${{\mathit \Lambda}{(1405)}}$ MASS

EXTRAPOLATIONS BELOW ${{\mathit N}}{{\overline{\mathit K}}}$ THRESHOLD

INSPIRE   PDGID:
B037M2
VALUE (MeV) DOCUMENT ID TECN  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
$\text{1407.56 or 1407.50}$ 1
KIMURA
2000
potential model
$1411$ 2
MARTIN
1981
K-matrix fit
$1406$ 3
CHAO
1973
DPWA 0$-$range fit (sol. B)
$1421$
MARTIN
1970
RVUE Constant K-matrix
$1416$ $\pm4$
MARTIN
1969
HBC Constant K-matrix
$1403$ $\pm3$
KIM
1967
HBC K-matrix fit
$1407.5$ $\pm1.2$ 4
KITTEL
1966
HBC 0$-$effective-range fit
$1410.7$ $\pm1.0$
KIM
1965
HBC 0$-$effective-range fit
$1409.6$ $\pm1.7$ 4
SAKITT
1965
HBC 0$-$effective-range fit
1  The KIMURA 2000 values are from fits A and B from a coupled-channel potential model using low-energy ${{\overline{\mathit K}}}{{\mathit N}}$ and ${{\mathit \Sigma}}{{\mathit \pi}}$ data, kaonic-hydrogen x-ray measurements, and our ${{\mathit \Lambda}{(1405)}}$ mass and width. The results bear mainly on the $\mathit nature$ of the ${{\mathit \Lambda}{(1405)}}$: three-quark state or ${{\overline{\mathit K}}}{{\mathit N}}$ bound state.
2  The MARTIN 1981 fit includes the ${{\mathit K}^{\pm}}{{\mathit p}}$ forward scattering amplitudes and the dispersion relations they must satisfy.
3  See also the accompanying paper of THOMAS 1973.
4  Data of SAKITT 1965 are used in the fit by KITTEL 1966.
References