5/2/08 William Horowitz Yale-Columbia Fest 2008 1 Zero th Order Heavy Quark Photon/Gluon Bremsstrahlung William Horowitz Columbia University Frankfurt.

Slides:



Advertisements
Similar presentations
W. A. Horowitz Quark Matter 2005 A Promising Solution to the Elliptic Quench Puzzle at RHIC William A. Horowitz Columbia University August 4-5, 2005.
Advertisements

Charm & bottom RHIC Shingo Sakai Univ. of California, Los Angeles 1.
21/05/07 William Horowitz CERN Heavy Ion Forum 1 Possible String Theoretic Deviations from pQCD in Heavy Quark Energy Loss at LHC William Horowitz Columbia.
M. Djordjevic 1 Open questions in heavy flavor physics at RHIC Magdalena Djordjevic The Ohio State University.
M. Djordjevic 1 Heavy quark energy loss puzzle at RHIC Magdalena Djordjevic The Ohio State University.
Understanding Jet Energy Loss with Angular Correlation Studies in PHENIX Ali Hanks for the PHENIX Collaboration 24 th Winter Workshop on Nuclear Dynamics.
Andrej Ficnar Columbia University INT 10-2A June 25, 2010 High order DGLV Monte Carlo and q models of jet quenching ^
#: 1... and your jet energy loss calculation? What drives you? aka Perturbative jet energy loss mechanisms: Learning from RHIC, extrapolating to LHC Simon.
4/9/08 William Horowitz WWND Zero th Order Heavy Quark Photon/Gluon Bremsstrahlung William Horowitz Columbia University Frankfurt Institute for.
Understanding Jet Energy Loss with Angular Correlation Studies in PHENIX Ali Hanks for the PHENIX Collaboration 24 th Winter Workshop on Nuclear Dynamics.
Luan Cheng (Institute of Particle Physics, Huazhong Normal University) I. Introduction II. Interaction Potential with Flow III. Flow Effects on Light Quark.
Single & Dihadron Suppression at RHIC and LHC Xin-Nian Wang Lawrence Berkeley National Laboratory Last call for prediction for LHC, CERN, May 29-June 2,2007.
1 Heavy Quark Energy Loss Tatia Engelmore Journal Club 7/21.
6/1/07 William Horowitz CERN Heavy Ion Forum 1 Possible String Theoretic Deviations from pQCD in Heavy Quark Energy Loss at LHC William Horowitz Columbia.
2/7/09 William Horowitz High-p T Physics at LHC1 Testing AdS/CFT at LHC William Horowitz The Ohio State University February 6, 2009 With many thanks to.
M. Djordjevic 1 Effect of dynamical QCD medium on radiative heavy quark energy loss Magdalena Djordjevic The Ohio State University.
M. Djordjevic 1 Heavy quark energy loss in a dynamical QCD medium Magdalena Djordjevic The Ohio State University M. Djordjevic and U. Heinz, arXiv:
Marco van Leeuwen, Marta Verweij, Utrecht University Energy loss in a realistic geometry.
7/7/09 William Horowitz WHDG Brick and Comparing WHDG to ASW-SH William Horowitz The Ohio State University July 7, 2009 With many thanks to Brian Cole,
Light quarks in AdS/CFT can be modeled by strings with one endpoint ending on a D7-brane in the bulk of AdS 5. A possible way to model a light quark-anti.
6/26/07 William Horowitz SQM pQCD vs. AdS/CFT Tested by Heavy Quark Energy Loss William Horowitz Columbia University Frankfurt Institute for Advanced.
1/31/07William Horowitz Yale-Columbia Fest Spring ‘07 1 pQCD vs. String Theory: LHC Heavy Flavors to Decide William Horowitz Columbia University January.
11/15/06 William Horowitz 1 LHC Predictions 1 from an extended theory 2 with Elastic, Inelastic, and Path Length Fluctuating Jet Energy Loss William Horowitz.
6/6/06William Horowitz Hard Probes Overcoming Fragility William Horowitz Columbia University June 14, 2006 With many thanks to Simon Wicks, Azfar.
10/26/07 William Horowitz AdS Strings Intersect with Nuclear Beams at Columbia 1 Probing AdS/CFT with Heavy Quarks William Horowitz Columbia University.
6/6/06William Horowitz RHIC & AGS Annual Users’ Meeting ‘06 1 Heavy Quark Energy Loss William Horowitz Columbia University June 6, 2006 With many thanks.
11/1/06William Horowitz 1 Jet Quenching at RHIC and the LHC William Horowitz Columbia University November 1, 2006 With many thanks to Simon Wicks, Azfar.
Luan Cheng (Institute of Particle Physics, Huazhong Normal University) I.Introduction II. Potential Model with Flow III.Flow Effects on Parton Energy Loss.
Jet energy loss at RHIC and LHC including collisional and radiative and geometric fluctuations Simon Wicks, QM2006 Work done with Miklos Gyulassy, William.
8/31/07 William Horowitz Nuclear Theory/RIKEN Seminar 1 pQCD vs. AdS/CFT Tested by Heavy Quark Energy Loss William Horowitz Columbia University Frankfurt.
