2007
DOI: 10.1103/physrevc.76.065203
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Simple parameterization of nuclear attenuation data

Abstract: Based on the nuclear attenuation data obtained by the HERMES experiment on nitrogen and krypton nuclei, it is shown that the nuclear attenuation R h M can be parametrised in a form of a linear polynomial P1 = a11 + τ a12, where τ is the formation time, which depends on the energy of the virtual photon ν and fraction of that energy z carried by the final hadron. Three widely known parameterizations for τ were used for the performed fit. The fit parameters a11 and a12 do not depend on ν and z.

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Cited by 11 publications
(16 citation statements)
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“…The wealth of theoretical model calculations and studies [18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35] reflect the strong interest of the community in hadron-multiplicities on nuclei, as they provide information on the space (time) structure of the hadronization process. It is beyond the scope of this paper to compare the results of the various models with the data.…”
Section: Introductionmentioning
confidence: 99%
“…The wealth of theoretical model calculations and studies [18][19][20][21][22][23][24][25][26][27][28][29][30][31][32][33][34][35] reflect the strong interest of the community in hadron-multiplicities on nuclei, as they provide information on the space (time) structure of the hadronization process. It is beyond the scope of this paper to compare the results of the various models with the data.…”
Section: Introductionmentioning
confidence: 99%
“…where n exp and n par are numbers of experimental points and parameters; R h M (theor) is the theoretical value for ratio at given point; (15). In version with τ c (4) ( Table 2) for each choice of σ str we have approximately equal values ofχ 2 for NDFs from (15) and (16).…”
Section: Details Of Fit and Resultsmentioning
confidence: 99%
“…2 Fit of version with τ c (4) can depend from the standard Lund model parameter C. The widely using value of this parameter is C = 0.3 [32]. For study the dependence of fit from this parameter we performed three parametric fit with τ c (4), σ str (10), NDF from (15). As parameters serve σ q , parameter c, and Lund parameter C, which in our fit can changes in limits 0.2 ≤ C ≤ 0.5.…”
Section: Details Of Fit and Resultsmentioning
confidence: 99%
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“…[7][8][9][10][11][12] and references therein. It is beyond the scope of this report to compare the results of the various models with the data.…”
Section: Pos(dis 2010)119mentioning
confidence: 99%