Study of the process e+e- →π+π-π0 using initial state radiation with BABAR

Lees, J.P.; Poireau, V.; Tisserand, V.; Grauges, E.; Palano, A.; Eigen, G.; Brown, D.N.; Kolomensky, Y.G.; Fritsch, M.; Koch, H.; Schroeder, T.; Cheaib, R.; Hearty, C.; Mattison, T.S.; Mckenna, J.A.; R. Y., S.; Blinov, V.E.; Buzykaev, A.R.; Druzhinin, V.P.; Golubev, V.B.; Kozyrev, E.A.; Kravchenko, E.A.; Onuchin, A.P.; Serednyakov, S.I.; Skovpen, Y.I.; Solodov, E.P.; Todyshev, K.Y.; Lankford, A.J.; Dey, B.; Gary, J.W.; Long, O.; Eisner, A.M.; Lockman, W.S.; Panduro Vazquez, W.; Chao, D.S.; Cheng, C.H.; Echenard, B.; Flood, K.T.; Hitlin, D.G.; Kim, J.; Li, Y.; Lin, D.X.; Middleton, S.; Miyashita, T.S.; Ongmongkolkul, P.; Oyang, J.; Porter, F.C.; Rohrken, M.; Huard, Z.; Meadows, B.T.; Pushpawela, B.G.; Sokoloff, M.D.; Sun, L.; Smith, J.G.; Wagner, S.R.; Bernard, D.; Verderi, M.; Bettoni, D.; Bozzi, C.; Calabrese, R.; Cibinetto, G.; Fioravanti, E.; Garzia, I.; Luppi, E.; Santoro, V.; Calcaterra, A.; De Sangro, R.; Finocchiaro, G.; Martellotti, S.; Patteri, P.; Peruzzi, I.M.; Piccolo, M.; Rotondo, M.; Zallo, A.; Passaggio, S.; Patrignani, C.; Shuve, B.J.; Lacker, H.M.; Bhuyan, B.; Mallik, U.; Chen, C.; Cochran, J.; Prell, S.; Gritsan, A.V.; Arnaud, N.; Davier, M.; Le Diberder, F.; Lutz, A.M.; Wormser, G.; Lange, D.J.; Wright, D.M.; Coleman, J.P.; Gabathuler, E.; Hutchcroft, D.E.; Payne, D.J.; Touramanis, C.; Bevan, A.J.; Di Lodovico, F.; Sacco, R.; Cowan, G.; Banerjee, S.; Brown, D.N.; Davis, C.L.; Denig, A.G.; Gradl, W.; Griessinger, K.; Hafner, A.; Schubert, K.R.; Barlow, R.J.; Lafferty, G.D.; Cenci, R.; Jawahery, A.; Roberts, D.A.; Cowan, R.; Robertson, S.H.; Seddon, R.M.; Neri, N.; Palombo, F.; Cremaldi, L.; Godang, R.; Summers, D.J.; Taras, P.; De Nardo, G.; Sciacca, C.; Raven, G.; Jessop, C.P.; Losecco, J.M.; Honscheid, K.; Kass, R.; Gaz, A.; Margoni, M.; Posocco, M.; Simi, G.; Simonetto, F.; Stroili, R.; Akar, S.; Ben-Haim, E.; Bomben, M.; Bonneaud, G.R.; Calderini, G.; Chauveau, J.; Marchiori, G.; Ocariz, J.; Biasini, M.; Manoni, E.; Rossi, A.; Batignani, G.; Bettarini, S.; Carpinelli, M.; Casarosa, G.; Chrzaszcz, M.; Forti, F.; Giorgi, M.A.; Lusiani, A.; Oberhof, B.; Paoloni, E.; Rama, M.; Rizzo, G.; Walsh, J.J.; Zani, L.; Smith, A.J.S.; Anulli, F.; Faccini, R.; Ferrarotto, F.; Ferroni, F.; Pilloni, A.; Piredda, G.; Bunger, C.; Dittrich, S.; Grunberg, O.; Hess, M.; Leddig, T.; Voss, C.; Waldi, R.; Adye, T.; Wilson, F.F.; Emery, S.; Vasseur, G.; Aston, D.; Cartaro, C.; Convery, M.R.; Dorfan, J.; Dunwoodie, W.; Ebert, M.; Field, R.C.; Fulsom, B.G.; Graham, M.T.; Hast, C.; Innes, W.R.; Kim, P.; Leith, D.W.G.S.; Luitz, S.; Macfarlane, D.B.; Muller, D.R.; Neal, H.; Ratcliff, B.N.; Roodman, A.; Sullivan, M.K.; Va'Vra, J.; Wisniewski, W.J.; Purohit, M.V.; Wilson, J.R.; Randle-Conde, A.; Sekula, S.J.; Ahmed, H.; Tasneem, N.; Bellis, M.; Burchat, P.R.; Puccio, E.M.T.; Alam, M.S.; Ernst, J.A.; Gorodeisky, R.; Guttman, N.; Peimer, D.R.; Soffer, A.; Spanier, S.M.; Ritchie, J.L.; Schwitters, R.F.; Izen, J.M.; Lou, X.C.; Bianchi, F.; De Mori, F.; Filippi, A.; Gamba, D.; Lanceri, L.; Vitale, L.; Martinez-Vidal, F.; Oyanguren, A.; Albert, J.; Beaulieu, A.; Bernlochner, F.U.; King, G.J.; Kowalewski, R.; Lueck, T.; Miller, C.; Nugent, I.M.; Roney, J.M.; Sobie, R.J.; Gershon, T.J.; Harrison, P.F.; Latham, T.E.; Prepost, R.; S. L., W.

