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"Table 159" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2018
${\Delta\Phi}^{t\bar{t}}$ covariance matrix for absolute differential cross-section in parton level
"Table 156" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2018
$|{p_{out}}^{t\bar{t}}|$ correlation matrix for absolute differential cross-section in parton level
"Table 158" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2018
$|{p_{out}}^{t\bar{t}}|$ correlation matrix for relative differential cross-section in parton level
"Table 166" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2019
$H_{T}^{t\bar{t}}$ correlation matrix for the normalized differential cross-section at parton level
"Table 158" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ col…
2019
$|{p_{out}}^{t\bar{t}}|$ correlation matrix for the normalized differential cross-section at parton level
Disidentità: una sola moltitudine o solo molta solitudine?
2011
Abstract: Gli sviluppi gruppo analitici italiani hanno ereditato dalle teorie foulkesiane un modello di lettura della psiche basato sulla corrispondenza tra individuo e società. Pertanto, essi ci aiutano a comprendere le ragioni della “battuta d’arresto” in cui sembra incagliarsi, oggi, la dialettica Io-mondo, e conseguentemente, le difficoltà inerenti lo sviluppo dell’identità. In particolare, questo studio, che analizza da un canto la povertà del processo d'interiorizzazione, e dall'altro la difficoltà a ri-concepire ciò che si è interiorizzato, interroga il senso del disagio post-moderno rintracciandone le radici nella difettività della fondazione intersoggettiva della mente: nella dimen…
Decoherence without entanglement and quantum Darwinism
2020
It is often assumed that decoherence arises as a result of the entangling interaction between a quantum system and its environment, as a consequence of which the environment effectively measures the system, thus washing away its quantum properties. Moreover, this interaction results in the emergence of a classical objective reality, as described by quantum Darwinism. In this Rapid Communication, we show that the idea that entanglement is needed for decoherence is imprecise. We propose a dynamical mixing mechanism capable of inducing decoherence dynamics on a system without creating any entanglement with its quantum environment. We illustrate this mechanism by introducing a simple and exactl…
"Table 2" of "Search for Higgs boson decays into a $Z$ boson and a light hadronically decaying resonance using 13 TeV $pp$ collision data from the AT…
2020
Efficiencies of the MLP selection, complete selection and total expected signal yields for each signal sample, assuming B$(H\to Z(Q/a))=100\%$ and $\sigma(pp\to H) = \sigma_\text{SM}(pp\to H)$. Pythia 8 branching fractions of $a$ are assumed using a $\tan\beta$ value of 1. The MLP efficiencies, total efficiencies, and expected yields are determined using MC samples, with uncertainties due to MC sample statistics, except for the expected background yield. The expected background yield and its uncertainty is calculated as described in the main text of the paper.
"Table 1" of "Search for Higgs boson decays into a $Z$ boson and a light hadronically decaying resonance using 13 TeV $pp$ collision data from the AT…
2020
Observed number of data events and expected number of background events in the signal region.
"Table 70" of "Measurements of $t\bar{t}$ differential cross-sections of highly boosted top quarks decaying to all-hadronic final states in $pp$ coll…
2019
$\Delta \phi(t_{1}, t_{2})$ correlation matrix for the normalized differential cross-section at particle level