- Juricic, I;
- Goldhaber, G;
- Gidal, G;
- Abrams, G;
- Amidei, D;
- Baden, AR;
- Boyer, J;
- Butler, F;
- Carithers, WC;
- Gold, MS;
- Golding, L;
- Haggerty, J;
- Herrup, D;
- Kadyk, JA;
- Levi, ME;
- Nelson, ME;
- Rowson, PC;
- Schellman, H;
- Schmidke, WB;
- Sheldon, PD;
- Trilling, GH;
- Wood, DR;
- Barklow, T;
- Boyarski, A;
- Breidenbach, M;
- Burchat, P;
- Burke, DL;
- Cords, D;
- Dorfan, JM;
- Feldman, GJ;
- Gladney, L;
- Hanson, G;
- Hayes, K;
- Hitlin, DG;
- Hollebeek, RJ;
- Innes, WR;
- Jaros, JA;
- Karlen, D;
- Klein, SR;
- Lankford, AJ;
- Larsen, RR;
- LeClaire, BW;
- Lockyer, NS;
- Lüth, V;
- Ong, RA;
- Perl, ML;
- Richter, B;
- Riles, K;
- Ross, MC;
- Schindler, RH;
- Yelton, JM;
- Schaad, T;
- Schwitters, RF
Four data sets collected with the Mark II detector during its operation at the SPEAR and PEP e+e- storage rings at SLAC are used to study the Bose-Einstein correlation between pairs and triplets of like-sign charged pions. The data sets represent four different regions of energy available for hadron production: the J at s =3.095 GeV, typical hadronic energy of 5 GeV in two-photon events, and annihilation in the energy regions s =47 GeV above the J, and s =29 GeV. The Bose-Einstein correlation is studied as a function of Q2, the four-momentum difference squared of the pair, and of Q32, an analogous quantity defined for triplets. After corrections for Coulomb effects and pion misidentification, pair analyses indicate a nearly full Bose-Einstein enhancement (1) in the J and the two-photon data, and about half the maximum value in the two higher-energy data sets. The pair analysis parameter r lies within a band of ±0.1 fm around 0.7 fm and is essentially the same for all four data sets. Pion triplet analyses give consistent results for the triplet parameters 3 and r3. In an attempt to investigate the shape of the pion source, we also study the Bose-Einstein correlation in pion pairs using two-dimensional distributions in components of Q2. © 1989 The American Physical Society.