1 / 22

Diffractive Higgs (and c ) production

Diffractive Higgs (and c ) production. K aidalov, K hoze, M artin, R yskin, S tirling. Introduction SM Higgs pp  p + H + p Calculation of bb bar background 0 + and 0 - Higgs diffractive production SUSY Higgs diffractive production diffractive c meson production.

tavia
Télécharger la présentation

Diffractive Higgs (and c ) production

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. Diffractive Higgs (and c) production Kaidalov,Khoze,Martin,Ryskin,Stirling • Introduction • SM Higgs pp  p + H + p • Calculation of bbbar background • 0+ and 0-Higgs diffractive production • SUSY Higgs diffractive production • diffractive c meson production DIS 2004, Strbske Pleso, Slovakia Alan Martin (IPPP,Durham)

  2. pp p + H + p

  3. no emission when (l ~ 1/kt) > (d ~ 1/Qt) i.e. only emission withkt > Qt

  4. calculated using detailed 2-channel eikonal global analysis of soft pp data S2 = 0.026 at LHC S2 = 0.05 at Tevatron Lonnblad Monte Carlo S2 = 0.026 S2 = 0.040 MH=120GeV

  5. + collinearity + “gapiness”

  6. Summary for SM diffractive signal

  7. ppp1 + higgs + p2 higgs

  8. rescatt. corr. omitted S2=1

  9. more peripheral p1T,p2T correlations reflect spin-parity of central system: can distinguish 0- from 0+ pp  p1 + H + p2

  10. decoupling regime: mA ~ mH large h = SM intense coup: mh ~ mA ~ mH gg,WW.. coup. suppressed

  11. SM: pp  p + (Hbb) + p S/B~11/4 with DM = 1 GeV, at LHC with 30 fb-1 e.g. mA = 130 GeV, tan b = 50 (difficult for conventional detection, but exclusive diffractive favourable) S B mh = 124.4 GeV 71 3 events mH = 135.5 GeV 124 2 mA = 130 GeV 1 2 enhancement

  12. 5s signal at LHC 30 fb-1 300 fb-1

  13. KMR+Stirling Diffractive c production only order-of-magnitude estimates possible for c production

  14. Conclusions Proton tagging is a valuable weapon in LHC Higgs physics pp  p + H + p: S/B~3, DMmiss~1GeV, Mmiss = Mbb SUSY Higgs: unique signals in certain domains of MSSM tan b large (i) mh~mH~mA (s enhanced), (ii) mA large Exclusive double diff. prod. strongly favours 0+ Azimuthal correlations are valuable spin-parity analyzer Distinguish 0- from 0+ Higgs Large rate for diffractive c production: probes low x, low Q2 gluons  pQCD ?  probes dynamics -- potential spin-parity (quantum no.) analyzer

More Related