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We investigate mesons in the bosonized massive Schwinger model in the light-front Tamm-Dancoff approximation in the strong coupling region. We confirm that the three-meson bound state has a few percent fermion six-body component in the…

High Energy Physics - Theory · Physics 2009-10-28 koji Harada , Atsushi Okazaki , Masa-aki Taniguchi

We calculate numerically scattering phases for elastic meson-meson scattering processes in the strongly coupled massive Schwinger-model with an SU(2) flavour symmetry. These calculations are based on Luescher's method in which finite size…

High Energy Physics - Lattice · Physics 2009-10-31 C. Gutsfeld , H. A. Kastrup , K. Stergios

It was found that the most simple analysis in the linear \sigma- model, where the sigma meson couples in vacuum to two virtual pions, predicted the most typical values for the \sigma-mass and total decay width as 486+/-7MeV and 340+/-20MeV…

Nuclear Theory · Physics 2010-03-19 M. C. Menchaca Maciel , J. R. Morones Ibarra

The spectrum and dominant strong decay properties of the doubly heavy baryons are revisited by using a chiral effective model with chiral partner structure. By regarding the doubly heavy baryons in the ground states and light angular…

High Energy Physics - Phenomenology · Physics 2015-07-29 Yong-Liang Ma , Masayasu Harada

In strongly interacting massive particle (SIMP) scenarios, dark matter is comprised of stable dark pions whose $3\to 2$ or $4\to 2$ reactions set the dark matter relic abundance. Recent work has shown that shallow two-pion bound states…

High Energy Physics - Phenomenology · Physics 2025-12-10 Xiaoyong Chu , Josef Pradler , Daris Samart

We study the Schwinger model with $N_{\rm f} \geq 2$ degenerate fermion flavors, by means of lattice simulations. We use dynamical Wilson fermions for $N_{\rm f} = 2$, and re-weighted quenched configurations for overlap-hypercube fermions…

High Energy Physics - Lattice · Physics 2023-10-16 Jaime Fabián Nieto Castellanos , Ivan Hip , Wolfgang Bietenholz

We explore some aspects of $Sp(4)$ gauge theory with two fundamental fermions in the context of composite Goldstone Dark Matter. We present preliminary lattice results for the mass of the pseudoscalar iso-singlet meson $\eta'$ using…

High Energy Physics - Lattice · Physics 2022-10-21 Fabian Zierler , Jong-Wan Lee , Axel Maas , Felix Pressler

We study the most general scalar potential of the Georgi-Machacek model, which adds isospin-triplet scalars to the Standard Model (SM) in a way that preserves custodial SU(2) symmetry. We show that this model possesses a decoupling limit,…

High Energy Physics - Phenomenology · Physics 2014-07-16 Katy Hartling , Kunal Kumar , Heather E. Logan

An antiferromagnetic S=1/2 Heisenberg chain is mapped to the two-flavor massless Schwinger model at \theta=\pi. The electromagnetic coupling constant and velocity of light in the Schwinger model are determined in terms of the Heisenberg…

High Energy Physics - Theory · Physics 2009-10-31 Yutaka Hosotani

The fermion mass spectrum is studied in the quenched approximation in the strong coupling vortex phase (VXS) of a globally U(1)$_L \otimes$U(1)$_R$ symmetric scalar-fermion model in two dimensions. In this phase fermion doublers can be…

High Energy Physics - Lattice · Physics 2009-10-22 Wolfgang Bock , Asit K. De , Erich Focht , Jan Smit

We propose to construct a chirally broken model based on the infrared fixed point of a conformal system by raising the mass of some flavors while keeping the others massless. In the infrared limit the massive fermions decouple and the…

High Energy Physics - Phenomenology · Physics 2016-04-29 R. C. Brower , A. Hasenfratz , C. Rebbi , E. Weinberg , O. Witzel

We present new results from our ongoing study of the SU(3) sextet model with two flavors in the two-index symmetric representation of the gauge group. In the simulations use unimproved Wilson fermions to investigate the infrared properties…

High Energy Physics - Lattice · Physics 2017-09-13 Martin Hansen , Claudio Pica

We suggest a dark matter scenario which could contribute the possible anomaly observed by Fermi-LAT $\gamma$-ray space telescope. It is based on the model recently proposed by Weinberg. In our scenario the gamma-ray line signal comes from…

High Energy Physics - Phenomenology · Physics 2015-06-17 Seungwon Baek , Hiroshi Okada

The weak decay of the kaon to two pions is studied within the NJL Model. Using the standard effective weak Hamiltonian, both the decay amplitude arising from an intermediate state \sigma-meson and the direct decay amplitude are calculated.…

