The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment
Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate...
Ausführliche Beschreibung
Autor*in: |
Topko, Yu. A. [verfasserIn] |
---|
Format: |
Artikel |
---|---|
Sprache: |
Englisch |
Erschienen: |
2022 |
---|
Anmerkung: |
© Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. |
---|
Übergeordnetes Werk: |
Enthalten in: Physics of particles and nuclei - Pleiades Publishing, 1993, 53(2022), 2 vom: Apr., Seite 398-402 |
---|---|
Übergeordnetes Werk: |
volume:53 ; year:2022 ; number:2 ; month:04 ; pages:398-402 |
Links: |
---|
DOI / URN: |
10.1134/S1063779622020812 |
---|
Katalog-ID: |
OLC2130454828 |
---|
LEADER | 01000naa a22002652 4500 | ||
---|---|---|---|
001 | OLC2130454828 | ||
003 | DE-627 | ||
005 | 20230506014211.0 | ||
007 | tu | ||
008 | 230506s2022 xx ||||| 00| ||eng c | ||
024 | 7 | |a 10.1134/S1063779622020812 |2 doi | |
035 | |a (DE-627)OLC2130454828 | ||
035 | |a (DE-He213)S1063779622020812-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 Topko, Yu. A. |e verfasserin |4 aut | |
245 | 1 | 4 | |a The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment |
264 | 1 | |c 2022 | |
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 © Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. | ||
520 | |a Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker. | ||
700 | 1 | |a Khabarov, S. V. |4 aut | |
700 | 1 | |a Zamyatin, N. I. |4 aut | |
700 | 1 | |a Topko, B. L. |4 aut | |
700 | 1 | |a Tarasov, O. G. |4 aut | |
700 | 1 | |a Zubarev, E. V. |4 aut | |
700 | 1 | |a Kopylov, Yu. A. |4 aut | |
700 | 1 | |a Streletskaya, E. A. |4 aut | |
773 | 0 | 8 | |i Enthalten in |t Physics of particles and nuclei |d Pleiades Publishing, 1993 |g 53(2022), 2 vom: Apr., Seite 398-402 |w (DE-627)171192710 |w (DE-600)1163604-X |w (DE-576)038718081 |x 1063-7796 |7 nnns |
773 | 1 | 8 | |g volume:53 |g year:2022 |g number:2 |g month:04 |g pages:398-402 |
856 | 4 | 1 | |u https://doi.org/10.1134/S1063779622020812 |z lizenzpflichtig |3 Volltext |
912 | |a GBV_USEFLAG_A | ||
912 | |a SYSFLAG_A | ||
912 | |a GBV_OLC | ||
912 | |a SSG-OLC-PHY | ||
951 | |a AR | ||
952 | |d 53 |j 2022 |e 2 |c 04 |h 398-402 |
author_variant |
y a t ya yat s v k sv svk n i z ni niz b l t bl blt o g t og ogt e v z ev evz y a k ya yak e a s ea eas |
---|---|
matchkey_str |
article:10637796:2022----::hdvlpetfiiobatakrnbapoioe |
hierarchy_sort_str |
2022 |
publishDate |
2022 |
allfields |
10.1134/S1063779622020812 doi (DE-627)OLC2130454828 (DE-He213)S1063779622020812-p DE-627 ger DE-627 rakwb eng 530 VZ Topko, Yu. A. verfasserin aut The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker. Khabarov, S. V. aut Zamyatin, N. I. aut Topko, B. L. aut Tarasov, O. G. aut Zubarev, E. V. aut Kopylov, Yu. A. aut Streletskaya, E. A. aut Enthalten in Physics of particles and nuclei Pleiades Publishing, 1993 53(2022), 2 vom: Apr., Seite 398-402 (DE-627)171192710 (DE-600)1163604-X (DE-576)038718081 1063-7796 nnns volume:53 year:2022 number:2 month:04 pages:398-402 https://doi.org/10.1134/S1063779622020812 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 53 2022 2 04 398-402 |
spelling |
10.1134/S1063779622020812 doi (DE-627)OLC2130454828 (DE-He213)S1063779622020812-p DE-627 ger DE-627 rakwb eng 530 VZ Topko, Yu. A. verfasserin aut The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker. Khabarov, S. V. aut Zamyatin, N. I. aut Topko, B. L. aut Tarasov, O. G. aut Zubarev, E. V. aut Kopylov, Yu. A. aut Streletskaya, E. A. aut Enthalten in Physics of particles and nuclei Pleiades Publishing, 1993 53(2022), 2 vom: Apr., Seite 398-402 (DE-627)171192710 (DE-600)1163604-X (DE-576)038718081 1063-7796 nnns volume:53 year:2022 number:2 month:04 pages:398-402 https://doi.org/10.1134/S1063779622020812 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 53 2022 2 04 398-402 |
allfields_unstemmed |
