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Title: Light-front wave functions of vector mesons in an algebraic model

Journal Article · · Physical Review. D.
 [1];  [2]; ORCiD logo [3]; ORCiD logo [4];  [4]; ORCiD logo [5]
  1. University of Sonora (Mexico); Pablo de Olavide University (Spain)
  2. University of Sonora (Mexico)
  3. Michoacan Univ. of San Nicolas de Hidalgo, Morelia (Mexico); Thomas Jefferson National Accelerator Facility (TJNAF), Newport News, VA (United States)
  4. University of Huelva (Spain)
  5. Pablo de Olavide University (Spain)

Inspired by the recent development of an algebraic model which provides an adequate and unified description of the internal structure of the lowest-lying pseudo-scalar mesons, belonging both to the light quarks sector and to the one of heavy quarks, we perform its first extension to the vector-meson case. The algebraic model describes meson's structure in terms of the spectral density function that appears in a Nakanishi integral representation of the covariant quark-antiquark bound-state amplitude, \emph{i.e.}, the Bethe-Salpeter amplitude. We compute the leading-twist light-front wave functions of the $$\rho(770)$$, $$\phi(1020)$$, $$J/\psi$$ and $$\Upsilon(1S)$$ mesons through their connection with the parton distribution amplitudes. Among the results we present, the following are of particular interest: (i) transverse light-front wave functions can be obtained algebraically from the corresponding parton distribution amplitudes, whereas that is not the case for longitudinal light-front wave functions, which requires an intermediate step where a spectral density function must be derived from the particular parton distribution amplitude; (ii) the derived spectral density functions show marked differences between light and heavy vector mesons, the latter being narrower as compared to the former; these are also non-positive definite, although the integral over the entire curve is larger than zero as expected; and (iii) the longitudinal and transverse light-front wave functions of vector mesons with light quark content exhibit steep $$x$$- and $$p_\perp^2$$-dependence, while those of the $$J/\psi$$ and $$\Upsilon(1S)$$ mesons are characterized by narrow distributions in the $$x$$-range but, comparatively, much more gradual fall-offs with respect to the $$p_\perp^2$$-range depicted.

Research Organization:
Thomas Jefferson National Accelerator Facility (TJNAF), Newport News, VA (United States)
Sponsoring Organization:
USDOE Office of Science (SC), Nuclear Physics (NP); USDOE
Grant/Contract Number:
AC05-6OR23177
OSTI ID:
1971552
Alternate ID(s):
OSTI ID: 1971776
Report Number(s):
JLAB-THY-23-3779; arXiv:2303.09581; DOE/OR/23177-5788; TRN: US2313719
Journal Information:
Physical Review. D., Vol. 107, Issue 7; ISSN 2470-0010
Publisher:
American Physical Society (APS)Copyright Statement
Country of Publication:
United States
Language:
English

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