Search Results - "Block, Martin M."

Decoupling the NLO coupled DGLAP evolution equations: an analytic solution to pQCD by Block, Martin M., Durand, Loyal, Ha, Phuoc, McKay, Douglas W.

“…Using repeated Laplace transforms, we turn coupled, integral-differential singlet DGLAP equations into NLO (next-to-leading) coupled algebraic equations, which…”
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Experimental confirmation that the proton is asymptotically a black disk by Block, Martin M, Halzen, Francis

“…Although experimentally accessible energies cannot probe "asymptopia", recent measurements of inelastic pp cross sections at the LHC at 7000 GeV and by Auger…”
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A new numerical method for inverse Laplace transforms used to obtain gluon distributions from the proton structure function by Block, Martin M., Durand, Loyal

“…We recently derived a very accurate and fast new algorithm for numerically inverting the Laplace transforms needed to obtain gluon distributions from the…”
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Addendum to: A new numerical method for obtaining gluon distribution functions G(x,Q2)=xg(x,Q2), from the proton structure function by Block, Martin M.

“…Since publication of M.M. Block in Eur. Phys. J. C 65, 1 ( 2010 ), we have discovered that the algorithm of Block ( 2010 ) does not work if g ( s )→0 less…”
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A new numerical method for obtaining gluon distribution functions G(x,Q2)=xg(x,Q2), from the proton structure function by Block, Martin M.

“…An exact expression for the leading-order (LO) gluon distribution function G ( x , Q 2 )= xg ( x , Q 2 ) from the DGLAP evolution equation for the proton…”
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A new numerical method for obtaining gluon distribution functions G(x,Q 2)=xg(x,Q 2), from the proton structure function $F_{2}^{\gamma p}(x,Q^{2}) by Block, Martin M.

“…An exact expression for the leading-order (LO) gluon distribution function G(x,Q super(2))=xg(x,Q super(2)) from the DGLAP evolution equation for the proton…”
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Forward hadronic scattering at 7 TeV: An update on predictions for the LHC by Block, Martin M., Halzen, Francis

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Implications of a Froissart bound saturation of γ − p deep inelastic scattering. I. Quark distributions at ultra small x by Block, Martin M., Durand, Loyal, Ha, Phuoc, McKay, Douglas W.

“…We argue that the deep inelastic structure function F[[sub 2] [sup gamma p]] (x, O[sup 2]), regarded as a cross section for virtual [ gamma [sup *]] p…”
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Implications of a Froissart bound saturation of γ − p deep inelastic scattering. II. Ultrahigh energy neutrino interactions by Block, Martin M., Durand, Loyal, Ha, Phuoc, McKay, Douglas W.

“…In part I we argued that the structure function F[[sub 2] [sup gamma p]] in deep inelastic ep scattering, regarded as a cross section for virtual [ gamma [sup…”
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Forward hadronic scattering at 8 TeV: Predictions for the LHC by Block, Martin M., Halzen, Francis

“…The Large Hadron Collider (LHC) recently started operating at 8 TeV. In this paper, we update our earlier LHC forward hadronic scattering predictions [Phys…”
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Evidence for an energy-invariant "edge" in proton-proton scattering at very high energies by Block, Martin M, Durand, Loyal, Halzen, Francis, Stodolsky, Leo, Weller, Thomas J

“…Accurate fits to pp and pp cross section, data up to Tevatron energies, incorporating the constraints imposed by analyticity and unitarity, successfully…”
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Addendum to: A new numerical method for obtaining gluon distribution functions G(x,Q 2)=xg(x,Q 2), from the proton structure function $F_{2}^{\gamma p}(x,Q^{2}) by Block, Martin M.

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A new numerical method for obtaining gluon distribution functions G(x, Q2) = x g(x, Q2), from the proton structure function Fγp2(x, Q2) by BLOCK, Martin M

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Addendum to: A new numerical method for obtaining gluon distribution functions G(x, Q2) = xg (x, Q2), from the proton structure function Fγp2(x, Q2) by BLOCK, Martin M

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Commentary on “Total Hadronic Cross-Section Data and the Froissart–Martin Bound,” by Fagundes, Menon, and Silva by Block, Martin M., Halzen, Francis

“…This commentary on the paper “Total Hadronic Cross-Section Data and the Froissart–Martin Bound,” by Fagundes, Menon, and Silva (Braz. J. Phys. doi:…”
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Addendum to: a new numerical method for obtaining gluon distribution functions G by Block, Martin M

“…Since publication of M.M. Block in Eur. Phys. J. C 65, 1 (2010), we have discovered that the algorithm of Block (2010) does not work if g(s) → 0 less rapidly…”
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A new numerical method for obtaining gluon distribution functions G by Block, Martin M

“…An exact expression for the leading-order (LO) gluon distribution function G(x, [Q.sup.2]) = xg(x, [Q.sup.2]) from the DGLAP evolution equation for the proton…”
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Evidence for an energy-invariant “edge” in proton-proton scattering at very high energies by Block, Martin M., Durand, Loyal, Halzen, Francis, Stodolsky, Leo, Weiler, Thomas J.

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New experimental evidence that the proton develops asymptotically into a black disk by Block, Martin M., Halzen, Francis

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Comprehensive fits to high energy data for σ , ρ , and B , and the asymptotic black-disk limit by Block, Martin M., Durand, Loyal, Ha, Phuoc, Halzen, Francis

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