M. Djordjevic 1 Theoretical predictions of jet suppression: a systematic comparison with RHIC and LHC data Magdalena Djordjevic Institute of Physics Belgrade,
11/02/07 William Horowitz Heavy Quark Workshop, LBNL 1 Falsifying AdS/CFT Drag or pQCD Heavy Quark Energy Loss with A+A at RHIC and LHC William Horowitz.
1/22/08 William Horowitz Heavy Quark Physics in Nucleus-Nucleus Collisions, UCLA 1 Shock Treatment: Heavy Quark Drag in Novel AdS Geometries William Horowitz.
NEUTRAL MESON PRODUCTION IN PP AND PB-PB COLLISIONS AT LHC Dmitry Blau, for the ALICE collaboration NRC “Kurchatov Institute” LHC on the March
Simon Wicks Columbia University Work done with William Horowitz, Magdalena Djordjevic and Miklos Gyulassy with input from Azfar Adil BNL Heavy Flavor Workshop,
Direct photon production in heavy-ion collisions Ben-Wei Zhang T-16, Los Alamos National Laboratory Collaborator: Ivan Vitev.
1 Fukutaro Kajihara (CNS, University of Tokyo) for the PHENIX Collaboration Heavy Quark Measurement by Single Electrons in the PHENIX Experiment.
Radiative heavy quark energy loss in QCD matter Magdalena Djordjevic and Miklos Gyulassy Columbia University.
Diagnosing energy loss: PHENIX results on high-p T hadron spectra Baldo Sahlmüller, University of Münster for the PHENIX collaboration.
Heavy Quark Energy Loss with Twist Expansion Approach Ben-Wei Zhang Institute of Particle Physics Central China Normal Univeristy CCAST, Beijing --- Augest.
Elastic, Inelastic and Path Length Fluctuations in Jet Tomography Simon Wicks Hard Probes 2006 Work done with William Horowitz, Magdalena Djordjevic and.
Enke Wang (Institute of Particle Physics, Huazhong Normal University) I. Introduction II. Ineraction Potential with Flow III.Flow Effects on Light Quark.
QM04 1/12/04M. Djordjevic 1 Heavy quark energy loss-Applications to RHIC Magdalena Djordjevic and Miklos Gyulassy Columbia University The Ter-Mikayelian.
12/16/08 William Horowitz TECHQM 2 nd Workshop, LBNL 1 DGLV : M. Djordjevic and M. Gyulassy, Nucl.Phys.A733, 265 (2004) [nucl-th/ ] WHDG : S. Wicks,
M. Djordjevic 1 Heavy Quark Energy Loss in Nucleus-Nucleus Collisions Magdalena Djordjevic The Ohio State University.
Heavy quark energy loss in hot and dense nuclear matter Shanshan Cao In Collaboration with G.Y. Qin, S.A. Bass and B. Mueller Duke University.
M. Djordjevic 1 Heavy flavor suppression in a dynamical medium with finite magnetic mass Magdalena Djordjevic Institute of Physics Belgrade, University.
M. Djordjevic 1 Heavy quark energy loss in a dynamical QCD medium Magdalena Djordjevic The Ohio State University M. Djordjevic and U. Heinz, arXiv:
M. Djordjevic 1 Hard probes at RHIC and LHC Magdalena Djordjevic Ohio State University.
M. Djordjevic 1 Suppression and energy loss in Quark-Gluon Plasma Magdalena Djordjevic Institute of Physics Belgrade, University of Belgrade.
Heavy Flavor Measurements at RHIC&LHC W. Xie (Purdue University, West Lafayette) W. Xie (Purdue University, West Lafayette) Open Heavy Flavor Workshop.
12/12/05William Horowitz Heavy Flavor Productions Workshop Role of Dynamic Geometry in Jet Tomography William Horowitz Columbia University December 12,
Jet fragmentation photons in ultrarelativistic heavy-ion collisions Koichi Hattori, Larry McLerran, Bjoern Schenke Quark Matter Sep Oct.
2/9/08 William Horowitz Quark Matter Testing AdS/CFT Drag and pQCD Heavy Quark Energy Loss William Horowitz Columbia University Frankfurt Institute.
Jet Quenching of Massive Quark in Nuclear Medium Ben-Wei Zhang Institute of Particle Physics Central China Normal Univeristy ICHEP, Beijing --- Augest.
Probing QGP-medium interactions
Jet shape & jet cross section: from hadrons to nuclei
Zeroth Order Heavy Quark Photon/Gluon Bremsstrahlung
Probing AdS/CFT with Heavy Quarks
William Horowitz Columbia University
Qualitative Successes of AdS/CFT at RHIC
Modification of Fragmentation Function in Strong Interacting Medium
pQCD vs. AdS/CFT Tested by Heavy Quark Energy Loss
Motivation for Studying Heavy Quarks
William Horowitz Columbia University
William Horowitz Columbia University June 14, 2006
of Hadronization in Nuclei
Energy Loss in the Hot QCD Brick I
Uncertainties and Consistency (?) in pQCD and AdS/CFT Jet Physics
张汉中 Institute of Particle Physics, Central China Normal University,
Presentation transcript:

