: 09. Feb., Seite 2323-2327 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:26 year:2012 number:6 day:09 month:02 pages:2323-2327 https://dx.doi.org/10.1007/s10948-012-1455-y lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702 33.74 ASE AR 26 2012 6 09 02 2323-2327
language	English
source	Enthalten in Journal of superconductivity 26(2012), 6 vom: 09. Feb., Seite 2323-2327 volume:26 year:2012 number:6 day:09 month:02 pages:2323-2327
sourceStr	Enthalten in Journal of superconductivity 26(2012), 6 vom: 09. Feb., Seite 2323-2327 volume:26 year:2012 number:6 day:09 month:02 pages:2323-2327
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Composites Superconducting ceramics Manganites
dewey-raw	530
isfreeaccess_bool	false
container_title	Journal of superconductivity
authorswithroles_txt_mv	Paredes, O. @@aut@@ Baca, E. @@aut@@ Morán, O. @@aut@@
publishDateDaySort_date	2012-02-09T00:00:00Z
hierarchy_top_id	313651175
dewey-sort	3530
id	SPR014884089
language_de	englisch
fullrecord	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR014884089</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111012855.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2012 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10948-012-1455-y</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR014884089</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10948-012-1455-y-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.74</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Paredes, O.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2012</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Composites</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Superconducting ceramics</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Manganites</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Baca, E.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Morán, O.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of superconductivity</subfield><subfield code="d">Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988</subfield><subfield code="g">26(2012), 6 vom: 09. Feb., Seite 2323-2327</subfield><subfield code="w">(DE-627)313651175</subfield><subfield code="w">(DE-600)2000540-4</subfield><subfield code="x">1572-9605</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:26</subfield><subfield code="g">year:2012</subfield><subfield code="g">number:6</subfield><subfield code="g">day:09</subfield><subfield code="g">month:02</subfield><subfield code="g">pages:2323-2327</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/s10948-012-1455-y</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_SPRINGER</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_32</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_74</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_90</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_100</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_101</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_120</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_138</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_152</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_171</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_187</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_224</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_250</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_281</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_702</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.74</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">26</subfield><subfield code="j">2012</subfield><subfield code="e">6</subfield><subfield code="b">09</subfield><subfield code="c">02</subfield><subfield code="h">2323-2327</subfield></datafield></record></collection>
author	Paredes, O.
spellingShingle	Paredes, O. ddc 530 bkl 33.74 misc Composites misc Superconducting ceramics misc Manganites Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films
authorStr	Paredes, O.
ppnlink_with_tag_str_mv	@@773@@(DE-627)313651175
format	electronic Article
dewey-ones	530 - Physics
delete_txt_mv	keep
author_role	aut aut aut
collection	springer
remote_str	true
illustrated	Not Illustrated
issn	1572-9605
topic_title	530 ASE 33.74 bkl Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films Composites (dpeaa)DE-He213 Superconducting ceramics (dpeaa)DE-He213 Manganites (dpeaa)DE-He213
topic	ddc 530 bkl 33.74 misc Composites misc Superconducting ceramics misc Manganites
topic_unstemmed	ddc 530 bkl 33.74 misc Composites misc Superconducting ceramics misc Manganites
topic_browse	ddc 530 bkl 33.74 misc Composites misc Superconducting ceramics misc Manganites
format_facet	Elektronische Aufsätze Aufsätze Elektronische Ressource
format_main_str_mv	Text Zeitschrift/Artikel
carriertype_str_mv	cr
hierarchy_parent_title	Journal of superconductivity
hierarchy_parent_id	313651175
dewey-tens	530 - Physics
hierarchy_top_title	Journal of superconductivity
isfreeaccess_txt	false
familylinks_str_mv	(DE-627)313651175 (DE-600)2000540-4
title	Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films
ctrlnum	(DE-627)SPR014884089 (SPR)s10948-012-1455-y-e
title_full	Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films
author_sort	Paredes, O.
journal	Journal of superconductivity
journalStr	Journal of superconductivity
lang_code	eng
isOA_bool	false
dewey-hundreds	500 - Science
recordtype	marc
publishDateSort	2012
contenttype_str_mv	txt
container_start_page	2323
author_browse	Paredes, O. Baca, E. Morán, O.
container_volume	26
class	530 ASE 33.74 bkl
format_se	Elektronische Aufsätze
author-letter	Paredes, O.
doi_str_mv	10.1007/s10948-012-1455-y
dewey-full	530
author2-role	verfasserin
title_sort	interplay between diamagnetic and ferromagnetic phase in (bi2223)1−y(lsmo)y composites thick films
title_auth	Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films
abstract	Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase.
abstractGer	Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase.
abstract_unstemmed	Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase.
collection_details	GBV_USEFLAG_A SYSFLAG_A GBV_SPRINGER GBV_ILN_20 GBV_ILN_22 GBV_ILN_23 GBV_ILN_24 GBV_ILN_31 GBV_ILN_32 GBV_ILN_39 GBV_ILN_40 GBV_ILN_60 GBV_ILN_62 GBV_ILN_69 GBV_ILN_70 GBV_ILN_73 GBV_ILN_74 GBV_ILN_90 GBV_ILN_95 GBV_ILN_100 GBV_ILN_101 GBV_ILN_105 GBV_ILN_110 GBV_ILN_120 GBV_ILN_138 GBV_ILN_152 GBV_ILN_161 GBV_ILN_171 GBV_ILN_187 GBV_ILN_224 GBV_ILN_250 GBV_ILN_281 GBV_ILN_285 GBV_ILN_293 GBV_ILN_370 GBV_ILN_602 GBV_ILN_702
container_issue	6
