Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y
We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are...
Ausführliche Beschreibung
Autor*in: |
---|
Format: |
E-Artikel |
---|---|
Sprache: |
Englisch |
Erschienen: |
1988 |
---|
Reproduktion: |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
---|---|
Übergeordnetes Werk: |
in: Physica C: Superconductivity and its applications - Amsterdam : Elsevier, 156(1988), 4, Seite 592-598 |
Übergeordnetes Werk: |
volume:156 ; year:1988 ; number:4 ; pages:592-598 |
Links: |
---|
Katalog-ID: |
NLEJ177930683 |
---|
LEADER | 01000caa a22002652 4500 | ||
---|---|---|---|
001 | NLEJ177930683 | ||
003 | DE-627 | ||
005 | 20210706063704.0 | ||
007 | cr uuu---uuuuu | ||
008 | 070505s1988 xx |||||o 00| ||eng c | ||
035 | |a (DE-627)NLEJ177930683 | ||
035 | |a (DE-599)GBVNLZ177930683 | ||
040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
041 | |a eng | ||
245 | 1 | 0 | |a Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y |
264 | 1 | |c 1988 | |
336 | |a nicht spezifiziert |b zzz |2 rdacontent | ||
337 | |a nicht spezifiziert |b z |2 rdamedia | ||
338 | |a nicht spezifiziert |b zu |2 rdacarrier | ||
520 | |a We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed. | ||
533 | |f Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 | ||
700 | 1 | |a Ginley, D.S. |4 oth | |
700 | 1 | |a Kwak, J.F. |4 oth | |
700 | 1 | |a Hellmer, R.P. |4 oth | |
700 | 1 | |a Baughman, R.J. |4 oth | |
700 | 1 | |a Venturini, E.L. |4 oth | |
700 | 1 | |a Mitchell, M.A. |4 oth | |
700 | 1 | |a Morosin, B. |4 oth | |
773 | 0 | 8 | |i in |t Physica C: Superconductivity and its applications |d Amsterdam : Elsevier |g 156(1988), 4, Seite 592-598 |w (DE-627)NLEJ177038349 |w (DE-600)1467152-9 |x 0921-4534 |7 nnns |
773 | 1 | 8 | |g volume:156 |g year:1988 |g number:4 |g pages:592-598 |
856 | 4 | 0 | |u http://linkinghub.elsevier.com/retrieve/pii/0921-4534(88)90027-5 |
912 | |a GBV_USEFLAG_H | ||
912 | |a ZDB-1-SDJ | ||
912 | |a GBV_NL_ARTICLE | ||
951 | |a AR | ||
952 | |d 156 |j 1988 |e 4 |h 592-598 |
matchkey_str |
article:09214534:1988----::uecnutntiflsflc2ac3yn |
---|---|
hierarchy_sort_str |
1988 |
publishDate |
1988 |
allfields |
(DE-627)NLEJ177930683 (DE-599)GBVNLZ177930683 DE-627 ger DE-627 rakwb eng Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y 1988 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Ginley, D.S. oth Kwak, J.F. oth Hellmer, R.P. oth Baughman, R.J. oth Venturini, E.L. oth Mitchell, M.A. oth Morosin, B. oth in Physica C: Superconductivity and its applications Amsterdam : Elsevier 156(1988), 4, Seite 592-598 (DE-627)NLEJ177038349 (DE-600)1467152-9 0921-4534 nnns volume:156 year:1988 number:4 pages:592-598 http://linkinghub.elsevier.com/retrieve/pii/0921-4534(88)90027-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 156 1988 4 592-598 |
spelling |
(DE-627)NLEJ177930683 (DE-599)GBVNLZ177930683 DE-627 ger DE-627 rakwb eng Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y 1988 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Ginley, D.S. oth Kwak, J.F. oth Hellmer, R.P. oth Baughman, R.J. oth Venturini, E.L. oth Mitchell, M.A. oth Morosin, B. oth in Physica C: Superconductivity and its applications Amsterdam : Elsevier 156(1988), 4, Seite 592-598 (DE-627)NLEJ177038349 (DE-600)1467152-9 0921-4534 nnns volume:156 year:1988 number:4 pages:592-598 http://linkinghub.elsevier.com/retrieve/pii/0921-4534(88)90027-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 156 1988 4 592-598 |
allfields_unstemmed |
(DE-627)NLEJ177930683 (DE-599)GBVNLZ177930683 DE-627 ger DE-627 rakwb eng Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y 1988 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Ginley, D.S. oth Kwak, J.F. oth Hellmer, R.P. oth Baughman, R.J. oth Venturini, E.L. oth Mitchell, M.A. oth Morosin, B. oth in Physica C: Superconductivity and its applications Amsterdam : Elsevier 156(1988), 4, Seite 592-598 (DE-627)NLEJ177038349 (DE-600)1467152-9 0921-4534 nnns volume:156 year:1988 number:4 pages:592-598 http://linkinghub.elsevier.com/retrieve/pii/0921-4534(88)90027-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 156 1988 4 592-598 |
allfieldsGer |
(DE-627)NLEJ177930683 (DE-599)GBVNLZ177930683 DE-627 ger DE-627 rakwb eng Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y 1988 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Ginley, D.S. oth Kwak, J.F. oth Hellmer, R.P. oth Baughman, R.J. oth Venturini, E.L. oth Mitchell, M.A. oth Morosin, B. oth in Physica C: Superconductivity and its applications Amsterdam : Elsevier 156(1988), 4, Seite 592-598 (DE-627)NLEJ177038349 (DE-600)1467152-9 0921-4534 nnns volume:156 year:1988 number:4 pages:592-598 http://linkinghub.elsevier.com/retrieve/pii/0921-4534(88)90027-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 156 1988 4 592-598 |
