Abstract
We present an analysis of the octet baryon masses and the πN andKN σ-terms in the framework of heavy baryon chiral perturbation theory. At next-to-leading order,O(q 3), knowledge of the baryon masses and σπN (0) allows to determine the three corresponding finite low-energy constants and to predict the twoKN σ-terms σ (1,2) KN (0). We also include the spin-3/2 decuplet in the effective theory. The presence of the non-vanishing energy scale due to the octet-decuplet splitting shifts the average octet baryon mass by an infinite amount and leads to infinite renormalizations of the low-energy constants. The first observable effect of the decuplet intermediate states to the baryon masses starts out at orderq 4. We argue that it is not sufficient to retain only these but no other higher order terms to achieve a consistent description of the three-flavor scalar sector of baryon CHPT. In addition, we critically discuss anSU (2) result which allows to explain the large shift σπN (2M 2π )-σπN (0) via intermediate Δ (1232) states.
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J. Gasser, H. Leutwyler: Ann. Phys. (N.Y.) 158 (1984) 142; Nucl. Phys. B250 (1985) 465
J. Gasser, M.E. Sainio, A. Švarc: Nucl. Phys. B307 (1988) 779
E. Jenkins, A.V. Manohar: Phys. Lett. B255 (1991) 558
J. Gasser, H. Leutwyler: Phys. Rep. C87 (1982) 77
S. Weinberg: Nucl. Phys. B363 (1991) 3
V. Bernard, N. Kaiser, J. Kambor, Ulf-G. Meißner: Nucl. Phys. B388 (1992) 315
E. Jenkins, A.V. Manohar: Phys. Lett. B259 (1991) 353
E. Jenkins: Nucl. Phys. B368 (1992) 190
E. Jenkins: Nucl. Phys. B375 (1992) 561
M.N. Butler, M.J. Savage: Phys. Lett. B294 (1992) 369
J. Bijnens, H. Sonoda, M.B. Wise: Nucl. Phys. B261 (1985) 185
J. Gasser: Ann. Phys. (N.Y.) 136 (1981) 62
J. Gasser, H. Leutwyler, M.E. Sainio: Phys. Lett. 253B (1991) 252 260
J.F. Donoghue, C.R. Nappi: Phys. Lett. B168 (1986) 105
V. Bernard, R.L. Jaffe, Ulf-G. Meißner: Nucl. Phys. B308 (1988) 753
E. Jenkins, A.V. Manohar: Phys. Lett. B281 (1992) 336
Ulf-G. Meißner: Int. J. Mod. Phys. E1 (1992) 561
E. Jenkins, A.V. Manohar: in: Effective field theories of the Standard Model, Ulf-G. Meißner (ed.). Singapore: World Scientific 1992
Ulf-G. Meißner: Bern University preprint BUTP-93/01, 1993, Rep. Prog. Phys., in print
H. Pagels, W. Pardee: Phys. Rev. D4 (1971) 3225
J. Gasser, A. Zepeda: Nucl. Phys. B174 (1980) 445
M. Bourquin et al.: Z. Phys. C21 (1983) 27
R.L. Jaffe, A.V. Manohar: Nucl. Phys. B337 (1990) 509
R.L. Jaffe, C. Korpa: Comments Nucl. Part. Phys. 17 (1987) 163
I. Jameson, A.W. Thomas, G. Chanfray: J. Phys. G 18 (1992) L159
C. Ordonez, U. van Kolck: Phys. Lett. B291 (1992) 459
Ulf-G. Meißner: Comments Nucl. Part. Phys. 20, (1991) 119
P.M. Gensini: J. Phys. G7 (1981) 1177
P.M. Gensini: in πN Newsletter no. 6, R.E. Cutkowsky, G. Höhler, W. Kluge B.M.K. Nefkens, (eds.) April 1992
H. Pagels: Phys. Rep. C17 (1975) 219
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Work supported in part by Deutsche Forschungsgemeinschaft and by Schweizerischer Nationalfonds
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Bernard, V., Kaiser, N. & Meißner, U.G. Critical analysis of baryon masses and sigma-terms in heavy baryon chiral perturbation theory. Z. Phys. C - Particles and Fields 60, 111–119 (1993). https://doi.org/10.1007/BF01650436
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DOI: https://doi.org/10.1007/BF01650436