the future of spin physics at rhic steve vigdor for sam aronson spin2008, charlottesville october...
DESCRIPTION
RHIC: World’s Only Polarized Hadron Collider RIKEN/RBRC DOE/RIKEN/RBRC BRAHMS & PP2PP STAR PHENIX AGS LINAC BOOSTER Pol. H - Source Solenoid Partial Siberian Snake 200 MeV Polarimeter AGS Internal Polarimeter Rf Dipole Strong AGS Snake PHOBOS Spin flipper Siberian Snakes RHIC Polarimeters Spin Rotators muon detector AGS pC Polarimeter Warm AGS Snake Polarized atomic H jet Siberian snakes: built into design from the start ! No snakes ~1000 depolarizing resonances With snakes no first order resonances Two partial AGS snakes (11 and 27 spin rotators)TRANSCRIPT
The Future of Spin Physics at
RHIC Steve Vigdor for Sam AronsonSPIN2008, Charlottesville
October 10, 2008I. Present status and plans to
improve luminosity & polarization
II. Spin performance milestones & 6-year run plan to achieve them
III. Recent highlights and future projections from RHIC Spin
IV. eRHIC and possible stagingV. Precision experiments with
stored polarized beams
p-p at RHIC addresses:
1) What does the share of p spin carried by gluons and sea quarks/ antiquarks reveal about effective degrees of freedom?
2) How is parton orbital motion (on the light front) in p manifested in transverse spin asymmetries?
e-N at EIC would exploit scaling viola-tions & exclusive reactions to extend study to completely gluon-dominated region at low momentum fraction.
Nucleon Spin Structure at RHIC and an Electron-Ion Collider
RHIC: World’s Only Polarized Hadron Collider
RIKEN/RBRC
DOE/RIKEN/RBRC
BRAHMS & PP2PP
STAR
PHENIX
AGS
LINAC BOOSTERPol. H- Source
Solenoid Partial Siberian Snake
200 MeV Polarimeter AGS Internal Polarimeter
Rf DipoleStrong AGS Snake
PHOBOS
Spin flipper
Siberian SnakesSiberian Snakes
RHIC Polarimeters
Spin RotatorsSpin Rotators
muon detector
AGS pC Polarimeter
Warm AGS Snake
Polarized atomic H jet
Siberian snakes: built into
design from the start !
No snakes ~1000 depolarizing resonancesWith snakes no first order resonancesTwo partial AGS snakes (11 and 27 spin rotators)
0
10
20
30
40
50
0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15Weeks into run
Nuc
leon
pai
r lu
min
osity
L
NN
[pb-1
]
2003P=34%
2005P=46%
2006P=60%
2008P=45%
P L(pb^-1) Results2002 15% 0.15 first pol. pp collisions! 2003 30% 1.6 pi^0, photon cross
section, A_LL(pi^0)
2004 40% 3.0 absolute beam polarization
with polarized H jet2005 50% 13 large gluon pol. ruled out (P^4 x L = 0.8) 2006 60% 46 first long spin run * (P^4 x L = 6) 2007 no spin running
2008 50% (short) run
* support for 2006 run from Renaissance Tech. crucial for program
Polarized Collision Performance at RHIC
2006, P=60%
2008, P=45%
2005, P=46%
2003, P=34%
Delivered luminosity at s = 200 GeV
Further development ( long runs!) needed to reach “enhanced” design goals: P=70%, L = 6 1031 cm2s1 (or 15 pb1/week) at s = 200 GeV
Absolute beam polarization calibration to better than 5% design goal achieved!
Polarized proton acceleration to 250 GeV demon-strated. First collision run anticipated 2009.
45 % polarization on first acceleration to 250 GeV!
