A new search signature for excited leptons is explored. Excited muons are sought in the channel ${pp} o mu {mu }^{* } o mu mu {
m{jet}};{
m{jet}}$, assuming both the production and decay occur via a contact interaction. The analysis is based on 20.3 fb−1 of pp collision data at a centre-of-mass energy of $sqrt{s};=;8;{
m{TeV}}$ taken with the ATLAS detector at the large hadron collider. No evidence of excited muons is found, and limits are set at the 95% confidence level on the cross section times branching ratio as a function of the excited-muon mass ${m}_{{mu }^{* }}$. For ${m}_{{mu }^{* }}$ between 1.3 and 3.0 TeV, the upper limit on $sigma B({mu }^{* } o mu qar{q}$) is between 0.6 and 1 fb. Limits on $sigma B$ are converted to lower bounds on the compositeness scale Λ. In the limiting case ${
m{Lambda }}={m}_{{mu }^{* }}$, excited muons with a mass below 2.8 TeV are excluded. With the same model assumptions, these limits at larger ${mu }^{* }$ masses improve upon previous limits from traditional searches based on the gauge-mediated decay ${mu }^{* } o mu gamma $.
Aad, G., Abbott, B., Abdallah, J., Abdinov, O., Abeloos, B., Aben, R., et al. (2016). A search for an excited muon decaying to a muon and two jets in pp collisions at √ s = 8 TeV with the ATLAS detector. NEW JOURNAL OF PHYSICS, 18(7), 073021 [10.1088/1367-2630/18/7/073021].
A search for an excited muon decaying to a muon and two jets in pp collisions at √ s = 8 TeV with the ATLAS detector
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2016-01-01
Abstract
A new search signature for excited leptons is explored. Excited muons are sought in the channel ${pp} o mu {mu }^{* } o mu mu {
m{jet}};{
m{jet}}$, assuming both the production and decay occur via a contact interaction. The analysis is based on 20.3 fb−1 of pp collision data at a centre-of-mass energy of $sqrt{s};=;8;{
m{TeV}}$ taken with the ATLAS detector at the large hadron collider. No evidence of excited muons is found, and limits are set at the 95% confidence level on the cross section times branching ratio as a function of the excited-muon mass ${m}_{{mu }^{* }}$. For ${m}_{{mu }^{* }}$ between 1.3 and 3.0 TeV, the upper limit on $sigma B({mu }^{* } o mu qar{q}$) is between 0.6 and 1 fb. Limits on $sigma B$ are converted to lower bounds on the compositeness scale Λ. In the limiting case ${
m{Lambda }}={m}_{{mu }^{* }}$, excited muons with a mass below 2.8 TeV are excluded. With the same model assumptions, these limits at larger ${mu }^{* }$ masses improve upon previous limits from traditional searches based on the gauge-mediated decay ${mu }^{* } o mu gamma $.
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Il report seguente simula gli indicatori relativi alla propria produzione scientifica in relazione alle soglie ASN 2023-2025 del proprio SC/SSD. Si ricorda che il superamento dei valori soglia (almeno 2 su 3) è requisito necessario ma non sufficiente al conseguimento dell'abilitazione. La simulazione si basa sui dati IRIS e sugli indicatori bibliometrici alla data indicata e non tiene conto di eventuali periodi di congedo obbligatorio, che in sede di domanda ASN danno diritto a incrementi percentuali dei valori. La simulazione può differire dall'esito di un’eventuale domanda ASN sia per errori di catalogazione e/o dati mancanti in IRIS, sia per la variabilità dei dati bibliometrici nel tempo. Si consideri che Anvur calcola i valori degli indicatori all'ultima data utile per la presentazione delle domande. La presente simulazione è stata realizzata sulla base delle specifiche raccolte sul tavolo ER del Focus Group IRIS coordinato dall’Università di Modena e Reggio Emilia e delle regole riportate nel DM 589/2018 e allegata Tabella A. Cineca, l’Università di Modena e Reggio Emilia e il Focus Group IRIS non si assumono alcuna responsabilità in merito all’uso che il diretto interessato o terzi faranno della simulazione. Si specifica inoltre che la simulazione contiene calcoli effettuati con dati e algoritmi di pubblico dominio e deve quindi essere considerata come un mero ausilio al calcolo svolgibile manualmente o con strumenti equivalenti.