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We determine the mass and strength of the scalar meson from NN scattering data by renormalizing the One Boson Exchange Potential. This procedure provides a great insensitivity to the unknown short distance interaction making the vector…

Nuclear Theory · Physics 2011-08-31 A. Calle Cordon , E. Ruiz Arriola

In the framework of the Bethe-Salpeter formalism used in previous papers to evaluate the quarkonium spectrum, here we reverse the point of view to extract an ``experimental'' running coupling alpha_s(Q^2) in the infrared (IR) region from…

High Energy Physics - Phenomenology · Physics 2008-11-26 M. Baldicchi , G. M. Prosperi , C. Simolo

We study nucleon-nucleon ($NN$) scattering by applying the $N/D$ method in chiral perturbation theory up to next-to-next-to-leading (NNLO) order in the calculation of the imaginary part of the $NN$ partial-wave amplitudes along the…

Nuclear Theory · Physics 2014-02-13 J. A. Oller

Near threshold pion production experiments have been recently carried out and used to extract S--wave $\pi\pi$ scattering lengths. We emphasize here that at present these processes are related only at the tree level (and its first…

High Energy Physics - Phenomenology · Physics 2014-11-17 M. G. Olsson , Ulf-G. Meißner , N. Kaiser , V. Bernard

We determine the $\pi NN$ and $\pi N\Delta$ formfactors from the $P_{11}$ resp. $P_{33}$ partial wave of $\pi N$ scattering by dressing corresponding bare vertices with the help of $\pi N$ non--pole contributions. The underlying model is…

Nuclear Theory · Physics 2008-11-26 C. Schütz , K. Holinde

We report a next-to-leading-order (NLO) chiral perturbation theory calculation of the neutron-proton scattering cross section in the ${}^1S_0$ channel using a cut-off regularization. The inclusion of two-pion exchanges in the irreducible…

Nuclear Theory · Physics 2014-11-18 C. H. Hyun , T. -S. Park , D. -P. Min

Associative photoproduction of $\omega$-meson and $N^{*}(1440)$ on nucleons, $\gamma+N\to\omega+N^{*}(1440)$, in the near threshold region is investigated in a framework employing effective Lagrangians. Besides $\pi$-exchange in t-channel,…

Nuclear Theory · Physics 2009-11-07 H. Babacan , T. Babacan

The compatibility of theoretically calculated values for the strong coupling constant,through the renormalization group approach with experimental data is studied. There exist considerable divergence in-between theoretical and experimental…

High Energy Physics - Phenomenology · Physics 2021-05-28 K. Javidan , M. M. Yazdanpanah , H. Nematollahi

We reinvestigate the QCD sum rule for the pi NN coupling constant, g, starting from the vacuum-to-pion matrix element of the correlation function of the interpolating fields of two nucleons. We study in detail the physical content of the…

Nuclear Theory · Physics 2009-11-07 Yoshihiko Kondo , Osamu Morimatsu

The leading-order nucleon-nucleon (NN) potential derived from chiral perturbation theory consists of one-pion exchange plus a short-distance contact interaction. We show that in the 1S0 and 3S1-3D1 channels renormalization of the…

Nuclear Theory · Physics 2008-11-26 C. -J. Yang , Ch. Elster , D. R. Phillips

New solutions on the scalar -- isoscalar $\pi\pi$ phase shifts are analysed together with previous $K\bar{K}$ results using a separable potential model of three coupled channels ($\pi\pi$, $K\bar{K}$ and an effective $2\pi 2\pi$ system).…

High Energy Physics - Phenomenology · Physics 2008-11-26 R. Kaminski , L. Lesniak , B. Loiseau

In the large $N_c$ approximation to $QCD$, the leading $\pp$ scattering amplitude is expressed as the sum of an infinite number of tree diagrams. We investigate the possibility that an adequate approximation at energies up to somewhat more…

High Energy Physics - Phenomenology · Physics 2009-10-28 F. Sannino , J. Schechter

We report the first double-differential cross section measurement of neutral-current neutral pion (NC$\pi^0$) production in neutrino-argon scattering, as well as single-differential measurements of the same channel in terms of final states…