Loss at strong intrinsic resonance (136 GeV); correctable by adjusting betatron tunes.
injection 250 GeV
RHIC Spin Luminosity and Polarization Goals
Parameter unit Achieved Luminosityupgrade
p- p operation (2006/08) (~ 2012)Energy GeV 100 100 (250)No of bunches … 111 111Bunch intensity 1011 1.5 2.0Ave. delivered lum.** 1030 cm-2s-1 23 80 (200)Polarization % 60 70
** without vertex cuts
Planned luminosity improvements: reduce * from 1.0 to 0.5 m mitigate 10 Hz quad triplet vibration near-integer working point
non-linear chromaticity correction transfer line and booster mods. 9 MHz and 56 MHz RF upgrades
Planned polarization improvements: horizontal tune jumps in AGS improved orbit control in RHIC snakes
Further p Beam Improvements Under Development: Electron Lenses
p-p luminosity limited by head-on beam-beam tune spread Low energy (~5 keV) e beam interacting with proton beam can
compensate head-on beam-beam tune spread ( 2 luminosity?) Single and multi-particle simulation underway Possible implementation in RHIC by 2014
w/o beam-beam compensation with half and full beam-beam compensation
Large tune spread luminosity loss
See T. Roser talk, 10/11/08.
Further p Beam Improvements Under Development: Coherent Electron Cooling
CeC of high-energy hadron beams: high-gain FEL based on high-brightness ERL (V. Litvinenko & Y. Derbenev) boost LHC and EIC luminosities?
Wiggler: FEL amplification (x 102-3) of e-beam modulations, while chicane adds dispersion to h beam
Kicker: attraction to e-beam density peak re-duces ion-beam E spread.
Modulator: hadron beam structure intro-duces density modu-lation in e-beam
Uses 20 MeV R&D ERL already under
develop-ment at BNLPlan proof-of-principle test @ RHIC by 2014 with Au beam.
Does not address beam-beam limit on RHIC p+p luminosity.
Year Due
# Milestone
2013 HP8 Measure flavor-identified q and q contributions to the spin of the proton via the longitudinal-spin asymmetry of W production.
2013 HP12(update of HP1)
Utilize polarized proton collisions at center of mass energies of 200 and 500 GeV, in combination with global QCD analyses, to determine if gluons have appreciable polarization over any range of momentum fraction between 1 and 30% of the momentum of a polarized proton.
2015 HP13(new)
Test unique QCD predictions for relations between single-transverse spin phenomena in p-p scattering and those observed in deep-inelastic lepton scattering
Near-Term RHIC Spin Program Addresses Three Specific DOE Hadron Physics Performance Milestones
A few brief comments on the physics goals to follow…
Tentative RHIC Run Plan Following 2008 PAC Recommendations(assumes 6-month FY09 CR, 2-species runs in FY10-14 & best info on detector upgrade schedules)
Fiscal Year
Colliding Beam Species/Energy
Comments
2009 200 GeV p+p~12 physics weeks to complete 200 GeV ALL measurements – could be swapped with 500 GeV Run 10 if >6-month FY09 CR likely; STAR DAQ1000 fully operational
2010500 GeV p+p ~5-6 physics weeks to commission collisions, work on polarization & luminosity and
obtain first W production signal to meet 2011 RIKEN milestone
200 GeV Au+Au 9-10 physics weeks with PHENIX HBD, STAR DAQ1000 & TOF permits low-mass dilepton response map and 1st HI collision test of transverse stochastic cooling (one ring)
2011
Au+Au at assorted low E
1st energy scan for critical point search, using top-off mode for luminosity improvement – energies and focus signals to be decided; commission PHENIX VTX (at least prototype)
200 GeV U+U 1st U+U run with EBIS, to increase energy density coverage
2012500 GeV p+p 1st long 500 GeV p+p run, with PHENIX muon trigger and STAR FGT upgrades, to
reach ~100 pb-1 for substantial statistics on W production and G measurements
200 GeV Au+Au Long run with full stochastic cooling, PHENIX VTX and prototype STAR HFT installed; focus on RHIC-II goals: heavy flavor, -jet, quarkonium, multi-particle correlations
2013500 GeV p+p Reach ~300 pb-1 to address 2013 DOE performance milestone on W production
200 GeV Au+Au or 2nd low-E scan
To be determined from 1st low-E scan and 1st upgraded luminosity runs, progress on low-E e-cooling, and on installation of PHENIX FVTX and NCC and full STAR HFT
2014
200 GeV Au+Au or 2nd low-E scan
Run option not chosen for 2013 run – low-E scan addresses 2015 DOE milestone on critical point, full-E run addresses 2014 (-jet) and 2016 (identified heavy flavor) milestones. Proof of principle test of coherent electron cooling.
