English
Related papers

Related papers: Froissart Bound on Total Cross-section without Unk…

200 papers

Recently Andr\'e Martin has proved a rigorous upper bound on the inelastic cross-section $\sigma_{inel}$ at high energy which is one-fourth of the known Froissart-Martin-Lukaszuk upper bound on $\sigma_{tot}$. Here we obtain an upper bound…

High Energy Physics - Phenomenology · Physics 2011-08-08 Tai Tsun Wu , André Martin , Shasanka Mohan Roy , Virendra Singh

Lattice QCD studies of hadron-hadron interactions are performed by computing the energy levels of the system in a finite box. The shifts in energy levels proportional to inverse powers of the volume are related to scattering parameters in a…

High Energy Physics - Lattice · Physics 2014-11-17 Paulo F. Bedaque , Ikuro Sato , Andre Walker-Loud

We have made a precise measurement of the inclusive jet cross section at $\sqrt{s}$=1800 GeV. The result is based on an integrated luminosity of 92 pb^{-1} collected at the Fermilab Tevatron $\bar{p}p$ Collider with the D\O detector. The…

High Energy Physics - Experiment · Physics 2019-08-14 Levan Babukhadia

We compute the ratio of pseudoscalar decay constants f_K/f_pi using domain-wall valence quarks and rooted improved Kogut-Susskind sea quarks. By employing continuum chiral perturbation theory, we extract the Gasser-Leutwyler low-energy…

High Energy Physics - Lattice · Physics 2008-11-26 S. R. Beane , P. F. Bedaque , K. Orginos , M. J. Savage

We analyze forward Compton scattering, using real analytic amplitudes. By fitting the total \gamma p scattering cross section data in the high energy region 5 GeV < \sqrt s < 20 GeV, using a cross section rising as \ln^2 s, we calculate…

High Energy Physics - Phenomenology · Physics 2009-11-07 M. M. Block

In Part I (in this journal) we argued that the structure function $F_2^{\gamma p}(x,Q^2)$ in deep inelastic $ep$ scattering, regarded as a cross section for virtual $\gamma^*p$ scattering, has a saturated Froissart-bounded form behaving as…

High Energy Physics - Phenomenology · Physics 2014-02-10 Martin M. Block , Loyal Durand , Phuoc Ha , Douglas W. McKay

CERN measurements of pi(-)p->pi(-)pi(+)n on polarized target at 17.2 GeV/c enable experimental determination of partial wave production amplitudes below 1080 MeV. The measured S-wave transversity amplitudes provide evidence for a narrow…

High Energy Physics - Phenomenology · Physics 2007-05-23 M. Svec

We show that the energy gap for the BCS gap equation is $ \Xi = \mu \left( 8 e^{-2} + o(1)\right) \exp\left( \frac{\pi}{2\sqrt{\mu} a}\right) $ in the low density limit $\mu \to 0$. Together with the similar result for the critical…

Mathematical Physics · Physics 2021-02-16 Asbjørn Bækgaard Lauritsen

Fits to high energy data alone cannot cleanly discriminate between asymptotic $\ln s$ and $\ln^2s$ behavior of total hadronic cross sections. We demonstrate that this is no longer true when we require that these amplitudes also describe, on…

High Energy Physics - Phenomenology · Physics 2014-11-18 M. M. Block , F. Halzen

We complete and improve the fits to experimental $\pi\pi$ scattering amplitudes, both at low and high energies, that we performed in the previous papers of this series. We then verify that the corresponding amplitudes satisfy analyticity…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Kaminski , J. R. Pelaez , F. J. Yndurain

We discuss the general behavior of the near-threshold scattering amplitude with channel couplings. The signal of the exotic hadrons near the threshold may manifest as a dip structure in the cross section originated from a zero point of the…

High Energy Physics - Phenomenology · Physics 2025-03-04 Katsuyoshi Sone , Tetsuo Hyodo

The cross section of the process e^+e^-\to \pi^+\pi^- was measured in the SND experiment at the VEPP-2M collider in the energy region 400<\sqrt[]{s}<1000 MeV. This measurement was based on about 12.4 \times 10^6 selected collinear events,…

Photoproduction of the $\omega$ meson on the proton has been experimentally studied near the threshold. The total cross sections are determined at incident energies ranging from 1.09 to 1.15 GeV. The 1/2 and 3/2 spin-averaged scattering…

