Bose-Einstein correlations in e/sup +/e/sup -/ collisions [electronic resource].
- Published
- Berkeley, Calif. : Lawrence Berkeley National Laboratory, 1987.
Oak Ridge, Tenn. : Distributed by the Office of Scientific and Technical Information, U.S. Dept. of Energy. - Physical Description
- Pages: 168 : digital, PDF file
- Additional Creators
- Lawrence Berkeley National Laboratory and United States. Department of Energy. Office of Scientific and Technical Information
Access Online
- Restrictions on Access
- Free-to-read Unrestricted online access
- Summary
- The MARK II detector is used to study the Bose-Einstein correlation between pairs and triplets of charged pions produced in hadronic decays of the J)psi), the ..sqrt..s = 4 to 7 GeV continuum above the J)psi), two photon events at ..sqrt..s = 29 GeV, and e/sup )plus/)e/sup )minus/) annihilation events at ..sqrt..s = 29 GeV as a function of Q/sup 2/, the four-momentum transfer squared. After corrections for Coulomb effects and pion misidentification, we find a nearly full Bose-Einstein enhancement ..cap alpha.. in the J)psi) and the two photon data and about half the maximum value in the other two data sets. The radius parameter )tau)(an average over space and time) given by pion pair analyses lies within a band of +-0.10 fm around 0.73 fm and is the same, within errors, for all four data sets. Pion triplet analyses also give a consistent radius of approx. 0.54 fm. fits to two-dimensional distributions R(q/sub T//sup 2/, q/sub C//sup 2/) of invariant components of Q/sup 2/ = q/sub T//sup 2/ )plus) q/sub C//sup 2/ give )tau)/sub T/ approx. )tau)C approx. )tau), where q/sub T/ is the transverse three-momentum difference calculated with respect to the net pair three-momentum, and q/sub C/ is in effect the longitudinal three-momentum difference in the pion pair rest frame. When q/sub T/ is calculated with respect to the jet axis for two-jet events in the e/sup )plus/)e/sup )minus/) annihilation data at ..sqrt..s = 29 GeV, a fit to R(q/sub T//sup 2/, q/sub C//sup 2/) also gives )tau)/sub T/ approx. )tau)/sub C/ approx. )tau). Noting that q/sub L/ and q/sub 0/ are not invariant, we make fits to R(/sub T//sup T/, q/sub L//sup 2/) and to R(q/sub T//sup 2/, q/sub 0//sup 2/) (Kopylov formulation), and we find )tau)/sub 0/ approx. )tau)/sub L/ approx. )23))tau)/sub T/ to )12))tau)/sub T/. 44 refs., 43 figs., 15 tabs
- Report Numbers
- E 1.99:lbl-24493
lbl-24493 - Subject(s)
- Other Subject(s)
- Electron-Positron Interactions
- Correlation Functions
- Pions
- Pair Production
- Bose-Einstein Statistics
- Data Analysis
- Distribution
- Drift Chambers
- J Psi-3097 Mesons
- Longitudinal Momentum
- Measuring Methods
- Pion Detection
- Transverse Momentum
- Bosons
- Charged Particle Detection
- Charmonium
- Detection
- Elementary Particles
- Functions
- Hadrons
- Interactions
- Lepton-Lepton Interactions
- Linear Momentum
- Measuring Instruments
- Mesons
- Multiwire Proportional Chambers
- Particle Interactions
- Proportional Counters
- Pseudoscalar Mesons
- Quarkonium
- Radiation Detection
- Radiation Detectors
- Vector Mesons
- Note
- Published through SciTech Connect.
12/01/1987.
"lbl-24493"
"DE88008207"
Juricic, I. - Funding Information
- AC03-76SF00098
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