allfieldsSound |
(DE-627)NLEJ177930683 (DE-599)GBVNLZ177930683 DE-627 ger DE-627 rakwb eng Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y 1988 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Ginley, D.S. oth Kwak, J.F. oth Hellmer, R.P. oth Baughman, R.J. oth Venturini, E.L. oth Mitchell, M.A. oth Morosin, B. oth in Physica C: Superconductivity and its applications Amsterdam : Elsevier 156(1988), 4, Seite 592-598 (DE-627)NLEJ177038349 (DE-600)1467152-9 0921-4534 nnns volume:156 year:1988 number:4 pages:592-598 http://linkinghub.elsevier.com/retrieve/pii/0921-4534(88)90027-5 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 156 1988 4 592-598 |
language |
English |
source |
in Physica C: Superconductivity and its applications 156(1988), 4, Seite 592-598 volume:156 year:1988 number:4 pages:592-598 |
sourceStr |
in Physica C: Superconductivity and its applications 156(1988), 4, Seite 592-598 volume:156 year:1988 number:4 pages:592-598 |
format_phy_str_mv |
Article |
institution |
findex.gbv.de |
isfreeaccess_bool |
false |
container_title |
Physica C: Superconductivity and its applications |
authorswithroles_txt_mv |
Ginley, D.S. @@oth@@ Kwak, J.F. @@oth@@ Hellmer, R.P. @@oth@@ Baughman, R.J. @@oth@@ Venturini, E.L. @@oth@@ Mitchell, M.A. @@oth@@ Morosin, B. @@oth@@ |
publishDateDaySort_date |
1988-01-01T00:00:00Z |
hierarchy_top_id |
NLEJ177038349 |
id |
NLEJ177930683 |
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">NLEJ177930683</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706063704.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1988 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ177930683</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ177930683</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="245" ind1="1" ind2="0"><subfield code="a">Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1988</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Elsevier Journal Backfiles on ScienceDirect 1907 - 2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ginley, D.S.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kwak, J.F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Hellmer, R.P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Baughman, R.J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Venturini, E.L.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Mitchell, M.A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Morosin, B.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Physica C: Superconductivity and its applications</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">156(1988), 4, Seite 592-598</subfield><subfield code="w">(DE-627)NLEJ177038349</subfield><subfield code="w">(DE-600)1467152-9</subfield><subfield code="x">0921-4534</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:156</subfield><subfield code="g">year:1988</subfield><subfield code="g">number:4</subfield><subfield code="g">pages:592-598</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0921-4534(88)90027-5</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_H</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SDJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">156</subfield><subfield code="j">1988</subfield><subfield code="e">4</subfield><subfield code="h">592-598</subfield></datafield></record></collection>
|
series2 |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
ppnlink_with_tag_str_mv |
@@773@@(DE-627)NLEJ177038349 |
format |
electronic Article |
delete_txt_mv |
keep |
collection |
NL |
remote_str |
true |
illustrated |
Not Illustrated |
issn |
0921-4534 |
topic_title |
Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y |
format_facet |
Elektronische Aufsätze Aufsätze Elektronische Ressource |
format_main_str_mv |
Text Zeitschrift/Artikel |
carriertype_str_mv |
zu |
author2_variant |
d g dg j k jk r h rh r b rb e v ev m m mm b m bm |
hierarchy_parent_title |
Physica C: Superconductivity and its applications |
hierarchy_parent_id |
NLEJ177038349 |
hierarchy_top_title |
Physica C: Superconductivity and its applications |
isfreeaccess_txt |
false |
familylinks_str_mv |
(DE-627)NLEJ177038349 (DE-600)1467152-9 |
title |
Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y |
spellingShingle |
Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y |
ctrlnum |
(DE-627)NLEJ177930683 (DE-599)GBVNLZ177930683 |
title_full |
Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y |
journal |
Physica C: Superconductivity and its applications |
journalStr |
Physica C: Superconductivity and its applications |
lang_code |
eng |
isOA_bool |
false |
