A cylindrically symmetric “micro-Mott” electron polarimeter

A small, novel, cylindrically symmetric Mott electron polarimeter is described. The effective Sherman function, Seff , or analyzing power, for 20 kV Au target bias with a 1.3 keV energy loss window is 0.16 ± 0.01, where uncertainty in the measurement is due primarily to uncertainty in the incident e...

Ausführliche Beschreibung

Gespeichert in:
Bibliographische Detailangaben
Veröffentlicht in:Review of scientific instruments 2016-05, Vol.87 (5), p.053302-053302
Hauptverfasser: Clayburn, N. B., Brunkow, E., Burtwistle, S. J., Rutherford, G. H., Gay, T. J.
Format: Artikel
Sprache:eng
Schlagworte:
Online-Zugang:Volltext
Tags: Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
container_end_page 053302
container_issue 5
container_start_page 053302
container_title Review of scientific instruments
container_volume 87
creator Clayburn, N. B.
Brunkow, E.
Burtwistle, S. J.
Rutherford, G. H.
Gay, T. J.
description A small, novel, cylindrically symmetric Mott electron polarimeter is described. The effective Sherman function, Seff , or analyzing power, for 20 kV Au target bias with a 1.3 keV energy loss window is 0.16 ± 0.01, where uncertainty in the measurement is due primarily to uncertainty in the incident electron polarization. For an energy loss window of 0.5 keV, Seff reaches its maximum value of 0.24 ± 0.02. The device’s maximum efficiency, I/Io , defined as the detected count rate divided by the incident particle rate, is 3.7 ± 0.2 × 10−4 at 20 keV. The figure-of-merit of the device, η, is defined as S eff 2 I I o and equals 9.0 ± 1.6 × 10−6. Potential sources of false asymmetries due to detector electronic asymmetry and beam misalignment have been investigated. The new polarimeter’s performance is compared to published results for similar compact retarding-field Mott polarimeters, and it is concluded that this device has a relatively large Seff and low efficiency. SIMION® electron trajectory simulations and Sherman function calculations are presented to explain the differences in performance between this device and previous designs. This design has an Seff that is insensitive to spatial beam fluctuations and, for an energy loss window >0.5 keV, negligible background due to spurious ion and X-ray production at the target.
doi_str_mv 10.1063/1.4946995
format Article
fullrecord <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_1793901163</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>1793901163</sourcerecordid><originalsourceid>FETCH-LOGICAL-c418t-3fb3064e4dbd796f898ae51a561070ddf5383e2fc8f033ae90767b16ad31122c3</originalsourceid><addsrcrecordid>eNp90N9KwzAUBvAgipvTC19ACt6o0JnTtElzJWP4DxRv9DqkaQodbVOTVujdHkRfbk9iZHOCgrk5BH58yfkQOgY8BUzJJUxjHlPOkx00BpzykNGI7KIxxiQOKYvTETpwboH9SQD20ShiUYJjzMfoahaooSqb3JZKVtUQuKGudedvwWr5XpfKmvDRdN1q-RHoSqvOmiZoTSVt6Zm2h2ivkJXTR5s5QS8318_zu_Dh6fZ-PnsIVQxpF5IiI5jGOs6znHFapDyVOgGZUMAM53mRkJToqFBpgQmRmmNGWQZU5gQgihSZoLN1bmvNa69dJ-rSKV1VstGmdwIYJxwDUOLp6S-6ML1t_O9EBJGHDGji1fla-Q2ds7oQrV9J2kEAFl-tChCbVr092ST2Wa3zrfyu0YOLNXCq7GRXmmZr3oz9SRJtXvyH_z79CajBjjo</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2121797165</pqid></control><display><type>article</type><title>A cylindrically symmetric “micro-Mott” electron polarimeter</title><source>AIP Journals Complete</source><source>Alma/SFX Local Collection</source><creator>Clayburn, N. B. ; Brunkow, E. ; Burtwistle, S. J. ; Rutherford, G. H. ; Gay, T. J.</creator><creatorcontrib>Clayburn, N. B. ; Brunkow, E. ; Burtwistle, S. J. ; Rutherford, G. H. ; Gay, T. J.</creatorcontrib><description>A small, novel, cylindrically symmetric Mott electron polarimeter is described. The effective Sherman function, Seff , or analyzing power, for 20 kV Au target bias with a 1.3 keV energy loss window is 0.16 ± 0.01, where uncertainty in the measurement is due primarily to uncertainty in the incident electron polarization. For an energy loss window of 0.5 keV, Seff reaches its maximum value of 0.24 ± 0.02. The device’s maximum efficiency, I/Io , defined as the detected count rate divided by the incident particle rate, is 3.7 ± 0.2 × 10−4 at 20 keV. The figure-of-merit of the device, η, is defined as S eff 2 I I o and equals 9.0 ± 1.6 × 10−6. Potential sources of false asymmetries due to detector electronic asymmetry and beam misalignment have been investigated. The new polarimeter’s performance is compared to published results for similar compact retarding-field Mott polarimeters, and it is concluded that this device has a relatively large Seff and low efficiency. SIMION® electron trajectory simulations and Sherman function calculations are presented to explain the differences in performance between this device and previous designs. This design has an Seff that is insensitive to spatial beam fluctuations and, for an energy loss window &gt;0.5 keV, negligible background due to spurious ion and X-ray production at the target.