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相关论文: Pole analysis on unitarized $SU(3)\times SU(3)$ on…

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In a previous paper (Commun. Theor. Phys. 57 (2012) 841), we proposed a method to distinguish poles of different dynamical origin, in a unitarized amplitude of $\pi\pi\, K\bar K$ system. That is based on the observation that `A Breit-Wigner…

高能物理 - 唯象学 · 物理学 2015-06-05 L. Y. Dai , X. G. Wang , H. Q. Zheng

Based on a dispersive approach, we apply the inverse amplitude method to unitarize one-loop SU(2) and SU(3) Chiral Perturbation Theory. Numerically, we find that this unitarization technique yields the correct complex analytic structure in…

高能物理 - 唯象学 · 物理学 2009-10-28 A. Dobado , J. R. Pelaez

We study I=0 $d$ wave $\pi\pi$ scattering phase shift using a proper unitarization approach. It is verified that the $f_2(1270)$ resonance corresponds to a twin pole structure: one on the second sheet, another one on the third sheet. Also…

高能物理 - 唯象学 · 物理学 2010-02-03 Jian-jun Wang , Z. Y. Zhou , H. Q. Zheng

Using the pole approach we determine the mass and width of the $f_0(980)$; in particular, we analyze the possibility that two nearby poles are associated to it. We restrict our analysis to a neighborhood of the resonance, using $\pi\pi$…

高能物理 - 唯象学 · 物理学 2014-11-17 R. Escribano , A. Gallegos , J. L. Lucio M. , G. Moreno , J. Pestieau

The axial vector meson $K_1(1270)$ was studied within the chiral unitary approach, where it was shown that it has a two-pole structure. We reanalyze the high-statistics WA3 experiment $K^- p\to K^-\pi^+\pi^- p$ at 63 GeV, which established…

高能物理 - 唯象学 · 物理学 2008-11-26 L. S. Geng , E. Oset , L. Roca , J. A. Oller

A coupled channel model is used to study the nature of the f0(980) resonance. It is shown that the existence of two poles close to KKbar threshold, as found in many data fits and confirmed here, can be reconciled with the KKbar molecular…

高能物理 - 唯象学 · 物理学 2008-11-26 M. P. Locher , V. E. Markushin , H. Q. Zheng

We estimate the di-photon coupling of $f_0(600)$, $f_0(980)$ and $f_2(1270)$ resonances in a coupled channel dispersive approach. The $f_0(600)$ di-photon coupling is also reinvestigated using a single channel $T$ matrix for $\pi\pi$…

高能物理 - 唯象学 · 物理学 2009-08-03 Yu Mao , Xuan-Gong Wang , Ou Zhang , H. Q. Zheng , Z. Y. Zhou

We assess possible axial-vector states with $G$-parity $\left(G=\pm 1\right)$ dynamically generated by pseudoscalar-vector interactions in coupled channels, driven by the Weinberg-Tomozawa term at leading order in chiral perturbation…

高能物理 - 唯象学 · 物理学 2025-12-03 Mao-Jun Yan , Chun-Sheng An , Cheng-Rong Deng

The available data on the a0(980), f0(980), f0(1300) and K*0(1430) mesons are fitted as a distorted 0++ nonet using only 6 parameters and a very general model. This includes all light two-pseudoscalar thresholds, constraints from Adler…

高能物理 - 唯象学 · 物理学 2007-05-23 Nils Tornqvist

Recent studies based on unitary chiral perturbation theory (U$\chi$PT) found that the low-lying axial vector mesons can be dynamically generated due to the interaction of the pseudoscalar octet of the pion and the vector nonet of the rho.…

高能物理 - 唯象学 · 物理学 2007-11-30 L. S. Geng , E. Oset , L. Roca , J. A. Oller

The so far only known charmed non-strange scalar meson is dubbed as $D_0^*(2400)$ in the Review of Particle Physics. We show, within the framework of unitarized chiral perturbation theory, that there are in fact two $(I=1/2, J^P=0^+)$ poles…

高能物理 - 唯象学 · 物理学 2017-04-05 Miguel Albaladejo , Pedro Fernandez-Soler , Feng-Kun Guo , Juan Nieves

Within the chiral unitary approach, the axial-vector resonance $K_1(1270)$ has been predicted to manifest a two-pole nature. The lowest pole has a mass of 1195 Mev and a width of 246 Mev and couples mostly to $K^*\pi$, and the highest pole…

高能物理 - 唯象学 · 物理学 2019-10-23 G. Y. Wang , L. Roca , E. Oset

In a combined analysis of the experimental data on the coupled processes $\pi\pi\to\pi\pi,K\bar{K}$ in the channel with $I^GJ^{PC}=0^+0^{++}$, the various scenarios of these reactions (with different numbers of resonances) are considered.…

高能物理 - 唯象学 · 物理学 2007-05-23 Yu. S. Surovtsev , D. Krupa , M. Nagy

We present results following from the coupled channel model of two a0 resonances decaying into the pi-eta and K anti-K mesons. The a0(980) resonance can be described by two distinct poles. It is shown that the discrepancy in the a0(980)…

高能物理 - 唯象学 · 物理学 2009-11-07 Agnieszka Furman , Leonard Lesniak

The $s-$wave meson-baryon scattering is analyzed for the strangeness S=0 sector in a Bethe-Salpeter coupled channel formalism incorporating Chiral Symmetry. Four channels have been considered: $\pi N$, $\eta N$, $K \Lambda$, $K \Sigma$. The…

高能物理 - 唯象学 · 物理学 2009-11-07 Juan Nieves , Enrique Ruiz Arriola

We use a non-perturbative approach which combines coupled channel Lippmann-Schwinger equations with meson-meson potentials provided by the lowest order chiral Lagrangian. By means of one parameter, a cut off in the momentum of the loop…

高能物理 - 唯象学 · 物理学 2007-05-23 J. A. Oller , E. Oset

A K-matrix re-analysis of the K-pi S-wave is performed in the mass region 900-2100 MeV, and solutions which describe the data well are found. The solution with two resonances in the (IJ^P=1/2 0^+)-wave has poles at (1415 pm 25)- i(165 pm…

高能物理 - 唯象学 · 物理学 2008-11-26 A. V. Anisovich , A. V. Sarantsev

In this work, the complete one loop calculation of meson-meson scattering amplitudes within U(3)\otimes U(3) chiral perturbation theory with explicit resonance states is carried out for the first time. Partial waves are unitarized from the…

高能物理 - 唯象学 · 物理学 2015-03-19 Zhi-Hui Guo , J. A. Oller

A coupled-channel S- and P-wave next-to-leading order chiral-unitary approach for strangeness $S=-1$ meson-baryon scattering is extended to include the new data from the KLOE and AMADEUS experiments as well as the $\Lambda\pi$ mass…

A study of three-pseudoscalar $\pi K \bar{K}$ and $\pi \pi \eta$ coupled system is made by solving the Faddeev equations within an approach based on unitary chiral dynamics. A resonance with total isospin one and spin-parity $J^\pi = 0^-$…

核理论 · 物理学 2015-05-28 A. Martínez Torres , K. P. Khemchandani , D. Jido , A. Hosaka
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