recordtype |
marc |
publishDateSort |
1988 |
contenttype_str_mv |
zzz |
container_start_page |
592 |
container_volume |
156 |
format_se |
Elektronische Aufsätze |
title_sort |
superconducting thin films of tl"2ca"2ba"2cu"3o"y and tl"2caba"2cu"2o"y |
title_auth |
Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y |
abstract |
We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed. |
abstractGer |
We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed. |
abstract_unstemmed |
We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed. |
collection_details |
GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE |
container_issue |
4 |
title_short |
Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y |
url |
http://linkinghub.elsevier.com/retrieve/pii/0921-4534(88)90027-5 |
remote_bool |
true |
author2 |
Ginley, D.S. Kwak, J.F. Hellmer, R.P. Baughman, R.J. Venturini, E.L. Mitchell, M.A. Morosin, B. |
author2Str |
Ginley, D.S. Kwak, J.F. Hellmer, R.P. Baughman, R.J. Venturini, E.L. Mitchell, M.A. Morosin, B. |
ppnlink |
NLEJ177038349 |
mediatype_str_mv |
z |
isOA_txt |
false |
hochschulschrift_bool |
false |
author2_role |
oth oth oth oth oth oth oth |
up_date |
2024-07-06T10:21:59.599Z |
_version_ |
1803824733459841024 |
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">NLEJ177930683</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706063704.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1988 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ177930683</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ177930683</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="245" ind1="1" ind2="0"><subfield code="a">Superconducting thin films of Tl"2Ca"2Ba"2Cu"3O"y and Tl"2CaBa"2Cu"2O"y</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1988</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zzz</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">z</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">nicht spezifiziert</subfield><subfield code="b">zu</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">We present techniques for preparing unoriented polycrystalline and epitaxial superconducting thin films of the Tl"2CaBa"2Cu"2O"y and Tl"2Ca"2Ba"2Cu"3O"y phases on a wide variety of substrates. The crucial steps determining the properties of the films are shown to be the air sintering and oxygen annealing following the initial metal deposition by electron beam evaporation under a slight oxygen overpressure. A sintered Tl-Ca-Ba-Cu-O pellet is employed as a source of excess Tl during sintering and annealing of the thin film. The Tl concentration in the final films controls the nature of the intergrain connections. The films are characterized by their structural, chemical, magnetic and transport properties. Zero resistance typically occurs at 97 K for Tl"2CaBa"2Cu"2O and at 106 K for Tl"2Ca"2Ba"2Cu"3O"y. Transport critical currents of up to 110 000 A/cm^2 have been obtained at 77 K for unoriented Tl"2CaBa"2Cu"2O"y, up to 160 000 A/cm^2 for epitaxial Tl"2Ca"2Ba"2Cu"3O"y and up to 240 000 A/cm^2 for unoriented Tl"2Ca"2Cu"3O"y films with little field dependence of the critical current observed.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Elsevier Journal Backfiles on ScienceDirect 1907 - 2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ginley, D.S.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kwak, J.F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Hellmer, R.P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Baughman, R.J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Venturini, E.L.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Mitchell, M.A.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Morosin, B.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Physica C: Superconductivity and its applications</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">156(1988), 4, Seite 592-598</subfield><subfield code="w">(DE-627)NLEJ177038349</subfield><subfield code="w">(DE-600)1467152-9</subfield><subfield code="x">0921-4534</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:156</subfield><subfield code="g">year:1988</subfield><subfield code="g">number:4</subfield><subfield code="g">pages:592-598</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0921-4534(88)90027-5</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_H</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SDJ</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_NL_ARTICLE</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">156</subfield><subfield code="j">1988</subfield><subfield code="e">4</subfield><subfield code="h">592-598</subfield></datafield></record></collection>
|
score |
7.4003124 |