Loading…
Optical beam-energy modulators
Four devices are discussed. In each of these, electromagnetic waves of wavelength /spl lambda/ (which may be in the optical range) are to be used to modulate the energy of extreme relativistic charged particle beams on a scale of /spl gsim//spl lambda//2. The devices are: (1) two-wave modulators; th...
Saved in:
Published in: | IEEE journal of quantum electronics 1997-02, Vol.33 (2), p.138-146 |
---|---|
Main Author: | |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites |
Online Access: | Get full text |
Tags: |
Add Tag
No Tags, Be the first to tag this record!
|
cited_by | |
---|---|
cites | cdi_FETCH-LOGICAL-c265t-e294995ebe64ded574c8b9ebf0f52b57d31bb5c2f66335cd16804699dc270d733 |
container_end_page | 146 |
container_issue | 2 |
container_start_page | 138 |
container_title | IEEE journal of quantum electronics |
container_volume | 33 |
creator | Csonka, P.L. |
description | Four devices are discussed. In each of these, electromagnetic waves of wavelength /spl lambda/ (which may be in the optical range) are to be used to modulate the energy of extreme relativistic charged particle beams on a scale of /spl gsim//spl lambda//2. The devices are: (1) two-wave modulators; the well-known optical klystron is a special case and has been used in the past for energy modulation. The other three are proposed as appropriate alternatives, depending on the circumstances: (2) vacuum modulator; it is the simplest in construction, and its energy modulation amplitude is essentially the function of only the power carried by the wave (e.g., laser power) and not the geometry nor /spl lambda/; (3) Cherenkov modulator; and (4) resonator energy modulator. Their capabilities, including the energy modulation amplitude, and efficiency, are compared. |
doi_str_mv | 10.1109/3.552253 |
format | article |
fullrecord | <record><control><sourceid>proquest_ieee_</sourceid><recordid>TN_cdi_ieee_primary_552253</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><ieee_id>552253</ieee_id><sourcerecordid>28514937</sourcerecordid><originalsourceid>FETCH-LOGICAL-c265t-e294995ebe64ded574c8b9ebf0f52b57d31bb5c2f66335cd16804699dc270d733</originalsourceid><addsrcrecordid>eNo90MtLw0AQBvBFFKxV8OxBehDxkrqvye4epfiCQi96XvYxkUjSxN300P_elJSehmF-fDAfIbeMLhmj5lksATgHcUZmDEAXTDFxTmaUMl0YZtQlucr5d1yl1HRG7jf9UAfXLDy6tsAtpp_9ou3irnFDl_I1uahck_HmOOfk--31a_VRrDfvn6uXdRF4CUOB3EhjAD2WMmIEJYP2Bn1FK-AeVBTMewi8KkshIERWaipLY2LgikYlxJw8Trl96v52mAfb1jlg07gtdrtsuQYmjVAjfJpgSF3OCSvbp7p1aW8ZtYcCrLBTASN9OGa6PH5YJbcNdT55DpqDgpHdTaxGxNP1mPEP0URgcQ</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>28514937</pqid></control><display><type>article</type><title>Optical beam-energy modulators</title><source>IEEE Electronic Library (IEL) Journals</source><creator>Csonka, P.L.</creator><creatorcontrib>Csonka, P.L.</creatorcontrib><description>Four devices are discussed. In each of these, electromagnetic waves of wavelength /spl lambda/ (which may be in the optical range) are to be used to modulate the energy of extreme relativistic charged particle beams on a scale of /spl gsim//spl lambda//2. The devices are: (1) two-wave modulators; the well-known optical klystron is a special case and has been used in the past for energy modulation. The other three are proposed as appropriate alternatives, depending on the circumstances: (2) vacuum modulator; it is the simplest in construction, and its energy modulation amplitude is essentially the function of only the power carried by the wave (e.g., laser power) and not the geometry nor /spl lambda/; (3) Cherenkov modulator; and (4) resonator energy modulator. Their capabilities, including the energy modulation amplitude, and efficiency, are compared.</description><identifier>ISSN: 0018-9197</identifier><identifier>EISSN: 1558-1713</identifier><identifier>DOI: 10.1109/3.552253</identifier><identifier>CODEN: IEJQA7</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Amplitude modulation ; Beam optics ; Charged-particle beams ; Electromagnetic scattering ; Electromagnetism; electron and ion optics ; Exact sciences and technology ; Fundamental areas of phenomenology (including applications) ; Klystrons ; Optical beams ; Optical devices ; Optical modulation ; Optical resonators ; Particle beam optics ; Particle beams ; Physics ; Ultraviolet sources</subject><ispartof>IEEE journal of quantum electronics, 1997-02, Vol.33 (2), p.138-146</ispartof><rights>1997 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c265t-e294995ebe64ded574c8b9ebf0f52b57d31bb5c2f66335cd16804699dc270d733</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/552253$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,54796</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=2582575$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Csonka, P.L.</creatorcontrib><title>Optical beam-energy modulators</title><title>IEEE journal of quantum electronics</title><addtitle>JQE</addtitle><description>Four devices are discussed. In each of these, electromagnetic waves of wavelength /spl lambda/ (which may be in the optical range) are to be used to modulate the energy of extreme relativistic charged particle beams on a scale of /spl gsim//spl lambda//2. The devices are: (1) two-wave modulators; the well-known optical klystron is a special case and has been used in the past for energy modulation. The other three are proposed as appropriate alternatives, depending on the circumstances: (2) vacuum modulator; it is the simplest in construction, and its energy modulation amplitude is essentially the function of only the power carried by the wave (e.g., laser power) and not the geometry nor /spl lambda/; (3) Cherenkov modulator; and (4) resonator energy modulator. Their capabilities, including the energy modulation amplitude, and efficiency, are compared.