2006
DOI: 10.1016/j.cpc.2006.06.004
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Solving constrained Markovian evolution in QCD with the help of the non-Markovian Monte Carlo

Abstract: We present the constrained Monte Carlo (CMC) algorithm for the QCD evolution. The constraint resides in that the total longitudinal energy of the emissions in the MC and in the underlying QCD evolution is predefined (constrained). This CMC implements exactly the full DGLAP evolution of the parton distributions in the hadron with respect to the logarithm of the energy scale. The algorithm of the CMC is referred to as the non-Markovian type. The non-Markovian MC algorithm is defined as the one in which the multi… Show more

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Cited by 23 publications
(43 citation statements)
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References 25 publications
(33 reference statements)
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“…In this sense, it is close in spirit to the works in refs. [43][44][45][46][47][48][49][50][51], in refs. [52][53][54][55][56][57][58], and in refs.…”
Section: Jhep01(2018)070mentioning
confidence: 99%
“…In this sense, it is close in spirit to the works in refs. [43][44][45][46][47][48][49][50][51], in refs. [52][53][54][55][56][57][58], and in refs.…”
Section: Jhep01(2018)070mentioning
confidence: 99%
“…In addition, our new CMCs will not only generalize the solutions of ref. [8], but will be described in such a way that any future extension to other types of evolution kernels will be rather easy. In the following sub-chapters we shall present the details of our generalized solutions in detail.…”
Section: Constrained Monte Carlo For Pure Bremsstrahlungmentioning
confidence: 99%
“…[8] the first CMC algorithm of the class I was found and tested for DGLAP kernel, that is for our case (A). This algorithm is based on the observation that for the product of steeply rising functions, proportional to 1/y i , the δ-function constraint is effectively resolved by a single (let's say) y k , while all other y i , can be considered as unconstrained.…”
Section: Constrained Monte Carlo For Pure Bremsstrahlungmentioning
confidence: 99%
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