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The energy spectrum of the extended attractive potential of a crystallographic row for negatively charged particles has quasi-bound states. It follows that a negatively charged particle with small transversal momentum component ($p_{\bot} R…

Mesoscale and Nanoscale Physics · Physics 2015-01-12 Gennady V. Kovalev

The masses of the low lying charmonium states, namely, the $J/\Psi$, $\Psi(3686)$, and $\Psi(3770)$ are shifted downwards due to the second order Stark effect. In $\bar p + \text{Au}$ collisions at $6-10$ GeV we study their in\,-\,medium…

High Energy Physics - Phenomenology · Physics 2018-02-28 Gy. Wolf , G. Balassa , P. Kovács , M. Zétényi , S. H. Lee

The charm quark density-density correlation is calculated for $1S$ and $1P$ conventional charmonia and $J^{PC}=1^{-+},0^{+-}$ charmoniumlike states from lattice QCD and are interpreted as spatial wave functions of these states with some…

High Energy Physics - Phenomenology · Physics 2025-08-05 Qingyang Liu , Xiangyu Jiang , Ying Chen , Chunjiang Shi , Wei Sun

We calculate the Equation of State of a quark system interacting through a phenomenological potential: the Richardson's potential, at finite baryon density and zero temperature. In particular we study three different cases with different…

High Energy Physics - Phenomenology · Physics 2009-11-10 S. Terranova , A. Bonasera

We measure the cross section of $e^+e^-\rightarrow\eta_c J/\psi$ at the $\Upsilon(nS) (n=1$ -- $5)$ on-resonance and 10.52 GeV off-resonance energy points using the full data sample collected by the Belle detector with an integrated…

High Energy Physics - Experiment · Physics 2023-08-08 Belle Collaboration , J. H. Yin , Y. B. Li , E. Won , I. Adachi , H. Aihara , S. Al Said , D. M. Asner , T. Aushev , R. Ayad , V. Babu , Sw. Banerjee , P. Behera , K. Belous , J. Bennett , M. Bessner , T. Bilka , D. Biswas , D. Bodrov , G. Bonvicini , J. Borah , A. Bozek , M. Bračko , P. Branchini , T. E. Browder , A. Budano , D. Červenkov , M. -C. Chang , B. G. Cheon , K. Chilikin , H. E. Cho , K. Cho , S. -K. Choi , Y. Choi , S. Choudhury , D. Cinabro , J. Cochran , S. Das , G. De Nardo , G. De Pietro , R. Dhamija , F. Di Capua , J. Dingfelder , Z. Doležal , T. V. Dong , D. Epifanov , T. Ferber , D. Ferlewicz , B. G. Fulsom , V. Gaur , A. Giri , P. Goldenzweig , E. Graziani , T. Gu , Y. Guan , K. Gudkova , C. Hadjivasiliou , S. Halder , T. Hara , K. Hayasaka , H. Hayashii , D. Herrmann , W. -S. Hou , C. -L. Hsu , T. Iijima , N. Ipsita , A. Ishikawa , R. Itoh , M. Iwasaki , W. W. Jacobs , Q. P. Ji , S. Jia , Y. Jin , K. K. Joo , J. Kahn , A. B. Kaliyar , T. Kawasaki , C. Kiesling , C. H. Kim , D. Y. Kim , K. -H. Kim , Y. -K. Kim , H. Kindo , K. Kinoshita , P. Kodyš , A. Korobov , S. Korpar , E. Kovalenko , P. Križan , P. Krokovny , T. Kuhr , M. Kumar , R. Kumar , K. Kumara , T. Lam , J. S. Lange , S. C. Lee , L. K. Li , Y. Li , J. Libby , K. Lieret , Y. -R. Lin , D. Liventsev , M. Masuda , T. Matsuda , D. Matvienko , S. K. Maurya , F. Meier , M. Merola , F. Metzner , R. Mizuk , G. B. Mohanty , R. Mussa , I. Nakamura , D. Narwal , Z. Natkaniec , A. Natochii , L. Nayak , M. Nayak , N. K. Nisar , S. Nishida , S. Ogawa , H. Ono , P. Oskin , G. Pakhlova , S. Pardi , H. Park , J. Park , S. -H. Park , A. Passeri , S. Patra , S. Paul , R. Pestotnik , L. E. Piilonen , T. Podobnik , E. Prencipe , M. T. Prim , N. Rout , G. Russo , S. Sandilya , A. Sangal , L. Santelj , V. Savinov , G. Schnell , C. Schwanda , Y. Seino , K. Senyo , W. Shan , M. Shapkin , C. Sharma , J. -G. Shiu , E. Solovieva , M. Starič , Z. S. Stottler , M. Sumihama , M. Takizawa , K. Tanida , F. Tenchini , R. Tiwary , M. Uchida , T. Uglov , Y. Unno , S. Uno , Y. Usov , S. E. Vahsen , G. Varner , A. Vinokurova , D. Wang , E. Wang , M. -Z. Wang , X. L. Wang , S. Watanuki , O. Werbycka , X. Xu , B. D. Yabsley , W. Yan , S. B. Yang , J. Yelton , Y. Yook , C. Z. Yuan , Z. P. Zhang , V. Zhilich , V. Zhukova

