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Related papers: A Study in Depth of f0(1370)

200 papers

A summary is given of the main sets of data requiring the existence of f0(1370). Crystal Barrel data on pbar-p -> eta eta pizero contain a visible f0(1370) peak and require at least a 19 standard deviation contribution. This alone is…

High Energy Physics - Experiment · Physics 2007-10-25 D. V. Bugg

Four sets of data determining parameters of a0(1450) and a0(980) are re-analysed. These are Crystal Barrel data for pbar-p annihilation at rest to eta-pizero-pizero in (i) liquid hydrogen and (ii) gas, and to (iii) K0_L-picharged-Kcharged…

High Energy Physics - Experiment · Physics 2008-11-26 D. V. Bugg

The scalar meson f_0(1370) - indicated in particular in the low energy p\bar p \to 3 body reactions - is a crucial element in certain schemes of the scalar meson spectroscopy including glueballs. The most definitive results can be obtained…

High Energy Physics - Phenomenology · Physics 2015-05-18 Wolfgang Ochs

We establish the existence of the long-debated $f_0(1370)$ resonance in the dispersive analyses of meson-meson scattering data. For this, we present a novel approach using forward dispersion relations, valid for generic inelastic…

High Energy Physics - Phenomenology · Physics 2024-07-25 Jose Ramon Pelaez , Arkaitz Rodas , Jacobo Ruiz de Elvira

Data for phi -> gamma (eta-pizero) are analysed using the KK loop model and compared with parameters of a0(980) derived from Crystal Barrel data. The eta-pi mass spectrum agrees closely and the absolute normalisation lies just within…

High Energy Physics - Experiment · Physics 2008-11-26 D. V. Bugg

BES II data for the channel J/Psi -> gamma (piplus-piminus-piplus-piminus) are analysed from a sample of 58M J/Psi hadronic interactions. They reveal further detail in the J^{PC} = 0^{-+} sector for the 4pi channel. A broad 0^{-+} ->…

High Energy Physics - Experiment · Physics 2009-07-20 D. V. Bugg

There is a large discrepancy between results of Crystal Barrel and WA102 for the branching ratio R = BR[eta2(1870)->a2(1320)pi]/ BR[eta2(1870)->f2(1270)eta]. An extensive re-analysis of the Crystal Barrel data redetermines branching ratios…

High Energy Physics - Experiment · Physics 2011-02-09 A. V. Anisovich , C. J. Batty , D. V. Bugg , V. A. Nikonov , A. V. Sarantsev

A partial wave analysis of pbar-p -> eta-eta-pizero data from the Crystal Barrel experiment is made in terms of s-channel resonances. The decay channels a_0(980)-eta, f_0(1770)-pi and f_0(2105)-pi provide evidence for two I = 1 J^{PC} =…

High Energy Physics - Experiment · Physics 2015-05-30 A. V. Anisovich , C. A. Baker , C. J. Batty , D. V. Bugg , V. A. Nikonov , A. V. Sarantsev , V. V. Sarantsev , B. S. Zou

We report evidence for the decay B0->pi0pi0. The analysis is based on a data sample of 152million BBbar pairs collected at the Upsilon(4s) resonance with the Belle detector at the KEKB e+e- storage ring. We find…

High Energy Physics - Experiment · Physics 2008-11-26 The Belle Collaboration , S. H. Lee

The results of the patial wave analysis(PWA) of the pi+pi-pi- and omegapi-pi0 systems are presented. The a3 and a4(2040) signals are observed in the rho(770)pi and f2(1270)pi channels. Indications of the a1' meson existence was found in the…

High Energy Physics - Experiment · Physics 2007-05-23 V. Dorofeev , VES Collaboration

New Crystal Barrel data are reported for pbar-p -> omega-pizero and pbar-p -> omega eta-pizero with omega decaying to piplus-piminus-pizero. The shapes of angular distributions agree well with those for data where omega -> pizero-gamma;…

High Energy Physics - Experiment · Physics 2011-09-28 A. V. Anisovich , C. A. Baker , C. J. Batty , D. V. Bugg , L. Montanet , V. A. Nikonov , A. V. Sarantsev , V. V. Sarantsev , B. S. Zou

New Crystal Barrel data are reported for pbar-p -> omega-eta and pbar-p -> omega-pizero-pizero with omega decaying to piplus-piminus-pizero. The omega-eta data confirm angular distributions obtained earlier from data where omega ->…

High Energy Physics - Experiment · Physics 2011-09-29 A. V. Anisovich , C. A. Baker , C. J. Batty , D. V. Bugg , L. Montanet , V. A. Nikonov , A. V. Sarantsev , V. V. Sarantsev , B. S. Zou

Under the hypothesis that the $f_0(1370)$ is a $\kappa \bar{\kappa}$ molecular state, we calculate the partial widths of its various decay channels, including the two-body decay $K \bar{K}$, $\pi \pi$, $\eta \eta$ and the four-body decay…

High Energy Physics - Phenomenology · Physics 2026-03-06 Yin Cheng , Bing-Song Zou

We present data on pbar-p -> eta-eta-pizero at beam momenta of 600, 900, 1050, and 1200 MeV/c. At the higher three momenta, a signal is clearly visible due to pbar-p -> f_0(1770)-pizero, f_0(1770) -> eta-eta. It has mass 1770+-12 MeV and…

High Energy Physics - Experiment · Physics 2015-05-30 A. V. Anisovich , C. A. Baker , C. J. Batty , D. V. Bugg , R. P. Haddock , C. Hodd , V. A. Nikonov , A. V. Sarantsev , V. V. Sarantsev , I. Scott , B. S. Zou

