Higher order self-dual models for spin-3 particles in $D=2+1
Phys. Rev. D 98, 105002 (2018) In $D=2+1$ dimensions, elementary particles of a given helicity can be described by local Lagrangians (parity singlets). By means of a "soldering" procedure two opposite helicities can be joined together and give rise to massive spin-$s$ particles carrying bo...
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creator | Dalmazi, D Santos, A. L. R. dos Santos, R. R. Lino dos |
description | Phys. Rev. D 98, 105002 (2018) In $D=2+1$ dimensions, elementary particles of a given helicity can be
described by local Lagrangians (parity singlets). By means of a "soldering"
procedure two opposite helicities can be joined together and give rise to
massive spin-$s$ particles carrying both helicities $\pm s$ (parity doublets),
such Lagrangians can also be used in $D=3+1$ to describe massive spin-$s$
particles. From this point of view the parity singlets (self-dual models) in
$D=2+1$ are the building blocks of real massive elementary particles in
$D=3+1$. In the three cases $s=1,\, 3/2,\, 2$ there are $2s$ self-dual models
of order $1,2, \cdots, 2s$ in derivatives. In the spin-3 case the 5th order
model is missing in the literature. Here we deduce a 5th order spin-3 self-dual
model and fill up this gap. It is shown to be ghost free by means of a master
action which relates it with the top model of 6th order. We believe that our
approach can be generalized to arbitrary integer spin-$s$ in order to obtain
the models of order $2s$ and $2s-1$. We also comment on the difficulties in
relating the 5th order model with their lower order duals. |
doi_str_mv | 10.48550/arxiv.1810.08643 |
format | Article |
fullrecord | <record><control><sourceid>arxiv_GOX</sourceid><recordid>TN_cdi_arxiv_primary_1810_08643</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>1810_08643</sourcerecordid><originalsourceid>FETCH-arxiv_primary_1810_086433</originalsourceid><addsrcrecordid>eNpjYJA0NNAzsTA1NdBPLKrILNMztAAKGFiYmRhzMth4ZKZnpBYp5BelAMni1Jw03ZTSxByF3PyU1JxihbR8oGBBZp6usUJBYlFJZnJOarFCZp6CioutkbYhDwNrWmJOcSovlOZmkHdzDXH20AXbE19QlJmbWFQZD7IvHmyfMWEVAFkAM3M</addsrcrecordid><sourcetype>Open Access Repository</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Higher order self-dual models for spin-3 particles in $D=2+1</title><source>arXiv.org</source><creator>Dalmazi, D ; Santos, A. L. R. dos ; Santos, R. R. Lino dos</creator><creatorcontrib>Dalmazi, D ; Santos, A. L. R. dos ; Santos, R. R. Lino dos</creatorcontrib><description>Phys. Rev. D 98, 105002 (2018) In $D=2+1$ dimensions, elementary particles of a given helicity can be
described by local Lagrangians (parity singlets). By means of a "soldering"
procedure two opposite helicities can be joined together and give rise to
massive spin-$s$ particles carrying both helicities $\pm s$ (parity doublets),
such Lagrangians can also be used in $D=3+1$ to describe massive spin-$s$
particles. From this point of view the parity singlets (self-dual models) in
$D=2+1$ are the building blocks of real massive elementary particles in
$D=3+1$. In the three cases $s=1,\, 3/2,\, 2$ there are $2s$ self-dual models
of order $1,2, \cdots, 2s$ in derivatives. In the spin-3 case the 5th order
model is missing in the literature. Here we deduce a 5th order spin-3 self-dual
model and fill up this gap. It is shown to be ghost free by means of a master
action which relates it with the top model of 6th order. We believe that our
approach can be generalized to arbitrary integer spin-$s$ in order to obtain
the models of order $2s$ and $2s-1$. We also comment on the difficulties in
relating the 5th order model with their lower order duals.</description><identifier>DOI: 10.48550/arxiv.1810.08643</identifier><language>eng</language><subject>Physics - High Energy Physics - Theory</subject><creationdate>2018-10</creationdate><rights>http://arxiv.org/licenses/nonexclusive-distrib/1.0</rights><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>228,230,780,885</link.rule.ids><linktorsrc>$$Uhttps://arxiv.org/abs/1810.08643$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.1103/PhysRevD.98.105002$$DView published paper (Access to full text may be restricted)$$Hfree_for_read</backlink><backlink>$$Uhttps://doi.org/10.48550/arXiv.1810.08643$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Dalmazi, D</creatorcontrib><creatorcontrib>Santos, A. L. R. dos</creatorcontrib><creatorcontrib>Santos, R. R. Lino dos</creatorcontrib><title>Higher order self-dual models for spin-3 particles in $D=2+1</title><description>Phys. Rev. D 98, 105002 (2018) In $D=2+1$ dimensions, elementary particles of a given helicity can be
