Test of a full scale sector for a 1 m long high resolution vertex chamber
We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial lay...
Ausführliche Beschreibung
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Englisch |
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1986 |
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Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 |
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in: Nuclear Instruments and Methods in Physics Research Section A: - Amsterdam : Elsevier, 252(1986), 2-3, Seite 379-383 |
Übergeordnetes Werk: |
volume:252 ; year:1986 ; number:2-3 ; pages:379-383 |
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NLEJ180948482 |
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520 | |a We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer. | ||
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(DE-627)NLEJ180948482 (DE-599)GBVNLZ180948482 DE-627 ger DE-627 rakwb eng Test of a full scale sector for a 1 m long high resolution vertex chamber 1986 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Deutschmann, M. oth Hawelka, P. oth Herten, U. oth Tonutti, M. oth in Nuclear Instruments and Methods in Physics Research Section A: Amsterdam : Elsevier 252(1986), 2-3, Seite 379-383 (DE-627)NLEJ180854372 (DE-600)1466532-3 0168-9002 nnns volume:252 year:1986 number:2-3 pages:379-383 http://linkinghub.elsevier.com/retrieve/pii/0168-9002(86)91208-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 252 1986 2-3 379-383 |
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(DE-627)NLEJ180948482 (DE-599)GBVNLZ180948482 DE-627 ger DE-627 rakwb eng Test of a full scale sector for a 1 m long high resolution vertex chamber 1986 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Deutschmann, M. oth Hawelka, P. oth Herten, U. oth Tonutti, M. oth in Nuclear Instruments and Methods in Physics Research Section A: Amsterdam : Elsevier 252(1986), 2-3, Seite 379-383 (DE-627)NLEJ180854372 (DE-600)1466532-3 0168-9002 nnns volume:252 year:1986 number:2-3 pages:379-383 http://linkinghub.elsevier.com/retrieve/pii/0168-9002(86)91208-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 252 1986 2-3 379-383 |
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(DE-627)NLEJ180948482 (DE-599)GBVNLZ180948482 DE-627 ger DE-627 rakwb eng Test of a full scale sector for a 1 m long high resolution vertex chamber 1986 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Deutschmann, M. oth Hawelka, P. oth Herten, U. oth Tonutti, M. oth in Nuclear Instruments and Methods in Physics Research Section A: Amsterdam : Elsevier 252(1986), 2-3, Seite 379-383 (DE-627)NLEJ180854372 (DE-600)1466532-3 0168-9002 nnns volume:252 year:1986 number:2-3 pages:379-383 http://linkinghub.elsevier.com/retrieve/pii/0168-9002(86)91208-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 252 1986 2-3 379-383 |
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(DE-627)NLEJ180948482 (DE-599)GBVNLZ180948482 DE-627 ger DE-627 rakwb eng Test of a full scale sector for a 1 m long high resolution vertex chamber 1986 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Deutschmann, M. oth Hawelka, P. oth Herten, U. oth Tonutti, M. oth in Nuclear Instruments and Methods in Physics Research Section A: Amsterdam : Elsevier 252(1986), 2-3, Seite 379-383 (DE-627)NLEJ180854372 (DE-600)1466532-3 0168-9002 nnns volume:252 year:1986 number:2-3 pages:379-383 http://linkinghub.elsevier.com/retrieve/pii/0168-9002(86)91208-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 252 1986 2-3 379-383 |
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(DE-627)NLEJ180948482 (DE-599)GBVNLZ180948482 DE-627 ger DE-627 rakwb eng Test of a full scale sector for a 1 m long high resolution vertex chamber 1986 nicht spezifiziert zzz rdacontent nicht spezifiziert z rdamedia nicht spezifiziert zu rdacarrier We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer. Elsevier Journal Backfiles on ScienceDirect 1907 - 2002 Deutschmann, M. oth Hawelka, P. oth Herten, U. oth Tonutti, M. oth in Nuclear Instruments and Methods in Physics Research Section A: Amsterdam : Elsevier 252(1986), 2-3, Seite 379-383 (DE-627)NLEJ180854372 (DE-600)1466532-3 0168-9002 nnns volume:252 year:1986 number:2-3 pages:379-383 http://linkinghub.elsevier.com/retrieve/pii/0168-9002(86)91208-8 GBV_USEFLAG_H ZDB-1-SDJ GBV_NL_ARTICLE AR 252 1986 2-3 379-383 |
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test of a full scale sector for a 1 m long high resolution vertex chamber |
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Test of a full scale sector for a 1 m long high resolution vertex chamber |
abstract |
We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer. |
abstractGer |
We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer. |
abstract_unstemmed |
We have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer. |
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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">NLEJ180948482</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20210706141348.0</controlfield><controlfield tag="007">cr uuu---uuuuu</controlfield><controlfield tag="008">070505s1986 xx |||||o 00| ||eng c</controlfield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)NLEJ180948482</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVNLZ180948482</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">Test of a full scale sector for a 1 m long high resolution vertex chamber</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">1986</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 have tested a 1 m long prototype sector consisting of 170 rectangular drift cells. The sector is arranged in 25 radial layers, of which the 13 inner layers have cell sizes of 10 mm x 15 mm and the 12 outer layers of 14 mm x 21 mm. To measure the coordinates of a track along the wire, 13 axial layers are interleaved with 12 stereo layers. Special care was taken to keep cell sizes as homogeneous as possible to obtain the same space vs drift-time relation for all layers of the same cell size.A low diffusion gas mixture of 85% CO"2 plus 15% isobutane was used in a closed loop gas system, including a purifier, run at an absolute pressure of 1 and 2 bar and stabilized within a few mbars by a microprocessor system.The chamber signals were read-out with TDCs. In the central part of the drift length we achieved space resolutions of 35 μm per cell at atmospheric pressure and 25 μm per cell at 2 bar pressure. These figures correspond to axial resolutions of 0.5 to 1 mm per stereo layer.</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">Deutschmann, M.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Hawelka, P.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Herten, U.</subfield><subfield code="4">oth</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Tonutti, M.</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 Section A:</subfield><subfield code="d">Amsterdam : Elsevier</subfield><subfield code="g">252(1986), 2-3, Seite 379-383</subfield><subfield code="w">(DE-627)NLEJ180854372</subfield><subfield code="w">(DE-600)1466532-3</subfield><subfield code="x">0168-9002</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:252</subfield><subfield code="g">year:1986</subfield><subfield code="g">number:2-3</subfield><subfield code="g">pages:379-383</subfield></datafield><datafield tag="856" ind1="4" ind2="0"><subfield code="u">http://linkinghub.elsevier.com/retrieve/pii/0168-9002(86)91208-8</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">252</subfield><subfield code="j">1986</subfield><subfield code="e">2-3</subfield><subfield code="h">379-383</subfield></datafield></record></collection>
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