${{\boldsymbol \rho}_{{3}}{(2250)}}$ MASS

$\boldsymbol S$-CHANNEL ${{\overline{\boldsymbol N}}}{{\boldsymbol N}}$ INSPIRE search

VALUE (MeV) DOCUMENT ID TECN CHG  COMMENT
• • • We do not use the following data for averages, fits, limits, etc. • • •
$2260$ $\pm20$ 1
ANISOVICH
2002
SPEC $0.6 - 1.9$ ${{\mathit p}}$ ${{\overline{\mathit p}}}$ $\rightarrow$ ${{\mathit \omega}}{{\mathit \pi}^{0}}$ , ${{\mathit \omega}}{{\mathit \eta}}{{\mathit \pi}^{0}}$ , ${{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$
$\sim$$2190$ 2
CUTTS
1978B
 CNTR 0.97$-$3 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\overline{\mathit N}}}{{\mathit N}}$
$2155$ $\pm15$ 3, 2
COUPLAND
1977
CNTR 0 0.7$-$2.4 ${{\overline{\mathit p}}}$ ${{\mathit p}}$ $\rightarrow$ ${{\overline{\mathit p}}}{{\mathit p}}$
$2193$ $\pm2$ 2, 4
ALSPECTOR
1973
CNTR ${{\overline{\mathit p}}}{{\mathit p}}$ $\mathit S$ channel
$2190$ $\pm10$ 5
ABRAMS
1970
CNTR $\mathit S$ channel ${{\overline{\mathit p}}}{{\mathit N}}$
1  From the combined analysis of ANISOVICH 2000J, ANISOVICH 2001D, ANISOVICH 2001E, and ANISOVICH 2002 .
2  Isospins 0 and 1 not separated.
3  From a fit to the total elastic cross section.
4  Referred to as ${{\mathit T}}$ or ${{\mathit T}}$ region by ALSPECTOR 1973 .
5  Seen as bump in $\mathit I = 1$ state. See also COOPER 1968 . PEASLEE 1975 confirm ${{\overline{\mathit p}}}{{\mathit p}}$ results of ABRAMS 1970 , no narrow structure.
  References:
ANISOVICH 2002
PL B542 8 Combined Analysis of Meson Channels with $\mathit I$ = 1, $\mathit C$ = -1 from 1940 to 2410-MeV
CUTTS 1978B
PR D17 16 Antiproton Proton Charge Exchange between 1 and 3 ${\mathrm {GeV/}}\mathit c$
COUPLAND 1977
PL 71B 460 Antiproton Proton Total Elastic Cross Sections in the ${{\mathit T}}$ and ${{\mathit U}}$ Regions (0.69 to 2.43 ${\mathrm {GeV/}}\mathit c$)
ALSPECTOR 1973
PRL 30 511 High Statistics Investigation of the Broad ${{\mathit T}}$ and ${{\mathit U}}$ Peaks in Antiproton Interactions
ABRAMS 1970
PR D1 1917 Total Cross Sections of ${{\mathit K}^{\pm}}$ Mesons and Antiprotons on Nucleons up to 3.3 ${\mathrm {GeV/}}\mathit c$