Left-right symmetry at LHC and precise 1-loop low energy data
A bstract Despite many tests, even the Minimal Manifest Left-Right Symmetric Model (MLRSM) has never been ultimately confirmed or falsified. LHC gives a new possibility to test directly the most conservative version of left-right symmetric models at so far not reachable energy scales. If we take int...
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description | A
bstract
Despite many tests, even the Minimal Manifest Left-Right Symmetric Model (MLRSM) has never been ultimately confirmed or falsified. LHC gives a new possibility to test directly the most conservative version of left-right symmetric models at so far not reachable energy scales. If we take into account precise limits on the model which come from low energy processes, like the muon decay, possible LHC signals are strongly limited through the correlations of parameters among heavy neutrinos, heavy gauge bosons and heavy Higgs particles. To illustrate the situation in the context of LHC, we consider the “golden” process
pp
→
e
+
N
. For instance, in a case of degenerate heavy neutrinos and heavy Higgs masses at 15 TeV (in agreement with FCNC bounds) we get σ(
pp
→
e
+
N
)
>
10 fb at
which is consistent with muon decay data for a very limited
W
2
masses in the range (3008 GeV, 3040 GeV). Without restrictions coming from the muon data,
W
2
masses would be in the range (1.0 TeV, 3.5 TeV). Influence of heavy Higgs particles themselves on the considered LHC process is negligible (the same is true for the light, SM neutral Higgs scalar analog). In the paper decay modes of the right-handed heavy gauge bosons and heavy neutrinos are also discussed. Both scenarios with typical see-saw light heavy neutrino mixings and the mixings which are independent of heavy neutrino masses are considered. In the second case heavy neutrino decays to the heavy charged gauge bosons not necessarily dominate over decay modes which include only light, SM-like particles. |
doi_str_mv | 10.1007/JHEP07(2012)038 |
format | Article |
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bstract
Despite many tests, even the Minimal Manifest Left-Right Symmetric Model (MLRSM) has never been ultimately confirmed or falsified. LHC gives a new possibility to test directly the most conservative version of left-right symmetric models at so far not reachable energy scales. If we take into account precise limits on the model which come from low energy processes, like the muon decay, possible LHC signals are strongly limited through the correlations of parameters among heavy neutrinos, heavy gauge bosons and heavy Higgs particles. To illustrate the situation in the context of LHC, we consider the “golden” process
pp
→
e
+
N
. For instance, in a case of degenerate heavy neutrinos and heavy Higgs masses at 15 TeV (in agreement with FCNC bounds) we get σ(
pp
→
e
+
N
)
>
10 fb at
which is consistent with muon decay data for a very limited
W
2
masses in the range (3008 GeV, 3040 GeV). Without restrictions coming from the muon data,
W
2
masses would be in the range (1.0 TeV, 3.5 TeV). Influence of heavy Higgs particles themselves on the considered LHC process is negligible (the same is true for the light, SM neutral Higgs scalar analog). In the paper decay modes of the right-handed heavy gauge bosons and heavy neutrinos are also discussed. Both scenarios with typical see-saw light heavy neutrino mixings and the mixings which are independent of heavy neutrino masses are considered. In the second case heavy neutrino decays to the heavy charged gauge bosons not necessarily dominate over decay modes which include only light, SM-like particles.</description><identifier>ISSN: 1029-8479</identifier><identifier>EISSN: 1029-8479</identifier><identifier>DOI: 10.1007/JHEP07(2012)038</identifier><language>eng</language><publisher>Berlin/Heidelberg: Springer-Verlag</publisher><subject>Bosons ; Classical and Quantum Gravitation ; Elementary Particles ; High energy physics ; Muons ; Neutrinos ; Particle decay ; Physics ; Physics and Astronomy ; Quantum Field Theories ; Quantum Field Theory ; Quantum Physics ; Relativity Theory ; Signal processing ; String Theory ; Symmetry</subject><ispartof>The journal of high energy physics, 2012-07, Vol.2012 (7), Article 38</ispartof><rights>SISSA 2012</rights><rights>SISSA 2012.