200 GeV p+p Address 2015 DOE milestone on transverse SSA for -jet; reference data with new detector subsystems; test e-lenses for p+p beam-beam tune spread reduction
Present and Future Constraints on Gluon Polarization in the Proton:
1st NLO pQCD analysis incorporating RHIC spin inclusive jet and 0 ALL (2006) data (arXiv:0804.0422) by de Florian, Sassot, Stratmann & Vogelsang DIS and RHIC spin impose comparable constraints to date on shape & magnitude of gluon polarization vs. x; RHIC spin data should dominate after next long 200 GeV p+p run, with new jet+jet coincidence data significantly constraining x-dependence.
w/ Run 6 RHIC data
w/ projected
Run 9 RHIC data
Future Constraints on Sea Anti-quark Polarization s = 500 GeV p + p W + + X (u+d W + e + or + )
W + X (d+u W e or )
Measure 1-spin PV helicity asymmetry AL for 2 beams 2 charge states u/u, d/d in valence region ( “self-calibration” of technique) d/d, u/u for x ~ 0.02 - 0.2 check prediction of many nucleon structure models that |u d | > |d u | (sizable from FNAL E866)
Anticipate: 1st 500 GeV collision run in 2009
~100 pb1 by 2012
~300 pb1 by 2013
Similar sensitivity for PHENIX
Program relies on ongoing upgrades to PHENIX trigger, STAR forward tracking
STAR projections for mid-rapidity e+ from W+
STAR projec-tions for mid-rapidity e from W
300 pb1, P=0.7, 70% efficiency
0.2
0
0.2
0.4
0.6
0.8
0
0.2
0.2
0.4
0.6
0.8
AL
AL
20 30 40 50 20 30 40 50Lepton ET (GeV)
0.1 0.2 0.3 x
Constraining Origin of Transverse Spin Asymmetries:
0RHIC II Drell-Yan Projections
0
HERMES Sivers
Results
Large AN observed for pp forward hadron inclusive can arise from entrance- (Sivers) or exit-channel (Collins jet fragmentation) transverse spin-momentum correlations. Sivers asyms. sensitive to quark and gluon orbital ang. mom. on light front same frame where G, measured frame for Ji sum rule AN
Sivers(SIDIS, FSI among outgoing partons) = ANSivers(DY, ISI)
prediction sensitive to all aspects of pQCD treatment
Test predicted sign change first in inclusive p+p +X in time for 2015 DOE milestone.
PHENIX
STAR
e-ion detector
eRHIC
Main ERL (1.9 GeV)
Low energy recirculation pass
Beam dump
Electronsource
Possible locationsfor additional e-ion detectors
Four recirculation passes
Long-Term (>2020) Future of Spin Physics at RHIC: EIC eRHIC
Subsequent stages/ alternative layouts could increase e-beam & ion-beam energies and L from nominal 10 250 GeV, ~3 1033 cm2s1 e+p
Add ERL injector with polarized e source to enable e+p,3He and e+A (up to Uranium) to study matter in gluon-dominated regime
10 GeV electron design energy.Possible upgrade to 20 GeV by doubling main linac length.
5 recirculation passes ( 4 in RHIC tunnel) Multiple electron-hadron interaction points
(IPs) permit multiple detectors; Full polarization transparency at all
energies for the electron beam; Ability to take full advantage of transverse
cooling of the hadron beams; Possible options to include polarized
positrons at lower luminosity: compact storage ring or ILC-type e+ source
R&D already under way on various accelerator issues; more to come.
EIC probes weak coupling regime of very high gluon density, where gauge boson occupancy >> 1. All ordinary matter has at its heart an intense, semi-classical force field -- can we demonstrate its universal behavior?
Search for supersymmetry @ LHC, ILC (?): seeking to unify matter and forces
Electron-Ion Collider: reveal that Nature blurs the distinction
Gluons dominate the soft constituents of hadrons! But density must saturate…
Deep inelastic scattering @ HERA
EIC Science: Study of Force (Gluon)-Dominated Matter
See R. Milner talk, 10/6/08
Polarized e + N at EIC
See R. Milner talk, 10/6/08; Note INT workshops on EIC science, Fall ’09 and ’10.