5/2/08 William Horowitz Yale-Columbia Fest Zero th Order Heavy Quark Photon/Gluon Bremsstrahlung William Horowitz Columbia University Frankfurt Institute for Advanced Studies (FIAS) May 2, 2008 With many thanks to Miklos Gyulassy, Simon Wicks, Ivan Vitev, Hendrik van Hees

5/2/08 William Horowitz Yale-Columbia Fest A Talk in Two Parts pQCD vs. AdS/CFT Drag 0 th Order Production Radiation

5/2/08 William Horowitz Yale-Columbia Fest Testing pQCD vs. AdS/CFT Drag Energy Loss Mechanisms (In Five Slides) arXiv: (LHC predictions) arXiv: (RHIC predictions)

5/2/08 William Horowitz Yale-Columbia Fest (Proper) Subset of Mechanisms DGLV, AdS/CFT Drag, Diffusion… Use heavy quark R AA to test these two dp T /dt ~ -(T 2 /M q ) p T LPM: dp T /dt ~ -LT 3 log(p T /M q )

5/2/08 William Horowitz Yale-Columbia Fest –LHC Prediction Zoo: What a Mess! –Let’s go through step by step –Unfortunately, large suppression pQCD similar to AdS/CFT–Large suppression leads to flattening –Use of realistic geometry and Bjorken expansion allows saturation below.2 –Significant rise in R AA (p T ) for pQCD Rad+El–Naïve expectations met in full numerical calculation: dR AA (p T )/dp T > 0 => pQCD; dR AA (p T )/dp T ST LHC c, b R AA p T Dependence WH, M. Gyulassy, arXiv:

5/2/08 William Horowitz Yale-Columbia Fest LHC R c AA (p T )/R b AA (p T ) Prediction Recall the Zoo: –Taking the ratio cancels most normalization differences seen previously –pQCD ratio asymptotically approaches 1, and more slowly so for increased quenching (until quenching saturates) –AdS/CFT ratio is flat and many times smaller than pQCD at only moderate p T WH, M. Gyulassy, arXiv: [nucl-th]

5/2/08 William Horowitz Yale-Columbia Fest RHIC R cb Ratio Wider distribution of AdS/CFT curves at RHIC due to large n power law production: increased sensitivity to input parameters Advantage of RHIC: lower T => higher AdS speed limits WH, M. Gyulassy, arXiv: pQCD AdS/CFT pQCD AdS/CFT

5/2/08 William Horowitz Yale-Columbia Fest Conclusions AdS/CFT Drag observables calculated Generic differences (pQCD vs. AdS/CFT Drag) seen in R AA –Masked by extreme pQCD Enhancement from ratio of c to b R AA –Discovery potential in Year 1 LHC Run Understanding regions of self- consistency crucial RHIC measurement possible

