${\boldsymbol m}_{{{\boldsymbol K}^{*}{(892)}^{0}}}–{\boldsymbol m}_{{{\boldsymbol K}^{*}{(892)}^{\pm}}}$ INSPIRE search

VALUE (MeV) EVTS DOCUMENT ID TECN CHG  COMMENT
$\bf{ 6.7 \pm1.2}$ OUR AVERAGE
$7.7$ $\pm1.7$ 2980
AGUILAR-BENIT..
1978B
HBC $\pm{}$0 0.76 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{\mp}}{{\mathit K}_S^0}$ ${{\mathit \pi}^{\pm}}$
$5.7$ $\pm1.7$ 7338
AGUILAR-BENIT..
1971B
HBC -0 3.9,4.6 ${{\mathit K}^{-}}{{\mathit p}}$
$6.3$ $\pm4.1$ 283 1
BARASH
1967B
HBC 0.0 ${{\overline{\mathit p}}}{{\mathit p}}$
1  Number of events in peak reevaluated by us.
  References:
AGUILAR-BENITEZ 1978B
NP B141 101 A New Experimental Determination of the ${{\mathit K}^{*}{(892)}}$ Electromagnetic Mass Difference
AGUILAR-BENITEZ 1971B
PR D4 2583 Properties of the ${{\mathit K}^{*}{(890)}}$ and ${{\mathit K}^{*}{(1420)}}$ in ${{\mathit K}^{-}}{{\mathit p}}$ Interactions at 3.9 and 4.6 ${\mathrm {GeV/}}\mathit c$
BARASH 1967B
PR 156 1399 Annihilations of Antiprotons at Rest in Hydrogen. VI. Kaonic Final States