</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c351t-791f8cb1c15907b648d6c16aca00594577ebaa5443c5a94a862d234296161e2d3</citedby><cites>FETCH-LOGICAL-c351t-791f8cb1c15907b648d6c16aca00594577ebaa5443c5a94a862d234296161e2d3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1007/JHEP07(2012)038$$EPDF$$P50$$Gspringer$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://doi.org/10.1007/JHEP07(2012)038$$EHTML$$P50$$Gspringer$$Hfree_for_read</linktohtml><link.rule.ids>314,780,784,27915,27916,41111,41479,42180,42548,51310,51567</link.rule.ids></links><search><creatorcontrib>Chakrabortty, J.</creatorcontrib><creatorcontrib>Gluza, J.</creatorcontrib><creatorcontrib>Sevillano, R.</creatorcontrib><creatorcontrib>Szafron, R.</creatorcontrib><title>Left-right symmetry at LHC and precise 1-loop low energy data</title><title>The journal of high energy physics</title><addtitle>J. High Energ. Phys</addtitle><description>A
bstract
Despite many tests, even the Minimal Manifest Left-Right Symmetric Model (MLRSM) has never been ultimately confirmed or falsified. LHC gives a new possibility to test directly the most conservative version of left-right symmetric models at so far not reachable energy scales. If we take into account precise limits on the model which come from low energy processes, like the muon decay, possible LHC signals are strongly limited through the correlations of parameters among heavy neutrinos, heavy gauge bosons and heavy Higgs particles. To illustrate the situation in the context of LHC, we consider the “golden” process
pp
→
e
+
N
. For instance, in a case of degenerate heavy neutrinos and heavy Higgs masses at 15 TeV (in agreement with FCNC bounds) we get σ(
pp
→
e
+
N
)
>
10 fb at
which is consistent with muon decay data for a very limited
W
2
masses in the range (3008 GeV, 3040 GeV). Without restrictions coming from the muon data,
W
2
masses would be in the range (1.0 TeV, 3.5 TeV). Influence of heavy Higgs particles themselves on the considered LHC process is negligible (the same is true for the light, SM neutral Higgs scalar analog). In the paper decay modes of the right-handed heavy gauge bosons and heavy neutrinos are also discussed. Both scenarios with typical see-saw light heavy neutrino mixings and the mixings which are independent of heavy neutrino masses are considered. In the second case heavy neutrino decays to the heavy charged gauge bosons not necessarily dominate over decay modes which include only light, SM-like particles.</description><subject>Bosons</subject><subject>Classical and Quantum Gravitation</subject><subject>Elementary Particles</subject><subject>High energy physics</subject><subject>Muons</subject><subject>Neutrinos</subject><subject>Particle decay</subject><subject>Physics</subject><subject>Physics and Astronomy</subject><subject>Quantum Field Theories</subject><subject>Quantum Field Theory</subject><subject>Quantum Physics</subject><subject>Relativity Theory</subject><subject>Signal processing</subject><subject>String Theory</subject><subject>Symmetry</subject><issn>1029-8479</issn><issn>1029-8479</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2012</creationdate><recordtype>article</recordtype><sourceid>C6C</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><recordid>eNp1kDFPwzAQhS0EEqUws1pigSH0zrGTeGBAUaGgSDDAbLmOU1q1SbBdofx7XAUJFqZ7w_feSR8hlwi3CJDPnhfzV8ivGSC7gbQ4IhMEJpOC5_L4Tz4lZ95vAFCghAm5q2wTErdefQTqh93OBjdQHWi1KKlua9o7a9beUky2XdfTbfdFbWvdaqC1DvqcnDR66-3Fz52S94f5W7lIqpfHp_K-SkwqMCS5xKYwSzQoJOTLjBd1ZjDTRgMIyUWe26XWgvPUCC25LjJWs5QzmWGGltXplFyNu73rPvfWB7Xp9q6NLxVLZRHROByp2UgZ13nvbKN6t95pNygEdXCkRkfq4EhFR7EBY8NHsl1Z97v7X-UbcQJmCg</recordid><startdate>20120701</startdate><enddate>20120701</enddate><creator>Chakrabortty, J.</creator><creator>Gluza, J.</creator><creator>Sevillano, R.</creator><creator>Szafron, R.