Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers

Abstract Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ}...
Ausführliche Beschreibung

Gespeichert in:

Autor*in:	Baca, E. [verfasserIn] Morán, O. [verfasserIn] Saldarriaga, W. [verfasserIn] Romano, P. [verfasserIn] Polcari, A. [verfasserIn] Guarino, A. [verfasserIn] Vecchione, A. [verfasserIn]

Format:	E-Artikel
Sprache:	Englisch

Erschienen:	2012

Schlagwörter:	Trilayers Manganites HTS superconductors

Übergeordnetes Werk:	Enthalten in: Journal of superconductivity - Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988, 25(2012), 7 vom: 26. Aug., Seite 2103-2108
Übergeordnetes Werk:	volume:25 ; year:2012 ; number:7 ; day:26 ; month:08 ; pages:2103-2108

Links:	Volltext

DOI / URN:	10.1007/s10948-012-1746-3

Katalog-ID:	SPR014878542

Internformat


LEADER	01000caa a22002652 4500
001	SPR014878542
003	DE-627
005	20220111012849.0
007	cr uuu---uuuuu
008	201006s2012 xx \|\|\|\|\|o 00\| \|\|eng c
024	7		\|a 10.1007/s10948-012-1746-3 \|2 doi
035			\|a (DE-627)SPR014878542
035			\|a (SPR)s10948-012-1746-3-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 Baca, E. \|e verfasserin \|4 aut
245	1	0	\|a Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers
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 Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions.
650		4	\|a Trilayers \|7 (dpeaa)DE-He213
650		4	\|a Manganites \|7 (dpeaa)DE-He213
650		4	\|a HTS superconductors \|7 (dpeaa)DE-He213
700	1		\|a Morán, O. \|e verfasserin \|4 aut
700	1		\|a Saldarriaga, W. \|e verfasserin \|4 aut
700	1		\|a Romano, P. \|e verfasserin \|4 aut
700	1		\|a Polcari, A. \|e verfasserin \|4 aut
700	1		\|a Guarino, A. \|e verfasserin \|4 aut
700	1		\|a Vecchione, A. \|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 25(2012), 7 vom: 26. Aug., Seite 2103-2108 \|w (DE-627)313651175 \|w (DE-600)2000540-4 \|x 1572-9605 \|7 nnns
773	1	8	\|g volume:25 \|g year:2012 \|g number:7 \|g day:26 \|g month:08 \|g pages:2103-2108
856	4	0	\|u https://dx.doi.org/10.1007/s10948-012-1746-3 \|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 25 \|j 2012 \|e 7 \|b 26 \|c 08 \|h 2103-2108

