<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>S</mml:mi></mml:math>-wave<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:mi>K</mml:mi><mml:msup><mml:mrow><mml:mi>K</mml:mi></mml:mrow><mml:mrow><mml:mo>*</mml:mo></mml:mrow></mml:msup></mml:mrow></mml:math>interactions in a finite volume and the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mrow><mml:msub><mml:mrow><mml:mi>f</mml:mi></mml:mrow><mml:mro

Geng, Li-Sheng; Ren, Xiu-Lei; Zhou, Yu; Chen, Hua-Xing; Oset, E.

doi:10.1103/physrevd.92.014029

Cited by 29 publications

(35 citation statements)

References 84 publications

Supporting

Mentioning

Contrasting

Order By: Relevance

“…quasi-bound molecular structure. There has also been recent investigation of the f 1 (1285) state on the lattice by Dudek et al [27] and by Geng et al [28]. The present results may help these studies, for instance through better determination of the width of the state.…”

Section: Introductionsupporting

confidence: 60%

Photoproduction of thef1(1285)meson

Dickson¹,

Schumacher²,

Adhikari³

et al. 2016

Phys. Rev. C

View full text Add to dashboard Cite

The f1(1285) meson with mass 1281.0 ± 0.8 MeV/c 2 and width 18.4 ± 1.4 MeV (FWHM) was measured for the first time in photoproduction from a proton target using CLAS at Jefferson Lab. Differential cross sections were obtained via the ηπ + π − , K +K 0 π − , and K − K 0 π + decay channels from threshold up to a center-of-mass energy of 2.8 GeV. The mass, width, and an amplitude analysis of the ηπ + π − final-state Dalitz distribution are consistent with the axial-vector J P = 1 + f1(1285) identity, rather than the pseudoscalar 0 − η(1295). The production mechanism is more consistent with s-channel decay of a high-mass N * state, and not with t-channel meson exchange. Decays to ηππ go dominantly via the intermediate a ± 0 (980)π ∓ states, with the branching ratio Γ(a0π (noKK))/Γ(ηππ (all)) = 0.74±0.09. The branching ratios Γ(KKπ)/Γ(ηππ) = 0.216±0.033 and Γ(γρ 0 )/Γ(ηππ) = 0.047 ± 0.018 were also obtained. The first is in agreement with previous data for the f1(1285), while the latter is lower than the world average.

show abstract

Section: Introductionsupporting

confidence: 60%

Photoproduction of thef1(1285)meson

Dickson¹,

Schumacher²,

Adhikari³

et al. 2016

Phys. Rev. C

View full text Add to dashboard Cite

show abstract

“…We should note that, for a single channel, the Lüscher method is consistent with the Jülich-Valencia approach adopted in the present work (see, e.g., Ref. [59] for an explicit comparison in the case of K K * scattering).…”

Section: ) and Likewise For E[bk ( )]mentioning

confidence: 62%

“…In this work, we follow the method proposed in Ref. [59] to calculate the loop function G in finite volume in the dimensional regularization scheme. Introducing a finite-volume correction, δG,G can be written as…”

Section: B S π and Bk Interactions In Finite Volumementioning

confidence: 99%

See 1 more Smart Citation

$$B_s\pi $$ B s π – $$B\bar{K}$$ B K ¯ interactions in finite volume and X(5568)

Ren

Geng

2017

Eur. Phys. J. C

Self Cite

View full text Add to dashboard Cite

The recent observation of X (5568) by the D0 Collaboration has aroused a lot of interest both theoretically and experimentally. In the present work, we first point out that X (5568) and D * s0 (2317) cannot simultaneously be of molecular nature, from the perspective of heavy-quark symmetry and chiral symmetry, based on a previous study of the lattice QCD scattering lengths of DK and its coupled channels. Then we compute the discrete energy levels of the B s π and BK system in finite volume using unitary chiral perturbation theory. The comparison with the latest lattice QCD simulation, which disfavors the existence of X (5568), supports our picture where the B s π and BK interactions are weak and X (5568) cannot be a B s π and BK molecular state. In addition, we show that the extended Weinberg compositeness condition also indicates that X (5568) cannot be a molecular state made from B s π and BK interactions.

show abstract

“…Recently, a new form of quintessence potential, viz. steep exponential potential, have gained interest where the potential has the form [8] V (φ) = V 0 e α( φ Mp ) n , (1.1)…”

mentioning

confidence: 99%

Dynamical system analysis for steep potentials

Das

Banerjee

Roy

2019

J. Cosmol. Astropart. Phys.

View full text Add to dashboard Cite

In this work we have performed the dynamical system analysis for steep(er) exponential potentials considering different values of the steepness index n. We have performed the analysis using centre manifold theory as well as by employing numerical method. We have shown that in most of the cases, the higher values of steepness index corresponds to an unstable solution. We have shown that with this steep(er) potentials one can not have a phase transition from dark matter to dark energy in the past.

show abstract

S-waveKK*interactions in a finite volume and thef

Cited by 29 publications

References 84 publications

Photoproduction of thef1(1285)meson

Photoproduction of thef1(1285)meson

$$B_s\pi $$ B s π – $$B\bar{K}$$ B K ¯ interactions in finite volume and X(5568)

Dynamical system analysis for steep potentials

Contact Info

Product

Resources

About