Matches in SemOpenAlex for { <https://semopenalex.org/work/W2077803342> ?p ?o ?g. }
- W2077803342 abstract "We show that it is possible to fit all of the HERA deep inelastic scattering data on ${F}_{2}^{ensuremath{gamma}p}$ at small values of Bjorken $x$, including the data at very low ${Q}^{2}$, using a new model for ${F}_{2}^{ensuremath{gamma}p}$ which both includes an asymptotic (high-energy) part that satisfies a saturated Froissart bound behavior, with a vector-dominance-like mass factor in the parametrization, and extends smoothly to ${Q}^{2}=0$. We require that the corresponding part of the virtual ${ensuremath{gamma}}^{*}p$ cross section match the known asymptotic part of the real $ensuremath{gamma}p$ cross section at ${Q}^{2}=0$, a cross section which is determined by strong interactions and asymptotically satisfies a saturated Froissart bound of the form $ensuremath{alpha}+ensuremath{beta}mathrm{ln}s+ensuremath{gamma}{mathrm{ln}}^{2}s$. Using this model for the asymptotic part of ${F}_{2}^{ensuremath{gamma}p}$ plus a known valence contribution, we fit the asymptotic high--energy part of the HERA data with $xensuremath{le}0.1$ and $Wensuremath{ge}25text{ }text{ }mathrm{GeV}$; the fit is excellent. We find that the mass parameter in the fit lies in the region of the light vector mesons, somewhat above the $ensuremath{rho}$-meson mass, and is compatible with vector dominance. We use this fit to obtain accurate results for the high-energy $ep$ and isoscalar $ensuremath{nu}N$ total cross sections. Both cross sections obey an analytic expression of the type $a+bmathrm{ln}E+c{mathrm{ln}}^{2}E+d{mathrm{ln}}^{3}E$ at large energies $E$ of the incident particle, reflecting the fact that the underlying strong interaction parts of the ${ensuremath{gamma}}^{*}p$, ${Z}^{*}N$ and ${W}^{*}N$ cross sections satisfy the saturated Froissart bound. Since approximately 50% of the $ensuremath{nu}N$ center-of-mass (cms) energy is found in $W$---the cms energy of the strongly interacting intermediate vector boson--nucleon system---a study of ultra-high-energy neutrino-nucleon cross sections would allow us, for the first time, to explore strong interactions at incredibly high energies." @default.
- W2077803342 created "2016-06-24" @default.
- W2077803342 creator A5045166620 @default.
- W2077803342 creator A5066147419 @default.
- W2077803342 creator A5086823847 @default.
- W2077803342 date "2014-05-29" @default.
- W2077803342 modified "2023-10-07" @default.
- W2077803342 title "Connection of the virtual<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mrow><mml:msup><mml:mrow><mml:mi>γ</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msup><mml:mi>p</mml:mi></mml:mrow></mml:math>cross section of<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi>e</mml:mi><mml:mi>p</mml:mi></mml:math>deep inelastic scattering to real<mml:math xmlns:mml=http://www.w3.org/1998/Math/MathML display=inline><mml:mi…" @default.
- W2077803342 cites W1534372718 @default.
- W2077803342 cites W1685095454 @default.
- W2077803342 cites W1965255888 @default.
- W2077803342 cites W1975212065 @default.
- W2077803342 cites W1981424385 @default.
- W2077803342 cites W1987622489 @default.
- W2077803342 cites W1989494434 @default.
- W2077803342 cites W1996534810 @default.
- W2077803342 cites W1996928793 @default.
- W2077803342 cites W1998108391 @default.
- W2077803342 cites W1998174391 @default.
- W2077803342 cites W1999186887 @default.
- W2077803342 cites W2002673332 @default.
- W2077803342 cites W2003162311 @default.
- W2077803342 cites W2005429750 @default.
- W2077803342 cites W2011231580 @default.
- W2077803342 cites W2011731219 @default.
- W2077803342 cites W2018783688 @default.
- W2077803342 cites W2022065399 @default.
