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Efficient terahertz (THz) generation by nonlinear mixing of bicolor top-hat lasers in hot plasma
We report a theoretical model of radially polarized terahertz (THz) wave emission by nonlinear mixing of bicolor, radially polarized lasers having a top-hat envelope profile [ s ( profile index ) ≥ 1] in density modulated hot plasma. We investigate the effect of the laser profile index on the em...
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Published in: | Physics of plasmas 2020-02, Vol.27 (2) |
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container_title | Physics of plasmas |
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creator | Manendra Singh, Kunwar Pal Bhati, Ruchi Malik, Anil K |
description | We report a theoretical model of radially polarized terahertz (THz) wave emission by nonlinear mixing of bicolor, radially polarized lasers having a top-hat envelope profile [
s
(
profile
index
)
≥
1] in density modulated hot plasma. We investigate the effect of the laser profile index on the emitted THz field profile and found that THz field amplitude and peak location changes with the laser profile index. Our numerical investigations show that THz field amplitude is the highest around
ω
p
≈
ω
1
−
ω
2 (where
ω
p is the plasma frequency and
ω
1
and
ω
2 are the laser frequencies). We observe that phase matching can be achieved with the help of the plasma density modulation wave number. The plasma density modulation wave number increases with electron temperature and decreases with the frequency mismatch between
ω
p and
ω
1
−
ω
2. We found that the conversion efficiency is maximum at
ω
1
−
ω
2
≈
ω
p and increases fivefold with an increase in electron thermal velocity (
v
th) from
v
th
=
0 to
v
th
=
0.2
c, where c is the speed of light. |
doi_str_mv | 10.1063/1.5121913 |
format | article |
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s
(
profile
index
)
≥
1] in density modulated hot plasma. We investigate the effect of the laser profile index on the emitted THz field profile and found that THz field amplitude and peak location changes with the laser profile index. Our numerical investigations show that THz field amplitude is the highest around
ω
p
≈
ω
1
−
ω
2 (where
ω
p is the plasma frequency and
ω
1
and
ω
2 are the laser frequencies). We observe that phase matching can be achieved with the help of the plasma density modulation wave number. The plasma density modulation wave number increases with electron temperature and decreases with the frequency mismatch between
ω
p and
ω
1
−
ω
2. We found that the conversion efficiency is maximum at
ω
1
−
ω
2
≈
ω
p and increases fivefold with an increase in electron thermal velocity (
v
th) from
v
th
=
0 to
v
th
=
0.2
c, where c is the speed of light.</description><identifier>ISSN: 1070-664X</identifier><identifier>EISSN: 1089-7674</identifier><identifier>DOI: 10.1063/1.5121913</identifier><identifier>CODEN: PHPAEN</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Amplitudes ; Electron energy ; Lasers ; Modulation ; Phase matching ; Plasma ; Plasma density ; Plasma frequencies ; Plasma physics ; Wavelengths</subject><ispartof>Physics of plasmas, 2020-02, Vol.27 (2)</ispartof><rights>Author(s)</rights><rights>2020 Author(s). Published under license by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c292t-c1afaf3622e7dc476220e37c9755261dab8f58677fc13ca637323b130239ba003</citedby><cites>FETCH-LOGICAL-c292t-c1afaf3622e7dc476220e37c9755261dab8f58677fc13ca637323b130239ba003</cites><orcidid>0000-0002-0100-1625 ; 0000-0002-9653-3068 ; 0000-0001-7185-2866</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/pop/article-lookup/doi/10.1063/1.5121913$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,780,782,784,795,27924,27925,76383</link.rule.ids></links><search><creatorcontrib>Manendra</creatorcontrib><creatorcontrib>Singh, Kunwar Pal</creatorcontrib><creatorcontrib>Bhati, Ruchi</creatorcontrib><creatorcontrib>Malik, Anil K</creatorcontrib><title>Efficient terahertz (THz) generation by nonlinear mixing of bicolor top-hat lasers in hot plasma</title><title>Physics of plasmas</title><description>We report a theoretical model of radially polarized terahertz (THz) wave emission by nonlinear mixing of bicolor, radially polarized lasers having a top-hat envelope profile [
s
(
profile
index
)
≥
1] in density modulated hot plasma. We investigate the effect of the laser profile index on the emitted THz field profile and found that THz field amplitude and peak location changes with the laser profile index. Our numerical investigations show that THz field amplitude is the highest around
ω
p
≈
ω
1
−
ω
2 (where
ω
p is the plasma frequency and
ω
1
and
ω