The Froissart asymptotic behavior of cross-sections is usually considered in a parton picture as corresponding to the collision of two almost black disks filled with partons. In this article we mainly concentrate on the examination of the…

High Energy Physics - Phenomenology · Physics 2007-05-23 O. V. Kancheli

The cross-section for inclusive phi meson production in pp collisions at a centre-of-mass energy of sqrt(s) = 7 TeV has been measured with the LHCb detector at the Large Hadron Collider. The differential cross-section is measured as a…

High Energy Physics - Experiment · Physics 2011-10-25 LHCb Collaboration , R. Aaij , B. Adeva , M. Adinolfi , C. Adrover , A. Affolder , Z. Ajaltouni , J. Albrecht , F. Alessio , M. Alexander , G. Alkhazov , P. Alvarez Cartelle , A. A. Alves , S. Amato , Y. Amhis , J. Anderson , R. B. Appleby , O. Aquines Gutierrez , L. Arrabito , A. Artamonov , M. Artuso , E. Aslanides , G. Auriemma , S. Bachmann , J. J. Back , D. S. Bailey , V. Balagura , W. Baldini , R. J. Barlow , C. Barschel , S. Barsuk , W. Barter , A. Bates , C. Bauer , Th. Bauer , A. Bay , I. Bediaga , K. Belous , I. Belyaev , E. Ben-Haim , M. Benayoun , G. Bencivenni , S. Benson , J. Benton , R. Bernet , M. -O. Bettler , M. van Beuzekom , A. Bien , S. Bifani , A. Bizzeti , P. M. Bjørnstad , T. Blake , F. Blanc , C. Blanks , J. Blouw , S. Blusk , A. Bobrov , V. Bocci , A. Bondar , N. Bondar , W. Bonivento , S. Borghi , A. Borgia , T. J. V. Bowcock , C. Bozzi , T. Brambach , J. van den Brand , J. Bressieux , D. Brett , S. Brisbane , M. Britsch , T. Britton , N. H. Brook , A. Büchler-Germann , A. Bursche , J. Buytaert , S. Cadeddu , J. M. Caicedo Carvajal , O. Callot , M. Calvi , M. Calvo Gomez , A. Camboni , P. Campana , A. Carbone , G. Carboni , R. Cardinale , A. Cardini , L. Carson , K. Carvalho Akiba , G. Casse , M. Cattaneo , M. Charles , Ph. Charpentier , N. Chiapolini , X. Cid Vidal , P. E. L. Clarke , M. Clemencic , H. V. Cliff , J. Closier , C. Coca , V. Coco , J. Cogan , P. Collins , F. Constantin , G. Conti , A. Contu , A. Cook , M. Coombes , G. Corti , G. A. Cowan , R. Currie , B. D'Almagne , C. D'Ambrosio , P. David , I. De Bonis , S. De Capua , M. De Cian , F. De Lorenzi , J. M. De Miranda , L. De Paula , P. De Simone , D. Decamp , M. Deckenhoff , H. Degaudenzi , M. Deissenroth , L. Del Buono , C. Deplano , O. Deschamps , F. Dettori , J. Dickens , H. Dijkstra , P. Diniz Batista , D. Dossett , A. Dovbnya , F. Dupertuis , R. Dzhelyadin , C. Eames , S. Easo , U. Egede , V. Egorychev , S. Eidelman , D. van Eijk , F. Eisele , S. Eisenhardt , R. Ekelhof , L. Eklund , Ch. Elsasser , D. G. d'Enterria , D. Esperante Pereira , L. Estève , A. Falabella , E. Fanchini , C. Färber , G. Fardell , C. Farinelli , S. Farry , V. Fave , V. Fernandez Albor , M. Ferro-Luzzi , S. Filippov , C. Fitzpatrick , M. Fontana , F. Fontanelli , R. Forty , M. Frank , C. Frei , M. Frosini , S. Furcas , A. Gallas Torreira , D. Galli , M. Gandelman , P. Gandini , Y. Gao , J-C. Garnier , J. Garofoli , J. Garra Tico , L. Garrido , C. Gaspar , N. Gauvin , M. Gersabeck , T. Gershon , Ph. Ghez , V. Gibson , V. V. Gligorov , C. Göbel , D. Golubkov , A. Golutvin , A. Gomes , H. Gordon , M. Grabalosa Gándara , R. Graciani Diaz , L. A. Granado Cardoso , E. Graugés , G. Graziani , A. Grecu , S. Gregson , B. Gui , E. Gushchin , Yu. Guz , T. Gys , G. Haefeli , C. Haen , S. C. Haines , T. Hampson , S. Hansmann-Menzemer , R. Harji , N. Harnew , J. Harrison , P. F. Harrison , J. He , V. Heijne , K. Hennessy , P. Henrard , J. A. Hernando Morata , E. van Herwijnen , W. Hofmann , K. Holubyev , P. Hopchev , W. Hulsbergen , P. Hunt , T. Huse , R. S. Huston , D. Hutchcroft , D. Hynds , V. Iakovenko , P. Ilten , J. Imong , R. Jacobsson , A. Jaeger , M. Jahjah Hussein , E. Jans , F. Jansen , P. Jaton , B. Jean-Marie , F. Jing , M. John , D. Johnson , C. R. Jones , B. Jost , S. Kandybei , M. Karacson , T. M. Karbach , J. Keaveney , U. Kerzel , T. Ketel , A. Keune , B. Khanji , Y. M. Kim , M. Knecht , S. Koblitz , P. Koppenburg , A. Kozlinskiy , L. Kravchuk , K. Kreplin , G. Krocker , P. Krokovny , F. Kruse , K. Kruzelecki , M. Kucharczyk , S. Kukulak , R. Kumar , T. Kvaratskheliya , V. N. La Thi , D. Lacarrere , G. Lafferty , A. Lai , D. Lambert , R. W. Lambert , E. Lanciotti , G. Lanfranchi , C. Langenbruch , T. Latham , R. Le Gac , J. van Leerdam , J. -P. Lees , R. Lefèvre , A. Leflat , J. Lefrançois , O. Leroy , T. Lesiak , L. Li , Y. Y. Li , L. Li Gioi , M. Lieng , R. Lindner , C. Linn , B. Liu , G. Liu , J. H. Lopes , E. Lopez Asamar , N. Lopez-March , J. Luisier , F. Machefert , I. V. Machikhiliyan , F. Maciuc , O. Maev , J. Magnin , S. Malde , R. M. D. Mamunur , G. Manca , G. Mancinelli , N. Mangiafave , U. Marconi , R. Märki , J. Marks , G. Martellotti , A. Martens , L. Martin , A. Martín Sánchez , D. Martinez Santos , A. Massafferri , Z. Mathe , C. Matteuzzi , M. Matveev , E. Maurice , B. Maynard , A. Mazurov , G. McGregor , R. McNulty , C. Mclean , M. Meissner , M. Merk , J. Merkel , R. Messi , S. Miglioranzi , D. A. Milanes , M. -N. Minard , S. Monteil , D. Moran , P. Morawski , J. V. Morris , R. Mountain , I. Mous , F. Muheim , K. Müller , R. Muresan , B. Muryn , M. Musy , P. Naik , T. Nakada , R. Nandakumar , J. Nardulli , I. Nasteva , M. Nedos , M. Needham , N. Neufeld , C. Nguyen-Mau , M. Nicol , S. Nies , V. Niess , N. Nikitin , A. Oblakowska-Mucha , V. Obraztsov , S. Oggero , S. Ogilvy , O. Okhrimenko , R. Oldeman , M. Orlandea , J. M. Otalora Goicochea , B. Pal , J. Palacios , M. Palutan , J. Panman , A. Papanestis , M. Pappagallo , C. Parkes , C. J. Parkinson , G. Passaleva , G. D. Patel , M. Patel , S. K. Paterson , G. N. Patrick , C. Patrignani , C. Pavel-Nicorescu , A. Pazos Alvarez , A. Pellegrino , G. Penso , M. Pepe Altarelli , S. Perazzini , D. L. Perego , E. Perez Trigo , A. Pérez-Calero Yzquierdo , P. Perret , M. Perrin-Terrin , G. Pessina , A. Petrella , A. Petrolini , B. Pie Valls , B. Pietrzyk , T. Pilar , D. Pinci , R. Plackett , S. Playfer , M. Plo Casasus , G. Polok , A. Poluektov , E. Polycarpo , D. Popov , B. Popovici , C. Potterat , A. Powell , T. du Pree , J. Prisciandaro , V. Pugatch , A. Puig Navarro , W. Qian , J. H. Rademacker , B. Rakotomiaramanana , I. Raniuk , G. Raven , S. Redford , M. M. Reid , A. C. dos Reis , S. Ricciardi , K. Rinnert , D. A. Roa Romero , P. Robbe , E. Rodrigues , F. Rodrigues , P. Rodriguez Perez , G. J. Rogers , V. Romanovsky , J. Rouvinet , T. Ruf , H. Ruiz , G. Sabatino , J. J. Saborido Silva , N. Sagidova , P. Sail , B. Saitta , C. Salzmann , M. Sannino , R. Santacesaria , R. Santinelli , E. Santovetti , M. Sapunov , A. Sarti , C. Satriano , A. Satta , M. Savrie , D. Savrina , P. Schaack , M. Schiller , S. Schleich , M. Schmelling , B. Schmidt , O. Schneider , A. Schopper , M. -H. Schune , R. Schwemmer , A. Sciubba , M. Seco , A. Semennikov , K. Senderowska , N. Serra , J. Serrano , P. Seyfert , B. Shao , M. Shapkin , I. Shapoval , P. Shatalov , Y. Shcheglov , T. Shears , L. Shekhtman , O. Shevchenko , V. Shevchenko , A. Shires , R. Silva Coutinho , H. P. Skottowe , T. Skwarnicki , A. C. Smith , N. A. Smith , K. Sobczak , F. J. P. Soler , A. Solomin , F. Soomro , B. Souza De Paula , B. Spaan , A. Sparkes , P. Spradlin , F. Stagni , S. Stahl , O. Steinkamp , S. Stoica , S. Stone , B. Storaci , U. Straumann , N. Styles , S. Swientek , M. Szczekowski , P. Szczypka , T. Szumlak , S. T'Jampens , E. Teodorescu , F. Teubert , C. Thomas , E. Thomas , J. van Tilburg , V. Tisserand , M. Tobin , S. Topp-Joergensen , M. T. Tran , A. Tsaregorodtsev , N. Tuning , A. Ukleja , P. Urquijo , U. Uwer , V. Vagnoni , G. Valenti , R. Vazquez Gomez , P. Vazquez Regueiro , S. Vecchi , J. J. Velthuis , M. Veltri , K. Vervink , B. Viaud , I. Videau , X. Vilasis-Cardona , J. Visniakov , A. Vollhardt , D. Voong , A. Vorobyev , H. Voss , K. Wacker , S. Wandernoth , J. Wang , D. R. Ward , A. D. Webber , D. Websdale , M. Whitehead , D. Wiedner , L. Wiggers , G. Wilkinson , M. P. Williams , M. Williams , F. F. Wilson , J. Wishahi , M. Witek , W. Witzeling , S. A. Wotton , K. Wyllie , Y. Xie , F. Xing , Z. Yang , R. Young , O. Yushchenko , M. Zavertyaev , L. Zhang , W. C. Zhang , Y. Zhang , A. Zhelezov , L. Zhong , E. Zverev , A. Zvyagin