</creator><general>Springer-Verlag</general><general>Springer Nature B.V</general><scope>C6C</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>HCIFZ</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope></search><sort><creationdate>20120701</creationdate><title>Left-right symmetry at LHC and precise 1-loop low energy data</title><author>Chakrabortty, J. ; Gluza, J. ; Sevillano, R. ; Szafron, R.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c351t-791f8cb1c15907b648d6c16aca00594577ebaa5443c5a94a862d234296161e2d3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2012</creationdate><topic>Bosons</topic><topic>Classical and Quantum Gravitation</topic><topic>Elementary Particles</topic><topic>High energy physics</topic><topic>Muons</topic><topic>Neutrinos</topic><topic>Particle decay</topic><topic>Physics</topic><topic>Physics and Astronomy</topic><topic>Quantum Field Theories</topic><topic>Quantum Field Theory</topic><topic>Quantum Physics</topic><topic>Relativity Theory</topic><topic>Signal processing</topic><topic>String Theory</topic><topic>Symmetry</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chakrabortty, J.</creatorcontrib><creatorcontrib>Gluza, J.</creatorcontrib><creatorcontrib>Sevillano, R.</creatorcontrib><creatorcontrib>Szafron, R.</creatorcontrib><collection>Springer Nature OA Free Journals</collection><collection>CrossRef</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>SciTech Premium Collection</collection><collection>Advanced Technologies & Aerospace Database</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Publicly Available Content Database</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><jtitle>The journal of high energy physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chakrabortty, J.</au><au>Gluza, J.</au><au>Sevillano, R.</au><au>Szafron, R.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Left-right symmetry at LHC and precise 1-loop low energy data</atitle><jtitle>The journal of high energy physics</jtitle><stitle>J. High Energ. Phys</stitle><date>2012-07-01</date><risdate>2012</risdate><volume>2012</volume><issue>7</issue><artnum>38</artnum><issn>1029-8479</issn><eissn>1029-8479</eissn><abstract>A
bstract
Despite many tests, even the Minimal Manifest Left-Right Symmetric Model (MLRSM) has never been ultimately confirmed or falsified. LHC gives a new possibility to test directly the most conservative version of left-right symmetric models at so far not reachable energy scales. If we take into account precise limits on the model which come from low energy processes, like the muon decay, possible LHC signals are strongly limited through the correlations of parameters among heavy neutrinos, heavy gauge bosons and heavy Higgs particles. To illustrate the situation in the context of LHC, we consider the “golden” process
pp
→
e
+
N
. For instance, in a case of degenerate heavy neutrinos and heavy Higgs masses at 15 TeV (in agreement with FCNC bounds) we get σ(
pp
→
e
+
N
)
>
10 fb at
which is consistent with muon decay data for a very limited
W
2
masses in the range (3008 GeV, 3040 GeV). Without restrictions coming from the muon data,
W
2
masses would be in the range (1.0 TeV, 3.5 TeV). Influence of heavy Higgs particles themselves on the considered LHC process is negligible (the same is true for the light, SM neutral Higgs scalar analog). In the paper decay modes of the right-handed heavy gauge bosons and heavy neutrinos are also discussed. Both scenarios with typical see-saw light heavy neutrino mixings and the mixings which are independent of heavy neutrino masses are considered. In the second case heavy neutrino decays to the heavy charged gauge bosons not necessarily dominate over decay modes which include only light, SM-like particles.</abstract><cop>Berlin/Heidelberg</cop><pub>Springer-Verlag</pub><doi>10.1007/JHEP07(2012)038</doi><oa>free_for_read</oa></addata></record> |
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subjects | Bosons Classical and Quantum Gravitation Elementary Particles High energy physics Muons Neutrinos Particle decay Physics Physics and Astronomy Quantum Field Theories Quantum Field Theory Quantum Physics Relativity Theory Signal processing String Theory Symmetry |
title | Left-right symmetry at LHC and precise 1-loop low energy data |
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