${{\mathit K}^{*}{(892)}}$ MASS

NEUTRAL ONLY

INSPIRE   PDGID:
M018M2
VALUE (MeV) EVTS DOCUMENT ID TECN  COMMENT
$\bf{ 895.55 \pm0.20}$ OUR AVERAGE  Error includes scale factor of 1.7.  See the ideogram below.
$894.68$ $\pm0.25$ $\pm0.05$ 1
ABLIKIM
2016F
BES3 ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit e}^{+}}{{\mathit \nu}_{{{e}}}}$
$895.4$ $\pm0.2$ $\pm0.2$ 243k 2
DEL-AMO-SANCH..
2011I
BABR ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit e}^{+}}{{\mathit \nu}_{{{e}}}}$
$895.7$ $\pm0.2$ $\pm0.3$ 141k 3
BONVICINI
2008A
CLEO ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{+}}$
$895.41$ $\pm0.32$ ${}^{+0.35}_{-0.43}$ 18k 4
LINK
2005I
FOCS ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \mu}^{+}}{{\mathit \nu}_{{{\mu}}}}$
$896$ $\pm2$
BARBERIS
1998E
OMEG 450 ${{\mathit p}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit p}_{{{f}}}}{{\mathit p}_{{{s}}}}{{\mathit K}^{*}}{{\overline{\mathit K}}^{*}}$
$895.9$ $\pm0.5$ $\pm0.2$
ASTON
1988
LASS 11 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit n}}$
$894.52$ $\pm0.63$ 25k 5
ATKINSON
1986
OMEG 20$-$70 ${{\mathit \gamma}}{{\mathit p}}$
$894.63$ $\pm0.76$ 20k 5
ATKINSON
1986
OMEG 20$-$70 ${{\mathit \gamma}}{{\mathit p}}$
$897$ $\pm1$ 28k
EVANGELISTA
1980
OMEG 10 ${{\mathit \pi}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$( ${{\mathit \Lambda}}$ ,${{\mathit \Sigma}}$)
$898.4$ $\pm1.4$ 1180
AGUILAR-BENIT..
1978B
HBC 0.76 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{\mp}}{{\mathit K}_S^0}$ ${{\mathit \pi}^{\pm}}$
$894.9$ $\pm1.6$
WICKLUND
1978
ASPK 3,4,6 ${{\mathit K}^{\pm}}$ ${{\mathit N}}$ $\rightarrow$ ( ${{\mathit K}}{{\mathit \pi}}$) ${}^{0}$ ${{\mathit N}}$
$897.6$ $\pm0.9$
BOWLER
1977
DBC 5.4 ${{\mathit K}^{+}}$ ${{\mathit d}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}{{\mathit p}}{{\mathit p}}$
$895.5$ $\pm1.0$ 3600
MCCUBBIN
1975
HBC 3.6 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit n}}$
$897.1$ $\pm0.7$ 22k 5
PALER
1975
HBC 14.3 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ( ${{\mathit K}}{{\mathit \pi}}$) ${}^{0}$ X
$896.0$ $\pm0.6$ 10k
FOX
1974
RVUE 2 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit n}}$
$896.0$ $\pm0.6$
FOX
1974
RVUE 2 ${{\mathit K}^{+}}$ ${{\mathit n}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}{{\mathit p}}$
$896$ $\pm2$ 6
MATISON
1974
HBC 12 ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}{{\mathit \Delta}}$
$896$ $\pm1$ 3186
LEWIS
1973
HBC 2.1$-$2.7 ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}}{{\mathit \pi}}{{\mathit \pi}}{{\mathit p}}$
$894.0$ $\pm1.3$ 6
LINGLIN
1973
HBC 2$-$13 ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{+}}{{\mathit p}}$
$898.4$ $\pm1.3$ 1700 7
BUCHNER
1972
DBC 4.6 ${{\mathit K}^{+}}$ ${{\mathit n}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}{{\mathit p}}$
$897.9$ $\pm1.1$ 2934 7
AGUILAR-BENIT..
1971B
HBC 3.9,4.6 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit n}}$
$898.0$ $\pm0.7$ 5362 7
AGUILAR-BENIT..
1971B
HBC 3.9,4.6 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit p}}$
$895$ $\pm1$ 4300 8
HABER
1970
DBC 3 ${{\mathit K}^{-}}$ ${{\mathit N}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}$ X
$893.7$ $\pm2.0$ 10k
DAVIS
1969
HBC 12 ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}{{\mathit \pi}^{+}}{{\mathit p}}$
$894.7$ $\pm1.4$ 1040 7
DAUBER
1967B
HBC 2.0 ${{\mathit K}^{-}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}{{\mathit p}}$
• • We do not use the following data for averages, fits, limits, etc. • •
$895.50$ $\pm0.92$ $\pm2.6$ 9
ADUSZKIEWICZ
2020A
NA61 158 ${{\mathit p}}{{\mathit p}}$
$898.1$ $\pm1.0$ 4k 10
LEES
2017C
BABR ${{\mathit J / \psi}}$ $\rightarrow$ ${{\mathit K}_S^0}$ ${{\mathit K}^{\pm}}{{\mathit \pi}^{\mp}}$
$895.53$ $\pm0.17$
LEES
2013F
BABR ${{\mathit D}^{+}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$
$894.9$ $\pm0.5$ $\pm0.7$ 14.4k 11
MITCHELL
2009A
CLEO ${{\mathit D}_{{{s}}}^{+}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$
$896.2$ $\pm0.3$ 20k 12
AUBERT
2007AK
BABR 10.6 ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit K}^{*0}}{{\mathit K}^{\pm}}{{\mathit \pi}^{\mp}}{{\mathit \gamma}}$
$900.7$ $\pm1.1$ 5900
BARTH
1983
HBC 70 ${{\mathit K}^{+}}$ ${{\mathit p}}$ $\rightarrow$ ${{\mathit K}^{+}}{{\mathit \pi}^{-}}$ X
1  Taking also into account the ${{\mathit K}^{*}_{\mathrm 0}{(1430)}^{0}}$ and ${{\mathit K}^{*}_{\mathrm 2}{(1430)}^{0}}$.
2  Taking into account the ${{\mathit K}^{*}{(892)}^{0}}$, ${\mathit S}{\mathrm -wave}$ and ${\mathit P}{\mathrm -wave}$ (${{\mathit K}^{*}{(1410)}^{0}}$).
3  From the isobar model with a complex pole for the ${{\mathit \kappa}}$.
4  Fit to ${{\mathit K}}{{\mathit \pi}}$ mass spectrum includes a non-resonant scalar component.
5  Inclusive reaction. Complicated background and phase-space effects.
6  From pole extrapolation.
7  Mass errors enlarged by us to $\Gamma /\sqrt {\mathit N }$. See note.
8  Number of events in peak reevaluated by us.
9  For transverse momenta between 0.6 and 0.8 GeV/c and rapidity 0 $<$ y $<$ 0.5.
10  From a Dalitz plot analysis in an isobar model with charged and neutral ${{\mathit K}^{*}{(892)}}$ masses and widths floating.
11  This value comes from a fit with $\chi {}^{2}$ of 178/117.
12  Systematic uncertainties not estimated.

           ${{\mathit K}^{*}{(892)}^{0}}$ mass (MeV)
References