Antiproton-deuteron (${\bar p}d$) scattering is calculated at beam energies below 300 MeV within the Glauber approach, utilizing the amplitudes of the J\"ulich $\bar N N$ models. A good agreement is obtained with available experimental data…

Nuclear Theory · Physics 2015-05-28 Yu. N. Uzikov , J. Haidenbauer

Use of the effective Lagrangian incorporating both the scalar and pseudoscalar mesons gives a possibility to calculate the $\pi \pi$-scattering lengths without attraction of the ChPT theory.

High Energy Physics - Phenomenology · Physics 2016-06-22 E. P. Shabalin

We calculate the pi+ K+ scattering length in fully-dynamical lattice QCD with domain-wall valence quarks on MILC lattices with rooted staggered sea-quarks at a lattice spacing of b=0.125 fm, lattice spatial size of L =2.5 fm and at pion…

High Energy Physics - Lattice · Physics 2008-11-26 Silas R. Beane , Paulo F. Bedaque , Thomas C. Luu , Kostas Orginos , Elisabetta Pallante , Assumpta Parreno , Martin J. Savage

We consider the random fluctuations of the free energy in the $p$-spin version of the Sherrington-Kirkpatrick model in the high temperature regime. Using the martingale approach of Comets and Neveu as used in the standard SK model combined…

Disordered Systems and Neural Networks · Physics 2007-05-23 A. Bovier , I. Kurkova , M. Loewe

We investigate the determination of the pole associated to $\sigma$ from $\pi\pi$ scattering data below the $K\bar{K}$ threshold, including the new precise data from $K_{e4}$ decay reported recently by the NA48/2 Collaboration. Using a…

High Energy Physics - Phenomenology · Physics 2008-11-26 Irinel Caprini