FRINK Linked Data Fragments server

Matches in SemOpenAlex for { <https://semopenalex.org/work/W2064756417> ?p ?o ?g. }

• W2064756417 endingPage "525" @default.
• W2064756417 startingPage "508" @default.
• W2064756417 abstract "In an inclusive experiment, isotopically resolved fragments, $3ensuremath{le}Zensuremath{le}13$, produced in high-energy proton-nucleus collisions have been studied using a low mass time-of-flight, gas $ensuremath{Delta}E$-silicon $E$ spectrometer and an internal gas jet. Measurement of the kinetic energy spectra from 5 to 100 MeV enabled an accurate determination of fragment cross sections from both xenon and krypton targets. Fragment spectra showed no significant dependence on beam energy for protons between 80 and 350 GeV/c. The observed isobaric yield is given by $Yensuremath{alpha}{A}_{f}^{ensuremath{-}ensuremath{tau}}$, where $ensuremath{tau}ensuremath{sim}2.6$ for both targets; this also holds for correlated fragment data. The power law is the signature for the fragment formation mechanism. We treat the formation of fragments as a liquid-gas transition at the critical point. The critical temperature ${T}_{c}$ can be determined from the fragment isotopic yields, provided one can set an energy scale for the fragment free energy. The high energy tails of the kinetic energy spectra provide evidence that the fragments originate from a common remnant system somewhat lighter than the target which disassembles simultaneously via Coulomb repulsion into a multibody final state. Fragment Coulomb energies are about $frac{1}{10}$ of the tangent sphere values. The remnant is characterized by a parameter $T$, obtained from the high energy tails of the kinetic energy distributions. $T$ is interpreted as reflecting the Fermi momentum of a nucleon in this system. Since $Tensuremath{gg}{T}_{c}$, and $T$ is approximately that value expected for a cold nucleus, we conclude that the kinetic energy spectra are dominated by this nonthermal contribution.[NUCLEAR REACTIONS $mathrm{Xe}(mathrm{p},X)$, $mathrm{Kr}(mathrm{p},X)$, $80ensuremath{le}{E}_{q}ensuremath{le}350$ GeV; measured $ensuremath{sigma}(E,ensuremath{theta})$, $X=mathrm{Li} mathrm{to} mathrm{Al}$, $ensuremath{theta}={34}^{ensuremath{circ}}$. Fragmentation.]" @default.
• W2064756417 created "2016-06-24" @default.
• W2064756417 creator A5006281219 @default.
• W2064756417 creator A5009060646 @default.
• W2064756417 creator A5013040035 @default.
• W2064756417 creator A5017857047 @default.
• W2064756417 creator A5034553373 @default.
• W2064756417 creator A5046240723 @default.
• W2064756417 creator A5046922941 @default.
• W2064756417 creator A5061657100 @default.
• W2064756417 creator A5071291333 @default.
• W2064756417 date "1984-02-01" @default.
• W2064756417 modified "2023-10-12" @default.
• W2064756417 title "Experimental results from high energy proton-nucleus interactions, critical phenomena, and the thermal liquid drop model of fragment production" @default.
• W2064756417 cites W1975549353 @default.
• W2064756417 cites W1978554772 @default.
• W2064756417 cites W1979106816 @default.
• W2064756417 cites W1984160148 @default.
• W2064756417 cites W1990500056 @default.
• W2064756417 cites W1992125850 @default.
• W2064756417 cites W2002092152 @default.
• W2064756417 cites W2007109608 @default.
• W2064756417 cites W2007935939 @default.
• W2064756417 cites W2008241142 @default.
• W2064756417 cites W2016972073 @default.
• W2064756417 cites W2018612911 @default.
• W2064756417 cites W2020302935 @default.
• W2064756417 cites W2024927415 @default.
