Unparticle as a field with continuously distributed mass

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We point out that the notion of an unparticle, recently introduced by Georgi, can be interpreted as a particular case of a field with continuously distributed mass considered in ref.\cite{14}. We also point out that the simplest renormalizable extension of the $SU_c(3)\otimes SU_L(2)\otimes U(1)$ Standard Model is the extension with the replacement of the U(1) gauge propagator $\frac{1}{k^2} \to \frac{1}{k^2} + \int _0^{\infty}\frac{ρ(t)}{-t+k^2 +iε}dt$ with $\int_0^{\infty}ρ(t)dt < \infty $.
6 pages, added references, corrected typos

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