10.1134/S1063779622020812 doi (DE-627)OLC2130454828 (DE-He213)S1063779622020812-p DE-627 ger DE-627 rakwb eng 530 VZ Topko, Yu. A. verfasserin aut The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker. Khabarov, S. V. aut Zamyatin, N. I. aut Topko, B. L. aut Tarasov, O. G. aut Zubarev, E. V. aut Kopylov, Yu. A. aut Streletskaya, E. A. aut Enthalten in Physics of particles and nuclei Pleiades Publishing, 1993 53(2022), 2 vom: Apr., Seite 398-402 (DE-627)171192710 (DE-600)1163604-X (DE-576)038718081 1063-7796 nnns volume:53 year:2022 number:2 month:04 pages:398-402 https://doi.org/10.1134/S1063779622020812 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 53 2022 2 04 398-402 |
allfieldsGer |
10.1134/S1063779622020812 doi (DE-627)OLC2130454828 (DE-He213)S1063779622020812-p DE-627 ger DE-627 rakwb eng 530 VZ Topko, Yu. A. verfasserin aut The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker. Khabarov, S. V. aut Zamyatin, N. I. aut Topko, B. L. aut Tarasov, O. G. aut Zubarev, E. V. aut Kopylov, Yu. A. aut Streletskaya, E. A. aut Enthalten in Physics of particles and nuclei Pleiades Publishing, 1993 53(2022), 2 vom: Apr., Seite 398-402 (DE-627)171192710 (DE-600)1163604-X (DE-576)038718081 1063-7796 nnns volume:53 year:2022 number:2 month:04 pages:398-402 https://doi.org/10.1134/S1063779622020812 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 53 2022 2 04 398-402 |
allfieldsSound |
10.1134/S1063779622020812 doi (DE-627)OLC2130454828 (DE-He213)S1063779622020812-p DE-627 ger DE-627 rakwb eng 530 VZ Topko, Yu. A. verfasserin aut The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment 2022 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier © Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker. Khabarov, S. V. aut Zamyatin, N. I. aut Topko, B. L. aut Tarasov, O. G. aut Zubarev, E. V. aut Kopylov, Yu. A. aut Streletskaya, E. A. aut Enthalten in Physics of particles and nuclei Pleiades Publishing, 1993 53(2022), 2 vom: Apr., Seite 398-402 (DE-627)171192710 (DE-600)1163604-X (DE-576)038718081 1063-7796 nnns volume:53 year:2022 number:2 month:04 pages:398-402 https://doi.org/10.1134/S1063779622020812 lizenzpflichtig Volltext GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY AR 53 2022 2 04 398-402 |
language |
English |
source |
Enthalten in Physics of particles and nuclei 53(2022), 2 vom: Apr., Seite 398-402 volume:53 year:2022 number:2 month:04 pages:398-402 |
sourceStr |
Enthalten in Physics of particles and nuclei 53(2022), 2 vom: Apr., Seite 398-402 volume:53 year:2022 number:2 month:04 pages:398-402 |
format_phy_str_mv |
Article |
institution |
findex.gbv.de |
dewey-raw |
530 |
isfreeaccess_bool |
false |
container_title |
Physics of particles and nuclei |
authorswithroles_txt_mv |
Topko, Yu. A. @@aut@@ Khabarov, S. V. @@aut@@ Zamyatin, N. I. @@aut@@ Topko, B. L. @@aut@@ Tarasov, O. G. @@aut@@ Zubarev, E. V. @@aut@@ Kopylov, Yu. A. @@aut@@ Streletskaya, E. A. @@aut@@ |
publishDateDaySort_date |
2022-04-01T00:00:00Z |
hierarchy_top_id |
171192710 |
dewey-sort |
3530 |
id |
OLC2130454828 |
language_de |
englisch |
fullrecord |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000naa a22002652 4500</leader><controlfield tag="001">OLC2130454828</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230506014211.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">230506s2022 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1134/S1063779622020812</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2130454828</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)S1063779622020812-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">Topko, Yu. A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="4"><subfield code="a">The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</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">© Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Khabarov, S. V.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zamyatin, N. I.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Topko, B. L.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Tarasov, O. G.