High Energy Physics - Experiment · Physics 2025-04-29 MicroBooNE collaboration , P. Abratenko , O. Alterkait , D. Andrade Aldana , L. Arellano , J. Asaadi , A. Ashkenazi , S. Balasubramanian , B. Baller , A. Barnard , G. Barr , D. Barrow , J. Barrow , V. Basque , J. Bateman , O. Benevides Rodrigues , S. Berkman , A. Bhanderi , A. Bhat , M. Bhattacharya , M. Bishai , A. Blake , B. Bogart , T. Bolton , J. Y. Book , M. B. Brunetti , L. Camilleri , Y. Cao , D. Caratelli , F. Cavanna , G. Cerati , A. Chappell , Y. Chen , J. M. Conrad , M. Convery , L. Cooper-Troendle , J. I. Crespo-Anadon , R. Cross , M. Del Tutto , S. R. Dennis , P. Detje , R. Diurba , Z. Djurcic , R. Dorrill , K. Duffy , S. Dytman , B. Eberly , P. Englezos , A. Ereditato , J. J. Evans , R. Fine , B. T. Fleming , W. Foreman , D. Franco , A. P. Furmanski , F. Gao , D. Garcia-Gamez , S. Gardiner , G. Ge , S. Gollapinni , E. Gramellini , P. Green , H. Greenlee , L. Gu , W. Gu , R. Guenette , P. Guzowski , L. Hagaman , M. Handley , O. Hen , C. Hilgenberg , G. A. Horton-Smith , Z. Imani , B. Irwin , M. S. Ismail , C. James , X. Ji , J. H. Jo , R. A. Johnson , Y. J. Jwa , D. Kalra , N. Kamp , G. Karagiorgi , W. Ketchum , M. Kirby , T. Kobilarcik , I. Kreslo , N. Lane , I. Lepetic , J. -Y. Li , Y. Li , K. Lin , B. R. Littlejohn , H. Liu , W. C. Louis , X. Luo , C. Mariani , D. Marsden , J. Marshall , N. Martinez , D. A. Martinez Caicedo , S. Martynenko , A. Mastbaum , I. Mawby , N. McConkey , V. Meddage , J. Mendez , J. Micallef , K. Miller , K. Mistry , T. Mohayai , A. Mogan , M. Mooney , A. F. Moor , C. D. Moore , L. Mora Lepin , M. M. Moudgalya , S. Mulleria Babu , D. Naples , A. Navrer-Agasson , N. Nayak , M. Nebot-Guinot , J. Nowak , N. Oza , O. Palamara , N. Pallat , V. Paolone , A. Papadopoulou , V. Papavassiliou , H. Parkinson , S. F. Pate , N. Patel , Z. Pavlovic , E. Piasetzky , K. Pletcher , I. Pophale , X. Qian , J. L. Raaf , V. Radeka , A. Rafique , M. Reggiani-Guzzo , L. Ren , L. Rochester , J. Rodriguez Rondon , M. Rosenberg , M. Ross-Lonergan , I. Safa , G. Scanavini , D. W. Schmitz , A. Schukraft , W. Seligman , M. H. Shaevitz , R. Sharankova , J. Shi , E. L. Snider , M. Soderberg , S. Soldner-Rembold , J. Spitz , M. Stancari , J. St. John , T. Strauss , A. M. Szelc , W. Tang , N. Taniuchi , K. Terao , C. Thorpe , D. Torbunov , D. Totani , M. Toups , A. Trettin , Y. -T. Tsai , J. Tyler , M. A. Uchida , T. Usher , B. Viren , J. Wang , M. Weber , H. Wei , A. J. White , S. Wolbers , T. Wongjirad , M. Wospakrik , K. Wresilo , W. Wu , E. Yandel , T. Yang , L. E. Yates , H. W. Yu , G. P. Zeller , J. Zennamo , C. Zhang

This article presents a study of single $\pi^+$ production in neutrino neutral-current interactions (NC1$\pi^+$) using the FGD1 hydrocarbon target of the ND280 detector of the T2K experiment. We report the largest sample of such events…