High Energy Physics - Phenomenology · Physics 2015-02-02 Zhan-Wei Liu , Manuel E. Carrillo-Serrano , Anthony W. Thomas

I review the recent proposal that there are new isotriplet heavy baryons with masses approximately 2380 MeV and 5760 MeV. This prediction follows from the application of heavy spin-flavor and light $SU(3)$ symmetries to the observed charmed…

High Energy Physics - Phenomenology · Physics 2011-04-15 Adam F. Falk

We investigate the continuum spectrum of the SU(2) gauge theory with $N_f=2$ flavours of fermions in the fundamental representation. This model provides a minimal template which is ideal for a wide class of Standard Model extensions…

High Energy Physics - Lattice · Physics 2016-12-07 Rudy Arthur , Vincent Drach , Martin Hansen , Ari Hietanen , Claudio Pica , Francesco Sannino

We present the method and compute the strong couplings of the lowest and first orbitally excited heavy-light mesons to a soft pion in the static heavy quark limit on the lattice. Besides the usual g^ and \~g couplings, we were able to make…

High Energy Physics - Lattice · Physics 2012-03-02 Damir Becirevic , Emmanuel Chang , Alain Le Yaouanc

Dark photons are hypothetical massive vector particles that could mix with ordinary photons. The simplest theoretical model is fully characterised by only two parameters: the mass of the dark photon m$_{\gamma^{\mathrm{D}}}$ and its mixing…