</description><identifier>ISSN: 0034-6748</identifier><identifier>EISSN: 1089-7623</identifier><identifier>DOI: 10.1063/1.4946995</identifier><identifier>PMID: 27250409</identifier><identifier>CODEN: RSINAK</identifier><language>eng</language><publisher>United States: American Institute of Physics</publisher><subject>Background radiation ; Electron trajectories ; Electrons ; Energy dissipation ; Misalignment ; Polarimeters ; Scientific apparatus &amp; instruments ; Uncertainty ; Variation ; Windows (computer programs)</subject><ispartof>Review of scientific instruments, 2016-05, Vol.87 (5), p.053302-053302</ispartof><rights>Author(s)</rights><rights>2016 Author(s). Published by AIP Publishing.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c418t-3fb3064e4dbd796f898ae51a561070ddf5383e2fc8f033ae90767b16ad31122c3</citedby><cites>FETCH-LOGICAL-c418t-3fb3064e4dbd796f898ae51a561070ddf5383e2fc8f033ae90767b16ad31122c3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/rsi/article-lookup/doi/10.1063/1.4946995$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,784,794,4512,27924,27925,76384</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/27250409$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Clayburn, N. B.</creatorcontrib><creatorcontrib>Brunkow, E.</creatorcontrib><creatorcontrib>Burtwistle, S. J.</creatorcontrib><creatorcontrib>Rutherford, G. H.</creatorcontrib><creatorcontrib>Gay, T. J.</creatorcontrib><title>A cylindrically symmetric “micro-Mott” electron polarimeter</title><title>Review of scientific instruments</title><addtitle>Rev Sci Instrum</addtitle><description>A small, novel, cylindrically symmetric Mott electron polarimeter is described. The effective Sherman function, Seff , or analyzing power, for 20 kV Au target bias with a 1.3 keV energy loss window is 0.16 ± 0.01, where uncertainty in the measurement is due primarily to uncertainty in the incident electron polarization. For an energy loss window of 0.5 keV, Seff reaches its maximum value of 0.24 ± 0.02. The device’s maximum efficiency, I/Io , defined as the detected count rate divided by the incident particle rate, is 3.7 ± 0.2 × 10−4 at 20 keV. The figure-of-merit of the device, η, is defined as S eff 2 I I o and equals 9.0 ± 1.6 × 10−6. Potential sources of false asymmetries due to detector electronic asymmetry and beam misalignment have been investigated. The new polarimeter’s performance is compared to published results for similar compact retarding-field Mott polarimeters, and it is concluded that this device has a relatively large Seff and low efficiency. SIMION® electron trajectory simulations and Sherman function calculations are presented to explain the differences in performance between this device and previous designs. This design has an Seff that is insensitive to spatial beam fluctuations and, for an energy loss window &gt;0.5 keV, negligible background due to spurious ion and X-ray production at the target.</description><subject>Background radiation</subject><subject>Electron trajectories</subject><subject>Electrons</subject><subject>Energy dissipation</subject><subject>Misalignment</subject><subject>Polarimeters</subject><subject>Scientific apparatus &amp; instruments</subject><subject>Uncertainty</subject><subject>Variation</subject><subject>Windows (computer programs)</subject><issn>0034-6748</issn><issn>1089-7623</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNp90N9KwzAUBvAgipvTC19ACt6o0JnTtElzJWP4DxRv9DqkaQodbVOTVujdHkRfbk9iZHOCgrk5BH58yfkQOgY8BUzJJUxjHlPOkx00BpzykNGI7KIxxiQOKYvTETpwboH9SQD20ShiUYJjzMfoahaooSqb3JZKVtUQuKGudedvwWr5XpfKmvDRdN1q-RHoSqvOmiZoTSVt6Zm2h2ivkJXTR5s5QS8318_zu_Dh6fZ-PnsIVQxpF5IiI5jGOs6znHFapDyVOgGZUMAM53mRkJToqFBpgQmRmmNGWQZU5gQgihSZoLN1bmvNa69dJ-rSKV1VstGmdwIYJxwDUOLp6S-6ML1t_O9EBJGHDGji1fla-Q2ds7oQrV9J2kEAFl-tChCbVr092ST2Wa3zrfyu0YOLNXCq7GRXmmZr3oz9SRJtXvyH_z79CajBjjo</recordid><startdate>20160501</startdate><enddate>20160501</enddate><creator>Clayburn, N. B.</creator><creator>Brunkow, E.</creator><creator>Burtwistle, S. J.</creator><creator>Rutherford, G. H.</creator><creator>Gay, T. J.