Polarized DIS, -gluon fusion to determine gluon polarization down to x ~ few 104
Bjorken sum rule test to ≲ 2% precision SIDIS for low-x sea-quark polarization and transverse spin studies
More luminosity-hungry: Polarized DVCS, exclusive reactions + LQCD GPD’s map low-x transverse position-dep. PDF’s; Jq from Ji sum rule
Parity violation in e+p,d at high Q2 to study running of weak coupling below Z-pole
2 x (0.5-0.7) GeV SRF linacs
100 MeV injector2-4 passes, depending on top energy
IP
Stage I e-RHIC with ERL inside RHIC tunnel @ IP2: up to 2 (4) GeV e with RT (SC) magnets
Intermediate-Term Possibilities: 1st (Medium Energy) Stage of EIC?
Would enable few GeV e on 100 GeV/N heavy ions and 250 GeV p First look at saturation surface for nuclei in e+A DIS, confirmation of nuclear “oomph” factor; e+A diffraction tests of high gluon occupancy e-p program emphasizing transverse-spin SIDIS over broad Q2-range TMD evolution; detection of boosted target fragments to probe spin-dependent correlations, intrinsic heavy flavor in nucleon; extend DIS. Need to develop science case, detector design, cost estimate. Most equipment would be reused later in full EIC
ME-EIC parameters for e-p collisions (2 GeV option, 50 mA polarized e source, maintaining pp, pA, AA collisions at RHIC detectors)
not cooled pre-cooled high energy cooling
p e p e p e
Energy, GeV 250 2 250 2 250 2
Number of bunches 111 111 111
Bunch intensity, 1011 2.0 0.31 2.0 0.31 2.0 0.31
Bunch charge, nC 32 5 32 5 32 5
Normalized emittance, 1e-6 m, 95% for p / rms for e 15 37 6 14.7 1.5 3.7
rms emittance, nm 9.4 9.4 3.8 3.8 0.94 0.94
beta*, cm 50 50 50 50 50 50
rms bunch length, cm 40 1 40 1 40 1
beam-beam for p /disruption for e 1.5e-3 12 3.8e-3 31 0.015 120
Peak Luminosity, 1e32, cm-2s-1
0.93 2.3 9.3
Also a test-bed for high-energy coherent e-cooling to prepare for full EIC.
Possible Alternative Intermediate-Term Future: Precision Experiments in Storage Rings
g-2 ring @ AGS
Physics Beyond the Standard Model: Supersymmetry SUSY working group report: Les Houches 2007 (Feb 08 archive)
“The strongest hint for a TeV-scale modifica-tion of the Standard Model originates from theanomalous magnetic moment of the muon.”
History: muon anomalous magnetic moment @ AGS
See W. Marciano’s talk, 10/7/08
Novel Storage Ring EDM Exp’ts @ AGS ? Inject longitudinally pol’d p or d beam, via AGS, into dedicated storage ring Choose magic momentum + static E, B combination (B=0 for protons) to ~cancel (g-2) horizontal spin precession Search for EDM signature of vertical polarization build-up due to precession in strong E-field (static for p, v B for d)
Cancel many systematic errors by measuring for counter-rotating (vertically separated) beams simultaneously. Sensitivity goal ~ few 1029 ecm for p, ~ 1029 ecm for d If EDM 0 observed for n, p and/or d, the combination powerfully constrains the source. E.g., the three systems have quite different sensitivities to QCD vs. SUSY (latter strongly enhanced in d).
See Y. Semertzidis talk, 10/07/08.
Summary1) Strong progress in recent years on luminosity and
polarization for p+p collisions at RHIC, clear plans for reaching ‘enhanced’ design specs over next few years.
2) Despite budget-induced shortening of recent runs, RHIC spin data already important in constraining G(x) and origin of transverse spin asymmetries.
3) Next ~5 years should produce dramatic progress toward 3 milestones in nucleon spin structure, including 500 GeV W production for antiquark polarization.
4) Innovative electron lens and coherent e-cooling R&D plans can have great impact on future p+p and e+p luminosities.
5) eRHIC linac-ring concept, with possible 1st “medium-energy” stage viable strategy toward spin physics at very low x. Much R&D and strengthening of science case needed before next U.S. Nuclear Physics Long Range Plan (~2012-13).
6) Charged-particle EDM searches in storage rings intriguing possibility for complementary beyond-SM spin physics.