High Energy Physics - Experiment · Physics 2025-07-02 K. Abe , S. Abe , R. Akutsu , H. Alarakia-Charles , Y. I. Alj Hakim , S. Alonso Monsalve , L. Anthony , S. Aoki , K. A. Apte , T. Arai , T. Arihara , S. Arimoto , Y. Ashida , E. T. Atkin , N. Babu , V. Baranov , G. J. Barker , G. Barr , D. Barrow , P. Bates , L. Bathe-Peters , M. Batkiewicz-Kwasniak , N. Baudis , V. Berardi , L. Berns , S. Bhattacharjee , A. Blanchet , A. Blondel , S. Bolognesi , S. Bordoni , S. B. Boyd , C. Bronner , A. Bubak , M. Buizza Avanzini , J. A. Caballero , F. Cadoux , N. F. Calabria , S. Cao , S. Cap , D. Carabadjac , S. L. Cartwright , M. P. Casado , M. G. Catanesi , J. Chakrani , A. Chalumeau , A. Chvirova , G. Collazuol , F. Cormier , A. A. L. Craplet , A. Cudd , D. D'ago , C. Dalmazzone , T. Daret , P. Dasgupta , C. Davis , Yu. I. Davydov , G. De Rosa , T. Dealtry , C. Densham , A. Dergacheva , R. Dharmapal Banerjee , F. Di Lodovico , G. Diaz Lopez , S. Dolan , D. Douqa , T. A. Doyle , O. Drapier , K. E. Duffy , J. Dumarchez , P. Dunne , K. Dygnarowicz , A. Eguchi , J. Elias , S. Emery-Schrenk , G. Erofeev , A. Ershova , G. Eurin , D. Fedorova , S. Fedotov , M. Feltre , L. Feng , D. Ferlewicz , A. J. Finch , M. D. Fitton , C. Forza , M. Friend , Y. Fujii , Y. Fukuda , Y. Furui , J. García-Marcos , A. C. Germer , L. Giannessi , C. Giganti , V. Glagolev , M. Gonin , R. González Jiménez , J. González Rosa , E. A. G. Goodman , K. Gorshanov , P. Govindaraj , M. Grassi , M. Guigue , F. Y. Guo , D. R. Hadley , S. Han , D. A. Harris , R. J. Harris , T. Hasegawa , C. M. Hasnip , S. Hassani , N. C. Hastings , Y. Hayato , I. Heitkamp , D. Henaff , Y. Hino , J. Holeczek , A. Holin , T. Holvey , N. T. Hong Van , T. Honjo , M. C. F. Hooft , K. Hosokawa , J. Hu , A. K. Ichikawa , K. Ieki , M. Ikeda , T. Ishida , M. Ishitsuka , A. Izmaylov , N. Jachowicz , S. J. Jenkins , C. Jesús-Valls , M. Jia , J. J. Jiang , J. Y. Ji , T. P. Jones , P. Jonsson , S. Joshi , M. Kabirnezhad , A. C. Kaboth , H. Kakuno , J. Kameda , S. Karpova , V. S. Kasturi , Y. Kataoka , T. Katori , Y. Kawamura , M. Kawaue , E. Kearns , M. Khabibullin , A. Khotjantsev , T. Kikawa , S. King , V. Kiseeva , J. Kisiel , A. Klustová , L. Kneale , H. Kobayashi , L. Koch , S. Kodama , M. Kolupanova , A. Konaka , L. L. Kormos , Y. Koshio , K. Kowalik , Y. Kudenko , Y. Kudo , A. Kumar Jha , R. Kurjata , V. Kurochka , T. Kutter , L. Labarga , M. Lachat , K. Lachner , J. Lagoda , S. M. Lakshmi , M. Lamers James , A. Langella , D. H. Langridge , J. -F. Laporte , D. Last , N. Latham , M. Laveder , M. Lawe , D. Leon Silverio , S. Levorato , S. V. Lewis , B. Li , C. Lin , R. P. Litchfield , S. L. Liu , W. Li , A. Longhin , A. Lopez Moreno , L. Ludovici , X. Lu , T. Lux , L. N. Machado , L. Magaletti , K. Mahn , K. K. Mahtani , M. Mandal , S. Manly , A. D. Marino , D. G. R. Martin , D. A. Martinez Caicedo , L. Martinez , M. Martini , T. Matsubara , R. Matsumoto , V. Matveev , C. Mauger , K. Mavrokoridis , N. McCauley , K. S. McFarland , J. McKean , A. Mefodiev , G. D. Megias , L. Mellet , M. Mezzetto , S. Miki , V. Mikola , E. W. Miller , A. Minamino , O. Mineev , S. Mine , J. Mirabito , M. Miura , S. Moriyama , S. Moriyama , P. Morrison , Th. A. Mueller , D. Munford , A. Muñoz , L. Munteanu , Y. Nagai , T. Nakadaira , K. Nakagiri , M. Nakahata , Y. Nakajima , K. D. Nakamura , Y. Nakano , S. Nakayama , T. Nakaya , K. Nakayoshi , C. E. R. Naseby , D. T. Nguyen , V. Q. Nguyen , K. Niewczas , S. Nishimori , Y. Nishimura , Y. Noguchi , T. Nosek , F. Nova , J. C. Nugent , H. M. O'Keeffe , L. O'Sullivan , R. Okazaki , W. Okinaga , K. Okumura , T. Okusawa , N. Onda , N. Ospina , L. Osu , Y. Oyama , V. Paolone , J. Pasternak , M. Pfaff , L. Pickering , B. Popov , A. J. Portocarrero Yrey , M. Posiadala-Zezula , Y. S. Prabhu , H. Prasad , F. Pupilli , B. Quilain , P. T. Quyen , E. Radicioni , B. Radics , M. A. Ramirez , R. Ramsden , P. N. Ratoff , M. Reh , G. Reina , C. Riccio , D. W. Riley , E. Rondio , S. Roth , N. Roy , A. Rubbia , L. Russo , A. Rychter , W. Saenz , K. Sakashita , F. Sánchez , E. M. Sandford , Y. Sato , T. Schefke , C. M. Schloesser , K. Scholberg , M. Scott , Y. Seiya , T. Sekiguchi , H. Sekiya , T. Sekiya , D. Seppala , D. Sgalaberna , A. Shaikhiev , M. Shiozawa , Y. Shiraishi , A. Shvartsman , N. Skrobova , K. Skwarczynski , D. Smyczek , M. Smy , J. T. Sobczyk , H. Sobel , F. J. P. Soler , A. J. Speers , R. Spina , A. Srivastava , P. Stowell , Y. Stroke , I. A. Suslov , A. Suzuki , S. Y. Suzuki , M. Tada , S. Tairafune , A. Takeda , Y. Takeuchi , H. K. Tanaka , H. Tanigawa , V. V. Tereshchenko , N. Thamm , N. Tran , T. Tsukamoto , M. Tzanov , Y. Uchida , M. Vagins , M. Varghese , I. Vasilyev , G. Vasseur , E. Villa , U. Virginet , T. Vladisavljevic , T. Wachala , D. Wakabayashi , H. T. Wallace , J. G. Walsh , L. Wan , D. Wark , M. O. Wascko , A. Weber , R. Wendell , M. J. Wilking , C. Wilkinson , J. R. Wilson , K. Wood , C. Wret , J. Xia , K. Yamamoto , T. Yamamoto , Y. Yang , T. Yano , N. Yershov , U. Yevarouskaya , M. Yokoyama , Y. Yoshimoto , N. Yoshimura , R. Zaki , A. Zalewska , J. Zalipska , G. Zarnecki , J. Zhang , X. Y. Zhao , H. Zheng , H. Zhong , T. Zhu , M. Ziembicki , E. D. Zimmerman , M. Zito , S. Zsoldos

