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Extra resources for Predictions and Uncertainties for RHIC Spin Physics [RIKEN BNL Workshop proc]
Measurements of the nucleon structure functions F2 (5, Q2), helicity average, and 91(x, Q2), helicity difference, have explored the helicity conserving part of the In contrast, no information is presently available cross section with great experimental accuracy. on the helicity flip amplitude. The absence of experimental measurements is a consequence of the chiral odd nature of the helicity flip amplitude and the related “transversity quark distributions”, 6q(z, Q2), which prevents the appearance of helicity flip contributions at leading twist in inclusive DIS experiments.
S. Rev. D57. 5920(1998), J. Tang, hepph/9807560 i 1999). 54 and J. Tang, Thesis. 1IIT 5 _ --. _................................................. ....... . . . . . *.. )j.... $3 F \ & IF . 6.. 55 hl 0 ““,“” I , Fz zi ip.. : \ .. _ , ; + 1 \\ \ ’ \ 1 \ -~~ u-l ,\ 1 \g 56 Interference Fragmentation d2M 0~sin60eiao(K~&(z)+A~&&(z) dzdm2 sin 61e-z61+ . , ij, (z),&j, (z) : spin average and dif ference fragmentation functions e Bin + Non-vanishing only in the p “support” mass region! d Sufficient mass Resolution?
5 13. Jaffe et al.. Phys. Rev. D57. 5920(1998). ( 1999). J. J. Tarly. Thesis. \IIT Transversity Measurement with PHENIX Matthias Grosse Perdekamp, RIKEN BNL Center Hard lepton-nucleon and hadron-hadron scattering cross sections can be expressed with the help of three independent helicity ampliitudes. Measurements of the nucleon structure functions F~(z, Q2), helicity average, and gi (z, Q2), helicity difference, have explored the helicity conserving part of the cross section with great experimental accuracy.
Predictions and Uncertainties for RHIC Spin Physics [RIKEN BNL Workshop proc]