High Energy Physics - Experiment · Physics 2023-01-11 SHiP Collaboration , C. Ahdida , A. Akmete , R. Albanese , A. Alexandrov , A. Anokhina , S. Aoki , G. Arduini , E. Atkin , N. Azorskiy , J. J. Back , A. Bagulya , F. Baaltasar Dos Santos , A. Baranov , F. Bardou , G. J. Barker , M. Battistin , J. Bauche , A. Bay , V. Bayliss , G. Bencivenni , A. Y. Berdnikov , Y. A. Berdnikov , M. Bertani , C. Betancourt , I. Bezshyiko , O. Bezshyyko , D. Bick , S. Bieschke , A. Blanco , J. Boehm , M. Bogomilov , I. Boiarska , K. Bondarenko , W. M. Bonivento , J. Borburgh , A. Boyarsky , R. Brenner , D. Breton , V. Büscher , A. Buonaura , S. Buontempo , S. Cadeddu , A. Calcaterra , M. Calviani , M. Campanelli , M. Casolino , N. Charitonidis , P. Chau , J. Chauveau , A. Chepurnov , M. Chernyavskiy , K. -Y. Choi , A. Chumakov , P. Ciambrone , V. Cicero , L. Congedo , K. Cornelis , M. Cristinziani , A. Crupano , G. M. Dallavalle , A. Datwyler , N. D'Ambrosio , G. D'Appollonio , R. de Asmundis , J. De Carvalho Saraiva , G. De Lellis , M. de Magistris , A. De Roeck , M. De Serio , D. De Simone , L. Dedenko , P. Dergachev , A. Di Crescenzo , L. Di Giulio , N. Di Marco , C. Dib , H. Dijkstra , V. Dmitrenko , L. A. Dougherty , A. Dolmatov , D. Domenici , S. Donskov , V. Drohan , A. Dubreuil , O. Durhan , M. Ehlert , E. Elikkaya , T. Enik , A. Etenko , F. Fabbri , O. Fedin , F. Fedotovs , G. Felici , M. Ferrillo , M. Ferro-Luzzi , K. Filippov , R. A. Fini , P. Fonte , C. Franco , M. Fraser , R. Fresa , R. Froeschl , T. Fukuda , G. Galati , J. Gall , L. Gatignon , G. Gavrilov , V. Gentile , B. Goddard , L. Golinka-Bezshyyko , A. Golovatiuk , V. Golovtsov , D. Golubkov , A. Golutvin , P. Gorbounov , D. Gorbunov , S. Gorbunov , V. Gorkavenko , M. Gorshenkov , V. Grachev , A. L. Grandchamp , E. Graverini , J. -L. Grenard , D. Grenier , V. Grichine , N. Gruzinskii , A. M. Guler , Yu. Guz , G. J. Haefeli , C. Hagner , H. Hakobyan , I. W. Harris , E. van Herwijnen , C. Hessler , A. Hollnagel , B. Hosseini , M. Hushchyn , G. Iaselli , A. Iuliano , R. Jacobsson , D. Joković , M. Jonker , I. Kadenko , V. Kain , B. Kaiser , C. Kamiscioglu , D. Karpenkov , K. Kershaw , M. Khabibullin , E. Khalikov , G. Khaustov , G. Khoriauli , A. Khotyantsev , Y. G. Kim , V. Kim , N. Kitagawa , J. -W. Ko , K. Kodama , A. Kolesnikov , D. I. Kolev , V. Kolosov , M. Komatsu , A. Kono , N. Konovalova , S. Kormannshaus , I. Korol , I. Korol'ko , A. Korzenev , V. Kostyukhin , E. Koukovini Platia , S. Kovalenko , I. Krasilnikova , Y. Kudenko , E. Kurbatov , P. Kurbatov , V. Kurochka , E. Kuznetsova , H. M. Lacker , M. Lamont , G. Lanfranchi , O. Lantwin , A. Lauria , K. S. Lee , K. Y. Lee , J. -M. Lévy , V. P. Loschiavo , L. Lopes , E. Lopez Sola , V. Lyubovitskij , J. Maalmi , A. -M. Magnan , V. Maleev , A. Malinin , Y. Manabe , A. K. Managadze , M. Manfredi , S. Marsh , A. M. Marshall , A. Mefodev , P. Mermod , A. Miano , S. Mikado , Yu. Mikhaylov , D. A. Milstead , O. Mineev , A. Montanari , M. C. Montesi , K. Morishima , S. Movchan , Y. Muttoni , N. Naganawa , M. Nakamura , T. Nakano , S. Nasybulin , P. Ninin , A. Nishio , A. Novikov , B. Obinyakov , S. Ogawa , N. Okateva , B. Opitz , J. Osborne , M. Ovchynnikov , N. Owtscharenko , P. H. Owen , P. Pacholek , A. Paoloni , B. D. Park , A. Pastore , M. Patel , D. Pereyma , A. Perillo-Marcone , G. L. Petkov , K. Petridis , A. Petrov , D. Podgrudkov , V. Poliakov , N. Polukhina , J. Prieto Prieto , M. Prokudin , A. Prota , A. Quercia , A. Rademakers , A. Rakai , F. Ratnikov , T. Rawlings , F. Redi , S. Ricciardi , M. Rinaldesi , Volodymyr Rodin , Viktor Rodin , P. Robbe , A. B. Rodrigues Cavalcante , T. Roganova , H. Rokujo , G. Rosa , T. Rovelli , O. Ruchayskiy , T. Ruf , V. Samoylenko , V. Samsonov , F. Sanchez Galan , P. Santos Diaz , A. Sanz Ull , A. Saputi , O. Sato , E. S. Savchenko , J. S. Schliwinski , W. Schmidt-Parzefall , N. Serra , S. Sgobba , O. Shadura , A. Shakin , M. Shaposhnikov , P. Shatalov , T. Shchedrina , L. Shchutska , V. Shevchenko , H. Shibuya , S. Shirobokov , A. Shustov , S. B. Silverstein , S. Simone , R. Simoniello , M. Skorokhvatov , S. Smirnov , J. Y. Sohn , A. Sokolenko , E. Solodko , N. Starkov , L. Stoel , M. E. Stramaglia , D. Sukhonos , Y. Suzuki , S. Takahashi , J. L. Tastet , P. Teterin , S. Than Naing , I. Timiryasov , V. Tioukov , D. Tommasini , M. Torii , N. Tosi , D. Treille , R. Tsenov , S. Ulin , E. Ursov , A. Ustyuzhanin , Z. Uteshev , L. Uvarov , G. Vankova-Kirilova , F. Vannucci , V. Venturi , S. Vilchinski , Heinz Vincke , Helmut Vincke , C. Visone , K. Vlasik , A. Volkov , R. Voronkov , S. van Waasen , R. Wanke , P. Wertelaers , O. Williams , J. -K. Woo , M. Wurm , S. Xella , D. Yilmaz , A. U. Yilmazer , C. S. Yoon , Yu. Zaytsev , A. Zelenov , J. Zimmerman

Within the framework of the quantum molecular dynamics transport model, the pion production and constraint of the high-density symmetry energy in heavy-ion collisions near threshold energy have been thoroughly investigated. The energy…

Nuclear Theory · Physics 2024-06-10 Heng-Jin Liu , Ban Zhang , Yuan-Qing Guo , Hui-Gan Cheng , Si-Na Wei , Zhao-Qing Feng

We use the idea of partial compositeness in a minimal supersymmetric model to relate the fermion and sfermion masses. By assuming that the Higgs and third-generation matter is (mostly) elementary, while the first- and second-generation…

High Energy Physics - Phenomenology · Physics 2019-03-27 Yusuf Buyukdag , Tony Gherghetta , Andrew S. Miller
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