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Prog. Theor. Phys. Vol. 12 No. 1 (1954) pp. 94-98
On the Effective Hamiltonian for Pseudoscalar Meson with Pseudoscalar Coupling with Nucleon
Tomoya Akiba and
Katuro Sawada*
Department of Physics, Tohoku University
*Tokyo University
(Received April 15, 1954)
Abstract:
The method of canonical transformation is applied to the pseudo-scalar meson theory with pseudoscalar coupling. It well be shown that the Tani-Foldy transformation results as the best one when regarded as a variational function among the similar family of transformation. The resulting Hamiltonian was ordered assuming some cut-off for the virtual meson momentum, and performing the mass renormalization. This Hamiltonian shows a good tendency to account for the S-phase shifts for the nucleon π-meson scattering; the L-S coupling (τ·φ×π) in the isotopic spin space, which is positive for the T=3/2 state and negative for the T=1/2 state, becomes twice as large as obtained by the perturbation theory.
URL :
http://ptp.ipap.jp/link?PTP/12/94/
DOI : 10.1143/PTP.12.94
References:
- S. Tani, Prog. Theor. Phys. 6 (1950), 267[PTP].
-
L. L. Foldy, Wouthuysen, Phys. Rev. 78 (1950), 29[APS].
- The similar effective Hamiltonian for the Dyson transformation was obtained by
S. D. Drell and E. M. Henley, Phys. Rev. 88 (1952), 1053[APS].
- We take natural units, c=1, \hbar=1.
- Here we take, for simplicity, as arguments of the function f, the form (φ2)v2.
- The expression π·f(φ) mesons ½{π,f(φ)}+ and its vacuum expectation value <½{π, f(φ)}+>=0.
- <φ2>0 means <φi2>0 with i any one of 1, 2, 3, φ2=φ12+φ22+φ32..
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