${{\boldsymbol p}}$ ELECTRIC DIPOLE MOMENT INSPIRE search

A nonzero value is forbidden by both $\mathit T$ invariance and $\mathit P$ invariance.
VALUE ($ 10^{-23} $ $\mathit e~$cm) DOCUMENT ID TECN  COMMENT
$\bf{<0.021}$ 1
SAHOO
2017
Theory plus ${}^{199}\mathrm {Hg}$ atom EDM
• • • We do not use the following data for averages, fits, limits, etc. • • •
$<0.54$ 1
DMITRIEV
2003
Theory plus ${}^{199}\mathrm {Hg}$ atom EDM
$-3.7$ $\pm6.3$
CHO
1989
NMR Tl F molecules
$<400$
DZUBA
1985
THEO Uses ${}^{129}\mathrm {Xe}$ moment
$130$ $\pm200$ 2
WILKENING
1984
$900$ $\pm1400$ 3
WILKENING
1984
$700$ $\pm900$
HARRISON
1969
MBR Molecular beam
1  SAHOO 2017 and DMITRIEV 2003 are not direct measurements of the proton electric dipole moment. They use theory to calculate this limit from the limit on the electric dipole moment of the ${}^{199}\mathrm {Hg}$ atom.
2  This WILKENING 1984 value includes a finite-size effect and a magnetic effect.
3  This WILKENING 1984 value is more cautious than the other and excludes the finite-size effect, which relies on uncertain nuclear integrals.
  Conservation Laws:
TIME REVERSAL ($\mathit T$) INVARIANCE PARITY ($\mathit P$) INVARIANCE
  References:
SAHOO 2017
PR D95 013002 Improved Limits on the Hadronic and Semi-Hadronic $\mathit CP$ Violating Parameters and Role of a Dark Force Carrier in the Electric Dipole Moment of ${}^{199}\mathrm {Hg}$
DMITRIEV 2003
PRL 91 212303 Schiff Moment of the Mercury Nucleus and the Proton Dipole Moment
CHO 1989
PRL 63 2559 Tenfold Improvement of Limits on $\mathit T$ Violation in Thallium Fluoride
DZUBA 1985
PL 154B 93 Bounds on Electric Dipole Moments and $\mathit T$ Violating Weak Interactions of the Nucleons
WILKENING 1984
PR A29 425 Search for $\mathit P$ and $\mathit T$ Violations in the Hyperfine Structure of Thallium Fluoride
HARRISON 1969
PRL 22 1263 Experimental Limit on the Proton Electric Dipole Moment