QCD and Hadronic Nuclear Physics (hadrons and nucleons) · QCD and Hadronic Nuclear Physics...
Transcript of QCD and Hadronic Nuclear Physics (hadrons and nucleons) · QCD and Hadronic Nuclear Physics...
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Anthony W. Thomas
IUPAP WG.9 Nuclear Science Symposium
Frascati − May 31st 2013
QCD and Hadronic Nuclear Physics
(hadrons and nucleons)
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Outline
• QCD and Hadronic Physics
− chiral symmetry breaking
− confinement
• Hadron properties as emergent phenomena
• Recent progress in understanding nucleon structure
• Open challenges
• Facilities
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QCD within the Standard Model
• Standard Model is complete with Higgs discovery
• Built upon local gauge symmetries
• Strong sector is unique – fundamental degrees of
freedom (dof) do not exist outside hadrons!
− despite searching everywhere, including moon
rocks, deep ocean sediments, cosmic rays....
Confinement
• In our world the fundamental dof are almost massless
BUT we are not!
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Building Blocks of our Universe
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Force Carriers of the Universe
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QCD and the Origin of Mass
HOW is this possible?
No other sector of the Standard Model is like this
− tear a table into its constituent atoms and the
masses (of table and its components)are
identical to one part in a billion
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Dynamically Broken Chiral Symmetry
• Near massless quarks near degeneracy of
opposite parity states
• BUT N(940) and nearest negative parity is N(1535) !
• Goldstone’s theorem implies near massless pion
(and less so the K)
• Chiral limit crucial but bizarre
– p and n charge radii infinite
• Such a light pion completely undermines the
conventional picture of confinement
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Confinement for infinitely heavy quarks?
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Quark mass function through χSB
Lattice studies & Dyson-Schwinger
modelling in excellent agreement
− χSB is origin of constituent quark mass
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Three generations of quarks & leptons
While important the physics of c, b and t is
very different − χSB not of major importance
− fascinating new states around 3.8-4.2GeV
being found at BES (and Belle)
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Our challenges
• Discover how the properties of hadrons emerge
as non-perturbative properties of this beautiful,
non-linear theory
• Test that it is indeed fully correct
• Investigate the role of hadron structure for
atomic nuclei, dense matter, etc.
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Investigation of Hadron Structure
• Historically use electromagnetic and
weak probes to excite and study
• Anomalous magnetic moments showed nucleons
were not elementary Dirac particles in 1930s
• Elastic electron scattering (since 1950s) directly
measures the Fourier transforms of charge and
current distributions
− GE,M (Q2)
• Neutrino scattering adds GA (Q2)
and GP (Q2)
Stern
Hofstadter
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Highlights of what we have learnt
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N/Δ spectrum in PDG RPP 2012
All new candidate states need confirmation in independent analyses
Experiments at JLab and Mainz : new baryonic states
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Impressive results on excited states : lattice QCD
• Recent results from JLab (mπ = 391 MeV)
Edwards et al., arXiv:1212.5236 (JLab)
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....and from CSSM
Mahbub et al., arXiv:1302.2987
N½+
(Adelaide plot...)
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More detailed information coming − experiment & lattice!
arXiv:1304.0325
e.g. Nature of the Roper − 1450 MeV
Burkert et al., CLAS
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Proton Radius Puzzle?
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Initial Investigation of Charge vs Current in the Proton at SLAC
• Distribution of charge and magnetization in the proton seemed identical
• The experiments were limited by the precision of absolute cross section measurements
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Text Book Re-written
• High Intensity
• High Duty Factor
• High Polarization
Revolutionized
our knowledge
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Potential link to χSB
2
2
Small changes in M(p) within the
domain 1<p(GeV)<3
have striking effect on the electric
form factor
Ratio [μpGEp(Q2)/GMp(Q2)] provide
information on the nature of the
quark-quark interaction in the
transition region from pQCD to non-
perturbative QCD
I.C. Cloët et al.: “Revealing dressed-quarks via the
proton's charge distribution”, arXiv: 1304.0855 [nucl-th]
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Fundamental Test of Non-Perturbative QCD
• Strangeness contribution is a vacuum polarization
effect, analogous to Lamb shift in QED
It is a fundamental test of QCD
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A unique case : theory 10 times more accurate than data
Thomas Jefferson National
Accelerator Facility (JLab)
(plus Mainz & Bates)
CSSM – JLab
calculation
− culmination of 12 years work!
Experimental program
took three major
laboratories 20 years!
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Flavor separation of proton form factors now possible….
