1 / 12

A Tale of Two (Toy) Models

A Tale of Two (Toy) Models. CERN Courier: July, 2007 Harry Lee, Dan Carman, Reinhard Schumacher, MM Two possible pictures of how spin is transferred from virtual photon to the L. Carman, MM: photon to u-quark; through s-sbar spin correlation to L . Schumacher: directly from photon

nat
Télécharger la présentation

A Tale of Two (Toy) Models

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. A Tale of Two (Toy) Models CERN Courier: July, 2007 Harry Lee, Dan Carman, Reinhard Schumacher, MM Two possible pictures of how spin is transferred from virtual photon to the L. Carman, MM: photon to u-quark; through s-sbar spin correlation to L. Schumacher: directly from photon to s-sbar to L. Problem: both consistent with data! How (else) to distinguish models?

  2. Quark Pair Creation • Quark-pair creation: “kernel” of exclusive production • What field couples to the q-q current? u d S L ss produced From flux-tube s u s u K+ ss produced from photon K+ s u d L

  3. Using Exclusive Production to Study Quark Pair Creation • Lund model: successful phenomenology for hadron production; e.g. in e+e- reactions • color flux-tube broken by qq production • production rate depends on constituent quark mass • : : ~ 1 : 1 : 0.2 • Vector meson dominance: photon fluctuates into a virtual qq meson • production rate depends on quark charge • : : ~ 1: 0.25 : 0.25 ss ss uu uu dd dd

  4. Distinguish ModelsStudy ratios of s s : dd : uu • Measure ratios: K+L : p+n : p0p K+ p0 p+ s d u n p L s u d 0.2 : 1 : 1 Ratio : exponential in quark mass

  5. Distinguish Models • Measure ratios: K+L : p+n : p0p K+ L n p s d u s p+ p0 d u 1 : 1 : 4 Ratio : proportional to (charge)2

  6. 90k 420k 540k 480k • Missing Mass • 2-body final state (n) p+a P (p0)a ~0 84k 350k 910k forward f Lab Angle g backward

  7. 50k 150k 45k 5k K+ Missing Mass (L) K+a “Fake” plots mis-identified protons mis-identified pions forward f Lab Angle g backward

  8. Limits of the “quark model” ? Can the Lund model work in the limit of single qq pair production? • recent analysis of a Hall C p+(n) production experiment • Kaskulov, Gallmeister, Mosel; arXiv:0804.1834v4 [hep-ph] • model was developed to explain Rosenbluth separated exclusive electro-production of p+(n) asLdescribed well as t-channel exchange asTdescribed well as “quark-scattering followed by string-breaking” with Lund model parameters • model also works for un-separated data

  9. Exclusive np+: sum of two processes sT: DIS via LUND model sL: t-channel exchange u d d photon probes meson structure n photon couples to quark d u p+ t-channel no form factor: q2 independent form factor falls with q2

  10. Analysis goals and plans • Model-independent goal • measure ratio of p+n : p0p : K+L cross-sections • proportional to uu : dd : ss rate • Extend Kaskulov, Gallmeister, Mosel model • extend to dd and ss production • Analysis plan • identify final states (done) • decide on binning ( high/low bins for W, q2, t ) • tune PYTHIA/JETSET (fitting and MC generator) • Study single quark-pair creation

  11. An interesting observation …. For forward-going protons (qLAB < 200) : only recoil meson is the r0 ??

  12. And the winner is …. crude accepance correction done; kaon decay not corrected Ratio: K+L : p+n : p0p 0.23 : 0.88 : 1.12 errors ~ 20% ??

More Related