FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W3102287622> ?p ?o ?g. }

• W3102287622 endingPage "37" @default.
• W3102287622 startingPage "1" @default.
• W3102287622 abstract "We have recently established a new method for measuring the mass of unstable particles produced at hadron colliders based on the analysis of the energy distribution of a massless product from their two-body decays. The central ingredient of our proposal is the remarkable result that, for an unpolarized decaying particle, the location of the peak in the energy distribution of the observed decay product is identical to the (fixed) value of the energy that this particle would have in the rest-frame of the decaying particle, which, in turn, is a simple function of the involved masses. In addition, we utilized the property that this energy distribution is symmetric around the location of peak when energy is plotted on a logarithmic scale. The general strategy was demonstrated in several specific cases, including both beyond the standard model particles, as well as for the top quark. In the present work, we generalize this method to the case of a massive decay product from a two-body decay; this procedure is far from trivial because (in general) both the above-mentioned properties are no longer valid. Nonetheless, we propose a suitably modified parametrization of the energy distribution that was used successfully for the massless case, which can deal with the massive case as well. We test this parametrization on concrete examples of energy spectra of Z bosons from the decay of a heavier supersymmetric partner of top quark (stop) into a Z boson and a lighter stop. After establishing the accuracy of this parametrization, we study a realistic application for the same process, but now including dominant backgrounds and using foreseeable statistics at LHC14, in order to determine the performance of this method for an actual mass measurement. The upshot of our present and previous work is that, in spite of energy being a Lorentz-variant quantity, its distribution emerges as a powerful tool for mass measurement at hadron colliders." @default.
• W3102287622 created "2020-11-23" @default.
• W3102287622 creator A5013764105 @default.
• W3102287622 creator A5014442537 @default.
• W3102287622 creator A5053953466 @default.
• W3102287622 creator A5079042734 @default.
• W3102287622 date "2016-04-01" @default.
• W3102287622 modified "2023-09-25" @default.
• W3102287622 title "Energy spectra of massive two-body decay products and mass measurement" @default.
• W3102287622 cites W1525770335 @default.
• W3102287622 cites W1553281004 @default.
• W3102287622 cites W1556245918 @default.
• W3102287622 cites W1557310419 @default.
• W3102287622 cites W1759949217 @default.
• W3102287622 cites W1853996619 @default.
• W3102287622 cites W1917524157 @default.
• W3102287622 cites W1969740902 @default.
• W3102287622 cites W1971719128 @default.
• W3102287622 cites W1972887296 @default.
• W3102287622 cites W1986034677 @default.
• W3102287622 cites W2002265727 @default.
• W3102287622 cites W2004830428 @default.
• W3102287622 cites W2013870690 @default.
• W3102287622 cites W2020453148 @default.
• W3102287622 cites W2045055315 @default.
• W3102287622 cites W2045135295 @default.
• W3102287622 cites W2047229788 @default.
• W3102287622 cites W2068731054 @default.
• W3102287622 cites W2072717299 @default.
• W3102287622 cites W2076180633 @default.
• W3102287622 cites W2084429049 @default.
• W3102287622 cites W2090344627 @default.
• W3102287622 cites W2105309807 @default.
• W3102287622 cites W2105838210 @default.
• W3102287622 cites W2110999179 @default.
• W3102287622 cites W2126217975 @default.
• W3102287622 cites W2128179456 @default.
• W3102287622 cites W2131034562 @default.
• W3102287622 cites W2131169053 @default.
• W3102287622 cites W2138291582 @default.
• W3102287622 cites W2144142741 @default.
• W3102287622 cites W2158514057 @default.
• W3102287622 cites W2600683752 @default.
• W3102287622 cites W2949920378 @default.
• W3102287622 cites W2950411184 @default.
• W3102287622 cites W2963003722 @default.
• W3102287622 cites W3098187795 @default.
• W3102287622 cites W3099673264 @default.
• W3102287622 cites W3099678564 @default.
• W3102287622 cites W3099756583 @default.
• W3102287622 cites W3100357343 @default.
• W3102287622 cites W3100806184 @default.
• W3102287622 cites W3101457089 @default.
• W3102287622 cites W3101708131 @default.
• W3102287622 cites W3102016472 @default.
• W3102287622 cites W3102086449 @default.
• W3102287622 cites W3102618238 @default.
• W3102287622 cites W3102873965 @default.
• W3102287622 cites W3104300268 @default.
• W3102287622 cites W3104708536 @default.
• W3102287622 cites W3106069912 @default.
• W3102287622 cites W3106410913 @default.
• W3102287622 cites W3122116672 @default.
• W3102287622 cites W3123750486 @default.
• W3102287622 cites W3123889933 @default.
• W3102287622 cites W3125487731 @default.
• W3102287622 doi "https://doi.org/10.1007/jhep04(2016)151" @default.
• W3102287622 hasPublicationYear "2016" @default.
• W3102287622 type Work @default.
• W3102287622 sameAs 3102287622 @default.
• W3102287622 citedByCount "7" @default.
• W3102287622 countsByYear W31022876222015 @default.
• W3102287622 countsByYear W31022876222016 @default.
• W3102287622 countsByYear W31022876222017 @default.
• W3102287622 crossrefType "journal-article" @default.
• W3102287622 hasAuthorship W3102287622A5013764105 @default.
• W3102287622 hasAuthorship W3102287622A5014442537 @default.
• W3102287622 hasAuthorship W3102287622A5053953466 @default.
• W3102287622 hasAuthorship W3102287622A5079042734 @default.
• W3102287622 hasBestOaLocation W31022876221 @default.
• W3102287622 hasConcept C109214941 @default.
• W3102287622 hasConcept C121332964 @default.
• W3102287622 hasConcept C134222618 @default.
• W3102287622 hasConcept C151987854 @default.
• W3102287622 hasConcept C186370098 @default.
• W3102287622 hasConcept C202887219 @default.
• W3102287622 hasConcept C207206121 @default.
• W3102287622 hasConcept C54937798 @default.
• W3102287622 hasConcept C62520636 @default.
• W3102287622 hasConcept C74902906 @default.
• W3102287622 hasConcept C7602139 @default.
• W3102287622 hasConcept C79118098 @default.
• W3102287622 hasConcept C98444146 @default.
• W3102287622 hasConceptScore W3102287622C109214941 @default.
• W3102287622 hasConceptScore W3102287622C121332964 @default.
• W3102287622 hasConceptScore W3102287622C134222618 @default.
• W3102287622 hasConceptScore W3102287622C151987854 @default.
• W3102287622 hasConceptScore W3102287622C186370098 @default.

• next