- W2077803342 cites W2023338656 @default.
- W2077803342 cites W2023609273 @default.
- W2077803342 cites W2031354803 @default.
- W2077803342 cites W2033862778 @default.
- W2077803342 cites W2041736589 @default.
- W2077803342 cites W2047164550 @default.
- W2077803342 cites W2049553424 @default.
- W2077803342 cites W2049782442 @default.
- W2077803342 cites W2050124267 @default.
- W2077803342 cites W2056128073 @default.
- W2077803342 cites W2059311706 @default.
- W2077803342 cites W2060317691 @default.
- W2077803342 cites W2064465928 @default.
- W2077803342 cites W2084480984 @default.
- W2077803342 cites W2089919344 @default.
- W2077803342 cites W2091103968 @default.
- W2077803342 cites W2091919419 @default.
- W2077803342 cites W2097674566 @default.
- W2077803342 cites W2100118430 @default.
- W2077803342 cites W2113777973 @default.
- W2077803342 cites W2124822098 @default.
- W2077803342 cites W2125250794 @default.
- W2077803342 cites W2132977758 @default.
- W2077803342 cites W2138550345 @default.
- W2077803342 cites W2138896212 @default.
- W2077803342 cites W2140781439 @default.
- W2077803342 cites W2159774655 @default.
- W2077803342 cites W2166327671 @default.
- W2077803342 cites W2171296441 @default.
- W2077803342 cites W2204374793 @default.
- W2077803342 cites W2204476295 @default.
- W2077803342 cites W3101187986 @default.
- W2077803342 cites W3104115203 @default.
- W2077803342 cites W3121796360 @default.
- W2077803342 cites W4214652969 @default.
- W2077803342 doi "https://doi.org/10.1103/physrevd.89.094027" @default.
- W2077803342 hasPublicationYear "2014" @default.
- W2077803342 type Work @default.
- W2077803342 sameAs 2077803342 @default.
- W2077803342 citedByCount "56" @default.
- W2077803342 countsByYear W20778033422015 @default.
- W2077803342 countsByYear W20778033422016 @default.
- W2077803342 countsByYear W20778033422017 @default.
- W2077803342 countsByYear W20778033422018 @default.
- W2077803342 countsByYear W20778033422019 @default.
- W2077803342 countsByYear W20778033422020 @default.
- W2077803342 countsByYear W20778033422021 @default.
- W2077803342 countsByYear W20778033422022 @default.
- W2077803342 countsByYear W20778033422023 @default.
- W2077803342 crossrefType "journal-article" @default.
- W2077803342 hasAuthorship W2077803342A5045166620 @default.
- W2077803342 hasAuthorship W2077803342A5066147419 @default.
- W2077803342 hasAuthorship W2077803342A5086823847 @default.
- W2077803342 hasBestOaLocation W20778033422 @default.
- W2077803342 hasConcept C109214941 @default.
- W2077803342 hasConcept C117137515 @default.
- W2077803342 hasConcept C121332964 @default.
- W2077803342 hasConcept C186370098 @default.
- W2077803342 hasConcept C200006409 @default.
- W2077803342 hasConcept C2780070031 @default.
- W2077803342 hasConcept C2780234265 @default.
- W2077803342 hasConcept C62520636 @default.
- W2077803342 hasConcept C88407732 @default.
- W2077803342 hasConceptScore W2077803342C109214941 @default.
- W2077803342 hasConceptScore W2077803342C117137515 @default.
- W2077803342 hasConceptScore W2077803342C121332964 @default.
- W2077803342 hasConceptScore W2077803342C186370098 @default.
- W2077803342 hasConceptScore W2077803342C200006409 @default.
- W2077803342 hasConceptScore W2077803342C2780070031 @default.
- W2077803342 hasConceptScore W2077803342C2780234265 @default.
- W2077803342 hasConceptScore W2077803342C62520636 @default.
- W2077803342 hasConceptScore W2077803342C88407732 @default.
- W2077803342 hasIssue "9" @default.