Antiprotons for plasma heating
Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiproto...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
|---|
| Format: |
E-Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1997 |
|---|
| Umfang: |
8 |
|---|
| Reproduktion: |
Springer Online Journal Archives 1860-2002 |
|---|---|
| Übergeordnetes Werk: |
in: Hyperfine interactions - 1975, 109(1997) vom: Jan./Apr., Seite 323-330 |
| Übergeordnetes Werk: |
volume:109 ; year:1997 ; month:01/04 ; pages:323-330 ; extent:8 |
| Links: |
|---|
| Katalog-ID: |
NLEJ19432298X |
|---|
| LEADER | 01000caa a22002652 4500 | ||
|---|---|---|---|
| 001 | NLEJ19432298X | ||
| 003 | DE-627 | ||
| 005 | 20210707225553.0 | ||
| 007 | cr uuu---uuuuu | ||
| 008 | 070526s1997 xx |||||o 00| ||eng c | ||
| 035 | |a (DE-627)NLEJ19432298X | ||
| 040 | |a DE-627 |b ger |c DE-627 |e rakwb | ||
| 041 | |a eng | ||
| 245 | 1 | 0 | |a Antiprotons for plasma heating |
| 264 | 1 | |c 1997 | |
| 300 | |a 8 | ||
| 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 Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. | ||
| 533 | |f Springer Online Journal Archives 1860-2002 | ||
| 700 | 1 | |a Huber, Felix M. |4 oth | |
| 700 | 1 | |a Messerschmid, Ernst W. |4 oth | |
| 773 | 0 | 8 | |i in |t Hyperfine interactions |d 1975 |g 109(1997) vom: Jan./Apr., Seite 323-330 |w (DE-627)NLEJ188985573 |w (DE-600)2021614-2 |x 1572-9540 |7 nnns |
| 773 | 1 | 8 | |g volume:109 |g year:1997 |g month:01/04 |g pages:323-330 |g extent:8 |
| 856 | 4 | 0 | |u http://dx.doi.org/10.1023/A:1012630106392 |
| 912 | |a GBV_USEFLAG_U | ||
| 912 | |a ZDB-1-SOJ | ||
| 912 | |a GBV_NL_ARTICLE | ||
| 951 | |a AR | ||
| 952 | |d 109 |j 1997 |c 1/4 |h 323-330 |g 8 | ||
| matchkey_str |
article:15729540:1997----::nirtnfrls |
|---|---|
| hierarchy_sort_str |
1997 |
| publishDate |
1997 |
| allfields |
(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
| spelling |
(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
| allfields_unstemmed |
(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
| allfieldsGer |
(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
| allfieldsSound |
(DE-627)NLEJ19432298X DE-627 ger DE-627 rakwb eng Antiprotons for plasma heating 1997 8 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. Springer Online Journal Archives 1860-2002 Huber, Felix M. oth Messerschmid, Ernst W. oth in Hyperfine interactions 1975 109(1997) vom: Jan./Apr., Seite 323-330 (DE-627)NLEJ188985573 (DE-600)2021614-2 1572-9540 nnns volume:109 year:1997 month:01/04 pages:323-330 extent:8 http://dx.doi.org/10.1023/A:1012630106392 GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE AR 109 1997 1/4 323-330 8 |
| language |
English |
| source |
in Hyperfine interactions 109(1997) vom: Jan./Apr., Seite 323-330 volume:109 year:1997 month:01/04 pages:323-330 extent:8 |
| sourceStr |
in Hyperfine interactions 109(1997) vom: Jan./Apr., Seite 323-330 volume:109 year:1997 month:01/04 pages:323-330 extent:8 |
| format_phy_str_mv |
Article |
| institution |
findex.gbv.de |
| isfreeaccess_bool |
false |
| container_title |
Hyperfine interactions |
| authorswithroles_txt_mv |
Huber, Felix M. @@oth@@ Messerschmid, Ernst W. @@oth@@ |
| publishDateDaySort_date |
1997-01-01T00:00:00Z |
| hierarchy_top_id |
NLEJ188985573 |
| id |
NLEJ19432298X |
| 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">NLEJ19432298X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210707225553.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070526s1997 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ19432298X</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">Antiprotons for plasma heating</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1997</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">8</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">Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Springer Online Journal Archives 1860-2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Huber, Felix M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Messerschmid, Ernst W.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Hyperfine interactions</subfield><subfield code="d">1975</subfield><subfield code="g">109(1997) vom: Jan./Apr., Seite 323-330</subfield><subfield code="w">(DE-627)NLEJ188985573</subfield><subfield code="w">(DE-600)2021614-2</subfield><subfield code="x">1572-9540</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:109</subfield><subfield code="g">year:1997</subfield><subfield code="g">month:01/04</subfield><subfield code="g">pages:323-330</subfield><subfield code="g">extent:8</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://dx.doi.org/10.1023/A:1012630106392</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SOJ</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">109</subfield><subfield code="j">1997</subfield><subfield code="c">1/4</subfield><subfield code="h">323-330</subfield><subfield code="g">8</subfield></datafield></record></collection>