Very different behavior for u & d quarks suggests
apparent scaling in proton F2/F1 may be accidental
Cates, de Jager,
Riordan, Wojtsekhowski,
PRL 106 (2011) 252003
Q4F2q/k
Q4 F1q
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Direct confirmation of Quarks through Deep Inelastic Scattering
• At high energy and momentum transfer in inelastic
electron (muon and neutrino) scattering one
directly measures the momentum distribution of the
quarks
• Polarised electrons also enable the spin of the
quarks to be determined
• Later Drell-Yan (quark-anti-quark) annihilation added
crucial new information
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Unpolarized Structure Function F2
• Bjorken Scaling
• Scaling Violation
• Gluon radiation –
• QCD evolution
NLO: Next-to-Leading-
Order
…….
• One of the best
experimental tests of
QCD
SLAC
CERN
FNAL
DESY
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Parton Distribution Functions (CTEQ6)
JHEP 1001: 109 (2010)
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(93 authors)
= 14 ± 3 ± 10 % :
i.e. 86% of spin of p NOT carried by its quarks
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Probing G in pol. pp collisions
pp hX
h
f
fXff
ba
ba
h
f
fXff
LL
fXff
ba
ba
LLDdff
Dadff
dd
ddA
ba
baba
ˆ
ˆˆ
,
,
Double longitudinal spin asymmetry ALL is sensitive to G
Polarized pp collider at RHIC
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Where is the Spin of the proton?
• Modern data (Hermes, COMPASS) yields: = 0.33 ± 0.03 ± 0.05 (c.f. 0.14 ± 0.03 ± 0.10 originally)
• In addition, there is little or no polarized glue - COMPASS: gD
1 = 0 to x = 10-4 - ALL (0 and jets) at PHENIX & STAR: G ~ 0 - Hermes, COMPASS and JLab: G / G small
• Hence: axial anomaly plays at most a small role in explaining the spin crisis
• Suggests alternate explanation lost in the rush to explore the anomaly : chiral symmetry and gluon exchange
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Recent Result on Quark Spins for the Octet
Shanahan et al., Phys Rev Lett 110 (2013) 202001
• Rather than experimental measurements on the octet, we now
have lattice QCD - in this case QCDSF (Phys. Rev. D 84, 054509 (2011)
and Phys. Lett. B 714, 97 (2012) ) − see final column
• The other columns show the results for the cloudy bag model that
worked so well for the nucleon applied to whole octet
• Agreement remarkably good... suppression is not universal!
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GA - a fundamental test
Therefore still a caution on lattice QCD !
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Future challenges
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Spectroscopy
− how do excited states emerge from QCD
− what are the fundamental degrees of freedom
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Gluonic Excitations and the Origin of Confinement
QCD predicts a rich spectrum of as yet to be discovered
gluonic excitations
− their experimental verification
is crucial for our understanding of QCD in
the non-perturbative regime.
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Glueballs and hybrid mesons : Hall D at Jlab?
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Hybrid Baryons in LQCD
regular states
hybrid states
J.J. Dudek and R.G. Edwards, PRD85 (2012)
054016
1.3GeV
N
clustered
in mass
Hybrid states have same JP values as Q3 baryons. How to identify them?
- Overpopulation of N1/2+ and N3/2+ states compared to QM
projections?
- Transition form factors in electro-production
( different Q2 dependence )
T. Barnes and F.E. Close, PLB128, 277 (1983)
LQCD
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Gluon, too, has non-perturbative mass!
Running gluon mass
– Gluon is massless in UV,
in agreement with pQCD
– Massive in infrared
• mG(0) = 0.67-0.81 GeV
DSE prediction confirmed by
numerical simulations of
lattice-regularised QCD
Qin et al., Phys. Rev. C 84 042202(Rapid Comm.) (2011)
mG2(k2) ≈ mG
4/(k2+mG2)
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First results from J-PARC
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The H di-baryon again?
Using data from NPLQCD & HAL: H bound at larger ml
→ H-di-baryon almost bound at physical masses
Shanahan at al., Phys Rev Lett (arXiv:1106.2851)
mH – 2 mΛ = 13 ± 14 MeV
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Dibaryons re-visited
H prediction seems pretty good – what about S=-1?
Remarkably close to apparent state seen at
FINUDA in (K-,Λp) at 2.26 GeV on a variety of
nuclei : Agnello et al., Phys Rev Lett 94, 212303 (2005)
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Deep-Inelastic scattering
− spin and flavor structure
− symmetry breaking
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Neutron Structure Function at high-x
SU(6) symmetry
pQCD, uncorrelated Ψ
0+ qq only
Reviews:
S. Brodsky et al.
NP B441 (1995)
W. Melnitchouk et al.,
PL B377 (1996) 11
N. Isgur, PRD 59 (1999)
R.J. Holt & C.D. Roberts
RMP (2010)
DSE: “realistic”
Distribution of neutron’s momentum amongst quarks
on the valence-quark domain – UNKNOWN!
