ExB and angular effects in the avalanche localization along the wire with cathode pad read-out
A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the...
Ausführliche Beschreibung
Gespeichert in:
| Autor*in: |
|---|
| Format: |
E-Artikel |
|---|---|
| Sprache: |
Englisch |
| Erschienen: |
1983 |
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| Reproduktion: |
Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
|---|---|
| Übergeordnetes Werk: |
in: Nuclear Instruments and Methods In Physics Research - Amsterdam : Elsevier, 217(1983), 1-2, Seite 317-321 |
| Übergeordnetes Werk: |
volume:217 ; year:1983 ; number:1-2 ; pages:317-321 |
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NLEJ180612433 |
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| 520 | |a A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal. | ||
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| 700 | 1 | |a Batignani, G. |4 oth | |
| 700 | 1 | |a Dris, M. |4 oth | |
| 700 | 1 | |a Fidecaro, F. |4 oth | |
| 700 | 1 | |a Liello, F. |4 oth | |
| 700 | 1 | |a May, J. |4 oth | |
| 700 | 1 | |a Meyer, T. |4 oth | |
| 700 | 1 | |a Milotti, E. |4 oth | |
| 700 | 1 | |a Ragusa, F. |4 oth | |
| 700 | 1 | |a Richstein, J. |4 oth | |
| 700 | 1 | |a Rolandi, L. |4 oth | |
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(DE-627)NLEJ180612433 (DE-599)GBVNLZ180612433 DE-627 ger DE-627 rakwb eng ExB and angular effects in the avalanche localization along the wire with cathode pad read-out 1983 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Amendolia, S.R. oth Batignani, G. oth Dris, M. oth Fidecaro, F. oth Liello, F. oth May, J. oth Meyer, T. oth Milotti, E. oth Ragusa, F. oth Richstein, J. oth Rolandi, L. oth in Nuclear Instruments and Methods In Physics Research Amsterdam : Elsevier 217(1983), 1-2, Seite 317-321 (DE-627)NLEJ180600451 (DE-600)1466532-3 0167-5087 nnns volume:217 year:1983 number:1-2 pages:317-321 http://linkinghub.elsevier.com/retrieve/pii/0167-5087(83)90156-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 217 1983 1-2 317-321 |
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(DE-627)NLEJ180612433 (DE-599)GBVNLZ180612433 DE-627 ger DE-627 rakwb eng ExB and angular effects in the avalanche localization along the wire with cathode pad read-out 1983 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Amendolia, S.R. oth Batignani, G. oth Dris, M. oth Fidecaro, F. oth Liello, F. oth May, J. oth Meyer, T. oth Milotti, E. oth Ragusa, F. oth Richstein, J. oth Rolandi, L. oth in Nuclear Instruments and Methods In Physics Research Amsterdam : Elsevier 217(1983), 1-2, Seite 317-321 (DE-627)NLEJ180600451 (DE-600)1466532-3 0167-5087 nnns volume:217 year:1983 number:1-2 pages:317-321 http://linkinghub.elsevier.com/retrieve/pii/0167-5087(83)90156-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 217 1983 1-2 317-321 |
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(DE-627)NLEJ180612433 (DE-599)GBVNLZ180612433 DE-627 ger DE-627 rakwb eng ExB and angular effects in the avalanche localization along the wire with cathode pad read-out 1983 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Amendolia, S.R. oth Batignani, G. oth Dris, M. oth Fidecaro, F. oth Liello, F. oth May, J. oth Meyer, T. oth Milotti, E. oth Ragusa, F. oth Richstein, J. oth Rolandi, L. oth in Nuclear Instruments and Methods In Physics Research Amsterdam : Elsevier 217(1983), 1-2, Seite 317-321 (DE-627)NLEJ180600451 (DE-600)1466532-3 0167-5087 nnns volume:217 year:1983 number:1-2 pages:317-321 http://linkinghub.elsevier.com/retrieve/pii/0167-5087(83)90156-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 217 1983 1-2 317-321 |
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(DE-627)NLEJ180612433 (DE-599)GBVNLZ180612433 DE-627 ger DE-627 rakwb eng ExB and angular effects in the avalanche localization along the wire with cathode pad read-out 1983 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Amendolia, S.R. oth Batignani, G. oth Dris, M. oth Fidecaro, F. oth Liello, F. oth May, J. oth Meyer, T. oth Milotti, E. oth Ragusa, F. oth Richstein, J. oth Rolandi, L. oth in Nuclear Instruments and Methods In Physics Research Amsterdam : Elsevier 217(1983), 1-2, Seite 317-321 (DE-627)NLEJ180600451 (DE-600)1466532-3 0167-5087 nnns volume:217 year:1983 number:1-2 pages:317-321 http://linkinghub.elsevier.com/retrieve/pii/0167-5087(83)90156-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 217 1983 1-2 317-321 |
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(DE-627)NLEJ180612433 (DE-599)GBVNLZ180612433 DE-627 ger DE-627 rakwb eng ExB and angular effects in the avalanche localization along the wire with cathode pad read-out 1983 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Amendolia, S.R. oth Batignani, G. oth Dris, M. oth Fidecaro, F. oth Liello, F. oth May, J. oth Meyer, T. oth Milotti, E. oth Ragusa, F. oth Richstein, J. oth Rolandi, L. oth in Nuclear Instruments and Methods In Physics Research Amsterdam : Elsevier 217(1983), 1-2, Seite 317-321 (DE-627)NLEJ180600451 (DE-600)1466532-3 0167-5087 nnns volume:217 year:1983 number:1-2 pages:317-321 http://linkinghub.elsevier.com/retrieve/pii/0167-5087(83)90156-4 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 217 1983 1-2 317-321 |
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exb and angular effects in the avalanche localization along the wire with cathode pad read-out |
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ExB and angular effects in the avalanche localization along the wire with cathode pad read-out |
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A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal. |
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A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal. |
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A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal. |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a22002652 4500</leader><controlfield tag="001">NLEJ180612433</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706132216.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1983 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ180612433</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ180612433</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">ExB and angular effects in the avalanche localization along the wire with cathode pad read-out</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1983</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">A proportional drift chamber with a segmented cathode for the localization of the avalanche along the wire has been used to study the resolution in the presence of a magnetic field perpendicular to the cathode plane (ExB effect) and for tracks parallel to this plane but inclined with respect to the wires' direction (angular effect). Both effects are dominated by the clustering of the primary ionization. The ExB effect is reduced when several wires contribute to the cathode signal. The angular effect is reduced applying a correction for the fluctuations of the charge on the wires contributing to the cathode signal.</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">Amendolia, S.R.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Batignani, G.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Dris, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Fidecaro, F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Liello, F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">May, J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Meyer, T.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Milotti, E.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Ragusa, F.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Richstein, J.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Rolandi, L.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">in</subfield><subfield code="t">Nuclear Instruments and Methods In Physics Research</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">217(1983), 1-2, Seite 317-321</subfield><subfield code="w">(DE-627)NLEJ180600451</subfield><subfield code="w">(DE-600)1466532-3</subfield><subfield code="x">0167-5087</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:217</subfield><subfield code="g">year:1983</subfield><subfield code="g">number:1-2</subfield><subfield code="g">pages:317-321</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0167-5087(83)90156-4</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">217</subfield><subfield code="j">1983</subfield><subfield code="e">1-2</subfield><subfield code="h">317-321</subfield></datafield></record></collection>
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