</description><subject>Amplitude modulation</subject><subject>Beam optics</subject><subject>Charged-particle beams</subject><subject>Electromagnetic scattering</subject><subject>Electromagnetism; electron and ion optics</subject><subject>Exact sciences and technology</subject><subject>Fundamental areas of phenomenology (including applications)</subject><subject>Klystrons</subject><subject>Optical beams</subject><subject>Optical devices</subject><subject>Optical modulation</subject><subject>Optical resonators</subject><subject>Particle beam optics</subject><subject>Particle beams</subject><subject>Physics</subject><subject>Ultraviolet sources</subject><issn>0018-9197</issn><issn>1558-1713</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>1997</creationdate><recordtype>article</recordtype><recordid>eNo90MtLw0AQBvBFFKxV8OxBehDxkrqvye4epfiCQi96XvYxkUjSxN300P_elJSehmF-fDAfIbeMLhmj5lksATgHcUZmDEAXTDFxTmaUMl0YZtQlucr5d1yl1HRG7jf9UAfXLDy6tsAtpp_9ou3irnFDl_I1uahck_HmOOfk--31a_VRrDfvn6uXdRF4CUOB3EhjAD2WMmIEJYP2Bn1FK-AeVBTMewi8KkshIERWaipLY2LgikYlxJw8Trl96v52mAfb1jlg07gtdrtsuQYmjVAjfJpgSF3OCSvbp7p1aW8ZtYcCrLBTASN9OGa6PH5YJbcNdT55DpqDgpHdTaxGxNP1mPEP0URgcQ</recordid><startdate>19970201</startdate><enddate>19970201</enddate><creator>Csonka, P.L.</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>7U5</scope><scope>8FD</scope><scope>L7M</scope></search><sort><creationdate>19970201</creationdate><title>Optical beam-energy modulators</title><author>Csonka, P.L.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c265t-e294995ebe64ded574c8b9ebf0f52b57d31bb5c2f66335cd16804699dc270d733</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>1997</creationdate><topic>Amplitude modulation</topic><topic>Beam optics</topic><topic>Charged-particle beams</topic><topic>Electromagnetic scattering</topic><topic>Electromagnetism; electron and ion optics</topic><topic>Exact sciences and technology</topic><topic>Fundamental areas of phenomenology (including applications)</topic><topic>Klystrons</topic><topic>Optical beams</topic><topic>Optical devices</topic><topic>Optical modulation</topic><topic>Optical resonators</topic><topic>Particle beam optics</topic><topic>Particle beams</topic><topic>Physics</topic><topic>Ultraviolet sources</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Csonka, P.L.</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics & Communications Abstracts</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>IEEE journal of quantum electronics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Csonka, P.L.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Optical beam-energy modulators</atitle><jtitle>IEEE journal of quantum electronics</jtitle><stitle>JQE</stitle><date>1997-02-01</date><risdate>1997</risdate><volume>33</volume><issue>2</issue><spage>138</spage><epage>146</epage><pages>138-146</pages><issn>0018-9197</issn><eissn>1558-1713</eissn><coden>IEJQA7</coden><abstract>Four devices are discussed. In each of these, electromagnetic waves of wavelength /spl lambda/ (which may be in the optical range) are to be used to modulate the energy of extreme relativistic charged particle beams on a scale of /spl gsim//spl lambda//2. The devices are: (1) two-wave modulators; the well-known optical klystron is a special case and has been used in the past for energy modulation. The other three are proposed as appropriate alternatives, depending on the circumstances: (2) vacuum modulator; it is the simplest in construction, and its energy modulation amplitude is essentially the function of only the power carried by the wave (e.g., laser power) and not the geometry nor /spl lambda/; (3) Cherenkov modulator; and (4) resonator energy modulator. Their capabilities, including the energy modulation amplitude, and efficiency, are compared.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/3.552253</doi><tpages>9</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 0018-9197 |
ispartof | IEEE journal of quantum electronics, 1997-02, Vol.33 (2), p.138-146 |
issn | 0018-9197 1558-1713 |
language | eng |
recordid | cdi_ieee_primary_552253 |
source | IEEE Electronic Library (IEL) Journals |
subjects | Amplitude modulation Beam optics Charged-particle beams Electromagnetic scattering Electromagnetism electron and ion optics Exact sciences and technology Fundamental areas of phenomenology (including applications) Klystrons Optical beams Optical devices Optical modulation Optical resonators Particle beam optics Particle beams Physics Ultraviolet sources |
title | Optical beam-energy modulators |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-08T01%3A21%3A21IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_ieee_&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Optical%20beam-energy%20modulators&rft.jtitle=IEEE%20journal%20of%20quantum%20electronics&rft.au=Csonka,%20P.L.&rft.date=1997-02-01&rft.volume=33&rft.issue=2&rft.spage=138&rft.epage=146&rft.pages=138-146&rft.issn=0018-9197&rft.eissn=1558-1713&rft.coden=IEJQA7&rft_id=info:doi/10.1109/3.552253&rft_dat=%3Cproquest_ieee_%3E28514937%3C/proquest_ieee_%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c265t-e294995ebe64ded574c8b9ebf0f52b57d31bb5c2f66335cd16804699dc270d733%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=28514937&rft_id=info:pmid/&rft_ieee_id=552253&rfr_iscdi=true |