Accessing baryon-antibaryon generalized distribution amplitudes in <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"> <mml:msup> <mml:mi>e</mml:mi> <mml:mo>±</mml:mo> </mml:msup> <mml:mi>γ</mml:mi> <mml:mo stretchy="false">→</

<a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"> <a:msup> <a:mi>γ</a:mi> <a:mo>*</a:mo> </a:msup> <a:mi>γ</a:mi> <a:mo stretchy="false">→</a:mo> <a:mi>B</a:mi> <a:mover accent="true"> <a:mi>B</a:mi> <a:mo stretchy="false">¯</a:mo> </a:mover> </a:math> is the golden process to access chiral-even di-baryon generalized distribution amplitudes (GDAs) as deeply virtual Compton scattering has proven to be for the generalized parton distributions. In the framework of colinear quantum chromodynamics factorization, where the leading twist amplitude is the convolution of GDAs and a perturbatively calculable coefficient function, we study the scattering amplitude for the baryonic channels where <f:math xmlns:f="http://www.w3.org/1998/Math/MathML" display="inline"> <f:mi>B</f:mi> </f:math> is a spin <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"> <h:mn>1</h:mn> <h:mo>/</h:mo> <h:mn>2</h:mn> </h:math> baryon such as the nucleon or hyperon <j:math xmlns:j="http://www.w3.org/1998/Math/MathML" display="inline"> <j:mrow> <j:mi mathvariant="normal">Λ</j:mi> </j:mrow> </j:math> , <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"> <m:mrow> <m:mi mathvariant="normal">Σ</m:mi> </m:mrow> </m:math> . Taking into account the interfering quantum electrodynamics amplitude, we calculate the cross section of the <p:math xmlns:p="http://www.w3.org/1998/Math/MathML" display="inline"> <p:msup> <p:mi>e</p:mi> <p:mo>±</p:mo> </p:msup> <p:mi>γ</p:mi> <p:mo stretchy="false">→</p:mo> <p:msup> <p:mi>e</p:mi> <p:mo>±</p:mo> </p:msup> <p:mi>B</p:mi> <p:mover accent="true"> <p:mi>B</p:mi> <p:mo stretchy="false">¯</p:mo> </p:mover> </p:math> process, which can be experimentally studied in <u:math xmlns:u="http://www.w3.org/1998/Math/MathML" display="inline"> <u:msup> <u:mi>e</u:mi> <u:mo>−</u:mo> </u:msup> <u:msup> <u:mi>e</u:mi> <u:mo>+</u:mo> </u:msup> </u:math> as well as in electron-ion facilities. We explore both the final state polarization summed case and the polarization dependent effects. Numerical estimates are presented for <w:math xmlns:w="http://www.w3.org/1998/Math/MathML" display="inline"> <w:msup> <w:mi>e</w:mi> <w:mo>−</w:mo> </w:msup> <w:mi>γ</w:mi> <w:mo stretchy="false">→</w:mo> <w:msup> <w:mi>e</w:mi> <w:mo>−</w:mo> </w:msup> <w:mi>p</w:mi> <w:mover accent="true"> <w:mi>p</w:mi> <w:mo stretchy="false">¯</w:mo> </w:mover> </w:math> using motivated models for GDAs. Our results show that a first extraction of baryon-antibaryon GDAs from experimental measurements is feasible at Belle II.