Indexfelder

author_variant	e b eb o m om w s ws p r pr a p ap a g ag a v av
matchkey_str	article:15729605:2012----::tutrlneetiapoeteoeiaila2c_3n_l_3a2
hierarchy_sort_str	2012
bklnumber	33.74
publishDate	2012
allfields	10.1007/s10948-012-1746-3 doi (DE-627)SPR014878542 (SPR)s10948-012-1746-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Baca, E. verfasserin aut Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions. Trilayers (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 HTS superconductors (dpeaa)DE-He213 Morán, O. verfasserin aut Saldarriaga, W. verfasserin aut Romano, P. verfasserin aut Polcari, A. verfasserin aut Guarino, A. verfasserin aut Vecchione, A. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 25(2012), 7 vom: 26. Aug., Seite 2103-2108 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:25 year:2012 number:7 day:26 month:08 pages:2103-2108 https://dx.doi.org/10.1007/s10948-012-1746-3 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 25 2012 7 26 08 2103-2108
spelling	10.1007/s10948-012-1746-3 doi (DE-627)SPR014878542 (SPR)s10948-012-1746-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Baca, E. verfasserin aut Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions. Trilayers (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 HTS superconductors (dpeaa)DE-He213 Morán, O. verfasserin aut Saldarriaga, W. verfasserin aut Romano, P. verfasserin aut Polcari, A. verfasserin aut Guarino, A. verfasserin aut Vecchione, A. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 25(2012), 7 vom: 26. Aug., Seite 2103-2108 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:25 year:2012 number:7 day:26 month:08 pages:2103-2108 https://dx.doi.org/10.1007/s10948-012-1746-3 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 25 2012 7 26 08 2103-2108
allfields_unstemmed	10.1007/s10948-012-1746-3 doi (DE-627)SPR014878542 (SPR)s10948-012-1746-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Baca, E. verfasserin aut Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions. Trilayers (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 HTS superconductors (dpeaa)DE-He213 Morán, O. verfasserin aut Saldarriaga, W. verfasserin aut Romano, P. verfasserin aut Polcari, A. verfasserin aut Guarino, A. verfasserin aut Vecchione, A. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 25(2012), 7 vom: 26. Aug., Seite 2103-2108 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:25 year:2012 number:7 day:26 month:08 pages:2103-2108 https://dx.doi.org/10.1007/s10948-012-1746-3 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 25 2012 7 26 08 2103-2108
allfieldsGer	10.1007/s10948-012-1746-3 doi (DE-627)SPR014878542 (SPR)s10948-012-1746-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Baca, E. verfasserin aut Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions. Trilayers (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 HTS superconductors (dpeaa)DE-He213 Morán, O. verfasserin aut Saldarriaga, W. verfasserin aut Romano, P. verfasserin aut Polcari, A. verfasserin aut Guarino, A. verfasserin aut Vecchione, A. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 25(2012), 7 vom: 26. Aug., Seite 2103-2108 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:25 year:2012 number:7 day:26 month:08 pages:2103-2108 https://dx.doi.org/10.1007/s10948-012-1746-3 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 25 2012 7 26 08 2103-2108
allfieldsSound	10.1007/s10948-012-1746-3 doi (DE-627)SPR014878542 (SPR)s10948-012-1746-3-e DE-627 ger DE-627 rakwb eng 530 ASE 33.74 bkl Baca, E. verfasserin aut Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers 2012 Text txt rdacontent Computermedien c rdamedia Online-Ressource cr rdacarrier Abstract Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions. Trilayers (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 HTS superconductors (dpeaa)DE-He213 Morán, O. verfasserin aut Saldarriaga, W. verfasserin aut Romano, P. verfasserin aut Polcari, A. verfasserin aut Guarino, A. verfasserin aut Vecchione, A. verfasserin aut Enthalten in Journal of superconductivity Dordrecht [u.a.] : Springer Science + Business Media B.V., 1988 25(2012), 7 vom: 26. Aug., Seite 2103-2108 (DE-627)313651175 (DE-600)2000540-4 1572-9605 nnns volume:25 year:2012 number:7 day:26 month:08 pages:2103-2108 https://dx.doi.org/10.1007/s10948-012-1746-3 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 25 2012 7 26 08 2103-2108
language	English
source	Enthalten in Journal of superconductivity 25(2012), 7 vom: 26. Aug., Seite 2103-2108 volume:25 year:2012 number:7 day:26 month:08 pages:2103-2108
sourceStr	Enthalten in Journal of superconductivity 25(2012), 7 vom: 26. Aug., Seite 2103-2108 volume:25 year:2012 number:7 day:26 month:08 pages:2103-2108
format_phy_str_mv	Article
institution	findex.gbv.de
topic_facet	Trilayers Manganites HTS superconductors
dewey-raw	530
isfreeaccess_bool	false
container_title	Journal of superconductivity
authorswithroles_txt_mv	Baca, E. @@aut@@ Morán, O. @@aut@@ Saldarriaga, W. @@aut@@ Romano, P. @@aut@@ Polcari, A. @@aut@@ Guarino, A. @@aut@@ Vecchione, A. @@aut@@
publishDateDaySort_date	2012-08-26T00:00:00Z
hierarchy_top_id	313651175
dewey-sort	3530
id	SPR014878542
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">SPR014878542</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111012849.0</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/s10948-012-1746-3</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR014878542</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10948-012-1746-3-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">Baca, E.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers</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 Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Trilayers</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="650" ind1=" " ind2="4"><subfield code="a">HTS superconductors</subfield><subfield code="7">(dpeaa)DE-He213</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="700" ind1="1" ind2=" "><subfield code="a">Saldarriaga, W.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Romano, P.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Polcari, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Guarino, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Vecchione, A.</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">25(2012), 7 vom: 26. Aug., Seite 2103-2108</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:25</subfield><subfield code="g">year:2012</subfield><subfield code="g">number:7</subfield><subfield code="g">day:26</subfield><subfield code="g">month:08</subfield><subfield code="g">pages:2103-2108</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/s10948-012-1746-3</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">25</subfield><subfield code="j">2012</subfield><subfield code="e">7</subfield><subfield code="b">26</subfield><subfield code="c">08</subfield><subfield code="h">2103-2108</subfield></datafield></record></collection>
