logging in or signing up RHIC spin talk Heather Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 27 Category: Entertainment License: All Rights Reserved Like it (0) Dislike it (0) Added: November 15, 2007 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Slide1: March 9. 2004@RHIC-SPIN Discussion Y. Koike (BNL&Niigata Univ.) Single Transverse Spin Asymmetry : Theoretical OverviewSlide2: Content: Introduction: Basics for single spin asymmetry (SSA) Data, Ingredients of SSA, “T-odd” observable, SSA and chiral symmetry breaking. T-odd distribution and fragmentation functions. Twist-3 effects Summary Slide4: Single Spin Asymmetry (SSA) E704(’91) and STAR(’02) found big asymmetry in the forward direction !Slide5: FNAL-E704:Slide6: RHIC-STAR, hep-ex/0310068Slide7: Fundamentals of SSA: Ingredients for SSA BUT, in conventional twist-2: Other mechanisms necessary for a big SSA!Slide8: Origin of “T-Odd” observable By T-inv. (De Rujula et al. NP,B35(’71)365)Slide9: Usual twist-2:Slide10: “T-odd” Twist-3 Sivers Collins Qiu&StermanSlide12: “T-odd” mechanism: Introduction of nonperturbative intrinsic k_T of partons. Intuitively understandable. Smooth start of SSA at low P_T: (Collins’93) Factorization theorem ?Slide15: Applications of “T-odd” functionsSlide16: Applications of “T-odd” functions (continued)Slide17: (Sivers) (Collins)Slide18: FNAL-E704:Slide21: Twist-3 mechanism for SSA Systematic approach based on collinear factorization P_T is produced solely from the partonic hard cross section Suited for large-P_T production SSA is a probe of quark-gluon correlation. SSA is 1/Q suppressed: At what P_T, does the data fall on twist-3 mechanism? Twist-3 functions are all “T-even”.Slide23: Factorization for twist-3: three twist-3 cross sections (Qiu&Sterman’99) (Kanazawa&Koike’00) (Koike’02) Unpolarized: twist-2 :Hard partSlide26: Characteristics of the twist-3 analysis (cf. Qiu & Sterman ’91 for p+p↑→γ+X) Slide27: Characteristics of the twist-3 analysis (continued)Slide29: RHIC-STAR, hep-ex/0310068Slide31: FNAL-E704: P.L. B264 (’91) 462 P.L. B261 (’91) 201 A. Bravar, Proc. of Spin’96 Slide33: : Chiral-odd Summary table of “T-odd” and Soft-gluon-pole (SGP) functionsSlide34: Summary and outlook You do not have the permission to view this presentation. In order to view it, please contact the author of the presentation.
RHIC spin talk Heather Download Post to : URL : Related Presentations : Share Add to Flag Embed Email Send to Blogs and Networks Add to Channel Uploaded from authorPOINTLite Insert YouTube videos in PowerPont slides with aS Desktop Copy embed code: (To copy code, click on the text box) Embed: URL: Thumbnail: WordPress Embed Customize Embed The presentation is successfully added In Your Favorites. Views: 27 Category: Entertainment License: All Rights Reserved Like it (0) Dislike it (0) Added: November 15, 2007 This Presentation is Public Favorites: 0 Presentation Description No description available. Comments Posting comment... Premium member Presentation Transcript Slide1: March 9. 2004@RHIC-SPIN Discussion Y. Koike (BNL&Niigata Univ.) Single Transverse Spin Asymmetry : Theoretical OverviewSlide2: Content: Introduction: Basics for single spin asymmetry (SSA) Data, Ingredients of SSA, “T-odd” observable, SSA and chiral symmetry breaking. T-odd distribution and fragmentation functions. Twist-3 effects Summary Slide4: Single Spin Asymmetry (SSA) E704(’91) and STAR(’02) found big asymmetry in the forward direction !Slide5: FNAL-E704:Slide6: RHIC-STAR, hep-ex/0310068Slide7: Fundamentals of SSA: Ingredients for SSA BUT, in conventional twist-2: Other mechanisms necessary for a big SSA!Slide8: Origin of “T-Odd” observable By T-inv. (De Rujula et al. NP,B35(’71)365)Slide9: Usual twist-2:Slide10: “T-odd” Twist-3 Sivers Collins Qiu&StermanSlide12: “T-odd” mechanism: Introduction of nonperturbative intrinsic k_T of partons. Intuitively understandable. Smooth start of SSA at low P_T: (Collins’93) Factorization theorem ?Slide15: Applications of “T-odd” functionsSlide16: Applications of “T-odd” functions (continued)Slide17: (Sivers) (Collins)Slide18: FNAL-E704:Slide21: Twist-3 mechanism for SSA Systematic approach based on collinear factorization P_T is produced solely from the partonic hard cross section Suited for large-P_T production SSA is a probe of quark-gluon correlation. SSA is 1/Q suppressed: At what P_T, does the data fall on twist-3 mechanism? Twist-3 functions are all “T-even”.Slide23: Factorization for twist-3: three twist-3 cross sections (Qiu&Sterman’99) (Kanazawa&Koike’00) (Koike’02) Unpolarized: twist-2 :Hard partSlide26: Characteristics of the twist-3 analysis (cf. Qiu & Sterman ’91 for p+p↑→γ+X) Slide27: Characteristics of the twist-3 analysis (continued)Slide29: RHIC-STAR, hep-ex/0310068Slide31: FNAL-E704: P.L. B264 (’91) 462 P.L. B261 (’91) 201 A. Bravar, Proc. of Spin’96 Slide33: : Chiral-odd Summary table of “T-odd” and Soft-gluon-pole (SGP) functionsSlide34: Summary and outlook