| $\bf{-0.0024\text{ to }0.0047 }$ |
95 |
1 |
|
ATLS |
| • • • We do not use the following data for averages, fits, limits, etc. • • • |
| $-0.041$ ${}^{+0.012}_{-0.009}$ |
|
2, 3 |
|
ATLS |
| $-0.057\text{ to }0.024 $ |
95 |
2 |
|
ATLS |
| $0.001$ ${}^{+0.055}_{-0.089}$ |
|
4, 3 |
|
CMS |
| $-0.018$ $\pm0.017$ |
|
5, 3 |
|
DLPH |
| $<0.107$ |
95 |
6 |
|
L3 |
| $-0.007\text{ to }0.005 $ |
95 |
7 |
|
RVUE |
| $-0.052\text{ to }0.058 $ |
95 |
8 |
|
L3 |
| $-0.068\text{ to }0.065 $ |
95 |
9 |
|
OPAL |
| $-0.004\text{ to }0.006 $ |
95 |
10 |
|
RVUE |
| $<0.01$ |
95 |
11 |
|
RVUE |
| $<0.12$ |
90 |
|
|
RVUE |
| $<0.023$ |
95 |
12 |
|
RVUE |
|
1
AAD 2025BB limits are obtained by comparing the inclusive ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ fiducial cross-section in ${{\mathit p}}{{\mathit p}}$ collisions as a function of visible invariant mass at large masses to the Standard Model prediction.
|
|
2
AAD 2023BM measurement is derived from ${{\mathit \gamma}}$ ${{\mathit \gamma}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ total cross-section TeV. Authors report both the measured value and the corresponding 95$\%$ CL limit. from 1.44 nb${}^{-1}$ LHC ${}^{}\mathrm {Pb}−{}^{}\mathrm {Pb}$ collisions at $\sqrt {{{\mathit S}_{{{NN}}}} }$ = 5.02
|
|
3
Measurement ill-suited for a standard average because its likelihood appears to be remarkably non-Gaussian and asymmetric according to the model-dependent extraction procedure and the reported 95$\%$ CL limits.
|
|
4
TUMASYAN 2023AS measurement is derived from ${{\mathit \gamma}}$ ${{\mathit \gamma}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ total cross-section from 404 ${{\mathit \mu}}$b${}^{-1}$ LHC ${}^{}\mathrm {Pb}-{}^{}\mathrm {Pb}$ collisions at $\sqrt {{{\mathit S}_{{{NN}}}} }$ = 5.02 TeV.
|
|
5
ABDALLAH 2004K measurement is derived from ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ total cross-section measurements at $\sqrt {s }$ between 183 and 208 GeV. In addition to the measurement, the authors also quote 95$\%$ CL limits of $>$ -0.052 and $<$ 0.013.
|
|
6
ACHARD 2004G limit is derived from ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit e}^{+}}{{\mathit e}^{-}}{{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ total cross-section measurements at $\sqrt {s }$ between 189 and 206 GeV, and is on the absolute value of the magnetic moment anomaly.
|
|
7
GONZALEZ-SPRINBERG 2000 use data on tau lepton production at LEP1, SLC, and LEP2, and data from colliders and LEP2 to determine limits. Assume imaginary component is zero.
|
|
8
ACCIARRI 1998E use ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}{{\mathit \gamma}}$ events. In addition to the limits, the authors also quote a value of $0.004$ $\pm0.027$ $\pm0.023$.
|
|
9
ACKERSTAFF 1998N use ${{\mathit Z}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}{{\mathit \gamma}}$ events. The limit applies to an average of the form factor for off-shell ${{\mathit \tau}}$'s having $\mathit p{}^{2}$ ranging from ${{\mathit m}^{2}}_{{{\mathit \tau}}}$ to ($\mathit M_{{{\mathit Z}}}-{\mathit m}_{{{\mathit \tau}}}){}^{2}$.
|
|
10
ESCRIBANO 1997 use preliminary experimental results.
|
|
11
ESCRIBANO 1993 limit derived from $\Gamma\mathrm {( {{\mathit Z}} \rightarrow {{\mathit \tau}^{+}} {{\mathit \tau}^{-}})}$, and is on the absolute value of the magnetic moment anomaly.
|
|
12
SILVERMAN 1983 limit is derived from ${{\mathit e}^{+}}$ ${{\mathit e}^{-}}$ $\rightarrow$ ${{\mathit \tau}^{+}}{{\mathit \tau}^{-}}$ total cross-section measurements for $\mathit q{}^{2}$ up to (37 GeV)${}^{2}$.
|
