A high-finesse Fabry–Perot cavity with a frequency-doubled green laser for precision Compton polarimetry at Jefferson Lab
A high-finesse Fabry–Perot cavity with a frequency-doubled continuous wave green laser (532nm) has been built and installed in Hall A of Jefferson Lab for high precision Compton polarimetry. The infrared (1064nm) beam from a ytterbium-doped fiber amplifier seeded by a Nd:YAG nonplanar ring oscillato...
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creator | Rakhman, A. Hafez, M. Nanda, S. Benmokhtar, F. Camsonne, A. Cates, G.D. Dalton, M.M. Franklin, G.B. Friend, M. Michaels, R.W. Nelyubin, V. Parno, D.S. Paschke, K.D. Quinn, B.P. Souder, P.A. Tobias, W.A. |
description | A high-finesse Fabry–Perot cavity with a frequency-doubled continuous wave green laser (532nm) has been built and installed in Hall A of Jefferson Lab for high precision Compton polarimetry. The infrared (1064nm) beam from a ytterbium-doped fiber amplifier seeded by a Nd:YAG nonplanar ring oscillator laser is frequency doubled in a single-pass periodically poled MgO:LiNbO3 crystal. The maximum achieved green power at 5W infrared pump power is 1.74W with a total conversion efficiency of 34.8%. The green beam is injected into the optical resonant cavity and enhanced up to 3.7kW with a corresponding enhancement of 3800. The polarization transfer function has been measured in order to determine the intra-cavity circular laser polarization within a measurement uncertainty of 0.7%. The PREx experiment at Jefferson Lab used this system for the first time and achieved 1.0% precision in polarization measurements of an electron beam with energy and current of 1.06GeV and 50μA. |
doi_str_mv | 10.1016/j.nima.2016.03.085 |
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The infrared (1064nm) beam from a ytterbium-doped fiber amplifier seeded by a Nd:YAG nonplanar ring oscillator laser is frequency doubled in a single-pass periodically poled MgO:LiNbO3 crystal. The maximum achieved green power at 5W infrared pump power is 1.74W with a total conversion efficiency of 34.8%. The green beam is injected into the optical resonant cavity and enhanced up to 3.7kW with a corresponding enhancement of 3800. The polarization transfer function has been measured in order to determine the intra-cavity circular laser polarization within a measurement uncertainty of 0.7%. The PREx experiment at Jefferson Lab used this system for the first time and achieved 1.0% precision in polarization measurements of an electron beam with energy and current of 1.06GeV and 50μA.</description><identifier>ISSN: 0168-9002</identifier><identifier>EISSN: 1872-9576</identifier><identifier>DOI: 10.1016/j.nima.2016.03.085</identifier><language>eng</language><publisher>United States: Elsevier B.V</publisher><subject>Beams (radiation) ; Compton polarimetry ; Fabry-Perot ; Fabry–Perot cavity ; Holes ; INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY ; Laser beams ; Laser polarization ; Lasers ; Nuclear power generation ; Polarimetry ; Polarization ; Polarized electron beam</subject><ispartof>Nuclear instruments & methods in physics research. 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Section A, Accelerators, spectrometers, detectors and associated equipment</title><description>A high-finesse Fabry–Perot cavity with a frequency-doubled continuous wave green laser (532nm) has been built and installed in Hall A of Jefferson Lab for high precision Compton polarimetry. The infrared (1064nm) beam from a ytterbium-doped fiber amplifier seeded by a Nd:YAG nonplanar ring oscillator laser is frequency doubled in a single-pass periodically poled MgO:LiNbO3 crystal. The maximum achieved green power at 5W infrared pump power is 1.74W with a total conversion efficiency of 34.8%. The green beam is injected into the optical resonant cavity and enhanced up to 3.7kW with a corresponding enhancement of 3800. The polarization transfer function has been measured in order to determine the intra-cavity circular laser polarization within a measurement uncertainty of 0.7%. The PREx experiment at Jefferson Lab used this system for the first time and achieved 1.0% precision in polarization measurements of an electron beam with energy and current of 1.06GeV and 50μA.