| $\bf{\text{none 150 - 740}}$ |
95 |
1 |
|
CMS |
| $\bf{>1755}$ |
95 |
2 |
|
CMS |
| $\bf{>660}$ |
95 |
3 |
|
CMS |
| $> 304$ |
95 |
4 |
|
ZEUS |
| $>73$ |
95 |
5 |
|
DLPH |
| • • • We do not use the following data for averages, fits, limits, etc. • • • |
|
|
6 |
|
ICCB |
|
|
7 |
|
H1 |
| $> 300$ |
95 |
8 |
|
H1 |
|
|
9 |
|
D0 |
| $> 295$ |
95 |
10 |
|
H1 |
|
|
11 |
|
ZEUS |
| $>298$ |
95 |
12 |
|
ZEUS |
| $>197$ |
95 |
13 |
|
OPAL |
|
|
14 |
|
ZEUS |
| $>290$ |
95 |
15 |
|
H1 |
| $>204$ |
95 |
16 |
|
ZEUS |
|
|
17 |
|
ZEUS |
| $>161$ |
95 |
18 |
|
DLPH |
| $>200$ |
95 |
19 |
|
H1 |
|
|
20 |
|
ZEUS |
| $>168$ |
95 |
21 |
|
ZEUS |
|
1
SIRUNYAN 2018BJ search for single production of charge 2/3 scalar leptoquarks decaying to ${{\mathit \tau}}{{\mathit b}}$ in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 13 TeV. The limit above assumes B( ${{\mathit \tau}}{{\mathit b}}$ ) =1 and the leptoquark coupling strength $\lambda $ = 1.
|
|
2
KHACHATRYAN 2016AG search for single production of charge $\pm{}$1/3 scalar leptoquarks using ${{\mathit e}}{{\mathit e}}{{\mathit j}}$ events in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The limit above assumes B( ${{\mathit e}}{{\mathit q}}$ ) = 1 and the leptoquark coupling strength ${{\mathit \lambda}}$ = 1.
|
|
3
KHACHATRYAN 2016AG search for single production of charge $\pm{}$1/3 scalar leptoquarks using ${{\mathit \mu}}{{\mathit \mu}}{{\mathit j}}$ events in ${{\mathit p}}{{\mathit p}}$ collisions at $\sqrt {s }$ = 8 TeV. The limit above assumes B( ${{\mathit \mu}}{{\mathit q}}$ ) = 1 and the leptoquark coupling strength $\lambda $ = 1.
|
|
4
ABRAMOWICZ 2012A limit is for a scalar, weak isoscalar, charge $-1$/3 leptoquark coupled with ${{\mathit e}_{{R}}}$. See their Figs. $12 - 17$ and Table 4 for states with different quantum numbers.
|
|
5
Limit from single production in ${{\mathit Z}}$ decay. The limit is for a leptoquark coupling of electromagnetic strength and assumes B( ${{\mathit \ell}}{{\mathit q}}$ ) = 2/3. The limit is 77 GeV if first and second leptoquarks are degenerate.
|
|
6
DEY 2016 use the 2010-2012 IceCube PeV energy data set to constrain the leptoquark production cross section through the ${{\mathit \nu}}$ ${{\mathit q}}$ $\rightarrow$ LQ $\rightarrow$ ${{\mathit \nu}}{{\mathit q}}$ process. See their Figure 4 for the exclusion limit in the mass-coupling plane.
|
|
7
AARON 2011A search for various leptoquarks with lepton-flavor violating couplings. See their Figs.$~2 - 3$ and Tables$~1 - 4$ for detailed limits.
|
|
8
The quoted limit is for a scalar, weak isoscalar, charge $-1$/3 leptoquark coupled with ${{\mathit e}_{{R}}}$. See their Figs. $3 - 5$ for limits on states with different quantum numbers.
|
|
9
ABAZOV 2007E search for leptoquark single production through ${{\mathit q}}{{\mathit g}}$ fusion process in ${{\mathit p}}{{\overline{\mathit p}}}$ collisions. See their Fig. 4 for exclusion plot in mass-coupling plane.
|
|
10
AKTAS 2005B limit is for a scalar, weak isoscalar, charge $−$1/3 leptoquark coupled with ${{\mathit e}_{{R}}}$. See their Fig. 3 for limits on states with different quantum numbers.
|
|
11
CHEKANOV 2005 search for various leptoquarks with lepton-flavor violating couplings. See their Figs.6--10 and Tables 1--8 for detailed limits.
|
|
12
CHEKANOV 2003B limit is for a scalar, weak isoscalar, charge $−$1/3 leptoquark coupled with ${{\mathit e}_{{R}}}$. See their Figs.$~11 - 12$ and Table$~$5 for limits on states with different quantum numbers.
|
|
13
For limits on states with different quantum numbers and the limits in the mass-coupling plane, see their Fig.$~$4 and Fig.$~$5.
|
|
14
CHEKANOV 2002 search for various leptoquarks with lepton-flavor violating couplings. See their Figs.$~6 - 7$ and Tables$~5 - 6$ for detailed limits.
|
|
15
For limits on states with different quantum numbers and the limits in the mass-coupling plane, see their Fig.$~$3.
|
|
16
See their Fig.$~$14 for limits in the mass-coupling plane.
|
|
17
BREITWEG 2000E search for $\mathit F$=0 leptoquarks in ${{\mathit e}^{+}}{{\mathit p}}$ collisions. For limits in mass-coupling plane, see their Fig.$~$11.
|
|
18
ABREU 1999G limit obtained from process ${{\mathit e}}$ ${{\mathit \gamma}}$ $\rightarrow$ $\mathit LQ+q$. For limits on vector and scalar states with different quantum numbers and the limits in the coupling-mass plane, see their Fig.$~$4 and Table$~$2.
|
|
19
For limits on states with different quantum numbers and the limits in the mass-coupling plane, see their Fig.$~$13 and Fig.$~$14. ADLOFF 1999 also search for leptoquarks with lepton-flavor violating couplings. ADLOFF 1999 supersedes AID 1996B.
|
|
20
DERRICK 1997 search for various leptoquarks with lepton-flavor violating couplings. See their Figs.$~$5--8 and Table$~$1 for detailed limits.
|
|
21
DERRICK 1993 search for single leptoquark production in ${{\mathit e}}{{\mathit p}}$ collisions with the decay ${{\mathit e}}{{\mathit q}}$ and ${{\mathit \nu}}{{\mathit q}}$ . The limit is for leptoquark coupling of electromagnetic strength and assumes B( ${{\mathit e}}{{\mathit q}}$ ) = B( ${{\mathit \nu}}{{\mathit q}}$ ) = 1/2. The limit for B( ${{\mathit e}}{{\mathit q}}$ ) = 1 is 176 GeV. For limits on states with different quantum numbers, see their Table$~$3.
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