doi:10.1103/PhysRevD.104.112003

The process e+e-→π+π-π0γ is studied at a center-of-mass energy near the D(4S) resonance using a data sample of 469 fb-1 collected with the BABAR detector at the PEP-II collider. We have performed a precise measurement of the e+e-→π+π-π0 cross section in the center-of-mass energy range from 0.62 to 3.5 GeV. In the energy regions of the ω and φ resonances, the cross section is measured with a systematic uncertainty of 1.3%. The leading-order hadronic contribution to the muon magnetic anomaly calculated using the measured e+e-→π+π-π0 cross section from threshold to 2.0 GeV is (45.86±0.14±0.58)×10-10. From the fit to the measured 3π mass spectrum we have determined the resonance parameters Γ(ω→e+e-)B(ω→π+π-π0)=(0.5698±0.0031±0.0082) keV, Γ(φ→e+e-)B(φ→π+π-π0)=(0.1841±0.0021±0.0080) keV, and B(ρ→3π)=(0.88±0.23±0.30)×10-4. The significance of the ρ→3π signal is greater than 6σ. For the J/ψ resonance we have measured the product Γ(J/ψ→e+e-)B(J/ψ→3π)=(0.1248±0.0019±0.0026) keV.

Study of the process e+e- →π+π-π0 using initial state radiation with BABAR / J.P. Lees, V. Poireau, V. Tisserand, E. Grauges, A. Palano, G. Eigen, D.N. Brown, Y.G. Kolomensky, M. Fritsch, H. Koch, T. Schroeder, R. Cheaib, C. Hearty, T.S. Mattison, J.A. Mckenna, R.Y. So, V.E. Blinov, A.R. Buzykaev, V.P. Druzhinin, V.B. Golubev, E.A. Kozyrev, E.A. Kravchenko, A.P. Onuchin, S.I. Serednyakov, Y.I. Skovpen, E.P. Solodov, K.Y. Todyshev, A.J. Lankford, B. Dey, J.W. Gary, O. Long, A.M. Eisner, W.S. Lockman, W. Panduro Vazquez, D.S. Chao, C.H. Cheng, B. Echenard, K.T. Flood, D.G. Hitlin, J. Kim, Y. Li, D.X. Lin, S. Middleton, T.S. Miyashita, P. Ongmongkolkul, J. Oyang, F.C. Porter, M. Rohrken, Z. Huard, B.T. Meadows, B.G. Pushpawela, M.D. Sokoloff, L. Sun, J.G. Smith, S.R. Wagner, D. Bernard, M. Verderi, D. Bettoni, C. Bozzi, R. Calabrese, G. Cibinetto, E. Fioravanti, I. Garzia, E. Luppi, V. Santoro, A. Calcaterra, R. De Sangro, G. Finocchiaro, S. Martellotti, P. Patteri, I.M. Peruzzi, M. Piccolo, M. Rotondo, A. Zallo, S. Passaggio, C. Patrignani, B.J. Shuve, H.M. Lacker, B. Bhuyan, U. Mallik, C. Chen, J. Cochran, S. Prell, A.V. Gritsan, N. Arnaud, M. Davier, F. Le Diberder, A.M. Lutz, G. Wormser, D.J. Lange, D.M. Wright, J.P. Coleman, E. Gabathuler, D.E. Hutchcroft, D.J. Payne, C. Touramanis, A.J. Bevan, F. Di Lodovico, R. Sacco, G. Cowan, S. Banerjee, D.N. Brown, C.L. Davis, A.G. Denig, W. Gradl, K. Griessinger, A. Hafner, K.R. Schubert, R.J. Barlow, G.D. Lafferty, R. Cenci, A. Jawahery, D.A. Roberts, R. Cowan, S.H. Robertson, R.M. Seddon, N. Neri, F. Palombo, L. Cremaldi, R. Godang, D.J. Summers, P. Taras, G. De Nardo, C. Sciacca, G. Raven, C.P. Jessop, J.M. Losecco, K. Honscheid, R. Kass, A. Gaz, M. Margoni, M. Posocco, G. Simi, F. Simonetto, R. Stroili, S. Akar, E. Ben-Haim, M. Bomben, G.R. Bonneaud, G. Calderini, J. Chauveau, G. Marchiori, J. Ocariz, M. Biasini, E. Manoni, A. Rossi, G. Batignani, S. Bettarini, M. Carpinelli, G. Casarosa, M. Chrzaszcz, F. Forti, M.A. Giorgi, A. Lusiani, B. Oberhof, E. Paoloni, M. Rama, G. Rizzo, J.J. Walsh, L. Zani, A.J.S. Smith, F. Anulli, R. Faccini, F. Ferrarotto, F. Ferroni, A. Pilloni, G. Piredda, C. Bunger, S. Dittrich, O. Grunberg, M. Hess, T. Leddig, C. Voss, R. Waldi, T. Adye, F.F. Wilson, S. Emery, G. Vasseur, D. Aston, C. Cartaro, M.R. Convery, J. Dorfan, W. Dunwoodie, M. Ebert, R.C. Field, B.G. Fulsom, M.T. Graham, C. Hast, W.R. Innes, P. Kim, D.W.G.S. Leith, S. Luitz, D.B. Macfarlane, D.R. Muller, H. Neal, B.N. Ratcliff, A. Roodman, M.K. Sullivan, J. Va'Vra, W.J. Wisniewski, M.V. Purohit, J.R. Wilson, A. Randle-Conde, S.J. Sekula, H. Ahmed, N. Tasneem, M. Bellis, P.R. Burchat, E.M.T. Puccio, M.S. Alam, J.A. Ernst, R. Gorodeisky, N. Guttman, D.R. Peimer, A. Soffer, S.M. Spanier, J.L. Ritchie, R.F. Schwitters, J.M. Izen, X.C. Lou, F. Bianchi, F. De Mori, A. Filippi, D. Gamba, L. Lanceri, L. Vitale, F. Martinez-Vidal, A. Oyanguren, J. Albert, A. Beaulieu, F.U. Bernlochner, G.J. King, R. Kowalewski, T. Lueck, C. Miller, I.M. Nugent, J.M. Roney, R.J. Sobie, T.J. Gershon, P.F. Harrison, T.E. Latham, R. Prepost, S.L. Wu. - In: PHYSICAL REVIEW D. - ISSN 2470-0010. - 104:11(2021), pp. 112003.1-112003.31. [10.1103/PhysRevD.104.112003]

