Search results for "Physical phenomena"

showing 10 items of 5034 documents

"Table 5" of "The ALICE Transition Radiation Detector: construction, operation, and performance"

2017

Most probable charge deposit signal normalised to that of minimum ionising particles as a function of $\beta\gamma$ for cosmic-ray muons (dE/dx + TR). Statistical uncertainties as vertical error bars. Uncertainties in momentum and thus $\beta \gamma$ determination are drawn as horizontal error bars.

$Q_{\rm MPV}/Q_{\rm MPV}^{\rm mip}$Astrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::Experiment
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"Table 4" of "The ALICE Transition Radiation Detector: construction, operation, and performance"

2017

Most probable charge deposit signal normalised to that of minimum ionising particles as a function of $\beta\gamma$ for cosmic-ray muons (dE/dx). Statistical uncertainties as vertical error bars. Uncertainties in momentum and thus $\beta \gamma$ determination are drawn as horizontal error bars.

$Q_{\rm MPV}/Q_{\rm MPV}^{\rm mip}$Astrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::Experiment
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"Table 3" of "The ALICE Transition Radiation Detector: construction, operation, and performance"

2017

Most probable charge deposit signal normalised to that of minimum ionising particles as a function of $\beta\gamma$ for $\pi$, $\it{e}$ and proton in pp collisions ($\sqrt{s} = 7$ TeV). Statistical uncertainties as vertical error bars. Uncertainties in momentum and thus $\beta \gamma$ determination are drawn as horizontal error bars.

$Q_{\rm MPV}/Q_{\rm MPV}^{\rm mip}$Astrophysics::High Energy Astrophysical PhenomenaNuclear Experiment
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"Table 35" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Fraction of photons with a value of shower shape variable $\Delta E$ lower than the threshold, for photons originating from the BSM process $X\rightarrow\gamma\gamma$, where the $X$ particle is a high-mass narrow-width scalar particle originating from the gluon--gluon fusion process.

$pp\rightarrow X \rightarrow \gamma\gamma$Astrophysics::High Energy Astrophysical PhenomenaCategory fractionHigh Energy Physics::PhenomenologyHigh Energy Physics::Experiment13000Photon-jet
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"Table 28" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Fraction of reconstructed photons with a value of shower shape variable $\Delta E$ lower than the threshold, for reconstructed photons originating from the decay $a\rightarrow 3\pi^0\rightarrow 6\gamma$ with $m_a$ = 0.5 GeV.

$pp\rightarrow X \rightarrow aa \rightarrow 6\pi^0$Astrophysics::High Energy Astrophysical PhenomenaCategory fractionHigh Energy Physics::PhenomenologyHigh Energy Physics::Experiment13000Photon-jet
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"Table 32" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Fraction of reconstructed photons with a value of shower shape variable $\Delta E$ lower than the threshold, for reconstructed photons originating from the decay $a\rightarrow 3\pi^0\rightarrow 6\gamma$ with $m_a$ = 5 GeV.

$pp\rightarrow X \rightarrow aa \rightarrow 6\pi^0$Astrophysics::High Energy Astrophysical PhenomenaCategory fractionHigh Energy Physics::PhenomenologyHigh Energy Physics::Experiment13000Photon-jet
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"Table 33" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Fraction of reconstructed photons with a value of shower shape variable $\Delta E$ lower than the threshold, for reconstructed photons originating from the decay $a\rightarrow 3\pi^0\rightarrow 6\gamma$ with $m_a$ = 10 GeV.

$pp\rightarrow X \rightarrow aa \rightarrow 6\pi^0$Astrophysics::High Energy Astrophysical PhenomenaCategory fractionHigh Energy Physics::PhenomenologyHigh Energy Physics::Experiment13000Photon-jet
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"Table 29" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Fraction of reconstructed photons with a value of shower shape variable $\Delta E$ lower than the threshold, for reconstructed photons originating from the decay $a\rightarrow 3\pi^0\rightarrow 6\gamma$ with $m_a$ = 0.7 GeV.

$pp\rightarrow X \rightarrow aa \rightarrow 6\pi^0$Astrophysics::High Energy Astrophysical PhenomenaCategory fractionHigh Energy Physics::PhenomenologyHigh Energy Physics::Experiment13000Photon-jet
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"Table 31" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Fraction of reconstructed photons with a value of shower shape variable $\Delta E$ lower than the threshold, for reconstructed photons originating from the decay $a\rightarrow 3\pi^0\rightarrow 6\gamma$ with $m_a$ = 2 GeV.

$pp\rightarrow X \rightarrow aa \rightarrow 6\pi^0$Astrophysics::High Energy Astrophysical PhenomenaCategory fractionHigh Energy Physics::PhenomenologyHigh Energy Physics::Experiment13000Photon-jet
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"Table 30" of "Search for pairs of highly collimated photon-jets in $pp$ collisions at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

2018

Fraction of reconstructed photons with a value of shower shape variable $\Delta E$ lower than the threshold, for reconstructed photons originating from the decay $a\rightarrow 3\pi^0\rightarrow 6\gamma$ with $m_a$ = 1 GeV.

$pp\rightarrow X \rightarrow aa \rightarrow 6\pi^0$Astrophysics::High Energy Astrophysical PhenomenaCategory fractionHigh Energy Physics::PhenomenologyHigh Energy Physics::Experiment13000Photon-jet
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