</creator><general>American Institute of Physics</general><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>7X8</scope></search><sort><creationdate>20160501</creationdate><title>A cylindrically symmetric “micro-Mott” electron polarimeter</title><author>Clayburn, N. B. ; Brunkow, E. ; Burtwistle, S. J. ; Rutherford, G. H. ; Gay, T. J.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c418t-3fb3064e4dbd796f898ae51a561070ddf5383e2fc8f033ae90767b16ad31122c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Background radiation</topic><topic>Electron trajectories</topic><topic>Electrons</topic><topic>Energy dissipation</topic><topic>Misalignment</topic><topic>Polarimeters</topic><topic>Scientific apparatus &amp; instruments</topic><topic>Uncertainty</topic><topic>Variation</topic><topic>Windows (computer programs)</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Clayburn, N. B.</creatorcontrib><creatorcontrib>Brunkow, E.</creatorcontrib><creatorcontrib>Burtwistle, S. J.</creatorcontrib><creatorcontrib>Rutherford, G. H.</creatorcontrib><creatorcontrib>Gay, T. J.</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>MEDLINE - Academic</collection><jtitle>Review of scientific instruments</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Clayburn, N. B.</au><au>Brunkow, E.</au><au>Burtwistle, S. J.</au><au>Rutherford, G. H.</au><au>Gay, T. J.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>A cylindrically symmetric “micro-Mott” electron polarimeter</atitle><jtitle>Review of scientific instruments</jtitle><addtitle>Rev Sci Instrum</addtitle><date>2016-05-01</date><risdate>2016</risdate><volume>87</volume><issue>5</issue><spage>053302</spage><epage>053302</epage><pages>053302-053302</pages><issn>0034-6748</issn><eissn>1089-7623</eissn><coden>RSINAK</coden><abstract>A small, novel, cylindrically symmetric Mott electron polarimeter is described. The effective Sherman function, Seff , or analyzing power, for 20 kV Au target bias with a 1.3 keV energy loss window is 0.16 ± 0.01, where uncertainty in the measurement is due primarily to uncertainty in the incident electron polarization. For an energy loss window of 0.5 keV, Seff reaches its maximum value of 0.24 ± 0.02. The device’s maximum efficiency, I/Io , defined as the detected count rate divided by the incident particle rate, is 3.7 ± 0.2 × 10−4 at 20 keV. The figure-of-merit of the device, η, is defined as S eff 2 I I o and equals 9.0 ± 1.6 × 10−6. Potential sources of false asymmetries due to detector electronic asymmetry and beam misalignment have been investigated. The new polarimeter’s performance is compared to published results for similar compact retarding-field Mott polarimeters, and it is concluded that this device has a relatively large Seff and low efficiency. SIMION® electron trajectory simulations and Sherman function calculations are presented to explain the differences in performance between this device and previous designs. This design has an Seff that is insensitive to spatial beam fluctuations and, for an energy loss window &gt;0.5 keV, negligible background due to spurious ion and X-ray production at the target.</abstract><cop>United States</cop><pub>American Institute of Physics</pub><pmid>27250409</pmid><doi>10.1063/1.4946995</doi><tpages>8</tpages><oa>free_for_read</oa></addata></record>
fulltext fulltext
identifier ISSN: 0034-6748
ispartof Review of scientific instruments, 2016-05, Vol.87 (5), p.053302-053302
issn 0034-6748
1089-7623
language eng
recordid cdi_proquest_miscellaneous_1793901163
source AIP Journals Complete; Alma/SFX Local Collection
subjects Background radiation
Electron trajectories
Electrons
Energy dissipation
Misalignment
Polarimeters
Scientific apparatus & instruments
Uncertainty
Variation
Windows (computer programs)
title A cylindrically symmetric “micro-Mott” electron polarimeter
url https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-26T19%3A37%3A07IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=A%20cylindrically%20symmetric%20%E2%80%9Cmicro-Mott%E2%80%9D%20electron%20polarimeter&rft.jtitle=Review%20of%20scientific%20instruments&rft.au=Clayburn,%20N.%20B.&rft.date=2016-05-01&rft.volume=87&rft.issue=5&rft.spage=053302&rft.epage=053302&rft.pages=053302-053302&rft.issn=0034-6748&rft.eissn=1089-7623&rft.coden=RSINAK&rft_id=info:doi/10.1063/1.4946995&rft_dat=%3Cproquest_cross%3E1793901163%3C/proquest_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_pqid=2121797165&rft_id=info:pmid/27250409&rfr_iscdi=true