Study of the process e+e- →π+π-π0 using initial state radiation with BABAR

Lees J. P.;Poireau V.;Tisserand V.;Grauges E.;Palano A.;Eigen G.;Brown D. N.;Kolomensky Yu. G.;Fritsch M.;Koch H.;Schroeder T.;Cheaib R.;Hearty C.;Mattison T. S.;McKenna J. A.;So R. Y.;Blinov V. E.;Buzykaev A. R.;Druzhinin V. P.;Golubev V. B.;Kozyrev E. A.;Kravchenko E. A.;Onuchin A. P.;Serednyakov S. I.;Skovpen Yu. I.;Solodov E. P.;Todyshev K. Yu.;Lankford A. J.;Dey B.;Gary J. W.;Long O.;Eisner A. M.;Lockman W. S.;Panduro Vazquez W.;Chao D. S.;Cheng C. H.;Echenard B.;Flood K. T.;Hitlin D. G.;Kim J.;Li Y.;Lin D. X.;Middleton S.;Miyashita T. S.;Ongmongkolkul P.;Oyang J.;Porter F. C.;Rohrken M.;Huard Z.;Meadows B. T.;Pushpawela B. G.;Sokoloff M. D.;Sun L.;Smith J. G.;Wagner S. R.;Bernard D.;Verderi M.;Bettoni D.;Bozzi C.;Calabrese R.;Cibinetto G.;Fioravanti E.;Garzia I.;Luppi E.;Santoro V.;Calcaterra A.;De Sangro R.;Finocchiaro G.;Martellotti S.;Patteri P.;Peruzzi I. M.;Piccolo M.;Rotondo M.;Zallo A.;Passaggio S.;Patrignani C.;Shuve B. J.;Lacker H. M.;Bhuyan B.;Mallik U.;Chen C.;Cochran J.;Prell S.;Gritsan A. V.;Arnaud N.;Davier M.;Le Diberder F.;Lutz A. M.;Wormser G.;Lange D. J.;Wright D. M.;Coleman J. P.;Gabathuler E.;Hutchcroft D. E.;Payne D. J.;Touramanis C.;Bevan A. J.;Di Lodovico F.;Sacco R.;Cowan G.;Banerjee S.;Brown D. N.;Davis C. L.;Denig A. G.;Gradl W.;Griessinger K.;Hafner A.;Schubert K. R.;Barlow R. J.;Lafferty G. D.;Cenci R.;Jawahery A.;Roberts D. A.;Cowan R.;Robertson S. H.;Seddon R. M.;N. Neri;F. Palombo;Cremaldi L.;Godang R.;Summers D. J.;Taras P.;De Nardo G.;Sciacca C.;Raven G.;Jessop C. P.;Losecco J. M.;Honscheid K.;Kass R.;Gaz A.;Margoni M.;Posocco M.;Simi G.;Simonetto F.;Stroili R.;Akar S.;Ben-Haim E.;Bomben M.;Bonneaud G. R.;Calderini G.;Chauveau J.;Marchiori G.;Ocariz J.;Biasini M.;Manoni E.;Rossi A.;Batignani G.;Bettarini S.;Carpinelli M.;Casarosa G.;Chrzaszcz M.;F. Forti;Giorgi M. A.;Lusiani A.;Oberhof B.;Paoloni E.;Rama M.;Rizzo G.;Walsh J. J.;L. Zani;Smith A. J. S.;Anulli F.;Faccini R.;Ferrarotto F.;Ferroni F.;Pilloni A.;Piredda G.;Bunger C.;Dittrich S.;Grunberg O.;Hess M.;Leddig T.;Voss C.;Waldi R.;Adye T.;Wilson F. F.;Emery S.;Vasseur G.;Aston D.;Cartaro C.;Convery M. R.;Dorfan