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...
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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 |
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, 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.</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 & 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 >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 & 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 & 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 >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> |
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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 |
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