• W2064756417 cites W2027966993 @default.
• W2064756417 cites W2030046989 @default.
• W2064756417 cites W2031905781 @default.
• W2064756417 cites W2032415541 @default.
• W2064756417 cites W2033685400 @default.
• W2064756417 cites W2037320329 @default.
• W2064756417 cites W2056020334 @default.
• W2064756417 cites W2061446059 @default.
• W2064756417 cites W2065548148 @default.
• W2064756417 cites W2069488529 @default.
• W2064756417 cites W2075090218 @default.
• W2064756417 cites W2085469164 @default.
• W2064756417 cites W2087321214 @default.
• W2064756417 cites W2164013125 @default.
• W2064756417 cites W276905675 @default.
• W2064756417 cites W4238888089 @default.
• W2064756417 cites W63764427 @default.
• W2064756417 doi "https://doi.org/10.1103/physrevc.29.508" @default.
• W2064756417 hasPublicationYear "1984" @default.
• W2064756417 type Work @default.
• W2064756417 sameAs 2064756417 @default.
• W2064756417 citedByCount "236" @default.
• W2064756417 countsByYear W20647564172012 @default.
• W2064756417 countsByYear W20647564172013 @default.
• W2064756417 countsByYear W20647564172014 @default.
• W2064756417 countsByYear W20647564172015 @default.
• W2064756417 countsByYear W20647564172017 @default.
• W2064756417 countsByYear W20647564172018 @default.
• W2064756417 countsByYear W20647564172019 @default.
• W2064756417 countsByYear W20647564172020 @default.
• W2064756417 countsByYear W20647564172022 @default.
• W2064756417 countsByYear W20647564172023 @default.
• W2064756417 crossrefType "journal-article" @default.
• W2064756417 hasAuthorship W2064756417A5006281219 @default.
• W2064756417 hasAuthorship W2064756417A5009060646 @default.
• W2064756417 hasAuthorship W2064756417A5013040035 @default.
• W2064756417 hasAuthorship W2064756417A5017857047 @default.
• W2064756417 hasAuthorship W2064756417A5034553373 @default.
• W2064756417 hasAuthorship W2064756417A5046240723 @default.
• W2064756417 hasAuthorship W2064756417A5046922941 @default.
• W2064756417 hasAuthorship W2064756417A5061657100 @default.
• W2064756417 hasAuthorship W2064756417A5071291333 @default.
• W2064756417 hasConcept C121332964 @default.
• W2064756417 hasConcept C1276947 @default.
• W2064756417 hasConcept C135889238 @default.
• W2064756417 hasConcept C145148216 @default.
• W2064756417 hasConcept C146211579 @default.
• W2064756417 hasConcept C172695262 @default.
• W2064756417 hasConcept C184779094 @default.
• W2064756417 hasConcept C185544564 @default.
• W2064756417 hasConcept C198291218 @default.
• W2064756417 hasConcept C4839761 @default.
• W2064756417 hasConcept C54516573 @default.
• W2064756417 hasConcept C62520636 @default.
• W2064756417 hasConcept C69402668 @default.
• W2064756417 hasConcept C93282013 @default.
• W2064756417 hasConcept C97355855 @default.
• W2064756417 hasConceptScore W2064756417C121332964 @default.
• W2064756417 hasConceptScore W2064756417C1276947 @default.
• W2064756417 hasConceptScore W2064756417C135889238 @default.
• W2064756417 hasConceptScore W2064756417C145148216 @default.
• W2064756417 hasConceptScore W2064756417C146211579 @default.
• W2064756417 hasConceptScore W2064756417C172695262 @default.
• W2064756417 hasConceptScore W2064756417C184779094 @default.
• W2064756417 hasConceptScore W2064756417C185544564 @default.
• W2064756417 hasConceptScore W2064756417C198291218 @default.
• W2064756417 hasConceptScore W2064756417C4839761 @default.
• W2064756417 hasConceptScore W2064756417C54516573 @default.
• W2064756417 hasConceptScore W2064756417C62520636 @default.
• W2064756417 hasConceptScore W2064756417C69402668 @default.

• next