On Landau pole in the minimal 3-3-1 model
We show that in 3-3-1 models the existence of a Landau-like pole in the coupling constant related to the $U(1)_X$ factor, $g_X$, in a certain value of $\sin^2\theta_W $, arises only assuming that the condition to match the gauge coupling constants of the standard model, $g_{2L}$, with that of the 3-...
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creator | Franco, Edison T Pleitez, V |
description | We show that in 3-3-1 models the existence of a Landau-like pole in the
coupling constant related to the $U(1)_X$ factor, $g_X$, in a certain value of
$\sin^2\theta_W $, arises only assuming that the condition to match the gauge
coupling constants of the standard model, $g_{2L}$, with that of the 3-3-1
model, $g_{3L}$, is valid for all energies. However, if we impose that this
matching condition is valid only at a given energy, say $\mu = M_Z$, the pole
arises when $\sin^2\theta_X(\mu_{LP})=1$, which is the only weak mixing angle
in the models. The value of $\mu_{LP} $ depends on the energy scales, $\mu_m$
and $\mu_{331}$, in which the matching and the 3-3-1 symmetry is fully
realized, respectively. We also show that $g_{2L} $ and $g_{3L} $ have
different running with energy. Therefore, differently from what is usually
assumed in the literature, these couplings can not be considered equal for all
energies. As a consequence, the fermion couplings with neutral vector bosons
are different if we write them in terms of $\sin\theta_X$ instead of
$\sin\theta_W $. |
doi_str_mv | 10.48550/arxiv.1711.09866 |
format | Article |
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coupling constant related to the $U(1)_X$ factor, $g_X$, in a certain value of
$\sin^2\theta_W $, arises only assuming that the condition to match the gauge
coupling constants of the standard model, $g_{2L}$, with that of the 3-3-1
model, $g_{3L}$, is valid for all energies. However, if we impose that this
matching condition is valid only at a given energy, say $\mu = M_Z$, the pole
arises when $\sin^2\theta_X(\mu_{LP})=1$, which is the only weak mixing angle
in the models. The value of $\mu_{LP} $ depends on the energy scales, $\mu_m$
and $\mu_{331}$, in which the matching and the 3-3-1 symmetry is fully
realized, respectively. We also show that $g_{2L} $ and $g_{3L} $ have
different running with energy. Therefore, differently from what is usually
assumed in the literature, these couplings can not be considered equal for all
energies. As a consequence, the fermion couplings with neutral vector bosons
are different if we write them in terms of $\sin\theta_X$ instead of
$\sin\theta_W $.</description><identifier>DOI: 10.48550/arxiv.1711.09866</identifier><language>eng</language><subject>Physics - High Energy Physics - Experiment ; Physics - High Energy Physics - Phenomenology ; Physics - High Energy Physics - Theory</subject><creationdate>2017-11</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/1711.09866$$EView_record_in_Cornell_University$$FView_record_in_$$GCornell_University$$Hfree_for_read</linktorsrc><backlink>$$Uhttps://doi.org/10.48550/arXiv.1711.09866$$DView paper in arXiv$$Hfree_for_read</backlink></links><search><creatorcontrib>Franco, Edison T</creatorcontrib><creatorcontrib>Pleitez, V</creatorcontrib><title>On Landau pole in the minimal 3-3-1 model</title><description>We show that in 3-3-1 models the existence of a Landau-like pole in the
coupling constant related to the $U(1)_X$ factor, $g_X$, in a certain value of
$\sin^2\theta_W $, arises only assuming that the condition to match the gauge
coupling constants of the standard model, $g_{2L}$, with that of the 3-3-1
model, $g_{3L}$, is valid for all energies. However, if we impose that this
matching condition is valid only at a given energy, say $\mu = M_Z$, the pole
arises when $\sin^2\theta_X(\mu_{LP})=1$, which is the only weak mixing angle
in the models. The value of $\mu_{LP} $ depends on the energy scales, $\mu_m$
and $\mu_{331}$, in which the matching and the 3-3-1 symmetry is fully
realized, respectively. We also show that $g_{2L} $ and $g_{3L} $ have
different running with energy. Therefore, differently from what is usually
assumed in the literature, these couplings can not be considered equal for all
energies. As a consequence, the fermion couplings with neutral vector bosons
are different if we write them in terms of $\sin\theta_X$ instead of
$\sin\theta_W $.</description><subject>Physics - High Energy Physics - Experiment</subject><subject>Physics - High Energy Physics - Phenomenology</subject><subject>Physics - High Energy Physics - Theory</subject><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2017</creationdate><recordtype>article</recordtype><sourceid>GOX</sourceid><recordid>eNotzj1vwjAQgGEvHRDwA5jwyuDUh-0jGRFqASkSC3t07p3VSElAKaDy7_mc3u3Vo9QEbObzEOwn9f_1JYMFQGaLHHGgZrtOl9QxnfXx0IiuO336Fd3WXd1So51xBnR7YGlG6iNR8yfjd4dq__21X21MuVtvV8vSEC7QpDkFiCC5tWiJJXHgxDYERiSBWBBgTMQM3kbBn8JL8k6Ch1zmIZIbqulr-7RWx_7u6K_Vw1w9ze4GXT86nA</recordid><startdate>20171127</startdate><enddate>20171127</enddate><creator>Franco, Edison T</creator><creator>Pleitez, V</creator><scope>GOX</scope></search><sort><creationdate>20171127</creationdate><title>On Landau pole in the minimal 3-3-1 model</title><author>Franco, Edison T ; Pleitez, V</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a676-f2a51b1e80060adefd5dfd055d66ae1b9a16bfadd140be6c94ef43e5418e25ba3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2017</creationdate><topic>Physics - High Energy Physics - Experiment</topic><topic>Physics - High Energy Physics - Phenomenology</topic><topic>Physics - High Energy Physics - Theory</topic><toplevel>online_resources</toplevel><creatorcontrib>Franco, Edison T</creatorcontrib><creatorcontrib>Pleitez, V</creatorcontrib><collection>arXiv.org</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext_linktorsrc</fulltext></delivery><addata><au>Franco, Edison T</au><au>Pleitez, V</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>On Landau pole in the minimal 3-3-1 model</atitle><date>2017-11-27</date><risdate>2017</risdate><abstract>We show that in 3-3-1 models the existence of a Landau-like pole in the
coupling constant related to the $U(1)_X$ factor, $g_X$, in a certain value of
$\sin^2\theta_W $, arises only assuming that the condition to match the gauge
coupling constants of the standard model, $g_{2L}$, with that of the 3-3-1
model, $g_{3L}$, is valid for all energies. However, if we impose that this
matching condition is valid only at a given energy, say $\mu = M_Z$, the pole
arises when $\sin^2\theta_X(\mu_{LP})=1$, which is the only weak mixing angle
in the models. The value of $\mu_{LP} $ depends on the energy scales, $\mu_m$
and $\mu_{331}$, in which the matching and the 3-3-1 symmetry is fully
realized, respectively. We also show that $g_{2L} $ and $g_{3L} $ have
different running with energy. Therefore, differently from what is usually
assumed in the literature, these couplings can not be considered equal for all
energies. As a consequence, the fermion couplings with neutral vector bosons
are different if we write them in terms of $\sin\theta_X$ instead of
$\sin\theta_W $.</abstract><doi>10.48550/arxiv.1711.09866</doi><oa>free_for_read</oa></addata></record> |
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subjects | Physics - High Energy Physics - Experiment Physics - High Energy Physics - Phenomenology Physics - High Energy Physics - Theory |
title | On Landau pole in the minimal 3-3-1 model |
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