Answers are grounded in this paper and cite their sources.
We introduce an anomaly-based framework to probe quark electric dipole moments in exclusive hadronic final states produced in <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msup> <a:mi>e</a:mi> <a:mo>+</a:mo> </a:msup> <a:msup> <a:mi>e</a:mi> <a:mo>−</a:mo> </a:msup> </a:math> annihilation. Chern-Simons-induced anomalous couplings yield a clean T-odd asymmetry <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"> <c:msub> <c:mi>A</c:mi> <c:mi>T</c:mi> </c:msub> </c:math> from interference between the Standard-Model amplitude and dipole-moment contributions. As an application, <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"> <e:msup> <e:mi>γ</e:mi> <e:mo>*</e:mo> </e:msup> <e:mo stretchy="false">→</e:mo> <e:msup> <e:mi>K</e:mi> <e:mo>+</e:mo> </e:msup> <e:msup> <e:mi>K</e:mi> <e:mo>−</e:mo> </e:msup> <e:msup> <e:mi>π</e:mi> <e:mn>0</e:mn> </e:msup> </e:math> provides direct sensitivity to the strange-quark electric dipole moment (EDM) <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"> <h:msub> <h:mi>d</h:mi> <h:mi>s</h:mi> </h:msub> </h:math> in the chiral limit. The precision on <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"> <j:msub> <j:mi>d</j:mi> <j:mi>s</j:mi> </j:msub> </j:math> can reach <l:math xmlns:l="http://www.w3.org/1998/Math/MathML" display="inline"> <l:mi mathvariant="script">O</l:mi> <l:mo stretchy="false">(</l:mo> <l:msup> <l:mn>10</l:mn> <l:mrow> <l:mo>−</l:mo> <l:mn>16</l:mn> </l:mrow> </l:msup> <l:mo stretchy="false">)</l:mo> <l:mtext> </l:mtext> <l:mtext> </l:mtext> <l:mi>e</l:mi> <l:mtext> </l:mtext> <l:mi>cm</l:mi> </l:math> with existing CMD–3 data and <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"> <q:mrow> <q:mi mathvariant="script">O</q:mi> <q:mo stretchy="false">(</q:mo> <q:msup> <q:mrow> <q:mn>10</q:mn> </q:mrow> <q:mrow> <q:mo>−</q:mo> <q:mn>18</q:mn> </q:mrow> </q:msup> <q:mo stretchy="false">)</q:mo> <q:mtext> </q:mtext> <q:mtext> </q:mtext> <q:mi>e</q:mi> <q:mtext> </q:mtext> <q:mi>cm</q:mi> </q:mrow> </q:math> using current <v:math xmlns:v="http://www.w3.org/1998/Math/MathML" display="inline"> <v:mi>J</v:mi> <v:mo>/</v:mo> <v:mi>ψ</v:mi> </v:math> samples at BESIII, improving the current direct constraint from hyperon EDM by two to three orders.
No takes yet. Share an insight, caveat, or question.
Geng et al. (2026) studied this question.
Synapse has enriched 10 related papers. Consider them for comparative context: