Modulated structure and superconductivity in 2D electron-hole lattice system
Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
Kuwata, S. [verfasserIn] |
|---|
| Format: |
Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1994 |
|---|
| Anmerkung: |
© Plenum Publishing Corporation 1994 |
|---|
| Übergeordnetes Werk: |
Enthalten in: Journal of superconductivity - Kluwer Academic Publishers-Plenum Publishers, 1988, 7(1994), 4 vom: Aug., Seite 777-781 |
|---|---|
| Übergeordnetes Werk: |
volume:7 ; year:1994 ; number:4 ; month:08 ; pages:777-781 |
| Links: |
|---|
| DOI / URN: |
10.1007/BF00721663 |
|---|
| Katalog-ID: |
OLC2057263487 |
|---|
| LEADER | 01000caa a22002652 4500 | ||
|---|---|---|---|
| 001 | OLC2057263487 | ||
| 003 | DE-627 | ||
| 005 | 20230503152717.0 | ||
| 007 | tu | ||
| 008 | 200819s1994 xx ||||| 00| ||eng c | ||
| 024 | 7 | |a 10.1007/BF00721663 |2 doi | |
| 035 | |a (DE-627)OLC2057263487 | ||
| 035 | |a (DE-He213)BF00721663-p | ||
| 040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
| 041 | |a eng | ||
| 082 | 0 | 4 | |a 530 |q VZ |
| 100 | 1 | |a Kuwata, S. |e verfasserin |4 aut | |
| 245 | 1 | 0 | |a Modulated structure and superconductivity in 2D electron-hole lattice system |
| 264 | 1 | |c 1994 | |
| 336 | |a Text |b txt |2 rdacontent | ||
| 337 | |a ohne Hilfsmittel zu benutzen |b n |2 rdamedia | ||
| 338 | |a Band |b nc |2 rdacarrier | ||
| 500 | |a © Plenum Publishing Corporation 1994 | ||
| 520 | |a Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. | ||
| 700 | 1 | |a Kinase, W. |4 aut | |
| 773 | 0 | 8 | |i Enthalten in |t Journal of superconductivity |d Kluwer Academic Publishers-Plenum Publishers, 1988 |g 7(1994), 4 vom: Aug., Seite 777-781 |w (DE-627)130413186 |w (DE-600)623132-9 |w (DE-576)01866539X |x 0896-1107 |7 nnns |
| 773 | 1 | 8 | |g volume:7 |g year:1994 |g number:4 |g month:08 |g pages:777-781 |
| 856 | 4 | 1 | |u https://doi.org/10.1007/BF00721663 |z lizenzpflichtig |3 Volltext |
| 912 | |a GBV_USEFLAG_A | ||
| 912 | |a SYSFLAG_A | ||
| 912 | |a GBV_OLC | ||
| 912 | |a SSG-OLC-PHY | ||
| 912 | |a GBV_ILN_40 | ||
| 912 | |a GBV_ILN_70 | ||
| 912 | |a GBV_ILN_4036 | ||
| 912 | |a GBV_ILN_4313 | ||
| 912 | |a GBV_ILN_4318 | ||
| 951 | |a AR | ||
| 952 | |d 7 |j 1994 |e 4 |c 08 |h 777-781 | ||
| author_variant |
s k sk w k wk |
|---|---|
| matchkey_str |
article:08961107:1994----::ouaesrcuensprodciiyndlcr |
| hierarchy_sort_str |
1994 |
| publishDate |
1994 |
| allfields |
10.1007/BF00721663 doi (DE-627)OLC2057263487 (DE-He213)BF00721663-p DE-627 ger DE-627 rakwb eng 530 VZ Kuwata, S. verfasserin aut Modulated structure and superconductivity in 2D electron-hole lattice system 1994 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. Kinase, W. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 7(1994), 4 vom: Aug., Seite 777-781 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:7 year:1994 number:4 month:08 pages:777-781 https://doi.org/10.1007/BF00721663 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 AR 7 1994 4 08 777-781 |
| spelling |
10.1007/BF00721663 doi (DE-627)OLC2057263487 (DE-He213)BF00721663-p DE-627 ger DE-627 rakwb eng 530 VZ Kuwata, S. verfasserin aut Modulated structure and superconductivity in 2D electron-hole lattice system 1994 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. Kinase, W. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 7(1994), 4 vom: Aug., Seite 777-781 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:7 year:1994 number:4 month:08 pages:777-781 https://doi.org/10.1007/BF00721663 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 AR 7 1994 4 08 777-781 |
| allfields_unstemmed |
10.1007/BF00721663 doi (DE-627)OLC2057263487 (DE-He213)BF00721663-p DE-627 ger DE-627 rakwb eng 530 VZ Kuwata, S. verfasserin aut Modulated structure and superconductivity in 2D electron-hole lattice system 1994 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. Kinase, W. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 7(1994), 4 vom: Aug., Seite 777-781 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:7 year:1994 number:4 month:08 pages:777-781 https://doi.org/10.1007/BF00721663 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 AR 7 1994 4 08 777-781 |
| allfieldsGer |
10.1007/BF00721663 doi (DE-627)OLC2057263487 (DE-He213)BF00721663-p DE-627 ger DE-627 rakwb eng 530 VZ Kuwata, S. verfasserin aut Modulated structure and superconductivity in 2D electron-hole lattice system 1994 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. Kinase, W. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 7(1994), 4 vom: Aug., Seite 777-781 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:7 year:1994 number:4 month:08 pages:777-781 https://doi.org/10.1007/BF00721663 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 AR 7 1994 4 08 777-781 |
