In this paper we found the multiplicity distribution of the produced gluons in deep inelastic scattering at large z=ln ( Q²ₛ/Q²) \,\, \,\,1 z = ln Q s 2 / Q 2 ≫ 1 where Qₛ Q s is the saturation momentum and Q² Q 2 is the photon virtuality. It turns out that this distribution at large n > n̄ n > n ¯ almost reproduces the KNO scaling behaviour with the average number of gluons n̄ ∝ exp ( z²/2 κ ) n ¯ ∝ exp z 2 / 2 κ , where κ = 4.88 κ = 4.88 in the leading order of perturbative QCD. The KNO function Ψ ( nn̄) = exp ( -\,n/n̄) Ψ n n ¯ = exp - n / n ¯ . For n < n̄ n < n ¯ we found that σ ₙ ∝ ( z - √2 \,κ \,ln (n-1) )/(n-1) σ n ∝ ( z - 2 κ ln ( n - 1 ) ) / ( n - 1 ) . Such small n determine the value of entropy of produced gluons SE = 0.3\, z²/(2\,κ ) S E = 0.3 z 2 / ( 2 κ ) at large z . The factor 0.3 stems from the non-perturbative corrections that provide the correct behaviour of the saturation momentum at large b .
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E. Levin (2024) studied this question.
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