In this work, we discuss the quantum mechanics on the moduli space consisting of two maximally charged dilaton black holes. We study the quantum effects resulting from the different structure of the moduli space geometry in the scattering…

General Relativity and Quantum Cosmology · Physics 2007-05-23 Kenji Sakamoto , Kiyoshi Shiraishi

Pauli blocking of spontaneous emission is responsible for the stability of atoms. Higher electronic orbitals cannot decay to lower-lying states if they are already occupied -- this is Pauli blocking due to occupation of internal states.…

Quantum Physics · Physics 2021-12-13 Yair Margalit , Yu-Kun Lu , Furkan Cagri Top , Wolfgang Ketterle

The scattering phase shift of an electron transferred through a quantum dot is studied within a model Hamiltonian, accounting for both the electron--electron interaction in the dot and a finite temperature. It is shown that, unlike in an…

Condensed Matter · Physics 2009-10-28 Yuval Oreg , Yuval Gefen

The momentum diffusion effect of the quark pair due to the multiple scattering in a nuclear medium is studied to explain the observed J/psi yields in SPS experiments. The resulting suppression is found to be insufficient to reproduce the…

High Energy Physics - Phenomenology · Physics 2009-11-07 H. Fujii

Lattice QCD studies have shown the attractive character of the $^1S_0$ $\Omega_{QQQ}\Omega_{QQQ}$, $Q=s,c,b$, interaction, predicting deeply bound states as the mass of the heavy quark increases. This has led to the question of the possible…

High Energy Physics - Phenomenology · Physics 2025-02-04 H. Garcilazo , A. Valcarce

A slow J/psi excess exists in the inclusive B -> J/psi+X spectrum, and is indicative of some hadronic effect. From color octet nature of c cbar pair in b-> c cbar s decay, one such possibility would be B -> J/psi+ K_g decay, where K_g is a…

High Energy Physics - Phenomenology · Physics 2009-11-10 Chun-Khiang Chua , Wei-Shu Hou , Gwo-Guang Wong

The $J/\psi$ and $\psi(2S)$ charmonium states, composed of $c\bar{c}$ quark pairs and known since the 1970s, are widely believed to serve as ideal probes to test quantum chromodynamics in high-energy hadronic interactions. However, there is…

