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It is shown that there is a second properly normalized KNO scaling function, , which has certain advantages in the analysis of KNO scaling. First, the are not influenced by the statistical and systematic uncertainties of hence provides more selective power than the original KNO scaling function . Second, the new scaling function generates scale parameter since it depends only on the combination of and the scale parameter of . An analysis of is given using annihilation data for charged particle multiplicity distributions.

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