ACME Precision Measurement of the Electron Electric Dipole Moment (EDM)


Research Overview

acmeThe most precise limit on the size of the electron’s electric dipole moment (eEDM), |de| < 1.1 × 10−29e cm at 90% confidence, was set by the 2nd generation of our ACME collaboration in 2018. It presents an almost one order of magnitude improvement compared to the previous best limit of the electron EDM, which was set by the 1st generation of ACME in 2014. This result constrains any new time-reversal-symmetry-violating physics for broad classes of proposed beyond-standard-model particles in the mass range 3–30 TeV c−2. We are currently working on a series of upgrades for a next generation advanced ACME experiment. These upgrades feature a hexapole molecular lens to boost the EDM signal by almost 20 times using the metastable Q state of the Thorium Monoxide (ThO) molecules, a 4 times longer spin coherence time than previously used, about 2 times high quantum efficiency in detection by using the silicon photomultiplier, suppression of excess noise present in the last generation measruement, and many more. With all these demonstrated upgrades, we are looking forward to improving our electron EDM sensitivity by another order of magnitude in the coming months. So, stay tuned!



the hexapole electrostatic lens

(Should visit our electron EDM website for more details on the ACME collaboration.) 

The ACME experiment uses a cryogenic molecular beam of the heavy polar molecule ThO to measure the electron's electric dipole moment (EDM). The existence of an electron EDM would manifest itself as very small energy shifts in certain molecular states when the molecules are in an electric field. The electron EDM is a strong probe of physics beyond the Standard Model.

The molecular beam is created by buffer gas cooling an ablated sample of ThO, which then flows out of an orifice. The molecules enter a magnetically shielded vacuum chamber that contains uniform electric and magnetic fields. We optically pump the molecules into the "H" electronic (EDM sensitive) state, and then polarize them by optically pumping undesired polarizations out of the H state. The molecules then precess in the fields, and we read out the accumulated phase with polarized lasers. By reversing the electric field, we can reverse the amount of precession accumulated from the electron EDM; taking the difference between these two phases yields the electron EDM.

This idea is the basis for any permanent EDM search, whether it is for atoms, neutrons, or electrons, however our experiment has several features that enhance our sensitivity:

  • Polar Molecule. Polar molecules have the highest known sensitivity to an electron electric dipole moment. The electric field inside a polar molecule can be as large as tens of gigavolts per centimeter, almost a million times larger than any controlled field that can be created in a laboratory. Because the energy of a dipole moment in an electric field is proportional to the field strength, the electrons orbiting a polar molecule can experience these large fields and give proportionally larger energy shift. The electric field in ThO has been calculated to be 84 GV/cm, one of the largest known.
  • Internal Co-magnetometer. Since we measure tiny energy splittings, a small stray electric or magnetic field can could destroy our signal. Even worse, these stray fields could look like an EDM in certain situations, for example from leakage currents between the electric field plates. Our molecule has a parity doublet: two close-lying (a few hundred kilohertz in zero field) states of opposite parity in the ground rotational level of the H state. In addition to allowing complete polarization of the molecule in very weak fields, the two components of this doublet have equal yet opposite shifts from an electron EDM. In other words, the two different doublet states correspond to spectroscopically reversing the internal electric field experienced by the electron. Therefore, we can perform our field reversal without reversing any external fields, which will give us very powerful rejection of systematic errors. Other limiting systematics, such as geometric phases, can also be eliminated because they do not reverse between populating the different doublets.
  • Cryogenic Beam Source. Our hydrodynamically-enhanced buffer gas cooled beam is high flux, cold, and slow. We produce beams of ThO with time-averaged fluxes of over 10^13 molecules/state/sr/second moving with a forward velocity of 170 m/s, without the need for stark or optical deceleration.


We would like to thank the National Science Foundation (NSF) and the National Institute of Standards and Technology (NIST) for funding our experiment.