Department of Energy sPHENIX Science Review Jamie Nagle (University of Colorado, Boulder) - PowerPoint PPT Presentation

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Department of Energy sPHENIX Science Review Jamie Nagle (University of Colorado, Boulder)
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Department of Energy sPHENIX Science Review Jamie Nagle (University of Colorado, Boulder)

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  1. Department of Energy sPHENIX Science Review Jamie Nagle (University of Colorado, Boulder)

  2. Context • sPHENIX as a science project was initially outlined in the PHENIX Decadal Plan Document in 2010 • Science and Project review run by ALD Steve Vigdor in 2012 based on full MIE Proposal document - “strongly endorsed the science case” • Many developments in the field, technical developments (acquisition of the BaBar Superconducting Magnet), etc. • Development of EIC detector concept built around the BaBar magnet and sPHENIXcalorimetry documented in 2013 • Review of EIC detector concept in January 2014 very positive • “The review team was unanimous in its praise for the Letter of Intent.” • *All documents available at:

  3. Agenda for Today

  4. Review Charge to Assess: • The significance of scientific questions identified by the proposal and Brookhaven National Laboratory • The impact of the planned scientific program on the advancement of nuclear physics in the context of current and planned • world-wide capabilities • The new experimental and theoretical research efforts and technical capabilities needed to accomplish the proposed scientific program • The feasibility of the approach or method presented to carry out the proposed scientific program and the likelihood that significant results can be obtained in the first three years of detector operations

  5. Observables Roadmap Questions Observables Needs Is QGP Coupling Strongest near Tc? Jet inclusive spectra At what length scale does the QGP go from strong to weak coupling? Dijet correlations Jet fragmentation functions How do parton showers evolve in the QGP? g-jet/h correlations Heavy flavor tagged jets Are there quasiparticles in medium? Jet – global event structure observables Are there significant medium response modes to high energy partons? Upsilon three state suppression Large Acceptance High Rate Electron ID Photon ID Full Calorimetric Coverage Are there relevant screening lengths in QGP

  6. Fundamental Physics Goals Mission Need

  7. Emergent Phenomena Connection from the QCD Lagrangian to phenomena of confinement and asymptotic freedom was fundamental Connection from QCD to the emergent phenomena of near perfect fluidity of the Quark-Gluon Plasma near the phase transformation is just as fundamental Pinning down the fluid imperfection (h/s) tells us the nature of the QGP, while leaving open the “how” and “why” questions

  8. Probing the QGP across Length Scales To address these questions, need to probe the QGP at different length scales and particularly in the region of strongest coupling (RHIC) Hard Scattered Partons Traversing the QGP (Jets, Dijets, g-Jet, Fragmentation, Medium Response) length scale set by initial energy, coherent energy lost 20-50 GeV (0.01-0.004 fm), 1-5 GeV (0.2-0.05 fm) Beauty Quarkonia length scale set by size of state (U(1s,2s,3s) ~ 0.28, 0.56, 0.78 fm) Post-QM Meeting (Mont Sainte Odile) Krishna referred to this as microscopy of the QGP Critical to push jets to lower energy, looking for hard radiation to understand what it’s being scattered from?

  9. RHIC Probing Region of Strongest Coupling The textbook (or Wiki entry) on the Quark-Gluon Plasma will be incomplete without a fundamental explanation for how the perfect fluid emerges at strong coupling near Tc from an asymptotically free theory of quarks and gluons Jet observables at RHIC enabled by the sPHENIX upgrade are critical to providing this explanation by probing the QGP near 1-2 Tc and over a broad ranges of scales Measurements of jets only at the LHC will leave these questions with an incomplete answer (particularly right where the coupling may be strongest)

