pdgLive

PARITY ($\mathit P$) INVARIANCE

${{\mathit e}}$ electric dipole moment

$<1.1 \times 10^{-29}$ $\mathit e~$cm CL=90.0%

${{\mathit \mu}}$ electric dipole moment $\vert $d$\vert $

$<1.8 \times 10^{-19}$ $\mathit e~$cm CL=95.0%

Re($\mathit d_{{{\mathit \tau}}}$ = ${{\mathit \tau}}$ electric dipole moment)

$-1.85 \times 10^{-17}\text{ to }6.1 \times 10^{-18} $ $\mathit e~$cm CL=95.0%

$\Gamma\mathrm {( {{\mathit \eta}} \rightarrow 4 {{\mathit \pi}^{0}} )}$ $/$ $\Gamma\mathrm {(total)}$

$<6.9\times 10^{-7}$ CL=90.0%

$\Gamma\mathrm {( {{\mathit \eta}} \rightarrow 2 {{\mathit \pi}^{0}} )}$ $/$ $\Gamma\mathrm {(total)}$

$<3.5\times 10^{-4}$ CL=90.0%

$\Gamma\mathrm {( {{\mathit \eta}} \rightarrow {{\mathit \pi}^{+}} {{\mathit \pi}^{-}} )}$ $/$ $\Gamma\mathrm {(total)}$

$<4.4\times 10^{-6}$ CL=90.0%

$\Gamma\mathrm {( {{\mathit \eta}^{\,'}{(958)}} \rightarrow {{\mathit \pi}^{+}} {{\mathit \pi}^{-}} )}$ $/$ $\Gamma\mathrm {(total)}$

$<1.8\times 10^{-5}$ CL=90.0%

$\Gamma\mathrm {( {{\mathit \eta}^{\,'}{(958)}} \rightarrow {{\mathit \pi}^{0}} {{\mathit \pi}^{0}} )}$ $/$ $\Gamma\mathrm {(total)}$

$<4\times 10^{-4}$ CL=90.0%

$\Gamma\mathrm {( {{\mathit \eta}_{{c}}{(1S)}} \rightarrow {{\mathit K}_S^0} {{\mathit K}_S^0} )}$ $/$ $\Gamma\mathrm {(total)}$

$<3.1\times 10^{-4}$ CL=90.0%

$\Gamma\mathrm {( {{\mathit \eta}_{{c}}{(1S)}} \rightarrow {{\mathit K}^{+}} {{\mathit K}^{-}} )}$ $/$ $\Gamma\mathrm {(total)}$

$<6\times 10^{-4}$ CL=90.0%

$\Gamma\mathrm {( {{\mathit \eta}_{{c}}{(1S)}} \rightarrow {{\mathit \pi}^{0}} {{\mathit \pi}^{0}} )}$ $/$ $\Gamma\mathrm {(total)}$

$<4\times 10^{-5}$ CL=90.0%

$\Gamma\mathrm {( {{\mathit \eta}_{{c}}{(1S)}} \rightarrow {{\mathit \pi}^{+}} {{\mathit \pi}^{-}} )}$ $/$ $\Gamma\mathrm {(total)}$

$<1.1\times 10^{-4}$ CL=90.0%

${{\mathit p}}$ electric dipole moment

$<2.1 \times 10^{-25}$ $\mathit e~$cm

${{\mathit n}}$ electric dipole moment

$<1.8 \times 10^{-26}$ $\mathit e~$cm CL=90.0%

${{\mathit \Lambda}}$ electric dipole moment

$<1.5 \times 10^{-16}$ $\mathit e~$cm CL=95.0%

a$_{P}$( ${{\mathit \Lambda}_{{b}}^{0}}$ $\rightarrow$ ${{\mathit p}}{{\mathit \pi}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ )

$-0.040$ $\pm0.007$

a$_{P}$( ${{\mathit \Lambda}_{{b}}^{0}}$ $\rightarrow$ ${{\mathit p}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}{{\mathit \pi}^{-}}$ )

$-0.006$ $\pm0.009$

a$_{P}$( ${{\mathit \Lambda}_{{b}}^{0}}$ $\rightarrow$ ${{\mathit p}}{{\mathit K}^{-}}{{\mathit K}^{+}}{{\mathit \pi}^{-}}$ )

$0.04$ $\pm0.05$

a$_{P}$( ${{\mathit \Lambda}_{{b}}^{0}}$ $\rightarrow$ ${{\mathit p}}{{\mathit K}^{-}}{{\mathit K}^{+}}{{\mathit K}^{-}}$ )

$-0.016$ $\pm0.015$

a$_{P}$( ${{\mathit \Lambda}_{{b}}^{0}}$ $\rightarrow$ ${{\mathit p}}{{\mathit K}^{-}}{{\mathit \mu}^{+}}{{\mathit \mu}^{-}}$ )

$-0.05$ $\pm0.05$

a$_{P}$( ${{\mathit \Xi}_{{b}}^{0}}$ $\rightarrow$ ${{\mathit p}}{{\mathit K}^{-}}{{\mathit K}^{-}}{{\mathit \pi}^{+}}$ )

$-0.03$ $\pm0.05$

Except where otherwise noted, content of the 2023 Review of Particle Physics is licensed under a Creative Commons Attribution-NonCommercial 4.0 International (CC BY-NC 4.0) license. The publication of the Review of Particle Physics is supported by US DOE, MEXT (Japan), INFN (Italy), JPS and CERN. Individual collaborators receive support for their PDG activities from their respective institutes or funding agencies. © 2023. See LBNL disclaimers.