Light quark spectroscopy at the Fermilab antiproton accumulator

T. Armstrong; D. Bettoni; V. Bharadwaj; C. Biino; G. Borreani; D. Broemmelsiek; A. Buzzo; R. Calabrese; A. Ceccucci; R. Cester; M. Church; P. F. Dalpiaz; R. Dibenedetto; D. Dimitroyannis; M. G. Fabbri; J. Fast; A. Gianoli; C. Ginsburg; k. Gollwitzer; A. Hahn; M. A. Hasan; S. Hsueh; R. Lewis; E. Luppi; M. Macri; A. Majewska; M. Mandelkern; F. Marchetto; M. Marinelli; J. Marques; W. Marsh; M. Martini; M. Masuzawa; E. Menichetti; A. Migliori; R. Mussa; M. Pallavicini; S. Palestini; N. Pastrone; C. Patrignani; J. Peoples; L. Pesando; F. Petrucci; M. G. Pia; S. Pordes; P. Rapidis; R. Ray; J. Reid; G. Rinaudo; B. Roccuzzo; J. L. Rosen; A. Santroni; M. Sarmiento; M. Savrie; A. Scalisi; J. Schultz; K. K. Seth; A. Smith; G. A. Smith; M. Sozzi; S. Trokenheim; M. Weber; S. Werkema; Y. Zhang; J. L. Zhao; G. Zioulas

doi:10.1016/0375-9474(93)90382-8

Light quark spectroscopy at the Fermilab antiproton accumulator

T. Armstrong^*, D. Bettoni, V. Bharadwaj, C. Biino, G. Borreani, D. Broemmelsiek, A. Buzzo, R. Calabrese, A. Ceccucci, R. Cester, M. Church, P. F. Dalpiaz, R. Dibenedetto, D. Dimitroyannis, M. G. Fabbri, J. Fast, A. Gianoli, C. Ginsburg, k. Gollwitzer, A. HahnM. A. Hasan, S. Hsueh, R. Lewis, E. Luppi, M. Macri, A. Majewska, M. Mandelkern, F. Marchetto, M. Marinelli, J. Marques, W. Marsh, M. Martini, M. Masuzawa, E. Menichetti, A. Migliori, R. Mussa, M. Pallavicini, S. Palestini, N. Pastrone, C. Patrignani, J. Peoples, L. Pesando, F. Petrucci, M. G. Pia, S. Pordes, P. Rapidis, R. Ray, J. Reid, G. Rinaudo, B. Roccuzzo, J. L. Rosen, A. Santroni, M. Sarmiento, M. Savrie, A. Scalisi, J. Schultz, K. K. Seth, A. Smith, G. A. Smith, M. Sozzi, S. Trokenheim, M. Weber, S. Werkema, Y. Zhang, J. L. Zhao, G. Zioulas

^*Corresponding author for this work

Physics and Astronomy

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Abstract

Fermilab experiment E-760 has confirmed the f₂(1520) state in the 3π^o final state in antiproton-proton annihilations in-flight (~3.0 to 3.6 GeV c.m. energy), seen previously by Crystal Barrel and other groups at CERN at rest. The f₂(1520) is also seen in its 2π^o decay mode in the 2π^oη channel and 2η decay mode in the π^o2η channel. There are indications of this state in the 3η decay channel. The invariant mass spectrum is rich in states near 2 GeV, and amplitude and spin/parity analysis of the Dalitz plot is in progress in this mass region.

Original language	English (US)
Pages (from-to)	53-61
Number of pages	9
Journal	Nuclear Physics, Section A
Volume	558
Issue number	C
DOIs	https://doi.org/10.1016/0375-9474(93)90382-8
State	Published - Jun 7 1993

ASJC Scopus subject areas

Nuclear and High Energy Physics

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10.1016/0375-9474(93)90382-8

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Armstrong, T., Bettoni, D., Bharadwaj, V., Biino, C., Borreani, G., Broemmelsiek, D., Buzzo, A., Calabrese, R., Ceccucci, A., Cester, R., Church, M., Dalpiaz, P. F., Dibenedetto, R., Dimitroyannis, D., Fabbri, M. G., Fast, J., Gianoli, A., Ginsburg, C., Gollwitzer, K., ... Zioulas, G. (1993). Light quark spectroscopy at the Fermilab antiproton accumulator. Nuclear Physics, Section A, 558(C), 53-61. https://doi.org/10.1016/0375-9474(93)90382-8