5/2/08 William Horowitz Yale-Columbia Fest Some Investigations of 0 th Order Production Radiation

5/2/08 William Horowitz Yale-Columbia Fest Motivation Previous work: test pQCD or AdS/CFT energy loss –Heavy quark R Q AA and R c AA /R b AA Future goal: additional energy loss test using photon bremsstrahlung Zero th Order Calculation –Recent p + p fragmentation  data –Good warm-up and test problem Investigate running , low-p T, etc. –Reevaluate magnitude of Ter-Mikayelian

5/2/08 William Horowitz Yale-Columbia Fest New Fragmentation  Data A. Hanks, QM2008

5/2/08 William Horowitz Yale-Columbia Fest Motivating Example: Running  s –Fixed  s is simplification to speed up code Not a free parameter –Running  s will most likely introduce a large error –Want to understand systematics in 0 th Order S. Wicks, WH, M. Djordjevic, M Gyulassy, Nucl.Phys. A783 : ,2007

5/2/08 William Horowitz Yale-Columbia Fest Quark mass => Dead cone –Ultrarelativistic “searchlight” rad. pattern Gluon mass => Longitudinal modes, QCD Ter-Mikayelian –Reduction of production radiation compared to vacuum Alters DGLAP kernel Quark and Gluon/Photon Mass Effects  ~ M q /E Y. Dokshitzer and D. Kharzeev, Phys.Lett. B519 : ,2001 M. Djordjevic and M. Gyulassy, Phys.Rev. C68 :034914,2003

5/2/08 William Horowitz Yale-Columbia Fest Previous Calculation of Ter-Mikayelian Reduction of E-loss for charm quarks by ~ 30% E-loss from full HTL well approx. by fixed m g = m ∞ Small- x pQCD 0 th Order result: M. Djordjevic and M. Gyulassy, Phys.Rev. C68 :034914,2003

5/2/08 William Horowitz Yale-Columbia Fest Compare Classical E&M to “pQCD” –Classical E&M Recall Jackson: Soft photon limit => –Note charge conserved –Usual pQCD approach –Charge explicitly not conserved => Ward identity ( ) violated

5/2/08 William Horowitz Yale-Columbia Fest Classical/QFT Inconsistency –For m Q = m g = 0 and in the small x, large E + limit, both are equal: –For m Q, m g ≠ 0 and the small x, large E + limit, they differ:

5/2/08 William Horowitz Yale-Columbia Fest Not a Classical Error –Wrong classical calculation? Plugged in massive 4-vectors into massless formulae Rederive classical result using Proca Lagrangian –After several pages of work… Identical to

5/2/08 William Horowitz Yale-Columbia Fest Error from QFT Ward Violation Identical expressions are not a surprise QFT Calculation –Photon momentum carried away crucial for cancellation of photon mass Classical case neglects both; effects cancel

5/2/08 William Horowitz Yale-Columbia Fest Resulting Expression –To lowest order in 1/E + –New: (1- x ) 2 prefactor: naturally kills hard gluons m g 2 in numerator: fills in the dead cone!?! –What are the sizes of these effects? Call this LO

5/2/08 William Horowitz Yale-Columbia Fest LO Gluon Production Radiation Prefactor => % effect –Implications for in-medium radiative loss? Filling in dead code => 5-20% –Numerics includes k T and x limits » x large enough to create m g » x small enough that E Jet > M q –Fixed  =.5 GeV and  s =.5 »Similar to Magda full HTL propagator with running  s

5/2/08 William Horowitz Yale-Columbia Fest LO vs. All Orders Production Rad. Ter-Mikayelian similar for both Different normalizations –0-60% effect All orders calculation self-regulates for m g = 0 and p T → 0

5/2/08 William Horowitz Yale-Columbia Fest Conclusions No single satisfactory energy loss model Search for tests sensitive to mechanism –Ratio of charm to bottom R AA for pQCD vs. AdS/CFT –Future tests using photon bremsstrahlung Inclusion of away-side jet fills in dead cone –Ultimately leads to a relatively small (5-20%) effect Radiative calculations integrate over all x ; importance of large x behavior?

5/2/08 William Horowitz Yale-Columbia Fest Backups

5/2/08 William Horowitz Yale-Columbia Fest Reasonable Consistency with Magda b c M. Djordjevic and M. Gyulassy, Phys.Rev. C68 :034914,2003

5/2/08 William Horowitz Yale-Columbia Fest th Order % Differences