One limitation of rapidity gap techniques is that the requirement of a rapidity gap reduces the fiducial volume of the detector. The use of a scattered proton as the diffractive tag, on the other hand, allows the full rapidity range of the detector to be exploited to study the diffractive system. This would in turn allow a search for the effects of the super-hard pomeron, which is expected to frequently result in back-scattered jets in the rapidity interval normally used to tag rapidity gaps. The super-hard pomeron is of great theoretical interest [23], part of which stems from the fact that if the entire pomeron momentum participates in the hard scatter, there is a dramatic increase in the cross section for the diffractive production of heavy objects, such as b quarks [24]. The cross section for hard double pomeron exchange is also enhanced by super-hard pomeron exchange [25, 26].