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Related papers: Mass splittings in $\Sigma_b$ and $\Sigma_b^*$

200 papers

The hyperfine splittings $\Delta_D=(m_{D^*_s}-m_{D_s})-(m_{D^{*+}}-m_{D^+})$ and $\Delta_B=(m_{B^*_s}-m_{B_s})-(m_{B^{*0}}-m_{B^0})$ are analyzed in the framework of an effective lagrangian possessing chiral, heavy flavour and spin…

High Energy Physics - Phenomenology · Physics 2009-10-28 N. Di Bartolomeo , F. Feruglio , R. Gatto , G. Nardulli

We analyze the mixing between $\Sigma^0$ and $\Lambda^0$ based on the baryon masses. We distinguish the contributions from QCD and QED in the baryon mass splittings. We find that the mixing angle between $\Sigma^0$ and $\Lambda^0$ is…

High Energy Physics - Phenomenology · Physics 2020-03-18 C. Q. Geng , Chia-Wei Liu , Tien-Hsueh Tsai

We succeed in reproducing the $\ell=1$ $B$ mesons, $B_1(5720)$, $B_2^*(5745)$, and $B_{s2}^*(5839)$ that are recently reported by D0 and CDF, by using our semirelativistic quark potentila model, which also succeeded in predicting the mass…

High Energy Physics - Phenomenology · Physics 2008-11-26 Takayuki Matsuki , Toshiyuki Morii , Kazutaka Sudoh

Studying our semirelativistic potential model and the numerical results, which succeeds in predicting and reproducing recently discovered higher resonances of $D$, $D_s$, $B$, and $B_s$, we find a simple expression for the mass gap between…

High Energy Physics - Phenomenology · Physics 2008-03-29 Takayuki Matsuki , Toshiyuki Morii , Kazutaka Sudoh

We report on two spectroscopy results from CDF. First, we observe the orbitally excited $B^{**}$ mesons in $B \to \ell D^{(*)}X$ events. We find $28 \pm 6 \pm 3$% of light $B$ mesons produced are $B^{**}$ states. A collective mass fit…

High Energy Physics - Experiment · Physics 2007-05-23 G. Bauer

The recent observation of Sigma_b^{+-} (uub and ddb) and Xi_b^- (dsb) baryons at the Tevatron within 2 MeV of our theoretical predictions provides a strong motivation for applying the same theoretical approach, based on modeling the color…

High Energy Physics - Phenomenology · Physics 2007-08-31 Marek Karliner , Boaz Keren-Zur , Harry J. Lipkin , Jonathan L. Rosner

Threshold-state elementary particle lifetimes exhibit a scaling in powers of alpha = e^2/hslash*c, and a reciprocal electron-based 1/alpha scaling in particle masses that extends over two powers of 1/alpha. The m(e)/alpha coupling generates…

High Energy Physics - Phenomenology · Physics 2007-05-23 Malcolm H. Mac Gregor

We calculate the mass splittings within the heavy baryon isospin multiplets \Sigma_{c(b)} and \Xi_{c(b)}' in chiral perturbation theory to leading one-loop order. The pattern of the mass splittings in the \Sigma_c iso-triplet, which is…

High Energy Physics - Phenomenology · Physics 2008-11-26 Feng-Kun Guo , Christoph Hanhart , Ulf-G. Meißner

Recently the CDF Collaboration has announced a new precise measurement of the $W$-boson mass $M_W$ that deviates from the Standard Model (SM) prediction by $7\sigma$. The discrepancy in $M_W$ is about $\Delta_W\simeq70$ MeV and probably…

High Energy Physics - Phenomenology · Physics 2022-11-29 S. S. Afonin

We demonstrate that mass inequalities for hadrons with one or more heavy quarks arise primarily from the concavity of binding energies in the quark model, reflecting short-range Coulombic interactions and long-range confinement. Empirical…

High Energy Physics - Phenomenology · Physics 2026-04-02 Wen-Xuan Zhang , Wen-Nian Liu , Duojie Jia

We use QCD sum rule approach to calculate the masses of the ground-state Lambda_Q and Sigma_Q^(*) baryons. Contributions of the operators up to dimension six are included in operator product expansion. The resulting heavy baryonic masses…

High Energy Physics - Phenomenology · Physics 2008-11-26 Jian-Rong Zhang , Ming-Qiu Huang

Excited B mesons B_1 and B_2* are observed directly for the first time as two separate states in fully reconstructed decays to B+(*) pi-. The mass of B_1 is measured to be (5720.6 +- 2.4 +- 1.4) MeV/c^2 and the mass difference DeltaM…

High Energy Physics - Experiment · Physics 2008-11-26 D0 Collaboration , V. Abazov

A way is suggested to understand why the average masses of $(d,s,b)$ quarks are smaller than those of $(u,c,t)$ quarks. In contrast to previously proposed mechanisms relying on different Higgs boson vacuum expectation values or different…

High Energy Physics - Phenomenology · Physics 2007-05-23 Jonathan L. Rosner

We measure the mass difference, $\Delta m_+$, between the $D^{*}(2010)^+$ and the $D^+$ using the decay chain $D^{*}(2010)^+\to D^+ \pi^0$ with $D^+\to K^-\pi^+\pi^+$. The data were recorded with the BABAR detector at center-of-mass…

High Energy Physics - Experiment · Physics 2017-11-22 The BaBar Collaboration

The bottom quark 1S mass, $M_b^{1S}$, is determined using sum rules which relate the masses and the electronic decay widths of the $\Upsilon$ mesons to moments of the vacuum polarization function. The 1S mass is defined as half the…

High Energy Physics - Phenomenology · Physics 2008-11-26 A. H. Hoang

New double ratios of exponential moments of different two-point functions, which are less sensitive to the heavy quark mass and to the continuum effects than the commonly used ratio of moments, are presented for a more refined analysis of…

High Energy Physics - Phenomenology · Physics 2011-07-19 Stephan Narison

The mass of the eta_b(1S), measured recently by BABAR, is significantly lower than expected from QCD predictions for the Upsilon(1S) - eta_b(1S) hyperfine splitting. We suggest that the observed eta_b(1S) mass is shifted downwards due to a…

High Energy Physics - Phenomenology · Physics 2009-12-07 Florian Domingo , Ulrich Ellwanger , Miguel-Angel Sanchis-Lozano

Recent experiments have presented more accurate data on the $\Lambda\Lambda$-binding energies of a few $\Lambda\Lambda$- hypernuclei. This is important as the $\Lambda\Lambda$- bond energies ($\Delta B_{\Lambda\Lambda}$) of double-$\Lambda$…

Nuclear Theory · Physics 2018-09-25 Chhanda Samanta , Thomas A. Schmitt

Predicted masses of J^P=0^+ and 1^+ states of D_{sJ} and D by a potential model proposed some time ago by two of us (T.M. and T.M.), in which the Hamiltonian and wave functions are expanded in 1/m_Q with m_Q heavy quark mass respecting…

High Energy Physics - Phenomenology · Physics 2011-03-23 T. Matsuki , K. Mawatari , T. Morii , K. Sudoh

A simple regularity in anticipating P-wave excitation energies of states with heavy quarks is noted. It can apply to systems such as the negative-parity $\Sigma_c$, $\Sigma_b$, and $\Omega_c$, $\bar Q Q$ quarkonia, and the bottom-charmed…

High Energy Physics - Phenomenology · Physics 2018-10-31 Marek Karliner , Jonathan L. Rosner