${{\mathit K}^{*}{(892)}}$ RANGE PARAMETER INSPIRE search

All from partial wave amplitude analyses.
M018R
VALUE (GeV${}^{-1}$) EVTS DOCUMENT ID TECN CHG  COMMENT
$2.1$ $\pm0.5$ $\pm0.5$ 243k 1
DEL-AMO-SANCH..
2011I
 BABR 0 ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit e}^{+}}{{\mathit \nu}_{{{e}}}}$
$3.96$ $\pm0.54$ ${}^{+1.31}_{-0.90}$ 18k 2
LINK
2005I
 FOCS 0 ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{{\mu}}}}$
$3.4$ $\pm0.7$
ASTON
1988
LASS 0 11 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit n}}$
• • • We do not use the following data for averages, fits, limits, etc. • • •
$12.1$ $\pm3.2$ $\pm3.0$
BIRD
1989
LASS - 11 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\overline{\mathit K}}^{0}}{{\mathit \pi}^{-}}{{\mathit p}}$
1  Taking into account the ${{\mathit K}^{*}{(892)}^{0}}$, ${\mathit S}{\mathrm -wave}$ and ${\mathit P}{\mathrm -wave}$ (${{\mathit K}^{*}{(1410)}^{0}}$).
2  Fit to ${{\mathit K}}{{\mathit \pi}}$ mass spectrum includes a non-resonant scalar component.
  References:
DEL-AMO-SANCHEZ 2011I
PR D83 072001 Analysis of the ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit e}^{+}}{{\mathit \nu}_{{{e}}}}$ Decay Channel
LINK 2005I
PL B621 72 Hadronic Mass Spectrum Analysis of ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \mu}^{+}}{{\mathit \nu}}$ Decay and Measurement of the ${{\mathit K}^{*}{(892)}^{0}}$ Mass and Width
BIRD 1989
SLAC-332 Cerenkov Ring Imaging and Spectroscopy of Charged ${{\mathit K}^{*}}$ Interactions at 11 ${\mathrm {GeV/}}\mathit c$
ASTON 1988
NP B296 493 A Study of ${{\mathit K}^{-}}$ ${{\mathit \pi}^{+}}$ Scattering in the Reaction ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit n}}$ at 11 ${\mathrm {GeV/}}\mathit c$