author	Baca, E.
spellingShingle	Baca, E. ddc 530 bkl 33.74 misc Trilayers misc Manganites misc HTS superconductors Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers
authorStr	Baca, E.
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 aut aut aut aut
collection	springer
remote_str	true
illustrated	Not Illustrated
issn	1572-9605
topic_title	530 ASE 33.74 bkl Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers Trilayers (dpeaa)DE-He213 Manganites (dpeaa)DE-He213 HTS superconductors (dpeaa)DE-He213
topic	ddc 530 bkl 33.74 misc Trilayers misc Manganites misc HTS superconductors
topic_unstemmed	ddc 530 bkl 33.74 misc Trilayers misc Manganites misc HTS superconductors
topic_browse	ddc 530 bkl 33.74 misc Trilayers misc Manganites misc HTS superconductors
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	Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers
ctrlnum	(DE-627)SPR014878542 (SPR)s10948-012-1746-3-e
title_full	Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers
author_sort	Baca, E.
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	2103
author_browse	Baca, E. Morán, O. Saldarriaga, W. Romano, P. Polcari, A. Guarino, A. Vecchione, A.
container_volume	25
class	530 ASE 33.74 bkl
format_se	Elektronische Aufsätze
author-letter	Baca, E.
doi_str_mv	10.1007/s10948-012-1746-3
dewey-full	530
author2-role	verfasserin
title_sort	structural and electrical properties of epitaxial $ la_{2/3} %$ ca_{1/3} %$ mno_{3} $/$ la_{1/3} %$ ca_{2/3} %$ mno_{3} $/$ yba_{2} %$ cu_{3} %$ o_{7−δ} $ trilayers
title_auth	Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers
abstract	Abstract Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions.
abstractGer	Abstract Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions.
abstract_unstemmed	Abstract Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions.
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	7
title_short	Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers
url	https://dx.doi.org/10.1007/s10948-012-1746-3
remote_bool	true
author2	Morán, O. Saldarriaga, W. Romano, P. Polcari, A. Guarino, A. Vecchione, A.
author2Str	Morán, O. Saldarriaga, W. Romano, P. Polcari, A. Guarino, A. Vecchione, A.
ppnlink	313651175
mediatype_str_mv	c
isOA_txt	false
hochschulschrift_bool	false
doi_str	10.1007/s10948-012-1746-3
up_date	2024-07-04T03:21:23.352Z
_version_	1803617077409349632
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">SPR014878542</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220111012849.0</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/s10948-012-1746-3</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)SPR014878542</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(SPR)s10948-012-1746-3-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">Baca, E.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers</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 Trilayers made of perovskite-type ferromagnetic (F), antiferromagnetic (AF) and superconducting (S) films were fabricated and their microstructural properties studied. Epitaxially strained $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ (F/AF/S) trilayers were grown in situ by dc-sputtering technique onto (001)-oriented $ SrTiO_{3} $ (STO) substrates. Whereas the thickness of the bottom (F) and top (S) layer was fixed to 74 nm and 100 nm, respectively, that of the intermediate AF layer was varied between ∼4 nm and ∼9 nm. The crystalline quality of the samples was checked by X-Ray diffraction (XRD) analysis. The θ–2θ scans and reciprocal space maps at (002) and (013) Bragg reflections provided clear evidence for the heteroepitaxial growth of the trilayers as well as for the absence of secondary phases. Due to high epitaxiality of the trilayers, their magnetic response was already shown to develop an excellent magnetic anisotropy to clearly visualize the superconducting diamagnetism and ferromagnetic behavior at a same temperature. The superconducting diamagnetic response at 5 K has now been used to calculate the superconducting current density of the S layer as a function of an applied magnetic field. The results confirmed the uncoupling role of the AF layer. The presence of well defined AF barriers ($ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $) in the trilayers was also evidenced by recording the I–V characteristic in cross configuration, which showed an anisotropic behavior as well. The results achieved suggest that such oxide heterostructures could play an important role in the search for novel devices based on magnetic junctions.</subfield></datafield><datafield tag="650" ind1=" " ind2="4"><subfield code="a">Trilayers</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="650" ind1=" " ind2="4"><subfield code="a">HTS superconductors</subfield><subfield code="7">(dpeaa)DE-He213</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="700" ind1="1" ind2=" "><subfield code="a">Saldarriaga, W.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Romano, P.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Polcari, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Guarino, A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Vecchione, A.</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">25(2012), 7 vom: 26. Aug., Seite 2103-2108</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:25</subfield><subfield code="g">year:2012</subfield><subfield code="g">number:7</subfield><subfield code="g">day:26</subfield><subfield code="g">month:08</subfield><subfield code="g">pages:2103-2108</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">https://dx.doi.org/10.1007/s10948-012-1746-3</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">25</subfield><subfield code="j">2012</subfield><subfield code="e">7</subfield><subfield code="b">26</subfield><subfield code="c">08</subfield><subfield code="h">2103-2108</subfield></datafield></record></collection>
score	7.4003315

Nicht das Richtige dabei?

Schreiben Sie uns!

Structural and Electrical Properties of Epitaxial $ La_{2/3} %$ Ca_{1/3} %$ MnO_{3} $/$ La_{1/3} %$ Ca_{2/3} %$ MnO_{3} $/$ YBa_{2} %$ Cu_{3} %$ O_{7−δ} $ Trilayers

Nicht das Richtige dabei?

Zugang & Verfügbarkeit

Vorhandene Bände

Nicht das Richtige dabei?