Universality of the form factors and the structure functions in the dynamical resonance model
Author:
Publisher
Springer Science and Business Media LLC
Subject
General Medicine
Link
http://link.springer.com/content/pdf/10.1007/BF02747865.pdf
Reference32 articles.
1. A. Niégawa:Progr. Theor. Phys.,48, 513 (1972).
2. K. Kikkawa andH. Sato:Phys. Lett.,32 B, 280 (1970) (Erratum:33 B, 540 (1970));Progr. Theor. Phys.,45, 475 (1971).
3. The scaling functions are the functionsF 1,F 2 andF 3,e.g. F 1≡2mW 1,F 2≡νW 2, etc. (see ref. (4)). The definition ofW 2 in ref. (1) is given by an equation similar to (9) and the equation below (13) of this note. The usual scaling variableω is defined above (12).
4. J. Iizuka, M. Kobayashi andH. Nitto:Progr. Theor. Phys.,45, 482 (1971);J. Iizuka:Soryushiron Kenkyu (mimeographed circular in Japanese),43, A 78 (1971);J. Iizuka, M. Kobayashi andH. Nitto:Progr. Theor. Phys.,46, 1170 (1971).
5. The representative function is defined as the scaling functionF 2(ω) divided by a purely numerical counting factor (theSU 3 factor multiplied by a constant) (4). This function then has noSU 3 dependence as was proved in ref. (4,1). (See also the next paragraph.)
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