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zubarev, E. V.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kopylov, Yu. A.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Streletskaya, E. A.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Physics of particles and nuclei</subfield><subfield code="d">Pleiades Publishing, 1993</subfield><subfield code="g">53(2022), 2 vom: Apr., Seite 398-402</subfield><subfield code="w">(DE-627)171192710</subfield><subfield code="w">(DE-600)1163604-X</subfield><subfield code="w">(DE-576)038718081</subfield><subfield code="x">1063-7796</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:53</subfield><subfield code="g">year:2022</subfield><subfield code="g">number:2</subfield><subfield code="g">month:04</subfield><subfield code="g">pages:398-402</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1134/S1063779622020812</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="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">53</subfield><subfield code="j">2022</subfield><subfield code="e">2</subfield><subfield code="c">04</subfield><subfield code="h">398-402</subfield></datafield></record></collection>
|
author |
Topko, Yu. A. |
spellingShingle |
Topko, Yu. A. ddc 530 The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment |
authorStr |
Topko, Yu. A. |
ppnlink_with_tag_str_mv |
@@773@@(DE-627)171192710 |
format |
Article |
dewey-ones |
530 - Physics |
delete_txt_mv |
keep |
author_role |
aut aut aut aut aut aut aut aut |
collection |
OLC |
remote_str |
false |
illustrated |
Not Illustrated |
issn |
1063-7796 |
topic_title |
530 VZ The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment |
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 |
Physics of particles and nuclei |
hierarchy_parent_id |
171192710 |
dewey-tens |
530 - Physics |
hierarchy_top_title |
Physics of particles and nuclei |
isfreeaccess_txt |
false |
familylinks_str_mv |
(DE-627)171192710 (DE-600)1163604-X (DE-576)038718081 |
title |
The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment |
ctrlnum |
(DE-627)OLC2130454828 (DE-He213)S1063779622020812-p |
title_full |
The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment |
author_sort |
Topko, Yu. A. |
journal |
Physics of particles and nuclei |
journalStr |
Physics of particles and nuclei |
lang_code |
eng |
isOA_bool |
false |
dewey-hundreds |
500 - Science |
recordtype |
marc |
publishDateSort |
2022 |
contenttype_str_mv |
txt |
container_start_page |
398 |
author_browse |
Topko, Yu. A. Khabarov, S. V. Zamyatin, N. I. Topko, B. L. Tarasov, O. G. Zubarev, E. V. Kopylov, Yu. A. Streletskaya, E. A. |
container_volume |
53 |
class |
530 VZ |
format_se |
Aufsätze |
author-letter |
Topko, Yu. A. |
doi_str_mv |
10.1134/S1063779622020812 |
dewey-full |
530 |
title_sort |
development of silicon beam tracker and beam profilometer at the bmn experiment |
title_auth |
The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment |
abstract |
Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker. © Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. |
abstractGer |
Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker. © Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. |
abstract_unstemmed |
Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker. © Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2. |
collection_details |
GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY |
container_issue |
2 |
title_short |
The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment |
url |
https://doi.org/10.1134/S1063779622020812 |
remote_bool |
false |
author2 |
Khabarov, S. V. Zamyatin, N. I. Topko, B. L. Tarasov, O. G. Zubarev, E. V. Kopylov, Yu. A. Streletskaya, E. A. |
author2Str |
Khabarov, S. V. Zamyatin, N. I. Topko, B. L. Tarasov, O. G. Zubarev, E. V. Kopylov, Yu. A. Streletskaya, E. A. |
ppnlink |
171192710 |
mediatype_str_mv |
n |
isOA_txt |
false |
hochschulschrift_bool |
false |
doi_str |
10.1134/S1063779622020812 |