@article{ed60b352dc1f438baa63234ea0ec177e,

title = "Light quark spectroscopy at the Fermilab antiproton accumulator",

abstract = "Fermilab experiment E-760 has confirmed the f2(1520) state in the 3πo final state in antiproton-proton annihilations in-flight (~3.0 to 3.6 GeV c.m. energy), seen previously by Crystal Barrel and other groups at CERN at rest. The f2(1520) is also seen in its 2πo decay mode in the 2πoη channel and 2η decay mode in the πo2η channel. There are indications of this state in the 3η decay channel. The invariant mass spectrum is rich in states near 2 GeV, and amplitude and spin/parity analysis of the Dalitz plot is in progress in this mass region.",

author = "T. Armstrong and D. Bettoni and V. Bharadwaj and C. Biino and G. Borreani and D. Broemmelsiek and A. Buzzo and R. Calabrese and A. Ceccucci and R. Cester and M. Church and Dalpiaz, {P. F.} and R. Dibenedetto and D. Dimitroyannis and Fabbri, {M. G.} and J. Fast and A. Gianoli and C. Ginsburg and k. Gollwitzer and A. Hahn and Hasan, {M. A.} and S. Hsueh and R. Lewis and E. Luppi and M. Macri and A. Majewska and M. Mandelkern and F. Marchetto and M. Marinelli and J. Marques and W. Marsh and M. Martini and M. Masuzawa and E. Menichetti and A. Migliori and R. Mussa and M. Pallavicini and S. Palestini and N. Pastrone and C. Patrignani and J. Peoples and L. Pesando and F. Petrucci and Pia, {M. G.} and S. Pordes and P. Rapidis and R. Ray and J. Reid and G. Rinaudo and B. Roccuzzo and Rosen, {J. L.} and A. Santroni and M. Sarmiento and M. Savrie and A. Scalisi and J. Schultz and Seth, {K. K.} and A. Smith and Smith, {G. A.} and M. Sozzi and S. Trokenheim and M. Weber and S. Werkema and Y. Zhang and Zhao, {J. L.} and G. Zioulas",

note = "Funding Information: The f#520) state has been observedi n reactions( 1) and (3). Its mass and width have been measuredfo r reaction( 1) and they agreew ith the acceptedv alues 171B. ecauseo f inter-ferencew ith others tatest he f (1520)d oesn ot show up clearly in the Dalitz plot for reaction (21,b ut one can see it in the 6. 4-0.6 slice in Cos(8 *). The samplef or reaction (4) is small, but one does seei ndications of f2(1 520)i n this channel.T he Dalitz plots for the above reactions have many interestion featuresa bove the f2(1520)p eak region, but the amplitude analysis (in progress)i s not straight-forwarda s many highero rderp artialw avesa rep resent. We gratefully acknowledget he technicals upportf rom our collaboratingi nstitutions and the outstandingc ontribution of the Fermilab AcceleratorD ivision Antiproton Department. This work was funded by the U.S. Departmento f Energy, the National ScienceF oundation, and the Italian Istituto Nazionale di Fisica Nucleare.",

year = "1993",

month = jun,

day = "7",

doi = "10.1016/0375-9474(93)90382-8",

language = "English (US)",

volume = "558",

pages = "53--61",

journal = "Nuclear Physics A",

issn = "0375-9474",

publisher = "Elsevier",

number = "C",

}

Armstrong, T, Bettoni, D, Bharadwaj, V, Biino, C, Borreani, G, Broemmelsiek, D, Buzzo, A, Calabrese, R, Ceccucci, A, Cester, R, Church, M, Dalpiaz, PF, Dibenedetto, R, Dimitroyannis, D, Fabbri, MG, Fast, J, Gianoli, A, Ginsburg, C, Gollwitzer, K, Hahn, A, Hasan, MA, Hsueh, S, Lewis, R, Luppi, E, Macri, M, Majewska, A, Mandelkern, M, Marchetto, F, Marinelli, M, Marques, J, Marsh, W, Martini, M, Masuzawa, M, Menichetti, E, Migliori, A, Mussa, R, Pallavicini, M, Palestini, S, Pastrone, N, Patrignani, C, Peoples, J, Pesando, L, Petrucci, F, Pia, MG, Pordes, S, Rapidis, P, Ray, R, Reid, J, Rinaudo, G, Roccuzzo, B, Rosen, JL, Santroni, A, Sarmiento, M, Savrie, M, Scalisi, A, Schultz, J, Seth, KK, Smith, A, Smith, GA, Sozzi, M, Trokenheim, S, Weber, M, Werkema, S, Zhang, Y, Zhao, JL & Zioulas, G 1993, 'Light quark spectroscopy at the Fermilab antiproton accumulator', Nuclear Physics, Section A, vol. 558, no. C, pp. 53-61. https://doi.org/10.1016/0375-9474(93)90382-8

TY - JOUR

T1 - Light quark spectroscopy at the Fermilab antiproton accumulator

AU - Armstrong, T.