title_short	Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films
url	https://dx.doi.org/10.1007/s10948-012-1455-y
remote_bool	true
author2	Baca, E. Morán, O.
author2Str	Baca, E. Morán, O.
ppnlink	313651175
mediatype_str_mv	c
isOA_txt	false
hochschulschrift_bool	false
doi_str	10.1007/s10948-012-1455-y
up_date	2024-07-04T03:22:19.533Z
_version_	1803617136318349312
fullrecord_marcxml	<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">SPR014884089</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111012855.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">201006s2012 xx \|\|\|\|\|o 00\| \|\|eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/s10948-012-1455-y</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR014884089</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10948-012-1455-y-e</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">530</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">33.74</subfield><subfield code="2">bkl</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Paredes, O.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2012</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">Computermedien</subfield><subfield code="b">c</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Online-Ressource</subfield><subfield code="b">cr</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract Thick films of ((Bi,Pb)2$ Sr_{2} %$ Ca_{2} %$ Cu_{3} %$ O_{x} $)1−y($ La_{0.7} %$ Sr_{0.3} %$ MnO_{3} $)y [(Bi2223)1−y(LSMO)y] composites (y=0.01, 0.03, 0.05) are deposited by means of a simple melting-quenching-annealing method onto (001)-oriented $ LaAlO_{3} $(LAO) substrates. The constituent compounds Bi2223 and LSMO are prepared by standard solid-state reaction and sol–gel method, respectively. Measurements of the dependence of the magnetization on the temperature show the presence of superconducting and ferromagnetic phase below ∼54 K and ∼370 K, respectively. Current–voltage measurements on composites with y=0.01, 0.03 show that the superconducting critical current drop dramatically from Ic≈350 mA at T=15 K to zero at T≈0.5Tc (∼25 K). The dependence of the magnetization on the external magnetic field applied in-plane or out-of-plane at 5 K displays well defined hysteresis loops, which correspond to the superconducting, diamagnetic phase. For T>Tc, the ferromagnetic loop of LSMO is observed. The critical current density, Jc, was determined for samples with y=0.01 and 0.05 by applying Kim’s model to the superconducting, diamagnetic hysteresis recorded at 5 K. The calculated values for Jc(B) resulted to be smaller than those obtained for individual bulk Bi2223 samples due, probably, to the presence of LSMO particles whose ferromagnetic domains compete with the superconducting diamagnetic phase.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Composites</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Superconducting ceramics</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Manganites</subfield><subfield code="7">(dpeaa)DE-He213</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Baca, E.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Morán, O.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Journal of superconductivity</subfield><subfield code="d">Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988</subfield><subfield code="g">26(2012), 6 vom: 09. Feb., Seite 2323-2327</subfield><subfield code="w">(DE-627)313651175</subfield><subfield code="w">(DE-600)2000540-4</subfield><subfield code="x">1572-9605</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:26</subfield><subfield code="g">year:2012</subfield><subfield code="g">number:6</subfield><subfield code="g">day:09</subfield><subfield code="g">month:02</subfield><subfield code="g">pages:2323-2327</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/s10948-012-1455-y</subfield><subfield code="z">lizenzpflichtig</subfield><subfield code="3">Volltext</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SYSFLAG_A</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_SPRINGER</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_20</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_22</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_23</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_24</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_31</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_32</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_39</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_40</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_60</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_62</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_69</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_73</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_74</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_90</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_95</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_100</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_101</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_105</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_110</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_120</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_138</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_152</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_161</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_171</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_187</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_224</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_250</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_281</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_285</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_293</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_370</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_602</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_702</subfield></datafield><datafield tag="936" ind1="b" ind2="k"><subfield code="a">33.74</subfield><subfield code="q">ASE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">26</subfield><subfield code="j">2012</subfield><subfield code="e">6</subfield><subfield code="b">09</subfield><subfield code="c">02</subfield><subfield code="h">2323-2327</subfield></datafield></record></collection>
score	7.399269

Nicht das Richtige dabei?

Schreiben Sie uns!

Interplay Between Diamagnetic and Ferromagnetic Phase in (Bi2223)1−y(LSMO)y Composites Thick Films

Nicht das Richtige dabei?

Zugang & Verfügbarkeit

Vorhandene Bände

Nicht das Richtige dabei?