Quick Search:
Prog. Theor. Phys. Vol. 44 No. 5 (1970) pp. 1317-1339
The Reggeization of the Bethe-Salpeter Scattering Amplitudes
Hideki Matsumoto
Institute of Physics, College of General Education, University of Tokyo, Meguro-ku, Tokyo
(Received June 11, 1970)
Abstract:
The Reggeization of the Bethe-Salpeter amplitude is investigated with general kernels. Assuming some integral representations for the interaction kernels and the modified propagator of the scattering particles with unequal masses, we obtain a sufficient condition for the kernels to be of the Hilbert-Schmidt type. Provided that this condition is satisfied, we prove the following, by studying the meromorphy domain of the partial-wave amplitudes:
1) the Sommerfeld-Watson transformation can be performed,
2) the asymptotic behavior of the leading trajectory as s →-∞ (s: total mass squared) is determined by the rightmost fixed singularity of the kernels, and
3) if the spectral functions of the integral representations are non-negative definite, the derivative of the largest eignvalue µMax(s, l) = {λMin(s, l)}-1 with respect to the angular momentum l is negative for s < 0 and l > -1, and the leading trajectory is real for s < 0 and is nondegenerate.
URL :
http://ptp.ipap.jp/link?PTP/44/1317/
DOI : 10.1143/PTP.44.1317
References:
-
E. E. Salpeter and H. A. Bethe, Phys. Rev. 84 (1951), 1232[APS].
G. C. Wick, Phys. Rev. 96 (1954), 1124[APS].
R. E. Cutkosky, Phys. Rev. 96 (1954), 1135[APS].
-
B. W. Lee and R. F. Sawyer, Phys. Rev. 127 (1962), 1832[APS].
-
G. Tiktopoulos, Phys. Rev. 133 (1964), B1231[APS].
- H. Abe, G. Konishi and T. Ogimoto, Prog. Theor. Phys. 32 (1964), 348[PTP].
-
J. Kwiecinski and P. Suranyi, Phys. Lett. 9 (1964), 283[CrossRef].
-
J. D. Bjorken, J. Math. Phys. 5 (1964), 192[CrossRef].
-
P. Suranyi, Phys. Lett. 6 (1963), 59[CrossRef]; Doklady Akad. Nauk SSSR 154 (1964), 312 [Sov. Phys.-Doklady 9 (1964), 66].
-
M. Baker and I. J. Muzinich, Phys. Rev. 132 (1963), 2291[APS].
M. K. Banerjee, M. Kulger, C. A. Levinson and I. J. Muzinich, Phys. Rev. 137 (1965), B1280[APS].
- C. Cosenza, L. Sertorio and M. Toller, Nuovo Cim. 31 (1964), 1084; ibid. 35 (1965), 913.
- M. Martinis, Commun. Math. Phys. 6 (1965), 136.
A. P. Contogouris, Nuovo Cim. 36 (1965), 230.
- N. Nakanishi, Prog. Theor. Phys. Suppl. No. 43 (1969).
-
For the discussions by the use of integral representations, see N. Nakanishi, Phys. Rev. 133 (1964), B214[APS];
ibid. 133 (1964), B1224[APS].
- M. Ida, Prog. Theor. Phys. 43 (1970), 84[PTP]; ibid. 43 (1970), 808[PTP].
- N. Nakanishi, Graph Theory and Feynman Integrals (Preprint, 1968), Chap. 4; Prog. Theor. Phys. Suppl. No. 18 (1961), 1[PTP]; Prog. Theor. Phys. 26 (1961), 337[PTP]; ibid. 26 (1961), 927[PTP].
- The latter in reference 9), Appendix A.
- F. Smithies, Integral Equations (Cambridge University Press, Cambridge, 1958), Chap. 6.
- A. C. Zaanen, Linear Analysis (North-Holland Pub. Co., Amsterdam, 1964), Chap. 9, 11, 12 and 13.
- F. Riesz and B. Sz-Nagy, Functional Analysis (Frederick Ungar Pub. Co., New York, 1965), Chap. 4, 5 and 6.
- Roger G. Newton, The Complex l-Plane (W. A. Benjamin, INC., New York, 1964).
- J. D. Tamarkin, Ann. Math. 28 (1927), 127.
- lim
s →-∞λB(s) = +∞ is already proved by Nakanishi; N. Nakanishi, Prog. Theor. Phys. 41 (1969), 780[PTP].
- R. Gatto and P. Menotti, Nuovo Cim. A 68 (1970), 118.
-
M. Ciafaloni and P. Menotti, Phys. Rev. 140 (1965), B929[APS].
- J. Arafune, Preprint UT-24 (1969).
-
R. Gatto and P. Menotti, Phys. Lett. B 27 (1968), 381[CrossRef].
E. zur Linden, Nuovo Cim. A 63 (1969), 181; ibid. 63 (1969), 193.
J. Arafune, H. Ezawa, N. Murai and K. Nakamura, Nuovo Cim. Lett. 2 (1969), 394.