|
| series2 |
Springer Online Journal Archives 1860-2002 |
| ppnlink_with_tag_str_mv |
@@773@@(DE-627)NLEJ188985573 |
| format |
electronic Article |
| delete_txt_mv |
keep |
| collection |
NL |
| remote_str |
true |
| illustrated |
Not Illustrated |
| issn |
1572-9540 |
| topic_title |
Antiprotons for plasma heating |
| format_facet |
Elektronische Aufsätze Aufsätze Elektronische Ressource |
| format_main_str_mv |
Text Zeitschrift/Artikel |
| carriertype_str_mv |
zu |
| author2_variant |
f m h fm fmh e w m ew ewm |
| hierarchy_parent_title |
Hyperfine interactions |
| hierarchy_parent_id |
NLEJ188985573 |
| hierarchy_top_title |
Hyperfine interactions |
| isfreeaccess_txt |
false |
| familylinks_str_mv |
(DE-627)NLEJ188985573 (DE-600)2021614-2 |
| title |
Antiprotons for plasma heating |
| spellingShingle |
Antiprotons for plasma heating |
| ctrlnum |
(DE-627)NLEJ19432298X |
| title_full |
Antiprotons for plasma heating |
| journal |
Hyperfine interactions |
| journalStr |
Hyperfine interactions |
| lang_code |
eng |
| isOA_bool |
false |
| recordtype |
marc |
| publishDateSort |
1997 |
| contenttype_str_mv |
zzz |
| container_start_page |
323 |
| container_volume |
109 |
| physical |
8 |
| format_se |
Elektronische Aufsätze |
| title_sort |
antiprotons for plasma heating |
| title_auth |
Antiprotons for plasma heating |
| abstract |
Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. |
| abstractGer |
Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. |
| abstract_unstemmed |
Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas. |
| collection_details |
GBV_USEFLAG_U ZDB-1-SOJ GBV_NL_ARTICLE |
| title_short |
Antiprotons for plasma heating |
| url |
http://dx.doi.org/10.1023/A:1012630106392 |
| remote_bool |
true |
| author2 |
Huber, Felix M. Messerschmid, Ernst W. |
| author2Str |
Huber, Felix M. Messerschmid, Ernst W. |
| ppnlink |
NLEJ188985573 |
| mediatype_str_mv |
z |
| isOA_txt |
false |
| hochschulschrift_bool |
false |
| author2_role |
oth oth |
| up_date |
2024-07-06T00:24:15.843Z |
| _version_ |
1803787127589175296 |
| 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">NLEJ19432298X</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210707225553.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070526s1997 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ19432298X</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">Antiprotons for plasma heating</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1997</subfield></datafield><datafield tag="300" ind1=" " ind2=" "><subfield code="a">8</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">Abstract The design of the new Antiproton Decelerator (AD) at CERN will allow the easy measurement of the energy deposit of the antiproton-proton annihilation remnants within a hydrogen plasma. For this purpose, a reaction chamber filled with gaseous hydrogen is put into the beam line. The antiprotons coming directly from the AD at 7 MeV/c or from a Penning trap are injected into the chamber through a window in such a way, that they come to rest at the center of the chamber, where annihilation occurs. The resulting high energy annihilation products are trapped in the chamber using a pulsed magnetic bottle. The energy deposit in the hydrogen gas can then be measured using Schlieren optics or an interferometric set-up, by determining the density changes due to the temperature rise within the gas.</subfield></datafield><datafield tag="533" ind1=" " ind2=" "><subfield code="f">Springer Online Journal Archives 1860-2002</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Huber, Felix M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Messerschmid, Ernst W.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Hyperfine interactions</subfield><subfield code="d">1975</subfield><subfield code="g">109(1997) vom: Jan./Apr., Seite 323-330</subfield><subfield code="w">(DE-627)NLEJ188985573</subfield><subfield code="w">(DE-600)2021614-2</subfield><subfield code="x">1572-9540</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:109</subfield><subfield code="g">year:1997</subfield><subfield code="g">month:01/04</subfield><subfield code="g">pages:323-330</subfield><subfield code="g">extent:8</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://dx.doi.org/10.1023/A:1012630106392</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">GBV_USEFLAG_U</subfield></datafield><datafield tag="912" ind1=" " ind2=" "><subfield code="a">ZDB-1-SOJ</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">109</subfield><subfield code="j">1997</subfield><subfield code="c">1/4</subfield><subfield code="h">323-330</subfield><subfield code="g">8</subfield></datafield></record></collection>
|
| score |
7.4005327 |