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Nonlocal condensates and QCD sum rules for the pion wave function

Journal Article · · Physical Review, D (Particles Fields); (United States)
 [1];  [2]
  1. Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, Dubna (Russia) Rostov State University, Rostov on Don (Russia)
  2. Continuous Electron Beam Accelerator Facility, Newport News, Virginia 23606 (United States) Laboratory of Theoretical Physics, Joint Institute for Nuclear Research, Dubna (Russia)

The QCD-sum-rule calculation of the pion wave function by Chernyak and Zhitnitsky (CZ) implicitly assumes that the correlation length of vacuum fluctuations is large compared to the typical hadronic scale {similar to}1/{ital m}{sub {rho}}, so that one can substitute the original nonlocal objects such as {l angle}{ital {bar q}}(0){ital q}({ital z}){r angle} by constant {l angle}{ital {bar q}}(0){ital q}(0){r angle}-type values. We outline a formalism enabling one to work directly with the nonlocal condensates, and construct a modified sum rule for the moments {l angle}{xi}{sup {ital N}}{r angle} of the pion wave function. The results are rather sensitive to the value of the parameter {lambda}{sub {ital q}}{sup 2}={l angle}{ital {bar q}D}{sup 2}{ital q}{r angle}/{l angle}{ital {bar q}q}{r angle} specifying the average virtuality of the vacuum quarks. Varying it from the most popular value {lambda}{sub {ital q}}{sup 2}=0.4 GeV{sup 2} up to the value {lambda}{sub {ital q}}{sup 2}=1.2 GeV{sup 2} suggested by the instanton-liquid model, we obtain {l angle}{xi}{sup 2}{r angle}=0.25--0.20, to be compared to the CZ value {l angle}{xi}{sup 2}{r angle}=0.43 obtained with {lambda}{sub {ital q}}{sup 2}=0.

DOE Contract Number:
AC05-84ER40150
OSTI ID:
7235215
Journal Information:
Physical Review, D (Particles Fields); (United States), Journal Name: Physical Review, D (Particles Fields); (United States) Vol. 45:5; ISSN PRVDA; ISSN 0556-2821
Country of Publication:
United States
Language:
English