J.;Dunwoodie W.;Ebert M.;Field R. C.;Fulsom B. G.;Graham M. T.;Hast C.;Innes W. R.;Kim P.;Leith D. W. G. S.;Luitz S.;MacFarlane D. B.;Muller D. R.;Neal H.;Ratcliff B. N.;Roodman A.;Sullivan M. K.;Va'vra J.;Wisniewski W. J.;Purohit M. V.;Wilson J. R.;Randle-Conde A.;Sekula S. J.;Ahmed H.;Tasneem N.;Bellis M.;Burchat P. R.;Puccio E. M. T.;Alam M. S.;Ernst J. A.;Gorodeisky R.;Guttman N.;Peimer D. R.;Soffer A.;Spanier S. M.;Ritchie J. L.;Schwitters R. F.;Izen J. M.;Lou X. C.;Bianchi F.;De Mori F.;A. Filippi;Gamba D.;Lanceri L.;L. Vitale;Martinez-Vidal F.;Oyanguren A.;Albert J.;Beaulieu A.;Bernlochner F. U.;King G. J.;Kowalewski R.;Lueck T.;C. Miller;Nugent I. M.;Roney J. M.;Sobie R. J.;Gershon T. J.;Harrison P. F.;Latham T. E.;Prepost R.;Wu S. L.

2021

Abstract

The process e+e-→π+π-π0γ is studied at a center-of-mass energy near the D(4S) resonance using a data sample of 469 fb-1 collected with the BABAR detector at the PEP-II collider. We have performed a precise measurement of the e+e-→π+π-π0 cross section in the center-of-mass energy range from 0.62 to 3.5 GeV. In the energy regions of the ω and φ resonances, the cross section is measured with a systematic uncertainty of 1.3%. The leading-order hadronic contribution to the muon magnetic anomaly calculated using the measured e+e-→π+π-π0 cross section from threshold to 2.0 GeV is (45.86±0.14±0.58)×10-10. From the fit to the measured 3π mass spectrum we have determined the resonance parameters Γ(ω→e+e-)B(ω→π+π-π0)=(0.5698±0.0031±0.0082) keV, Γ(φ→e+e-)B(φ→π+π-π0)=(0.1841±0.0021±0.0080) keV, and B(ρ→3π)=(0.88±0.23±0.30)×10-4. The significance of the ρ→3π signal is greater than 6σ. For the J/ψ resonance we have measured the product Γ(J/ψ→e+e-)B(J/ψ→3π)=(0.1248±0.0019±0.0026) keV.

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	Settori scientifico-disciplinari dell'articolo
	
			Settore FIS/01 - Fisica Sperimentale
Settore FIS/04 - Fisica Nucleare e Subnucleare
		
	Data di pubblicazione
	
			2021
		
	Rivista in ANCE
	
			PHYSICAL REVIEW D
		
	DOI
	
			https://dx.doi.org/10.1103/PhysRevD.104.112003
		
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			01 - Articolo su periodico

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