  10. Getting at the Fundamental Science

  11. Quark-Gluon Plasma Physics Quark-Gluon Plasma physics is about the exploring the phase diagram, much like in Condensed Matter Physics Not Energy Frontier Physics Energy Excitation of Observables has proven to be the most valuable for both discovery and precision physics in the field of heavy ions Mix of condensed matter and particle physics terminology Shear viscosity/entropy density = h/s  String theory (quantum) conjectured lowest bound 1/4p  Closer to the bound, more strongly coupled, perfect fluidity (hydrodynamics) Jet quenching = modification of parton shower in the QGP  qhat = transverse momentum square scatter per path length Debye screening = lD = radius of electrostatic influence of charge in plasma

  12. Strongest QGP Coupling Near 1-2 Tc? What does Trace Anomaly tell us? P/T4 deviation from SB? Data from Phys. Rev. D80, 014504 (2009) Some say no information on coupling Caveats of AdS/CFT example RHIC and LHC give a key lever arm in Temperature. If the QGP properties are not different, why not?

  13. Perfect Fluidity Theory for Quark-Gluon Plasma is not yet well constrained on this question Many systems have minimum shear viscosity to entropy density near phase transformation

  14. Indications of Stronger Coupling at RHIC There are indications that the QGP is most strongly coupled as created at RHIC What are the underlying changes in QGP properties near the transition? Calculation from BjoernSchenke

  15. Mapping Out Strong Coupling with Jet Probes “Small Shear Viscosity Implies Strong Jet Quenching” A. Majumder, B. Muller, X.N. Wang, PRL (2007). ^ Key is independently measuring both sides of this equation!

  16. Super-Strong Coupling near Tc? “Jet Quenching is a few times stronger near Tc relative to the QGP at T > Tc.” Liao and Shuryak, PRL (2009) “The surprisingly transparent sQGP at the LHC [compared to RHIC]” Horowitz and Gyulassy, NPA (2011) “Large v2 is striking in that it exceeds expectations of pQCD models even at 10 GeV/c.” PHENIX, PRL (2010)

  17. NTC = Near Tc Enhancement Thorsten Renk: “Comparing weak coupling scenarios with data, NTC is favored. An answer to this question will require a systematic picture across several different high pT observables.” Theorists need to work on acronyms.

  18. Critical Knobs to Turn How do the parton shower and medium evolve together? Can we observe the strongest coupling near Tc definitively What are the inner workings? (quasiparticles, fields, modes)

  19. Virtuality Evolution “RHIC” Scenario T0=300 MeV Parton ET = 30 GeV “LHC” Scenario T0=390 MeV Parton ET = 200 GeV LHC Scenario B. Muller. Nucl.Phys., A855:74–82, 2011, RHIC/AGS Users Meeting 2011

  20. At what length scale is the medium probed? 1/l Do the highest energy jets at LHC see point-like color charges? What sets this scale? • the exchange gluon momentum? • total coherent energy loss? • impact of deconfinement? Do the lowest energy jets at RHIC scatter from coherent fields or only excite sound waves? W. Horowitz

  21. QGP Constituent Mass Dependence qhat scattering of leading parton radiation e-loss ehat  energy transferred to the QGP medium Jet ET = 30 GeV T = 350 MeV as = 0.3 Limit of infinitely massive scattering centers yields all radiative e-loss. Medium parton

  22. Ivan Vitev et al. Radiative + Collisional E-loss ±10% changes in coupling strength Radiative E-loss only E1 > 35 GeV, E2 > 5 GeV MARTINI + MUSIC (dash) Qin + Muller (solid) Au+Au 0-10%, anti-kT R = 0.4 Bjorn Schenke, Clint Young et al. Large effects! Different models matching LHC data disagree on RHIC predictions.

  23. PRL 2011 Guangyou Qin, Berndt Muller Larger modification at RHIC, more of parton shower equilibrated into medium.

  24. RHIC Jet Discriminating Power Major new detector project at RHIC Large coverage calorimetry coupled with high rates

  25. LHC Higher Energy Jet Observations Large suppression of balanced dijets with pT,1 > 120 GeV/c Fully calorimetric measurement, no low pT cutoff on constituents Original expectation is huge suppression of high z Fragmentation Functions. Not observed. Correlated bias in which jets and how much of their energy is reconstructed. Key check with g-jet/h

  26. STAR Jet Program Very good jet capabilities Large acceptance, tracking + EMCal Exciting recent results from QM2014 Trigger on jet > 20 GeV requiring online trigger of > 5.4 GeV in one EMCal tower and all pT > 2 GeV Expect Surface Bias on Trigger And Long Path on Opposite Side However, only modest suppression of balanced jets

  27. Now re-run jet algorithm with all particles around originally found jets Dijet asymmetry identical in pp and AA! Very different result from theory expectations and LHC results. If full jet energy recovered, real unbiased FF measurements available to sPHENIX. Biased di-jet case may select particular geometry. Perhaps biased towards both jets tangential.

  28. Bias Engineering Thorsten Renk has explored the ability to engineer the surface and energy loss bias to gain more information. Works particularly well at RHIC due to steeply falling jet spectrum. sPHENIX can measure these jets with no minimum pT selection and no online trigger bias. Thus, one can explore the full range of engineered geometries. High statistics and full jet energy range enabled. Systematic measurements enabled “tomography” Recently it was proposed that medium response can only be seen when energy loss near surface (so not damped out by medium)

  29. Calorimeter Measure Unbiased on FF Quark and Gluons have very different fragmentation functions sPHENIX calorimetric measurement gives the same energy scale and resolution. Critical for extracting longitudinal redistribution of energy.

  30. Required Theoretical Framework Charge #3: “The new experimental and theoretical research efforts and technical capabilities needed to accomplish the proposed scientific program” One needs robust connection with QCD techniques to calculate key jet observables. Different formalisms incorporating weak and strong coupling are needed to discriminate the underlying physics. March, 2012 at Duke University August, 2013 at Wayne State University Strong theory community, recent significant progress incorporating (1) Soft Co-linear Effective Theory and (2) modeling with transition from weak to strong coupling are good examples.

  31. Theory Tools A host of Monte Carlo parton shower codes are now available to fully interpret the combined set of sPHENIX, RHIC and LHC jet observables. The close collaboration between experimentalists and theorists is necessary to incorporate the full suite of observables and test the basic physics and then constrain the detail parameters. Continued RHIC and LHC data up through sPHENIX program fuels this collaboration. YaJEM (now publicly available) JEWEL (now publicly available) MARTINI CUJET MATTER Q-PYTHIA VNI

  32. sPHENIX Physics Delivery

  33. Physics  sPHENIX  Knowledge How does sPHENIX enable access to this physics?

  34. sPHENIX in a Nutshell BaBar Magnet 1.5 T Coverage |h| < 1.1 All silicon tracking Heavy flavor tagging Electromagnetic Calorimeter Two longitudinal Segment Hadronic Calorimeter Common Silicon Photomultiplier readout for Calorimeters Full clock speed digitizers, digital information for triggering High data acquisition rate capability ~ 10 kHz

  35. sPHENIX Run Plan Two years of physics running 2021 and 2022 with 30-cryo week runs 20 weeks Au+Au @ 200 GeV 10+ weeks p+p @ 200 GeV [comparable baseline statistics] 10+ weeks p+Au @ 200 GeV [comparable baseline/new physics stats] sPHENIX maintains very high PHENIX DAQ rate sPHENIX maintains fast detector capability – no pile up problems If we just record Au+Au minimum bias events (no trigger bias), in 20 weeks with current RHIC performance and PHENIX livetime, we record 50 billion events within |z| < 10 cm [optimal for silicon tracking] Note this is not sampled, but recorded. Full range of differential measurements and centralities with no trigger biases.

  36. Fantastic C-AD Performance Run-14 Au+Au @ 200 GeV has been so successful that with minimal trigger requirements, for high energy jets and photons [with acceptance over the whole z-vertex range] we could sample almost 200 billion in 20 weeks. This assumes no performance improvements from C-AD! Level-1 triggering: EmCal and HCal electronics digitize at full clock speed. Thus, fully digital triggering is a feature with entire calorimeter information brought into one electronics module (i.e. very flexible for jet patch triggering, pairs, etc.) . Also, crucial for p+p and p+Au with minimal bias on jet fragmentation functions, quark versus gluon jets, single high pT hadrons, etc.

