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We show that the cross section of the diffractive production of $b \bar b$can be described as the sum of two contributions: the first is proportional tothe probability of finding a small size $b \bar b$ color dipole in the fasthadron wave function before the interaction with a target, while the second isthe $b \bar b$-production after or during the interaction with the target. Theformulae are presented as well as the discussion of the interralation betweenthese two contributions and the Ingelman- Schlein and coherent diffractionmechanisms. The main precdition is that the coherent diffraction mechanismdominates at least at the Tevatron Energies, giving the unique possibility tostudy it experimentally.Comment: 23 pages, 10 figures, latex fil

physical review. d. particles, fields, gravitation, and cosmology/physical review. d. particles and fields

Diffractive production of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>b</mml:mi><mml:mrow><mml:mrow><mml:mover><mml:mrow><mml:mi>b</mml:mi></mml:mrow><mml:mrow><mml:mi>¯</mml:mi></mml:mrow></mml:mover></mml:mrow></mml:mrow></mml:math>in proton-antiproton collisions at the Fermilab Tevatron

Diffractive production ofbb¯in proton-antiproton collisions at the Fermilab Tevatron