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Related papers: Four fermion final states in $e^+e^-$ annihilation

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We introduce auxiliary quantum master equation - dual fermion approach (QME-DF) and argue that it presents a convenient way to describe steady-states of correlated impurity systems. The combined scheme yields an expansion around a reference…

Mesoscale and Nanoscale Physics · Physics 2019-05-14 Feng Chen , Guy Cohen , Michael Galperin

The current status of bounds on and limits of fermion determinants in two, three and four dimensions in QED and QCD is reviewed. A new lower bound on the two-dimensional QED determinant is derived. An outline of the demonstration of the…

High Energy Physics - Theory · Physics 2009-11-07 M. P. Fry

We consider the $\pi^+\pi^-\pi_0\gamma$ final state in electron-positron annihilation at cms energies not far from the threshold. Both initial and final state radiations of the hard photon is considered but without interference between…

High Energy Physics - Phenomenology · Physics 2009-11-07 A. Ahmedov , G. V. Fedotovich , E. A. Kuraev , Z. K. Silagadze

The package aITALC has been developed for fully automated calculations of two fermion production at e+ e- collider and other similar reactions. We emphasize the connection and interoperability between the different modules required for the…

High Energy Physics - Phenomenology · Physics 2009-11-11 A. Lorca

In the two papers published recently, we apply collinear expansion to both inclusive ($e^+ e^- \to h+X$) and semi-inclusive ($e^+ e^- \to h + \bar q + X$) hadron production in $e^+ e^-$ annihilation to derive a formalism suitable for a…

High Energy Physics - Phenomenology · Physics 2016-03-23 Shu-yi Wei

This article establishes the existence of a ground state and infinitely many solutions for the modified fourth-order elliptic equation: \[ \begin{aligned} \left\{ \begin{array}{ll} \Delta^2 u - \Delta u + u - \frac{1}{2}u\Delta(u^2) = f(u),…

Analysis of PDEs · Mathematics 2025-08-25 Lifeng Yin , Fan Wang

Because the staggered fermion determinant is complex at nonzero mu, taking its fourth root leads to phase ambiguities. These unphysical effects cause the measure to become discontinuous; the problem becomes acute when Re mu exceeds…

High Energy Physics - Lattice · Physics 2009-09-29 Benjamin Svetitsky , Yigal Shamir , Maarten Golterman

The origin of fractional quantum Hall effect (FQHE) at 4/11 and 5/13 has remained controversial. We make a compelling case that FQHE is possible here for fully spin polarized composite fermions, but with an unconventional underlying…

Mesoscale and Nanoscale Physics · Physics 2014-10-21 Sutirtha Mukherjee , Sudhansu S. Mandal , Ying-Hai Wu , Arkadiusz Wójs , Jainendra K. Jain

The multiple particle final states in modern data from $4 \pi$ detector experiments offer a wealth of information about higher hadronic resonances and hadron interactions. However, it requires careful analysis to extract model independent…

Nuclear Theory · Physics 2017-08-23 Norbert E. Ligterink

A Monte Carlo generator has been constructed to simulate the reaction e^+e^- \to \gamma + 4 \pi, where the photon is assumed to be observed in the detector. Only initial state radiation is considered. Additional collinear photon radiation…

High Energy Physics - Phenomenology · Physics 2009-01-07 H. Czyz , J. H. Kuehn

The phase structure of a four- and eight-fermion interaction model is investigated at finite temperature and chemical potential in arbitrary space-time dimensions, $2\leq D<4$. The effective potential and the gap equation are calculated in…

High Energy Physics - Phenomenology · Physics 2011-03-14 Masako Hayashi , Tomohiro Inagaki , Wataru Sakamoto

We suggest searching for excited charmonium states in $e^+e^-$ annihilation via double charmonium production at $\sqrt{s}=10.6$ GeV with $B$ factories, based on a more complete leading order calculation including both QCD and QED…

High Energy Physics - Phenomenology · Physics 2008-11-26 Kui-Yong Liu , Zhi-Guo He , Kuang-Ta Chao

We report results on studies of the e+e- annihilation into three-body Y(nS)pi+pi- (n=1,2,3) final states including measurements of cross sections and the full amplitude analysis. The cross sections measured at sqrt(s)=10.865 GeV and…