  37. sPHENIX Rates: Jets, Dijets, g-Jet Recording 50 billion Au+Au events in one year 107 jets > 20 GeV 106 jets > 30 GeV 80% are dijet events 104 direct g > 20 GeV p+p p(d)+A Differential measures With C-AD delivered results now, of order 200 billion sampled

  38. Direct Photon-Jet/h sPHENIX has excellent direct photon capabilities In Au+Au central collisions for pT > 20 GeV, direct photons dominate S/B > 3 Simple isolation cuts with full calorimetry give additional handle and enable p+p and p+A comparison measurements LHC RHIC

  39. RHIC dominated by “fake jets”? No. arXiv:1203.1353 Phys. Rev. C86 (2012) 024908 Simple Answer = Over Key Kinematic Ranges Jet Physics is accessible with sPHENIX without requiring jet bias cuts Multiple techniques being developed in the field to extract jet results. This is a demonstration of one such technique following the ATLAS method.

  40. Inclusive Jet Spectra 50 billion MB events Example ROOUNFOLD Iterative Bayes Method shows very good result. Full GEANT-4 simulation with FastJet Reconstruction gives good resolution. Jet Transverse Energy (GeV) Jet RAA measurable with high stats

  41. Dijet Asymmetries E1 > 35 GeV, R = 0.3 Truth = solid lines E1 > 35 GeV, R = 0.3 Truth = solid lines Boxes = Measure + Unfold • PYTHIA (vacuum case) • PYQUEN (quenched case) • Full jets + HIJING background + detector resolution + FastJet + underlying event subtraction • Very easily discriminated (large effect) Dijet AJ (E1-E2)/(E1+E2) Dijet AJ (E1-E2)/(E1+E2) Using core calorimeter energy cuts and also hybrid tracking methods one can also reproduce the STAR biased dijet result, again scanning the range of surface bias engineering

  42. Gauging the Sensitivity Using Coleman-Smith’s dijet asymmetry the effective coupling is varied, how well can our projected measurement for 35 GeV jets with R = 0.3 constrain this parameter. Of course, many observables need to be included since there is more than one unknown. The key is over-constraining the problem.

  43. Fragmentation Functions sPHENIX combination of excellent tracking and calorimetric jet reconstruction enable FF measurements Very beneficial that numerator (charge track) and denominator (jet energy) are measured separately. Dramatically reduces high-z backgrounds Again, key measurement across all Au+Au centralities and with different jet definitions Key to compare with g-h sPHENIX statistics for Au+Au in 20 weeks

  44. Beauty Tagged Jets Charm Beauty tagged jets with sPHENIX Substantial rate and tagged with large displaced vertex using inner silicon detector Beauty Run-14 Au+Au VTX DCA Resolution Key tests of mass dependence of radiative energy loss Again, crucial to have overlapping energy ranges with RHIC and LHC

  45. Length Scale QQbar Probes PHENIX, STAR, and CMS data consistent with melting of U(2s,3s) Controls: PHENIX d+Au J/y Npart y’

  46. sPHENIX Upsilon Measurements Extremely exciting LHC Upsilon results Key to map out temperature dependence in A+A combined with p+p and p+A with good statistics 46

  47. No one key Observable, Instead a Data Army Bulk QGP Constraints (h/s example) Very close coordinated effort by experimentalists and theorists spectra, v2 vn, HBT  HBT versus Yn, direct photons  photon vn Over-constraining the theory  Current “Standard Little Bang” Model Path to precision QGP bulk properties Jet Probe Physics Not one key observable alone. It is the army of observables in concert with theory that has the physics pay-off.

  48. Summary We believe in this physics and have an excited group of people who want to turn sPHENIX into reality Energy Excitation of Observables has proven to be the most valuable for both discovery and precision physics in the field of heavy ions

  49. Talk #2

  50. sPHENIX in World Context Jamie Nagle (University of Colorado, Boulder)