</description><subject>Beams (radiation)</subject><subject>Compton polarimetry</subject><subject>Fabry-Perot</subject><subject>Fabry–Perot cavity</subject><subject>Holes</subject><subject>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</subject><subject>Laser beams</subject><subject>Laser polarization</subject><subject>Lasers</subject><subject>Nuclear power generation</subject><subject>Polarimetry</subject><subject>Polarization</subject><subject>Polarized electron beam</subject><issn>0168-9002</issn><issn>1872-9576</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><recordid>eNp9UcuO1DAQtBBIDAs_wMnixCXBz8SWuKxGLA-NBAc4W47T3vEoEwfbsyjiwj_wh3wJjoYzfemWuqpV1YXQS0paSmj35tTO4WxbVueW8JYo-QjtqOpZo2XfPUa7ulCNJoQ9Rc9yPpFaulc79PMWH8P9sfFhhpwB39khrX9-_f4CKRbs7EMoK_4RyhFb7BN8v8Ds1maMl2GCEd8ngBlPNkPCPia8JHAhhzjjfTwvpfYlTjaFM5S0YlvwJ_AeUq6Lgx2eoyfeThle_Os36Nvdu6_7D83h8_uP-9tD4wQRpfGks8T1XFIxdIMeZSf0oJhnnkurleKWUsEckE5z4jwBcEoAVZ2UWkDv-A16db0bcwkmu1DAHV2cZ3DFUCYk5bqCXl9BS4rVZS7mHLKDabIzxEs2VDEpRE8Zr1B2hboUc07gzVIt2rQaSswWhzmZLQ6zxWEINzWOSnp7JUF1-hAgbULqM2EMadMxxvA_-l_9aZU3</recordid><startdate>20160621</startdate><enddate>20160621</enddate><creator>Rakhman, A.</creator><creator>Hafez, M.</creator><creator>Nanda, S.</creator><creator>Benmokhtar, F.</creator><creator>Camsonne, A.</creator><creator>Cates, G.D.</creator><creator>Dalton, M.M.</creator><creator>Franklin, G.B.</creator><creator>Friend, M.</creator><creator>Michaels, R.W.</creator><creator>Nelyubin, V.</creator><creator>Parno, D.S.</creator><creator>Paschke, K.D.</creator><creator>Quinn, B.P.</creator><creator>Souder, P.A.</creator><creator>Tobias, W.A.</creator><general>Elsevier B.V</general><general>Elsevier</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7U5</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><scope>OIOZB</scope><scope>OTOTI</scope></search><sort><creationdate>20160621</creationdate><title>A high-finesse Fabry–Perot cavity with a frequency-doubled green laser for precision Compton polarimetry at Jefferson Lab</title><author>Rakhman, A. ; Hafez, M. ; Nanda, S. ; Benmokhtar, F. ; Camsonne, A. ; Cates, G.D. ; Dalton, M.M. ; Franklin, G.B. ; Friend, M. ; Michaels, R.W. ; Nelyubin, V. ; Parno, D.S. ; Paschke, K.D. ; Quinn, B.P. ; Souder, P.A. ; Tobias, W.A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c404t-f06a0c73514b6b9d5649b82f2f35a9883a1142ce06930cf0eec84e1865594e7c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>Beams (radiation)</topic><topic>Compton polarimetry</topic><topic>Fabry-Perot</topic><topic>Fabry–Perot cavity</topic><topic>Holes</topic><topic>INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY</topic><topic>Laser beams</topic><topic>Laser polarization</topic><topic>Lasers</topic><topic>Nuclear power generation</topic><topic>Polarimetry</topic><topic>Polarization</topic><topic>Polarized electron beam</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Rakhman, A.</creatorcontrib><creatorcontrib>Hafez, M.</creatorcontrib><creatorcontrib>Nanda, S.</creatorcontrib><creatorcontrib>Benmokhtar, F.</creatorcontrib><creatorcontrib>Camsonne, A.</creatorcontrib><creatorcontrib>Cates, G.D.</creatorcontrib><creatorcontrib>Dalton, M.M.</creatorcontrib><creatorcontrib>Franklin, G.B.</creatorcontrib><creatorcontrib>Friend, M.</creatorcontrib><creatorcontrib>Michaels, R.W.</creatorcontrib><creatorcontrib>Nelyubin, V.</creatorcontrib><creatorcontrib>Parno, D.S.</creatorcontrib><creatorcontrib>Paschke, K.D.</creatorcontrib><creatorcontrib>Quinn, B.P.</creatorcontrib><creatorcontrib>Souder, P.A.</creatorcontrib><creatorcontrib>Tobias, W.A.</creatorcontrib><creatorcontrib>Thomas Jefferson National Accelerator Facility (TJNAF), Newport News, VA (United States)</creatorcontrib><collection>CrossRef</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>OSTI.GOV - Hybrid</collection><collection>OSTI.GOV</collection><jtitle>Nuclear instruments & methods in physics research. 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The polarization transfer function has been measured in order to determine the intra-cavity circular laser polarization within a measurement uncertainty of 0.7%. The PREx experiment at Jefferson Lab used this system for the first time and achieved 1.0% precision in polarization measurements of an electron beam with energy and current of 1.06GeV and 50μA.</abstract><cop>United States</cop><pub>Elsevier B.V</pub><doi>10.1016/j.nima.2016.03.085</doi><tpages>15</tpages><oa>free_for_read</oa></addata></record> |
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source | Elsevier ScienceDirect Journals |
subjects | Beams (radiation) Compton polarimetry Fabry-Perot Fabry–Perot cavity Holes INSTRUMENTATION RELATED TO NUCLEAR SCIENCE AND TECHNOLOGY Laser beams Laser polarization Lasers Nuclear power generation Polarimetry Polarization Polarized electron beam |
title | A high-finesse Fabry–Perot cavity with a frequency-doubled green laser for precision Compton polarimetry at Jefferson Lab |
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