2 are the laser frequencies). We observe that phase matching can be achieved with the help of the plasma density modulation wave number. The plasma density modulation wave number increases with electron temperature and decreases with the frequency mismatch between
ω
p and
ω
1
−
ω
2. We found that the conversion efficiency is maximum at
ω
1
−
ω
2
≈
ω
p and increases fivefold with an increase in electron thermal velocity (
v
th) from
v
th
=
0 to
v
th
=
0.2
c, where c is the speed of light.</description><subject>Amplitudes</subject><subject>Electron energy</subject><subject>Lasers</subject><subject>Modulation</subject><subject>Phase matching</subject><subject>Plasma</subject><subject>Plasma density</subject><subject>Plasma frequencies</subject><subject>Plasma physics</subject><subject>Wavelengths</subject><issn>1070-664X</issn><issn>1089-7674</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNp9kE1LAzEURYMoWEcX_oOAGytMzcckmVlKqVYouKngbsykSZsyTcYkBdtf7_Rj7erddzm8BweAe4xGGHH6jEcME1xhegEGGJVVLrgoLg9ZoJzz4usa3MS4RggVnJUD8D0xxiqrXYJJB7nSIe3h43y6H8Kldn2TrHew2UHnXWudlgFu7K91S-gNbKzyrQ8w-S5fyQRbGXWI0Dq48gl2_bqRt-DKyDbqu_PMwOfrZD6e5rOPt_fxyyxXpCIpV1gaaSgnRIuFKkQfkKZCVYIxwvFCNqVhJRfCKEyV5FRQQhtMEaFVIxGiGXg43e2C_9nqmOq13wbXv6wJZQWjRysZGJ4oFXyMQZu6C3Yjw67GqD4IrHF9FtizTyc2KpuOHv6B_wDTBW8F</recordid><startdate>202002</startdate><enddate>202002</enddate><creator>Manendra</creator><creator>Singh, Kunwar Pal</creator><creator>Bhati, Ruchi</creator><creator>Malik, Anil K</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0002-0100-1625</orcidid><orcidid>https://orcid.org/0000-0002-9653-3068</orcidid><orcidid>https://orcid.org/0000-0001-7185-2866</orcidid></search><sort><creationdate>202002</creationdate><title>Efficient terahertz (THz) generation by nonlinear mixing of bicolor top-hat lasers in hot plasma</title><author>Manendra ; Singh, Kunwar Pal ; Bhati, Ruchi ; Malik, Anil K</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c292t-c1afaf3622e7dc476220e37c9755261dab8f58677fc13ca637323b130239ba003</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Amplitudes</topic><topic>Electron energy</topic><topic>Lasers</topic><topic>Modulation</topic><topic>Phase matching</topic><topic>Plasma</topic><topic>Plasma density</topic><topic>Plasma frequencies</topic><topic>Plasma physics</topic><topic>Wavelengths</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Manendra</creatorcontrib><creatorcontrib>Singh, Kunwar Pal</creatorcontrib><creatorcontrib>Bhati, Ruchi</creatorcontrib><creatorcontrib>Malik, Anil K</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Physics of plasmas</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Manendra</au><au>Singh, Kunwar Pal</au><au>Bhati, Ruchi</au><au>Malik, Anil K</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Efficient terahertz (THz) generation by nonlinear mixing of bicolor top-hat lasers in hot plasma</atitle><jtitle>Physics of plasmas</jtitle><date>2020-02</date><risdate>2020</risdate><volume>27</volume><issue>2</issue><issn>1070-664X</issn><eissn>1089-7674</eissn><coden>PHPAEN</coden><abstract>We report a theoretical model of radially polarized terahertz (THz) wave emission by nonlinear mixing of bicolor, radially polarized lasers having a top-hat envelope profile [
s
(
profile
index
)
≥
1] in density modulated hot plasma. We investigate the effect of the laser profile index on the emitted THz field profile and found that THz field amplitude and peak location changes with the laser profile index. Our numerical investigations show that THz field amplitude is the highest around
ω
p
≈
ω
1
−
ω
2 (where
ω
p is the plasma frequency and
ω
1
and
ω
2 are the laser frequencies). We observe that phase matching can be achieved with the help of the plasma density modulation wave number. The plasma density modulation wave number increases with electron temperature and decreases with the frequency mismatch between
ω
p and
ω
1
−
ω
2. We found that the conversion efficiency is maximum at
ω
1
−
ω
2
≈
ω
p and increases fivefold with an increase in electron thermal velocity (
v
th) from
v
th
=
0 to
v
th
=
0.2
c, where c is the speed of light.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/1.5121913</doi><tpages>7</tpages><orcidid>https://orcid.org/0000-0002-0100-1625</orcidid><orcidid>https://orcid.org/0000-0002-9653-3068</orcidid><orcidid>https://orcid.org/0000-0001-7185-2866</orcidid></addata></record> |
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source | American Institute of Physics (AIP) Publications; American Institute of Physics:Jisc Collections:Transitional Journals Agreement 2021-23 (Reading list) |
subjects | Amplitudes Electron energy Lasers Modulation Phase matching Plasma Plasma density Plasma frequencies Plasma physics Wavelengths |
title | Efficient terahertz (THz) generation by nonlinear mixing of bicolor top-hat lasers in hot plasma |
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