Kaon-nucleon scattering from chiral Lagrangians
Résumé
The $ s $-wave $ K^{\pm} N $ scattering amplitude is computed up to one-loop order corresponding to next-to-next-to-leading order (or $ {\rm N}^ {\rm 2} {\rm LO} $ in short) with a heavy-baryon effective chiral Lagrangian. Constraining the low-energy constants by on-shell scattering lengths, we obtain contributions of each chiral order up to $ {\rm N}^ {\rm 2} {\rm LO} $ and find that the chiral corrections are \lq\lq natural\rq\rq\ in the sense of viable effective field theories. We have also calculated off-shell $ s $-wave $ K^-N $ scattering amplitudes relevant to kaonic atoms and $ K^- $ condensation in \lq\lq nuclear star\rq\rq\ matter including the effect of $ \Lambda( 1405). $ The $ K^-p $ amplitude is found to be quite sensitive to the intermediate $ \Lambda( 1405) $ contribution, while the $ K^-n $ amplitude varies smoothly with the C.M. energy. The crossing-even one-loop corrections are found to play an important role in determining the higher-order chiral corrections.
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