High Energy Physics - Experiment · Physics 2024-09-06 PHENIX Collaboration , N. J. Abdulameer , U. Acharya , C. Aidala , Y. Akiba , M. Alfred , V. Andrieux , S. Antsupov , N. Apadula , H. Asano , B. Azmoun , V. Babintsev , N. S. Bandara , E. Bannikov , K. N. Barish , S. Bathe , A. Bazilevsky , M. Beaumier , R. Belmont , A. Berdnikov , Y. Berdnikov , L. Bichon , B. Blankenship , D. S. Blau , J. S. Bok , V. Borisov , M. L. Brooks , J. Bryslawskyj , V. Bumazhnov , S. Campbell , R. Cervantes , D. Chen , M. Chiu , C. Y. Chi , I. J. Choi , J. B. Choi , Z. Citron , M. Connors , R. Corliss , N. Cronin , M. Csanád , T. Csörgő , T. W. Danley , M. S. Daugherity , G. David , K. DeBlasio , K. Dehmelt , A. Denisov , A. Deshpande , E. J. Desmond , A. Dion , D. Dixit , V. Doomra , J. H. Do , A. Drees , K. A. Drees , J. M. Durham , A. Durum , H. En'yo , A. Enokizono , R. Esha , B. Fadem , W. Fan , N. Feege , D. E. Fields , M. Finger, , M. Finger , D. Firak , D. Fitzgerald , S. L. Fokin , J. E. Frantz , A. Franz , A. D. Frawley , Y. Fukuda , P. Gallus , C. Gal , P. Garg , H. Ge , F. Giordano , Y. Goto , N. Grau , S. V. Greene , M. Grosse Perdekamp , T. Gunji , T. Guo , H. Guragain , T. Hachiya , J. S. Haggerty , K. I. Hahn , H. Hamagaki , H. F. Hamilton , J. Hanks , S. Y. Han , S. Hasegawa , T. O. S. Haseler , T. K. Hemmick , X. He , J. C. Hill , K. Hill , A. Hodges , R. S. Hollis , K. Homma , B. Hong , T. Hoshino , N. Hotvedt , J. Huang , K. Imai , M. Inaba , A. Iordanova , D. Isenhower , D. Ivanishchev , B. Jacak , M. Jezghani , X. Jiang , Z. Ji , B. M. Johnson , D. Jouan , D. S. Jumper , J. H. Kang , D. Kapukchyan , S. Karthas , D. Kawall , A. V. Kazantsev , V. Khachatryan , A. Khanzadeev , C. Kim , E. -J. Kim , M. Kim , D. Kincses , E. Kistenev , J. Klatsky , P. Kline , T. Koblesky , D. Kotov , L. Kovacs , S. Kudo , K. Kurita , Y. Kwon , J. G. Lajoie , A. Lebedev , S. Lee , M. J. Leitch , Y. H. Leung , S. H. Lim , M. X. Liu , X. Li , V. -R. Loggins , S. Lökös , D. A. Loomis , K. Lovasz , D. Lynch , T. Majoros , Y. I. Makdisi , M. Makek , V. I. Manko , E. Mannel , M. McCumber , P. L. McGaughey , D. McGlinchey , C. McKinney , M. Mendoza , A. C. Mignerey , A. Milov , D. K. Mishra , J. T. Mitchell , M. Mitrankova , Iu. Mitrankov , G. Mitsuka , S. Miyasaka , S. Mizuno , P. Montuenga , T. Moon , D. P. Morrison , B. Mulilo , T. Murakami , J. Murata , K. Nagai , K. Nagashima , T. Nagashima , J. L. Nagle , M. I. Nagy , I. Nakagawa , K. Nakano , C. Nattrass , T. Niida , R. Nouicer , N. Novitzky , T. Novák , G. Nukazuka , A. S. Nyanin , E. O'Brien , C. A. Ogilvie , J. D. Orjuela Koop , M. Orosz , J. D. Osborn , A. Oskarsson , G. J. Ottino , K. Ozawa , V. Pantuev , V. Papavassiliou , J. S. Park , S. Park , M. Patel , S. F. Pate , D. V. Perepelitsa , G. D. N. Perera , D. Yu. Peressounko , C. E. PerezLara , J. Perry , R. Petti , M. Phipps , C. Pinkenburg , R. P. Pisani , M. Potekhin , M. L. Purschke , K. F. Read , D. Reynolds , V. Riabov , Y. Riabov , D. Richford , T. Rinn , S. D. Rolnick , M. Rosati , Z. Rowan , A. S. Safonov , T. Sakaguchi , H. Sako , V. Samsonov , M. Sarsour , S. Sato , B. Schaefer , B. K. Schmoll , K. Sedgwick , R. Seidl , A. Seleznev , A. Sen , R. Seto , A. Sexton , D. Sharma , I. Shein , T. -A. Shibata , K. Shigaki , M. Shimomura , T. Shioya , P. Shukla , A. Sickles , C. L. Silva , D. Silvermyr , B. K. Singh , C. P. Singh , V. Singh , M. Slunečka , K. L. Smith , M. Snowball , R. A. Soltz , W. E. Sondheim , S. P. Sorensen , I. V. Sourikova , P. W. Stankus , S. P. Stoll , T. Sugitate , A. Sukhanov , T. Sumita , J. Sun , Z. Sun , J. Sziklai , K. Tanida , M. J. Tannenbaum , S. Tarafdar , G. Tarnai , R. Tieulent , A. Timilsina , T. Todoroki , M. Tomášek , C. L. Towell , R. S. Towell , I. Tserruya , Y. Ueda , B. Ujvari , H. W. van Hecke , J. Velkovska , M. Virius , V. Vrba , N. Vukman , X. R. Wang , Y. S. Watanabe , C. L. Woody , L. Xue , C. Xu , Q. Xu , S. Yalcin , Y. L. Yamaguchi , H. Yamamoto , A. Yanovich , I. Yoon , J. H. Yoo , I. E. Yushmanov , H. Yu , W. A. Zajc , A. Zelenski , L. Zou

