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showing 10 items of 346 documents

"Table 132" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2019

$|{y}^{t,2}|$ correlation matrix for absolute differential cross-section in parton level

PP -->$t\bar{t}$ ---> L_JET L_JETparton levelPP -->$t\bar{t}$ ---> all-hadronic$|{y}^{t2}|$13000
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"Table 101" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2019

$|{y}^{t,2}|$ normalized differential cross-section at parton level. The parton level phase-space is limited to the region $p_T^{t,1} > 500~$GeV, $p_T^{t,2} > 350~$GeV.

PP -->$t\bar{t}$ ---> L_JET L_JETparton levelPP -->$t\bar{t}$ ---> all-hadronic$|{y}^{t2}|$13000
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"Table 131" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2019

$|{y}^{t,2}|$ covariance matrix for the absolute differential cross-section at parton level

PP -->$t\bar{t}$ ---> L_JET L_JETparton levelPP -->$t\bar{t}$ ---> all-hadronic$|{y}^{t2}|$13000
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"Table 114" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2019

${p_{{T}}}^{t}$ correlation matrix for relative differential cross-section in parton level

PP -->$t\bar{t}$ ---> L_JET L_JETparton levelPP -->$t\bar{t}$ ---> all-hadronic13000${p_{{T}}}^{t}$
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"Table 107" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2019

$|{p_{out}}^{t\bar{t}}|$ relative differential cross-section in parton level

PP -->$t\bar{t}$ ---> L_JET L_JETparton levelPP -->$t\bar{t}$ ---> all-hadronic13000$|{p_{out}}^{t\bar{t}}|$
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"Table 171" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2018

all 15 variables correlation matrix for absolute differential cross-section in parton level

PP -->$t\bar{t}$ ---> L_JET L_JETparton levelall variables13000
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"Table 172" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…

2018

all 15 variables correlation matrix for relative differential cross-section in parton level

PP -->$t\bar{t}$ ---> L_JET L_JETparton levelall variables13000
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Quantum non-Markovianity induced by Anderson localization

2017

As discovered by P. W. Anderson, excitations do not propagate freely in a disordered lattice, but, due to destructive interference, they localise. As a consequence when an atom interacts with a disordered lattice one indeed observes, a non-trivial excitation exchange between atom and lattice. Such non-trivial atomic dynamics will in general be characterised also by a non-trivial quantum information backflow, a clear signature of non-Markovian dynamics. To investigate the above scenario we consider a quantum emitter, or atom, weakly coupled to a uniform coupled-cavity array (CCA). If initially excited, in the absence of disorder, the emitter undergoes a Markovian spontaneous emission by rele…

Physics---Anderson localizationQuantum PhysicsMultidisciplinaryFOS: Physical sciences01 natural sciencesArticleSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasNormal modeExcited stateQuantum mechanics0103 physical sciencesPhenomenological modelAtomSpontaneous emissionQuantum information010306 general physicsQuantum Physics (quant-ph)QuantumScientific Reports
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Local Quench, Majorana Zero Modes, and Disturbance Propagation in the Ising chain

2016

We study the generation and propagation of local perturbations in a quantum many-body spin system. In particular, we study the Ising model in transverse field in the presence of a local field defect at one edge. This system possesses a rich phase diagram with different regions characterized by the presence of one or two Majorana zero modes. We show that their localized character {\it i}) enables a characterization of the Ising phase transition through a local-only measurement performed on the edge spin, and {\it ii}) strongly affects the propagation of quasiparticles emitted after the sudden removal of the defect, so that the dynamics of the local magnetization show clear deviations from a …

Physics---Phase transitionQuantum PhysicsCondensed matter physicsFOS: Physical sciencesFermion01 natural sciences010305 fluids & plasmasMAJORANAQuantum Gases (cond-mat.quant-gas)Quantum mechanics0103 physical sciencesQuasiparticleIsing model010306 general physicsQuantum Physics (quant-ph)Condensed Matter - Quantum GasesLocal fieldPhase diagramSpin-½
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System-environment correlations and Markovian embedding of quantum non-Markovian dynamics

2018

We study the dynamics of a quantum system whose interaction with an environment is described by a collision model, i.e. the open dynamics is modelled through sequences of unitary interactions between the system and the individual constituents of the environment, termed "ancillas", which are subsequently traced out. In this setting non-Markovianity is introduced by allowing for additional unitary interactions between the ancillas. For this model, we identify the relevant system-environment correlations that lead to a non-Markovian evolution. Through an equivalent picture of the open dynamics, we introduce the notion of "memory depth" where these correlations are established between the syste…

Physics---Quantum PhysicsProcess (computing)Markov processFOS: Physical sciences01 natural sciencesUnitary stateSettore FIS/03 - Fisica Della Materia010305 fluids & plasmasRendering (computer graphics)open quantum systems non markovianitysymbols.namesakeHeat flux0103 physical sciencessymbolsQuantum systemEmbeddingStatistical physics010306 general physicsQuantum Physics (quant-ph)Quantum
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