High Energy Physics - Experiment · Physics 2015-04-16 A. Garmash , A. Bondar , A. Kuzmin , A. Abdesselam , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , V. Aulchenko , T. Aushev , R. Ayad , A. M. Bakich , A. Bala , V. Bhardwaj , A. Bobrov , G. Bonvicini , A. Bozek , M. Bracko , T. E. Browder , D. Cervenkov , V. Chekelian , A. Chen , B. G. Cheon , K. Chilikin , R. Chistov , K. Cho , V. Chobanova , Y. Choi , D. Cinabro , J. Dalseno , Z. Dolezal , A. Drutskoy , D. Dutta , S. Eidelman , D. Epifanov , H. Farhat , J. E. Fast , T. Ferber , A. Frey , O. Frost , V. Gaur , S. Ganguly , R. Gillard , R. Glattauer , Y. M. Goh , B. Golob , J. Haba , T. Hara , K. Hayasaka , H. Hayashii , X. H. He , Y. Hoshi , W. -S. Hou , Y. B. Hsiung , H. J. Hyun , T. Iijima , A. Ishikawa , R. Itoh , Y. Iwasaki , T. Iwashita , I. Jaegle , T. Julius , J. H. Kang , E. Kato , P. Katrenko , H. Kawai , T. Kawasaki , H. Kichimi , C. Kiesling , D. Y. Kim , J. B. Kim , J. H. Kim , K. T. Kim , M. J. Kim , Y. J. Kim , K. Kinoshita , J. Klucar , B. R. Ko , P. Kodys , S. Korpar , P. Krizan , P. Krokovny , T. Kuhr , Y. -J. Kwon , S. -H. Lee , Y. Li , L. Li Gioi , J. Libby , C. Liu , Z. Q. Liu , D. Liventsev , P. Lukin , D. Matvienko , K. Miyabayashi , H. Miyata , R. Mizuk , G. B. Mohanty , A. Moll , R. Mussa , E. Nakano , M. Nakao , Z. Natkaniec , M. Nayak , E. Nedelkovska , N. K. Nisar , S. Nishida , O. Nitoh , S. Okuno , W. Ostrowicz , P. Pakhlov , H. Park , H. K. Park , T. K. Pedlar , R. Pestotnik , M. Petric , L. E. Piilonen , E. Ribezl , M. Ritter , M. Rohrken , A. Rostomyan , S. Ryu , T. Saito , Y. Sakai , S. Sandilya , D. Santel , T. Sanuki , Y. Sato , O. Schneider , G. Schnell , A. J. Schwartz , D. Semmler , K. Senyo , M. E. Sevior , M. Shapkin , V. Shebalin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , B. Shwartz , F. Simon , Y. -S. Sohn , A. Sokolov , E. Solovieva , S. Stanic , M. Staric , M. Steder , T. Sumiyoshi , U. Tamponi , K. Tanida , G. Tatishvili , Y. Teramoto , K. Trabelsi , M. Uchida , Y. Unno , S. Uno , P. Urquijo , Y. Usov , C. Van Hulse , P. Vanhoefer , G. Varner , A. Vinokurova , V. Vorobyev , M. N. Wagner , C. H. Wang , P. Wang , X. L. Wang , M. Watanabe , Y. Watanabe , K. M. Williams , E. Won , H. Yamamoto , Y. Yamashita , S. Yashchenko , Y. Yook , C. Z. Yuan , Z. P. Zhang , V. Zhilich , A. Zupanc

The anticommuting properties of fermionic operators, together with the presence of parity conservation, affect the concept of entanglement in a composite fermionic system. Hence different points of view can give rise to different reasonable…

Quantum Physics · Physics 2007-09-05 Mari-Carmen Bañuls , J. Ignacio Cirac , Michael M. Wolf

Worldline representations were established as a powerful tool for studying bosonic lattice field theories at finite density. For fermions, however, the worldlines still may carry signs that originate from the Dirac algebra and from the…

High Energy Physics - Lattice · Physics 2022-11-29 Christof Gattringer

We examine the weakly interacting atoms in an ultracold Fermi gas leading to a state of macroscopic coherence, from a theoretical perspective. It has been shown that this state can be described as a fermionic coherent state. These coherent…

Quantum Physics · Physics 2013-04-05 Arnab Ghosh , Sudarson Sekhar Sinha , Deb Shankar Ray

The final states for the process $b \rightarrow s\ \gamma$ have been extensively discussed in the literature. Similarly-detailed analyses for the case $b \rightarrow s\ gluon$ have not been performed. Generally this process is searched for…

High Energy Physics - Phenomenology · Physics 2016-09-01 J. D. Swain

We consider corrections to bino annihilation due to sfermion mixing.

High Energy Physics - Phenomenology · Physics 2009-09-25 Toby Falk , Richard Madden , Keith A. Olive , Mark Srednicki

We show that the thermal relic abundance of dark matter can be affected by a new type of reaction: semi-annihilation. Semi-annihilation takes the schematic form X_i X_j -> X_k phi, where X_i are stable dark matter particles and phi is an…

High Energy Physics - Phenomenology · Physics 2015-03-13 Francesco D'Eramo , Jesse Thaler

Recent results concerning the relation of topology and low-lying fermion modes are summarized.

High Energy Physics - Lattice · Physics 2014-11-17 Robert G. Edwards