LIMITS ON CHARGED PARTICLES IN HADRONIC REACTIONS

Heavy Particle Production Differential Cross Section

INSPIRE   PDGID:
S015D
VALUE (cm${}^{2}$sr${}^{-1}$GeV${}^{-1}$) CL% DOCUMENT ID TECN CHG  COMMENT
• • We do not use the following data for averages, fits, limits, etc. • •
1
HAYRAPETYAN
2023F
CMS top $\rightarrow$ ${{\mathit \ell}}$s via EFT ops.
$<2.6 \times 10^{-36}$ 90 2
BALDIN
1976
CNTR - $\mathit Q$= 1, $\mathit m=2.1-9.4$ GeV
$<2.2 \times 10^{-33}$ 90 3
ALBROW
1975
SPEC $\pm{}$ $\mathit Q$= $\pm1$, $\mathit m=4-$15 GeV
$<1.1 \times 10^{-33}$ 90 3
ALBROW
1975
SPEC $\pm{}$ $\mathit Q$= $\pm2$, $\mathit m=6-$27 GeV
$<8. \times 10^{-35}$ 90 4
JOVANOVICH
1975
CNTR $\pm{}$ $\mathit m=15-$26 GeV
$<1.5 \times 10^{-34}$ 90 4
JOVANOVICH
1975
CNTR $\pm{}$ $\mathit Q$= $\pm2$, $\mathit m=3-$10 GeV
$<6. \times 10^{-35}$ 90 4
JOVANOVICH
1975
CNTR $\pm{}$ $\mathit Q$= $\pm2$, $\mathit m=10-$26 GeV
$<1. \times 10^{-31}$ 90 5
APPEL
1974
CNTR $\pm{}$ $\mathit m=3.2-7.2$ GeV
$<5.8 \times 10^{-34}$ 90 6
ALPER
1973
SPEC $\pm{}$ $\mathit m=1.5-$24 GeV
$<1.2 \times 10^{-35}$ 90 7
ANTIPOV
1971B
CNTR - $\mathit Q=–$, $\mathit m=2.2-2.8$
$<2.4 \times 10^{-35}$ 90 8
ANTIPOV
1971C
CNTR - $\mathit Q=–$, $\mathit m=1.2-1.7$, $2.1-$4
$<2.4 \times 10^{-35}$ 90
BINON
1969
CNTR - $\mathit Q=–$, $\mathit m=1-$1.8 GeV
$<1.5 \times 10^{-36}$ 9
DORFAN
1965
CNTR ${}^{}\mathrm {Be}$ target $\mathit m=3-$7 GeV
$<3.0 \times 10^{-36}$ 9
DORFAN
1965
CNTR ${}^{}\mathrm {Fe}$ target $\mathit m=3-$7 GeV
1  HAYRAPETYAN 2023F search for anomalous top $\rightarrow$ leptons decay via effective operators. No signal observed. Limits placed on EFT operators.
2  BALDIN 1976 is a 70 GeV Serpukhov experiment. Value is per ${}^{}\mathrm {Al}$ nucleus at $\theta $ = 0. For other charges in range $-0.5$ to $-3.0$, CL = 90$\%$ limit is ($2.6 \times 10^{-36})/\vert $(charge)$\vert $ for mass range (2.1$-$9.4 GeV)${\times }\vert $(charge)$\vert $. Assumes stable particle interacting with matter as do antiprotons.
3  ALBROW 1975 is a CERN ISR experiment with $\mathit E_{{\mathrm {cm}}}$ = 53 GeV. $\theta $ = 40 mr. See figure 5 for mass ranges up to 35 GeV.
4  JOVANOVICH 1975 is a CERN ISR 26$+26$ and 15$+15$ GeV ${{\mathit p}}{{\mathit p}}$ experiment. Figure 4 covers ranges $\mathit Q$ = 1/3 to 2 and $\mathit m$ = 3 to 26 GeV. Value is per GeV momentum.
5  APPEL 1974 is NAL 300 GeV ${{\mathit p}}{}^{}\mathrm {W}$ experiment. Studies forward production of heavy (up to 24 GeV) charged particles with momenta 24$-$200 GeV ($–$charge) and 40$-$150 GeV ($+$charge). Above typical value is for 75 GeV and is per GeV momentum per nucleon.
6  ALPER 1973 is CERN ISR 26$+26$ GeV ${{\mathit p}}{{\mathit p}}$ experiment. $\mathit p$ $>$0.9 GeV, 0.2 $<$ $\beta $ $<$0.65.
7  ANTIPOV 1971B is from same 70 GeV ${{\mathit p}}$ experiment as ANTIPOV 1971C and BINON 1969.
8  ANTIPOV 1971C limit inferred from flux ratio. 70 GeV ${{\mathit p}}$ experiment.
9  DORFAN 1965 is a 30 ${\mathrm {GeV/}}\mathit c$ ${{\mathit p}}$ experiment at BNL. Units are per GeV momentum per nucleus.
References