up_date |
2024-07-04T05:14:57.715Z |
_version_ |
1803624222776360960 |
fullrecord_marcxml |
<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000naa a22002652 4500</leader><controlfield tag="001">OLC2130454828</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20230506014211.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">230506s2022 xx ||||| 00| ||eng c</controlfield><datafield tag="024" ind1="7" ind2=" "><subfield code="a">10.1134/S1063779622020812</subfield><subfield code="2">doi</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC2130454828</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-He213)S1063779622020812-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">Topko, Yu. A.</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="4"><subfield code="a">The Development of Silicon Beam Tracker and Beam Profilometer at the BMN Experiment</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2022</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">© Pleiades Publishing, Ltd. 2022. ISSN 1063-7796, Physics of Particles and Nuclei, 2022, Vol. 53, No. 2, pp. 398–402. © Pleiades Publishing, Ltd., 2022. Russian Text © The Author(s), 2022, published in Fizika Elementarnykh Chastits i Atomnogo Yadra, 2022, Vol. 53, No. 2.</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">Abstract In the BMN experiment with a fixed target, a beam profilometer is used to tune the ion beam extracted from the Nuclotron accelerator (Joint Institute for Nuclear Research, Dubna), and a beam tracker is used to determine the reaction plane. The profilometer and tracker consist of coordinate planes based on thin (175 μm) double-sided silicon strip detectors placed in front of the target inside a vacuum beam pipe. The physical program of the BM@N experiment includes the use of a wide variety of accelerated ions (from carbon to gold with energies of up to 4 GeV/nucleon). To detect signals in a large dynamic range, the following two modifications of detector electronics are chosen: one with high amplification for light ions, and another one with low amplification for heavy ions. This article describes the design and main parameters of the profilometer and tracker.</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Khabarov, S. V.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zamyatin, N. I.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Topko, B. L.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Tarasov, O. G.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Zubarev, E. V.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Kopylov, Yu. A.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="700" ind1="1" ind2=" "><subfield code="a">Streletskaya, E. A.</subfield><subfield code="4">aut</subfield></datafield><datafield tag="773" ind1="0" ind2="8"><subfield code="i">Enthalten in</subfield><subfield code="t">Physics of particles and nuclei</subfield><subfield code="d">Pleiades Publishing, 1993</subfield><subfield code="g">53(2022), 2 vom: Apr., Seite 398-402</subfield><subfield code="w">(DE-627)171192710</subfield><subfield code="w">(DE-600)1163604-X</subfield><subfield code="w">(DE-576)038718081</subfield><subfield code="x">1063-7796</subfield><subfield code="7">nnns</subfield></datafield><datafield tag="773" ind1="1" ind2="8"><subfield code="g">volume:53</subfield><subfield code="g">year:2022</subfield><subfield code="g">number:2</subfield><subfield code="g">month:04</subfield><subfield code="g">pages:398-402</subfield></datafield><datafield tag="856" ind1="4" ind2="1"><subfield code="u">https://doi.org/10.1134/S1063779622020812</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="951" ind1=" " ind2=" "><subfield code="a">AR</subfield></datafield><datafield tag="952" ind1=" " ind2=" "><subfield code="d">53</subfield><subfield code="j">2022</subfield><subfield code="e">2</subfield><subfield code="c">04</subfield><subfield code="h">398-402</subfield></datafield></record></collection>
|
score |
7.3980246 |