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Conclusions

In summary, RHIC will access tex2html_wrap_inline2370 in the prompt- tex2html_wrap_inline2248 plus away-side jet channel at tex2html_wrap_inline2496 over the interval tex2html_wrap_inline2498 with a sensitivity on tex2html_wrap_inline2260 of about 0.05-0.1. The interpretation of other channels, like the inclusive prompt- tex2html_wrap_inline2248 (no away-side jet tagging), inclusive single jet and di-jet events, is more delicate. The tex2html_wrap_inline2240 region covered by RHIC (0.03-0.1) is lower than the tex2html_wrap_inline2240 interval covered in COMPASS (0.08-0.35). In Figure 2.3 the tex2html_wrap_inline2240 intervals covered in different measurements are compared. At RHIC the tex2html_wrap_inline2416 scale is about a few 100's GeV tex2html_wrap_inline2256 and in COMPASS tex2html_wrap_inline2514  10 GeV tex2html_wrap_inline2256 . The expected accuracy at RHIC for the prompt- tex2html_wrap_inline2248 plus away-side jet is similar to the one expected in COMPASS in the open charm process. In any case a deeper discussion of systematic effects at RHIC is desirable, before any final conclusion on that can be drawn. COMPASS can provide significant results on the proton spin structure already in 2002, while RHIC could most likely come up with first results not before the year 2003.

   figure763
Figure 2.3: Comparison of gluon momentum fraction intervals covered in different measurements.

It is clear that RHIC as a polarized collider will have a far reaching agenda and impact on spin physics for many years to come. However, on the short and medium time scale, COMPASS is likely to provide sooner crucial answers on the specific questions of the proton spin structure.



Lars Schmitt
Wed May 22 16:44:09 METDST 1996