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Measurement of Upsilon “Polarization”

Measurement of Upsilon “Polarization”. Matthew Jones Purdue University. Run I Quarkonia Cross Sections. Phys. Rev. Lett. 75 , 4358 (1995). Phys. Rev. Lett. 79, 572 (1997). Excess observed in both prompt J/ ψ and ϒ cross sections Color octet production mechanisms

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Measurement of Upsilon “Polarization”

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  1. Measurement of Upsilon “Polarization” Matthew Jones Purdue University CDF Collaboration Meeting

  2. Run I Quarkonia Cross Sections Phys. Rev. Lett. 75, 4358 (1995) Phys. Rev. Lett. 79, 572 (1997) • Excess observed in both prompt J/ψ and ϒ cross sections Color octet production mechanisms Polarization measurements Direct + feed-down from decays Direct CDF Collaboration Meeting

  3. Upsilon “Polarization” • A better term is spin alignment… • Transverse polarization: • Longitudinal polarization: μ+ θ* ϒ momentum μ- CDF Collaboration Meeting

  4. Published ϒ(1S) Polarization • CDF found no polarization in Run I • DØ finds it to be longitudinal, then transverse • The lack of polarization is somewhat unexpected… CDF Collaboration Meeting

  5. Maybe not even wrong... • The current situation is unsatisfactory... are we missing something obvious? • Back to the fundamentals: • General state for a spin-1 particle: • Angular distribution when decaying to μ+μ-: Pietro Faccioli emphasizes basic quantum mechanics... Un-polarized only when all λθ, λφ and λθφ are all zero. CDF Collaboration Meeting

  6. New CDF Analysis • Goals: • Measure all three parameters simultaneously • Measure in Collins-Soper and S-channel helicity frame • Test self-consistency by calculating rotationally invariant combinations of λθ, λφ and λθφ • Minimize sensitivity to modeling the ϒ(nS) resonance line shape • Explicit measurement of angular distribution of di-muon background CDF Collaboration Meeting

  7. Method • Uses 6.7 fb-1 of jbmm dataset • UPSILON_CMUP_CMU and UPSILON_CMUP_CMX trigger paths • Factor acceptance and angular distribution: • A(cosθ,φ) from high statistics Monte Carlo • w(cosθ,φ; λθ, λφ,λθφ ) from angular distribution • Performed binned likelihood fit to observed distribution of (cosθ,φ) to determine λθ, λφ,λθφ. CDF Collaboration Meeting

  8. Method • Level 1 trigger efficiency from Bs μ+μ- analysis. • Level 2 CMP trigger efficiency measured using J/ψ μ+μ- sample. • Generated, simulated and reconstructed well over 109 decays on namgrid. • Two component fit: • signal + background CDF Collaboration Meeting

  9. Background • The sub-sample containing a displaced track (|d0| > 150 μm) is a good description of the background under the ϒ(nS): CDF Collaboration Meeting

  10. Angular distributions in sidebands • Prompt (histogram) and displaced (error bars) angular distributions match in the sidebands. • We use the displaced muon sample to constrain the angular distribution of background under the ϒ(nS) peaks. CDF Collaboration Meeting

  11. Fits to signal + background • The fit provides a good description of the angular distribution in both background and in signal + background mass bins. Only background Signal + background CDF Collaboration Meeting

  12. Fitted Parameters Signal and background have very different angular distributions. Background is highly “polarized” but the signal is not. CDF Collaboration Meeting

  13. Consistency Tests It can be shown that the expression Is the same in all reference frames. We observe that indeed it is. CDF Collaboration Meeting

  14. Final Results for ϒ(1S) state • λθ • λφ • λθφ • Similar results for 2S and 3S states. • λθ • λφ • λθφ CDF Collaboration Meeting

  15. Comparison with previous results • Agrees with previous CDF publication, χ2/dof = 2.1/4 • Does not agree with result from DØ, χ2/dof = 35.2/7 • Maybe different rapidity coverage? CDF Collaboration Meeting

  16. Summary • First complete measurement of angular distribution of ϒ(nS) decays at a hadron collider. • First measurement ofany aspect of ϒ(3S) angular distribution. • First demonstration of consistency in multiple reference frames • Still not much evidence for the strong polarization predicted by NRQCD or kT models. • Invaluable input from Jonathan, Jim, Diego, Vaia, Rob. • Pre-blessed in early September, blessing today at noon. CDF Collaboration Meeting

  17. The Tevatron: a Quarkonium factory • DØ J/ψ production: • Phys. Lett. B370, 239 (1996). (Inclusive J/ψ) • Phys. Rev. Lett. 82, 35 (1999). (forward J/ψ) • CDF J/ψ and ψ(2S) production: • Phys. Rev. Lett. 79, 572 (1997). (J/ψ and ψ(2S) cross section) • Phys. Rev. D71, 032001 (2005). (Inclusive J/ψ) • Phys. Rev. D66, 092001 (2002). (forward J/ψ) • Phys. Rev. D80, 031103 (2009). (ψ(2S) cross section) • Phys. Rev. Lett. 99, 132001 (2007). (J/ψ and ψ(2S) polarization) • DØ ϒ(1S) cross section, polarization • Phys. Rev. Lett. 94, 232001 (2005). (ϒ(1S) cross section) • Phys. Rev. Lett. 100, 049902 (2008). (with updated integrated luminosity) • Phys. Rev. Lett. 101, 182004 (2008). (polarization) • CDF ϒ(1S) production • Phys. Rev. Lett. 75, 4358 (1995). (ϒ(ns) cross section) • Phys. Rev. Lett. 84, 2094 (2000). • Phys. Rev. Lett. 88, 161802 (2002). (ϒ(ns) cross section and polarization) CDF Collaboration Meeting

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