AU - Bettoni, D.

AU - Bharadwaj, V.

AU - Biino, C.

AU - Borreani, G.

AU - Broemmelsiek, D.

AU - Buzzo, A.

AU - Calabrese, R.

AU - Ceccucci, A.

AU - Cester, R.

AU - Church, M.

AU - Dalpiaz, P. F.

AU - Dibenedetto, R.

AU - Dimitroyannis, D.

AU - Fabbri, M. G.

AU - Fast, J.

AU - Gianoli, A.

AU - Ginsburg, C.

AU - Gollwitzer, k.

AU - Hahn, A.

AU - Hasan, M. A.

AU - Hsueh, S.

AU - Lewis, R.

AU - Luppi, E.

AU - Macri, M.

AU - Majewska, A.

AU - Mandelkern, M.

AU - Marchetto, F.

AU - Marinelli, M.

AU - Marques, J.

AU - Marsh, W.

AU - Martini, M.

AU - Masuzawa, M.

AU - Menichetti, E.

AU - Migliori, A.

AU - Mussa, R.

AU - Pallavicini, M.

AU - Palestini, S.

AU - Pastrone, N.

AU - Patrignani, C.

AU - Peoples, J.

AU - Pesando, L.

AU - Petrucci, F.

AU - Pia, M. G.

AU - Pordes, S.

AU - Rapidis, P.

AU - Ray, R.

AU - Reid, J.

AU - Rinaudo, G.

AU - Roccuzzo, B.

AU - Rosen, J. L.

AU - Santroni, A.

AU - Sarmiento, M.

AU - Savrie, M.

AU - Scalisi, A.

AU - Schultz, J.

AU - Seth, K. K.

AU - Smith, A.

AU - Smith, G. A.

AU - Sozzi, M.

AU - Trokenheim, S.

AU - Weber, M.

AU - Werkema, S.

AU - Zhang, Y.

AU - Zhao, J. L.

AU - Zioulas, G.

N1 - Funding Information: The f#520) state has been observedi n reactions( 1) and (3). Its mass and width have been measuredfo r reaction( 1) and they agreew ith the acceptedv alues 171B. ecauseo f inter-ferencew ith others tatest he f (1520)d oesn ot show up clearly in the Dalitz plot for reaction (21,b ut one can see it in the 6. 4-0.6 slice in Cos(8 *). The samplef or reaction (4) is small, but one does seei ndications of f2(1 520)i n this channel.T he Dalitz plots for the above reactions have many interestion featuresa bove the f2(1520)p eak region, but the amplitude analysis (in progress)i s not straight-forwarda s many highero rderp artialw avesa rep resent. We gratefully acknowledget he technicals upportf rom our collaboratingi nstitutions and the outstandingc ontribution of the Fermilab AcceleratorD ivision Antiproton Department. This work was funded by the U.S. Departmento f Energy, the National ScienceF oundation, and the Italian Istituto Nazionale di Fisica Nucleare.

PY - 1993/6/7

Y1 - 1993/6/7

N2 - Fermilab experiment E-760 has confirmed the f2(1520) state in the 3πo final state in antiproton-proton annihilations in-flight (~3.0 to 3.6 GeV c.m. energy), seen previously by Crystal Barrel and other groups at CERN at rest. The f2(1520) is also seen in its 2πo decay mode in the 2πoη channel and 2η decay mode in the πo2η channel. There are indications of this state in the 3η decay channel. The invariant mass spectrum is rich in states near 2 GeV, and amplitude and spin/parity analysis of the Dalitz plot is in progress in this mass region.

AB - Fermilab experiment E-760 has confirmed the f2(1520) state in the 3πo final state in antiproton-proton annihilations in-flight (~3.0 to 3.6 GeV c.m. energy), seen previously by Crystal Barrel and other groups at CERN at rest. The f2(1520) is also seen in its 2πo decay mode in the 2πoη channel and 2η decay mode in the πo2η channel. There are indications of this state in the 3η decay channel. The invariant mass spectrum is rich in states near 2 GeV, and amplitude and spin/parity analysis of the Dalitz plot is in progress in this mass region.

UR - http://www.scopus.com/inward/record.url?scp=43949167053&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=43949167053&partnerID=8YFLogxK

U2 - 10.1016/0375-9474(93)90382-8

DO - 10.1016/0375-9474(93)90382-8

M3 - Article

AN - SCOPUS:43949167053

SN - 0375-9474

VL - 558

SP - 53

EP - 61

JO - Nuclear Physics A

JF - Nuclear Physics A

IS - C

ER -

Light quark spectroscopy at the Fermilab antiproton accumulator

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