A partial wave analysis is presented of Crystal Barrel data on pbar-p -> pizero-pizero, eta-eta and eta-etaprime from 600 to 1940 MeV/c, combined with earlier data on d\sigma /d\Omega and P for pbar-p->piminus-piplus. The following…

High Energy Physics - Experiment · Physics 2015-05-30 A. V. Anisovich , C. A. Baker , C. J. Batty , D. V. Bugg , A. Hasan , C. Hodd , J. Kisiel , V. A. Nikonov , A. V. Sarantsev , V. V. Sarantsev , B. S. Zou

Using an improved "analytic K-matrix model", we reconsider the extraction of the sigma/f_0(600) and f_0(980) gamma-gamma widths from gamma-gamma to pi-pi scatterings data of Crystal Ball and Belle. Our main results are summarized in Tables…

High Energy Physics - Phenomenology · Physics 2011-01-04 G. Mennessier , S. Narison , X. -G. Wang

We systematically reconsider, within an improved "analytic K-matrix model", the extraction of the sigma = f_0(600) and f_0(980) masses, widths and hadronic couplings using new Ke4 = K-->pi-pi e nu_e data on pi-pi phase shift below 390 MeV…

High Energy Physics - Phenomenology · Physics 2014-11-20 G. Mennessier , S. Narison , X. -G. Wang

A pi-pi, Kbar-K, and rho-rho(omega-omega) fully coupled channel model is used to predict the lowest isospin S, P, D, F-wave phase shifts and inelasticities for elastic pi-pi scattering from threshold to 2.0 GeV. As input the S-matrix is…

Nuclear Theory · Physics 2009-10-30 W. M. Kloet , B. Loiseau

A search has been made for the decays B+ -> phi pi+ and B0->to phi pi0 in a data sample of approximately 232 x 10^6 B Bbar pairs recorded at the Upsilon(4S) resonance with the BaBar detector at the PEP-II B-meson Factory at SLAC. No…

High Energy Physics - Experiment · Physics 2010-03-19 The BABAR Collaboration , B. Aubert

We report a search for the charmless hadronic decay $B^0\to\eta \pi^0$ with a data sample corresponding to an integrated luminosity of 694 $\rm fb^{-1}$ containing $753\times10^6$ $B\bar{B}$ pairs. The data were collected by the Belle…

High Energy Physics - Experiment · Physics 2015-07-14 Belle Collaboration , B. Pal , A. J. Schwartz , A. Abdesselam , I. Adachi , H. Aihara , S. Al Said , K. Arinstein , D. M. Asner , V. Aulchenko , T. Aushev , R. Ayad , V. Babu , I. Badhrees , A. M. Bakich , A. Bobrov , G. Bonvicini , A. Bozek , M. Bračko , T. E. Browder , D. Červenkov , M. -C. Chang , V. Chekelian , A. Chen , B. G. Cheon , K. Cho , V. Chobanova , Y. Choi , D. Cinabro , J. Dalseno , Z. Doležal , Z. Drásal , A. Drutskoy , D. Dutta , S. Eidelman , H. Farhat , J. E. Fast , T. Ferber , O. Frost , B. G. Fulsom , V. Gaur , N. Gabyshev , S. Ganguly , A . Garmash , D. Getzkow , R. Gillard , R. Glattauer , Y. M. Goh , B. Golob , O. Grzymkowska , T. Hara , K. Hayasaka , H. Hayashii , X. H. He , W. -S. Hou , M. Huschle , H. J. Hyun , T. Iijima , A. Ishikawa , R. Itoh , Y. Iwasaki , I. Jaegle , T. Julius , K. H. Kang , E. Kato , C. Kiesling , D. Y. Kim , J. B. Kim , J. H. Kim , K. T. Kim , M. J. Kim , S. H. Kim , Y. J. Kim , K. Kinoshita , B. R. Ko , P. Kodyš , S. Korpar , P. Križan , P. Krokovny , T. Kuhr , T. Kumita , A. Kuzmin , Y. -J. Kwon , J. S. Lange , D. H. Lee , I. S. Lee , Y. Li , L. Li Gioi , J. Libby , D. Liventsev , P. Lukin , D. Matvienko , H. Miyata , G. B. Mohanty , A. Moll , H. K. Moon , K. R. Nakamura , E. Nakano , M. Nakao , T. Nanut , Z. Natkaniec , M. Nayak , S. Nishida , S. Ogawa , S. Okuno , P. Pakhlov , G. Pakhlova , C. W. Park , H. Park , T. K. Pedlar , L. Pesántez , M. Petrič , L. E. Piilonen , C. Pulvermacher , E. Ribežl , M. Ritter , A. Rostomyan , S. Ryu , Y. Sakai , S. Sandilya , D. Santel , L. Santelj , T. Sanuki , Y. Sato , O. Schneider , G. Schnell , C. Schwanda , K. Senyo , O. S eon , M. E. Sevior , M. Shapkin , V. Shebalin , C. P. Shen , T. -A. Shibata , J. -G. Shiu , A. Sibidanov , F. Simon , Y. -S. Sohn , E. Solovieva , S. Stanič , M. Starič , M. Su mihama , K. Sumisawa , T. Sumiyoshi , U. Tamponi , Y. Teramoto , F. Thorne , M. Uchida , S. Uehara , Y. Unno , S. Uno , Y. Usov , C. Van Hulse , P. Vanhoefer , G. Varner , A. Vinokur ova , V. Vorobyev , A. Vossen , M. N. Wagner , C. H. Wang , M. -Z. Wang , P. Wang , X. L. Wang , Y. Watanabe , E. Won , H. Yamamoto , J. Yamaoka , S. Yashchenko , Z. P. Zhang , V. Zhi lich , V. Zhulanov , A. Zupanc
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