Quantum field-theory is developed for treating electrons and holes in planar systems. Non-unitary representations of Dirac equation in the plane are developed. These equations can be used for treating holes-electron pairing in high TC…

Superconductivity · Physics 2013-09-26 Y. Ben-Aryeh

We propose a new basis state, which satisfies the Pauli principle in the nuclear cluster model. The basis state is defined as the generalized coherent state of the harmonic oscillator wave function using a pair of the creation operators and…

Nuclear Theory · Physics 2024-01-29 Takayuki Myo , Kiyoshi Kato

We make a systematic investigation on the two-body nonleptonic decays $B_c\rightarrow J/\Psi(\eta_c),M$ by employing the perturbative QCD approach based on $k_T$ factorization, where $M$ is a light pseudoscalar or vector or a heavy charmed…

High Energy Physics - Phenomenology · Physics 2015-01-06 Zhou Rui , Zhi-Tian Zou

The statistical properties of Charmonium energy spectrum determined by the Bethe-Salpeter equation are investigated. It is found that the regular motion of the $c\bar{c}$ system can be expected at a small value of color screening mass but…

Nuclear Theory · Physics 2009-10-31 Jianzhong Gu , Hongshi Zong , Yuxin Liu , Enguang Zhao

Recent breakthroughs in the transport spectroscopy of 2-D material quantum-dot platforms have engendered a fervent interest in spin-valley qubits. In this context, Pauli blockades in double quantum dot structures form an important basis for…

Mesoscale and Nanoscale Physics · Physics 2023-08-10 Anuranan Das , Adil Khan , Ankan Mukherjee , Bhaskaran Muralidharan

An interesting controversy has emerged challenging the widely accepted nature of the $X(3915)$ and the $X(3930)$ resonances, which had initially been assigned to the $\chi_{c0}(2P)$ and $\chi_{c2}(2P)$ $c\bar c$ states, respectively. To…

High Energy Physics - Phenomenology · Physics 2018-02-01 Pablo G. Ortega , Jorge Segovia , David R. Entem , Francisco Fernández

We analyze the behavior of a non-Hermitian opened one-dimensional quantum system with $\mathcal{PT}$ symmetry. This system is built by a dimer, with balanced gains and losses described by a parameter $\gamma$. By varying $\gamma$ the system…

Quantum Physics · Physics 2024-04-11 J. Colín-Gálvez , E. Castaño , G. Báez , V. Domínguez-Rocha

We study $\eta_{\rm c}$- and $J/\psi$-isoscalar meson bound states in the hadro-charmonium picture. In the hadro-charmonium, the four $q\bar q c \bar c$ quarks are arranged in terms of a compact charm-anticharm pair, $c \bar c$, embedded in…

High Energy Physics - Phenomenology · Physics 2018-06-26 J. Ferretti