In the standard model of particle physics, the electron’s electric dipole moment (EDM) should be somewhere around 10[sup]-38[/sup] e-cm. Current experimental limits sit around 10[sup]-27[/sup] e-cm. This new material, the authors say, should help the solid-state experimental technique push this limit down, initially to 10[sup]-28[/sup] e-cm, but groups are already aiming at 10[sup]-32[/sup] e-cm and beyond.
Why do we care?
A non-zero electron EDM is a fundamentally CP-violating phenomenon. Since the only known CP violation in the standard model comes from the weak interactions of quarks, and since electrons don’t interact with quarks directly via the weak interaction, a non-zero electron EDM comes about only through so-called loop corrections – smaller and smaller terms in the calculation’s perturbation series. [If it helps, note that a Taylor series is a type of perturbation series.] Each term in the series is representable by a Feynman diagram with some number of virtual particle loops, and the more loops you have, the smaller the term (more or less).
It turns out that if you add up all the 0-loop, 1-loop, and 2-loop contributions to the EDM, you get zero. You have to go to three loops before the standard model CP violation stops canceling out in the calculation. This is why the predicted value is so small. (That, plus the CP violation present in the quark sector isn’t all that great to begin with.)
The complete series involves all permutations of loops and particles and interactions. So, if you have a Feynman diagram that has an up-quark loop, you also have that same one with a top-quark loop. Since the up and top quarks have different masses, the terms that their diagrams represent have different values. (General rule: heavier loop particle, larger term).
Now, the calculation that leads to 10[sup]-38[/sup] e-cm includes all known particles and interactions in its list of Feynman diagram “permutations”. But, if there are unknown particles out there, perhaps ones too heavy to have yet been observed directly, they would add additional terms to the series. Some run-of-the-mill supersymmetry models, for example, include particles that, when included in the loop tallies, bring the EDM expectation up near the experimental limit (10[sup]-27[/sup] e-cm or so). [To be sure, there are models that would predict an EDM even larger, but they have already been ruled out.]
So, if one observes a larger-than-standard-model value for the electron EDM, it points immediately to new physics (one example of which I’ve hinted at above, although scores of possibilities are discussed.)