We use lattice formulation of $\phi^4$ theory in order to investigate non--perturbative features of its continuum limit in two dimensions. In particular, by means of Monte Carlo calculations, we obtain the critical coupling constant…

High Energy Physics - Lattice · Physics 2015-08-26 Paolo Bosetti , Barbara De Palma , Marco Guagnelli

We determine elastic and coupled-channel amplitudes for isospin-1 meson-meson scattering in $P$-wave, by calculating correlation functions using lattice QCD with light quark masses such that $m_\pi = 236$ MeV in a cubic volume of $\sim (4…

High Energy Physics - Phenomenology · Physics 2015-11-11 David J. Wilson , Raul A. Briceno , Jozef J. Dudek , Robert G. Edwards , Christopher E. Thomas

We estimate strong coupling constant between the negative parity nucleons with $\pi$ meson within the light cone QCD sum rules. A method for eliminating the unwanted contributions coming from the nucleon--nucleon and nucleon--negative…

High Energy Physics - Phenomenology · Physics 2017-04-05 T. M. Aliev , T. Barakat , M. Savcı

Motivated by the recent measurement of proton-proton spin-correlation parameters up to 2.5 GeV laboratory energy, we investigate models for nucleon-nucleon (NN) scattering above 1 GeV. Signatures for a gradual failure of the traditional…

Nuclear Theory · Physics 2009-11-10 K. O. Eyser , R. Machleidt , W. Scobel , the EDDA Collaboration

The neutron capture cross section on $^{26}$Mg was measured in the astrophysically relevant energy region from 25 keV to 220 keV. The experimental results agree well with a calculation using the Direct Capture (DC) model together with…

Nuclear Experiment · Physics 2007-05-23 P. Mohr , H. Oberhummer , H. Beer
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