| allfieldsSound |
10.1007/BF00721663 doi (DE-627)OLC2057263487 (DE-He213)BF00721663-p DE-627 ger DE-627 rakwb eng 530 VZ Kuwata, S. verfasserin aut Modulated structure and superconductivity in 2D electron-hole lattice system 1994 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Plenum Publishing Corporation 1994 Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. Kinase, W. aut Enthalten in Journal of superconductivity Kluwer Academic Publishers-Plenum Publishers, 1988 7(1994), 4 vom: Aug., Seite 777-781 (DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X 0896-1107 nnns volume:7 year:1994 number:4 month:08 pages:777-781 https://doi.org/10.1007/BF00721663 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 AR 7 1994 4 08 777-781 |
| language |
English |
| source |
Enthalten in Journal of superconductivity 7(1994), 4 vom: Aug., Seite 777-781 volume:7 year:1994 number:4 month:08 pages:777-781 |
| sourceStr |
Enthalten in Journal of superconductivity 7(1994), 4 vom: Aug., Seite 777-781 volume:7 year:1994 number:4 month:08 pages:777-781 |
| format_phy_str_mv |
Article |
| institution |
findex.gbv.de |
| dewey-raw |
530 |
| isfreeaccess_bool |
false |
| container_title |
Journal of superconductivity |
| authorswithroles_txt_mv |
Kuwata, S. @@aut@@ Kinase, W. @@aut@@ |
| publishDateDaySort_date |
1994-08-01T00:00:00Z |
| hierarchy_top_id |
130413186 |
| dewey-sort |
3530 |
| id |
OLC2057263487 |
| 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">OLC2057263487</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503152717.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s1994 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF00721663</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2057263487</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF00721663-p</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">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Kuwata, S.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Modulated structure and superconductivity in 2D electron-hole lattice system</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1994</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">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Plenum Publishing Corporation 1994</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kinase, W.</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">Kluwer Academic Publishers-Plenum Publishers, 1988</subfield><subfield code="g">7(1994), 4 vom: Aug., Seite 777-781</subfield><subfield code="w">(DE-627)130413186</subfield><subfield code="w">(DE-600)623132-9</subfield><subfield code="w">(DE-576)01866539X</subfield><subfield code="x">0896-1107</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:7</subfield><subfield code="g">year:1994</subfield><subfield code="g">number:4</subfield><subfield code="g">month:08</subfield><subfield code="g">pages:777-781</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF00721663</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_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</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_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4036</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4318</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">7</subfield><subfield code="j">1994</subfield><subfield code="e">4</subfield><subfield code="c">08</subfield><subfield code="h">777-781</subfield></datafield></record></collection>
|
| author |
Kuwata, S. |
| spellingShingle |
Kuwata, S. ddc 530 Modulated structure and superconductivity in 2D electron-hole lattice system |
| authorStr |
Kuwata, S. |
| ppnlink_with_tag_str_mv |
@@773@@(DE-627)130413186 |
| format |
Article |
| dewey-ones |
530 - Physics |
| delete_txt_mv |
keep |
| author_role |
aut aut |
| collection |
OLC |
| remote_str |
false |
| illustrated |
Not Illustrated |
| issn |
0896-1107 |
| topic_title |
530 VZ Modulated structure and superconductivity in 2D electron-hole lattice system |
| topic |
ddc 530 |
| topic_unstemmed |
ddc 530 |
| topic_browse |
ddc 530 |
| format_facet |
Aufsätze Gedruckte Aufsätze |
| format_main_str_mv |
Text Zeitschrift/Artikel |
| carriertype_str_mv |
nc |
| hierarchy_parent_title |
Journal of superconductivity |
| hierarchy_parent_id |
130413186 |
| dewey-tens |
530 - Physics |
| hierarchy_top_title |
Journal of superconductivity |
| isfreeaccess_txt |
false |
| familylinks_str_mv |
(DE-627)130413186 (DE-600)623132-9 (DE-576)01866539X |
| title |
Modulated structure and superconductivity in 2D electron-hole lattice system |
| ctrlnum |
(DE-627)OLC2057263487 (DE-He213)BF00721663-p |
| title_full |
Modulated structure and superconductivity in 2D electron-hole lattice system |
| author_sort |
Kuwata, S. |
| journal |
Journal of superconductivity |
| journalStr |