Melnitchouk, Accardi et al. Phys.Rev. D84 (2011) 117501
x>0.9
Melnitchouk, Arrington et al. Phys.Rev.Lett. 108 (2012) 252001
I.C. Cloët, C.D. Roberts, et al.
arXiv:0812.0416 [nucl-th],
Few Body Syst. 46 (2009) 1-36
D. J. Wilson, I. C. Cloët et al.,
arXiv:1112.2212 [nucl-th],
Phys. Rev. C85 (2012) 025205
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Hall A 11 GeV with HMS Hall B 11 GeV with CLAS12
Jlab 12 GeV : Unambiguous Flavor Structure x ~ 1
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and Unambiguous Resolution of Valence Spin
A1p at 11 GeV
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Chiral symmetry and the sea of the nucleon
− asymmetry in d – u and s – s
− polarization of the sea and vacuum structure
_ _ _
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Dependence of s- s on assumed cross-over _
SIDIS and EIC
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Charge Symmetry : Future EIC or LHeC
Hobbs et al., Phys Lett (arXiv:1101.3923 [hep-ph])
QED splitting
Plus
md-mu Total
including s-
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New observables
− 3D imaging of the nucleon
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TMDs
2+1 D picture in momentum space
Bacchetta, Conti, Radici
GPDs
2+1 D picture in impact-parameter space
QCDSF collaboration
3-D Imaging - Two Approaches
• intrinsic transverse motion
• spin-orbit correlations- relate to OAM
• non-trivial factorization
• accessible in SIDIS (and Drell-Yan)
• collinear but long. momentum transfer
• indicator of OAM; access to Ji’s total Jq,g
• existing factorization proofs
• DVCS, exclusive vector-meson production
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GPDs & Deeply Virtual Exclusive Processes
x
Deeply Virtual Compton Scattering (DVCS)
t
x+x x-x
hard vertices
x– longitudinal momentum transfer
x – quark momentum fraction
–t – Fourier conjugate to transverse impact parameter
g
- New Insight into Nucleon Structure
At large Q2 : QCD factorization theorem hard exclusive process can be
described by 4 transitions (Generalized Parton Distributions) :
Vector : H (x, ξ,t) Tensor : E (x, ξ ,t)
Axial-Vector : H (x, ξ, t) Pseudoscalar : E (x, ξ ,t)
~ ~
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transverse polarized target
3D Images of the Proton’s Quark Content
M. Burkardt PRD 66, 114005 (2002)
b - Impact parameter
T
u(x,b ) T d(x,b ) T uX(x,b ) T dX(x,b ) T
Hu Eu Hd Ed
quark flavor polarization
Accessed in Single Spin
Asymmetries.
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Experimental effort just beginning!
For the moment the analysis is highly model dependent ....
Myhrer-Thomas NLO
Myhrer-Thomas NLO
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The Facilities to address these questions
− hadrons
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Facilities
RHIC : Polarised p-p collisions
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The Facilities to address these questions
− electrons
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12 GeV Upgrade Project at JLab
Scope of the project includes:
• Doubling the accelerator beam energy
• New experimental Hall and beamline
• Upgrades to existing Experimental Halls
Maintain capability to
deliver lower pass
beam energies: 2.2, 4.4,
6.6….
New Hall
Add arc
Enhanced capabilities
in existing Halls
Add 5
cryomodules
Add 5
cryomodules
20 cryomodules
20 cryomodules
Upgrade arc magnets
and supplies
CHL
upgrade
Upgrade is designed to build on existing
facility: vast majority of accelerator and
experimental equipment have continued
use
The completion of the
12 GeV Upgrade of CEBAF
was ranked the highest
priority in the 2007 NSAC
Long Range Plan.
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EIC Plans
RHIC eRHIC
LHC LHeC
CEBAF
MEIC/EIC
FAIR ENC
HERA
EIC@HIAF
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Medium Energy EIC@JLab
JLab Concept
MEIC:
• 3-12 GeV on 20-100 GeV ep/eA collider
• fully-polarized, longitudinal and transverse
• luminosity: up to
few x 1034 e-nucleons cm-2 s-1
Upgradable to higher energies (250 GeV protons)
Pre-booster
Ion
source
Transfer
beam line
Medium
energy IP
Electron collider
ring
(3 to 12 GeV) Injector
12 GeV CEBAF
SRF
linac Warm large booster
(up to 20 GeV)
Cold ion
collider ring
(up to 100
GeV)
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EIC@HIAF
HIAF was approved, EIC on HIAF is being proposed
Schedule
1. HIAF Phase-1: ~2019: 3 x12 GeV
2. HIAF Phase-2: ~2030: 15 x 100 GeV
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Summary
• We have a wealth of exciting, fundamental questions to
address
• Lattice QCD, phenomenology and experiment working
beautifully together
• Appropriate investment is needed to:
− exploit the facilities now operating/nearing completion
− provide HPC facilities for further lattice QCD
(and share the fruits of those investments)
− build future EIC(s) at high luminosity
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