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Formation of delta(980) and A2(1320) in photon-photon collisions

D. Antreasyan, D. Aschman, D. Besset, J. K. Bienlein, E. D. Bloom, I. Brock, R. Cabenda, A. Cartacci, M. Cavalli-Sforza et al.

R. Clare, G. Conforto, S. Cooper, R. Cowan, D. Coyne, G. Drews, A. Engler, G. Folger, A. Fridman, J. Gaiser, D. Gelphman, G. Godfrey, F. H. Heimlich, R. Hofstadter, J. Irion, Z. Jakubowski, S. Keh, H. Kilian, I. Kirkbride, T. Kloiber, W. Koch, A. C. König, K. Königsmann, R. W. Kraemer, R. Lee, S. Leffler, R. Lekebusch, P. Lezoch, A. M. Litke, W. Lockman, S. Lowe, B. Lurz, D. Marlow, W. Maschmann, T. Matsui, P. McBride, F. Messing, W. J. Metzger, B. Monteleoni, R. Nernst, C. Newman-Holmes, B. Niczyporuk, G. Nowak, C. Peck, P. G. Pelfer, B. Pollock, F. C. Porter, D. Prindle, P. Ratoff, B. Renger, C. Rippich, M. Scheer, P. Schmitt, M. Schmitz, J. Schotanus, A. Schwarz, D. Sievers, T. Skwarnicki, K. Strauch, U. Strohbusch, J. Tompkins, H. -J. Trost, R. T. Van de Walle, H. Vogel, U. Volland, K. Wachs, K. Wacker, W. Walk, H. Wegener, D. Williams, and P. Zschorsch

  • California Institute of Technology, Pasadena, California 91125
  • University of Cape Town, Cape Town, South Africa
  • Carnegie-Mellon University, Pittsburgh, Pennsylvania 15213
  • Cracow Institute of Nuclear Physics, Cracow, Poland
  • Deutsches Elektronen Synchrotron DESY, Hamburg, Germany
  • Universitat Erlangen-Nürnberg, Erlangen, Germany
  • INFN and University of Firenze, Italy
  • Universitat Hamburg, I. Institut für Experimentalphysik, Hamburg, Germany
  • Harvard University, Cambridge, Massachusetts 02138
  • University of Nijmegen and NIKHEF-Nijmegen, The Netherlands
  • Princeton University, Princeton, New Jersey 08544
  • Department of Physics, HEPL, and Stanford Linear Accelerator Center, Stanford University, Stanford, California 94305
  • Universitat Würzburg, Würzburg, Germany ?Crystal Ball Collaboration)

Phys. Rev. D 33, 1847 – Published 1 April, 1986

DOI: https://doi.org/10.1103/PhysRevD.33.1847

Abstract

The reaction γγ→π0η has been investigated with the Crystal Ball detector at the DESY storage ring DORIS II. Formation of δ(980) and A2(1320) has been observed with γγ partial widths Γγγ(A2)=1.14±0.20±0.2 6 keV and Γγγ(δ)B(δ→πη)=0.19±0.07 0.07+0.10 keV.

References (19)

  1. Crystal Ball Collaboration, C. Edwards et al., Phys. Lett. 110 B, 82 (1982).
  2. Crystal Ball Collaboration, M. Oreglia et al., Phys. Rev. D 25, 2259 (1982); M. Oreglia, Ph.D. thesis, Stanford University, Report No. SLAC-236, 1980; J. Gaiser, Ph.D. thesis, Stanford University, Report No. SLAC-255, 1982.
  3. Particle Data Group, Rev. Mod. Phys. 56, S1 (1984).
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  6. σ γγ>R>πη(W)=8 π (2L+1) Γ γγ(R)B(R -> π η ) ΓR/ [(mR 2-W2)2 + mR ΓR2 2] with R= delta or A2 and L=0 or 2, respectively. We have used the following energy-dependent total width: ΓR(W)= ΓR(mR) (q/q0) 2L+1 DL(q0r)/DL(qr), where q is the pi momentum in the π eta rest frame and q0 is the same calculated for W=mR. DL is the Blatt-Weisskopf-barrier-penetration function. The interaction length r is set to 1 fm (Ref. 10).
  7. The large error is caused by our mass resolution being comparable to the natural linewidth.
  8. The sum of fractions was constrained to be equal to 1 in the fit, thus the errors are strongly correlated.
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  19. Γ γγ(A2)/mA2 3: Γ γγ (f) /mf3: Γ γγ (f prime )/ mfprime 3=3: (sintheta + sqrt 8 cos θ )2: ( sqrt 8 sin θ - cos θ )2, where theta is the singlet-octet mixing angle (Ref. 10).

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