Breakdown of collinear factorization in the exclusive photoproduction of a <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msup><mml:mi>π</mml:mi><mml:mn>0</mml:mn></mml:msup><mml:mi>γ</mml:mi></mml:math> pair with larg

We study the exclusive photoproduction of a <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:msup><a:mi>π</a:mi><a:mn>0</a:mn></a:msup><a:mi>γ</a:mi></a:math> pair with large invariant mass <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:msubsup><c:mi>M</c:mi><c:mrow><c:mi>γ</c:mi><c:mi>π</c:mi></c:mrow><c:mn>2</c:mn></c:msubsup></c:math>, which is sensitive to the exchange of either two quarks or two gluons in the <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:mi>t</e:mi></e:math> channel. In this paper, we show that the process involving two-gluon exchanges does factorize in the Bjorken limit at the leading twist. This can be explicitly demonstrated by the fact that there exist diagrams, which contribute at the leading twist, for which are , due to the pinching of the contour integration of the plus and minus component of the Glauber gluon momentum. For the same reason, <g:math xmlns:g="http://www.w3.org/1998/Math/MathML" display="inline"><g:msup><g:mi>π</g:mi><g:mn>0</g:mn></g:msup></g:math>-nucleon scattering to two photons also suffers from the same issue. On the other hand, we stress that there are no issues with respect to collinear factorization for the quark channels. By considering an analysis of all potential reduced diagrams of leading pinch-singular surfaces, we argue that the quark channel is safe from Glauber pinches, and therefore, a collinear factorization in that case follows through without any problems. This means that processes where gluon exchanges are forbidden, such as the exclusive photoproduction of <i:math xmlns:i="http://www.w3.org/1998/Math/MathML" display="inline"><i:msup><i:mi>π</i:mi><i:mo>±</i:mo></i:msup><i:mi>γ</i:mi></i:math> and <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:msup><k:mi>ρ</k:mi><k:mrow><k:mn>0</k:mn><k:mo>,</k:mo><k:mo>±</k:mo></k:mrow></k:msup><k:mi>γ</k:mi></k:math>, are unaffected by the factorization breaking effects we point out in this paper.