QUARK STRUCTURE OF THE PION AND PION FORM-FACTOR

被引:60
作者
ANISOVICH, V [1 ]
MELIKHOV, D [1 ]
NIKONOV, V [1 ]
机构
[1] MOSCOW MV LOMONOSOV STATE UNIV,INST NUCL PHYS,MOSCOW,RUSSIA
来源
PHYSICAL REVIEW D | 1995年 / 52卷 / 09期
关键词
D O I
10.1103/PhysRevD.52.5295
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
We consider the pion structure in the region of low and moderately high momentum transfers: at low Q(2), the pion is treated as a composite system of constituent quarks; at moderately high momentum transfers, Q(2) = 10-25 GeV2, the pion form factor is calculated within perturbative QCD taking into account one-gluon hard exchange. Using the data on the pion form factor at Q(2) < 3 GeV2 and the pion axial-vector decay constant, we reconstruct the pion wave function in the soft and intermediate regions. This very wave function combined with the one-gluon hard scattering amplitude allows a calculation of the pion form factor in the hard region Q(2) = 10-25 GeV2. A specific feature of the reconstructed pion wave function is a quasizone character of the q ($) over bar q excitations. On the basis of the obtained pion wave function and the data on deep inelastic scattering off the pion, the valence quark distribution in a constituent quark is determined.
引用
收藏
页码:5295 / 5307
页数:13
相关论文
共 38 条
[1]   A MEASUREMENT OF THE SPACE-LIKE PION ELECTROMAGNETIC FORM-FACTOR [J].
AMENDOLIA, SR ;
ARIK, M ;
BADELEK, B ;
BATIGNANI, G ;
BECK, GA ;
BEDESCHI, F ;
BELLAMY, EH ;
BERTOLUCCI, E ;
BETTONI, D ;
BILOKON, H ;
BOLOGNA, G ;
BOSISIO, L ;
BRADASCHIA, C ;
BUDINICH, M ;
CODINO, A ;
DELLORSO, M ;
PIAZZOLI, BD ;
ENORINI, M ;
FABBRI, FL ;
FIDECARO, F ;
FOA, L ;
FOCARDI, E ;
FRANK, SGF ;
GIAZOTTO, A ;
GIORGI, MA ;
GREEN, MG ;
HARVEY, J ;
HEATH, GP ;
LANDON, MPJ ;
LAURELLI, P ;
LIELLO, F ;
MANNOCCHI, G ;
MARCH, PV ;
MARROCCHESI, PS ;
MENZIONE, A ;
MERONI, E ;
MORONI, L ;
MILOTTI, E ;
PICCHI, P ;
RAGUSA, F ;
RISTORI, L ;
ROLANDI, L ;
SALA, S ;
SALTMARSH, CG ;
SAOUCHA, A ;
SATTA, L ;
SCRIBANO, A ;
SPILLANTINI, P ;
STEFANINI, A ;
STOREY, D .
NUCLEAR PHYSICS B, 1986, 277 (01) :168-196
[2]   WARD IDENTITIES AND SUM-RULES FOR COMPOSITE SYSTEMS DESCRIBED IN THE DISPERSION-RELATION TECHNIQUE - THE DEUTERON AS A COMPOSITE 2-NUCLEON SYSTEM [J].
ANISOVICH, VV ;
KOBRINSKY, MN ;
MELIKHOV, DI ;
SARANTSEV, AV .
NUCLEAR PHYSICS A, 1992, 544 (3-4) :747-792
[3]   THE BETHE-SALPETER-EQUATION AND THE DISPERSION-RELATION TECHNIQUE [J].
ANISOVICH, VV ;
MELIKHOV, DI ;
METSCH, BC ;
PETRY, HR .
NUCLEAR PHYSICS A, 1993, 563 (04) :549-583
[4]  
BADIER J, 1983, Z PHYS C PART FIELDS, V18, P281, DOI 10.1007/BF01573728
[5]   ELECTROPRODUCTION OF SINGLE PIONS AT LOW EPSILON AND A MEASUREMENT OF PION FORM-FACTOR UP TO Q2 = 10 GEV2 [J].
BEBEK, CJ ;
BROWN, CN ;
HOLMES, SD ;
KLINE, RV ;
PIPKIN, FM ;
RAITHER, S ;
SISTERSON, LK ;
BROWMAN, A ;
HANSON, KM ;
LARSON, D ;
SILVERMAN, A .
PHYSICAL REVIEW D, 1978, 17 (07) :1693-1705
[6]   DETERMINATION OF PION FORM-FACTOR UP TO Q2 = 4 GEV2 FROM SINGLE-CHARGED-PION ELECTROPRODUCTION [J].
BEBEK, CJ ;
BROWN, CN ;
HERZLINGER, M ;
HOLMES, SD ;
LICHTENSTEIN, CA ;
PIPKIN, FM ;
RAITHER, S ;
SISTERSON, LK .
PHYSICAL REVIEW D, 1976, 13 (01) :25-42
[7]  
BERESTETSKII VB, 1977, SOV J NUCL PHYS+, V25, P347
[8]  
BERESTETSKII VB, 1976, J NUCL PHYS, V24, P106
[9]   SOFT CONTRIBUTION TO THE PION FORM-FACTOR FROM LIGHT-CONE QCD SUM-RULES [J].
BRAUN, V ;
HALPERIN, I .
PHYSICS LETTERS B, 1994, 328 (3-4) :457-465
[10]  
Brodsky S. J., 1989, PERTURBATIVE QUANTUM, P93