Journal of superconductivity |
| lang_code |
eng |
| isOA_bool |
false |
| dewey-hundreds |
500 - Science |
| recordtype |
marc |
| publishDateSort |
1994 |
| contenttype_str_mv |
txt |
| container_start_page |
777 |
| author_browse |
Kuwata, S. Kinase, W. |
| container_volume |
7 |
| class |
530 VZ |
| format_se |
Aufsätze |
| author-letter |
Kuwata, S. |
| doi_str_mv |
10.1007/BF00721663 |
| dewey-full |
530 |
| title_sort |
modulated structure and superconductivity in 2d electron-hole lattice system |
| title_auth |
Modulated structure and superconductivity in 2D electron-hole lattice system |
| abstract |
Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. © Plenum Publishing Corporation 1994 |
| abstractGer |
Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. © Plenum Publishing Corporation 1994 |
| abstract_unstemmed |
Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively. © Plenum Publishing Corporation 1994 |
| collection_details |
GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_40 GBV_ILN_70 GBV_ILN_4036 GBV_ILN_4313 GBV_ILN_4318 |
| container_issue |
4 |
| title_short |
Modulated structure and superconductivity in 2D electron-hole lattice system |
| url |
https://doi.org/10.1007/BF00721663 |
| remote_bool |
false |
| author2 |
Kinase, W. |
| author2Str |
Kinase, W. |
| ppnlink |
130413186 |
| mediatype_str_mv |
n |
| isOA_txt |
false |
| hochschulschrift_bool |
false |
| doi_str |
10.1007/BF00721663 |
| up_date |
2024-07-03T14:32:09.791Z |
| _version_ |
1803568681885630464 |
| 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">OLC2057263487</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230503152717.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">200819s1994 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1007/BF00721663</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2057263487</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)BF00721663-p</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">VZ</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Kuwata, S.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Modulated structure and superconductivity in 2D electron-hole lattice system</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1994</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">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="500" ind1=" " ind2=" "><subfield code="a">© Plenum Publishing Corporation 1994</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract The close relationship between modulated structures and superconductivity in high-$ T_{c} $ oxide superconductors is explained by using a two-dimensional (2D) electron-hole lattice. The 2D electron-hole lattice is constructed on the crystal surface or between adjacent layers by neutralizing polarization charges caused by a local polarization along thec-axis. The local polarization in the oxide superconductors is often accompanied by a modulated structure, with the modulation period corresponding to the length of one side of the 2D electron-hole lattice,D. Assuming that the Cooper pairs can be formed through the exchange of the “phonons” of the 2D electron-hole lattice oscillation, we show that both the optimum carrier density and the peak value of the transition temperature are approximately proportional toD−3/2 andD−2, respectively, and that for a typical value ofD ∼ 15 Å, they are estimated to be on the order of $ 10^{14} $/$ cm^{2} $ and 100 K, respectively.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kinase, W.</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">Kluwer Academic Publishers-Plenum Publishers, 1988</subfield><subfield code="g">7(1994), 4 vom: Aug., Seite 777-781</subfield><subfield code="w">(DE-627)130413186</subfield><subfield code="w">(DE-600)623132-9</subfield><subfield code="w">(DE-576)01866539X</subfield><subfield code="x">0896-1107</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:7</subfield><subfield code="g">year:1994</subfield><subfield code="g">number:4</subfield><subfield code="g">month:08</subfield><subfield code="g">pages:777-781</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1007/BF00721663</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_OLC</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">SSG-OLC-PHY</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_70</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4036</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4313</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_ILN_4318</subfield></datafield><datafield tag="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">7</subfield><subfield code="j">1994</subfield><subfield code="e">4</subfield><subfield code="c">08</subfield><subfield code="h">777-781</subfield></datafield></record></collection>
|
| score |
7.399741 |