described by local Lagrangians (parity singlets). By means of a "soldering"
procedure two opposite helicities can be joined together and give rise to
massive spin-$s$ particles carrying both helicities $\pm s$ (parity doublets),
such Lagrangians can also be used in $D=3+1$ to describe massive spin-$s$
particles. From this point of view the parity singlets (self-dual models) in
$D=2+1$ are the building blocks of real massive elementary particles in
$D=3+1$. In the three cases $s=1,\, 3/2,\, 2$ there are $2s$ self-dual models
of order $1,2, \cdots, 2s$ in derivatives. In the spin-3 case the 5th order
model is missing in the literature. Here we deduce a 5th order spin-3 self-dual
model and fill up this gap. It is shown to be ghost free by means of a master
action which relates it with the top model of 6th order. We believe that our
approach can be generalized to arbitrary integer spin-$s$ in order to obtain
the models of order $2s$ and $2s-1$. We also comment on the difficulties in
relating the 5th order model with their lower order duals.</description><subject>Physics - High Energy Physics - Theory</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNpjYJA0NNAzsTA1NdBPLKrILNMztAAKGFiYmRhzMth4ZKZnpBYp5BelAMni1Jw03ZTSxByF3PyU1JxihbR8oGBBZp6usUJBYlFJZnJOarFCZp6CioutkbYhDwNrWmJOcSovlOZmkHdzDXH20AXbE19QlJmbWFQZD7IvHmyfMWEVAFkAM3M</recordid><startdate>20181019</startdate><enddate>20181019</enddate><creator>Dalmazi, D</creator><creator>Santos, A. L. R. dos</creator><creator>Santos, R. R. Lino dos</creator><scope>GOX</scope></search><sort><creationdate>20181019</creationdate><title>Higher order self-dual models for spin-3 particles in $D=2+1</title><author>Dalmazi, D ; Santos, A. L. R. dos ; Santos, R. R. Lino dos</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-arxiv_primary_1810_086433</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>Physics - High Energy Physics - Theory</topic><toplevel>online_resources</toplevel><creatorcontrib>Dalmazi, D</creatorcontrib><creatorcontrib>Santos, A. L. R. dos</creatorcontrib><creatorcontrib>Santos, R. R. Lino dos</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Dalmazi, D</au><au>Santos, A. L. R. dos</au><au>Santos, R. R. Lino dos</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Higher order self-dual models for spin-3 particles in $D=2+1</atitle><date>2018-10-19</date><risdate>2018</risdate><abstract>Phys. Rev. D 98, 105002 (2018) In $D=2+1$ dimensions, elementary particles of a given helicity can be
described by local Lagrangians (parity singlets). By means of a "soldering"
procedure two opposite helicities can be joined together and give rise to
massive spin-$s$ particles carrying both helicities $\pm s$ (parity doublets),
such Lagrangians can also be used in $D=3+1$ to describe massive spin-$s$
particles. From this point of view the parity singlets (self-dual models) in
$D=2+1$ are the building blocks of real massive elementary particles in
$D=3+1$. In the three cases $s=1,\, 3/2,\, 2$ there are $2s$ self-dual models
of order $1,2, \cdots, 2s$ in derivatives. In the spin-3 case the 5th order
model is missing in the literature. Here we deduce a 5th order spin-3 self-dual
model and fill up this gap. It is shown to be ghost free by means of a master
action which relates it with the top model of 6th order. We believe that our
approach can be generalized to arbitrary integer spin-$s$ in order to obtain
the models of order $2s$ and $2s-1$. We also comment on the difficulties in
relating the 5th order model with their lower order duals.</abstract><doi>10.48550/arxiv.1810.08643</doi><oa>free_for_read</oa></addata></record> |
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subjects | Physics - High Energy Physics - Theory |
title | Higher order self-dual models for spin-3 particles in $D=2+1 |
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