Facility for Antiproton and Ion Research (Very) ofBrief Description Walter F. Henning – GSI Darmstadt &•University Frankfurt DNP-APS Town Meeting, Rutgers University, Jan 12-14, 2007 of.

Download Report

Transcript Facility for Antiproton and Ion Research (Very) ofBrief Description Walter F. Henning – GSI Darmstadt &•University Frankfurt DNP-APS Town Meeting, Rutgers University, Jan 12-14, 2007 of.

Facility for Antiproton and Ion Research
(Very) ofBrief
Description
Walter F. Henning – GSI Darmstadt &•University
Frankfurt
DNP-APS Town Meeting, Rutgers University, Jan 12-14, 2007
of the Facility
• Experimental Program
(Strong Interaction Physics – QCD)
Darmstadt
----
Helmholtz Centre for Ion Research
GSI today
SIS 100/300
Future facility
SIS 18
UNILAC
CBM
ESR
Super
FRS
Rare-Isotope
Production Target
HESR
Antiproton
Production Target
PP /
AP
FLAIR
RESR
CR
Observers
NESR
100 m
CN
DE
ES
FI
FR
GB
GR
IN
IT
PL
RO
RU
SE
Two Stage Synchrotron SIS100/300
 SIS100: High Intensity Booster and
GSI today
Compressor
SIS 100/300
Future facility
rapidly-cycling s.c. magnets (Bmax = 2 T; dB/dt = 4SIS
T/s)18
U28+ up to 2.7 GeV/u
Protons
up
to
30
GeV
UNILAC
 SIS300 High Energy Ring and Stretcher
fast s.c. high-field magnets (Bmax = 4.5 T - dB/dt = 1 T/s)
ESR
U92+ up to 34 GeV/u (q/A=0.5 45 GeV/u)
28+
U at 1.5 to 2.7 GeV/u with 100% duty cycle
CBM
Super
FRS
Rare-Isotope
Production Target
HESR
Antiproton
Production Target
SIS100
Heavy Ion
Operation
U28+ :
Fast Extract.: 6x1011 ppp
Slow Extract. Possible
Proton Operation
p:
RESR
Fast Extract.: 2.5 – 5x1013 ppp CR
PP /
AP
FLAIR
SIS300
Heavy Ion
Stretcher Mode
U28+ :
11
Slow Extract.:
100 m3x10 pps
(d.c.)
Heavy Ion
High Energy Mode
U92+ :
Slow Extract.: 1x1010 pps
NESR
Fields of Research at FAIR
Nuclear Matter QCD-Physics
with
SIS 100/300
Future facility
HI beams (2 to 45 GeV/u)
Nuclear Structure & Astrophysics
GSI today
with
SIS 18
beams of UNILAC
short-lived nuclei (0-1.5 GeV/u)
CBM
Physics
of Rare-Isotope
Dense Plasmas
Super
Production
with Target
FRS
compressed ion beams & highintensity petawatt-laser
Antiproton
ESR
HESR
PP /
AP
Hadron Physics & QCD
with
stored and cooled antiproton beams
RESR
(0 to 15 GeV/c)
CR
Solid-state and biological
applications
100 m
with
ion (& antiproton?) beams
Production Target
Fundamental Symmetries
Ultra-high electro-magnetic fields
FLAIR
& Quantenelectrodynamics
with
highly stripped ions and antimatter
NESR
Accelerator Physics
Fields of Research at FAIR
Nuclear Matter QCD-Physics
SIS 100/300
NuclearGSI
Structure
& Astrophysics
with
today
Future facility
with
HI beams (2 to 45 GeV/u)
SIS 18
PANDA
beams of
short-lived
nuclei (0-1.5 GeV/u)
UNILAC
CBM
CBM
ESR
HESR
PP /
AP
Hadron Physics & QCD
with
stored and cooled antiproton beams
RESR
CR
(0 to 15 GeV/c)
100 m
Solid-state and biological
applications
with
ion (& antiproton?) beams
Physics of Rare-Isotope
Dense Plasmas
Super
Production Target
FRS
with
compressed ion beams & highAntiproton
intensity petawatt-laser
Production Target
Fundamental Symmetries
Ultra-high
FLAIRelectro-magnetic fields
& Quantenelectrodynamics
with
NESR
highly stripped ions and antimatter
Accelerator Physics
High Energy Storage Ring, HESR
• High Rates
–
–
Total σ ~ 55 mb
peak > 107 int/s
• Vertexing
–
(σp,KS,Λ,…)
• Charged particle ID
–
(e±,μ±,π±,p,…)
• Magnetic tracking
• El-mag. Calorimetry
–
(γ,π0,η)
• Forward capabilities
–
(leading particles)
• Sophisticated Trigger(s)
PANDA Physics Program
Charmonium spectroscopy
Exotics: charmed hybrids &
heavy glueballs
Time-like
form factors
Medium
modifications
of charmed mesons
Drell-Yan
processes
Hard
exclusive
processes
CP-violation
(D &  - sector)
Hypernuclei
PANDA Physics Program
Charmonium spectroscopy
Exotics: charmed hybrids &
heavy glueballs
Time-like
form factors
Medium
modifications
of charmed mesons
Drell-Yan
processes
Hard
exclusive
processes
CP-violation
(D &  - sector)
Hypernuclei
Charmed Hadrons @ PANDA
Antiproton momentum [GeV/c]
0
2
4
ΛΛ
ΣΣ
ΞΞ
Two body
thresholds
DD
DsDs
nng,ssg
Hybrids
ΛcΛc ΩcΩc
ΣcΣc
ΞcΞc
ccqq
ccg
nng,ssg
Hybrids+Recoil
ccg
ggg,gg
Glueball
exotic
charmonium
ggg
Glueball+Recoil
qq Mesons
8 10 12 15
qqqq
Quark molecules
Gluonic
excitations
ΩΩ
6
light qq
π,ρ,ω,f2,K,K*
1
2
cc
J/ψ, ηc, χcJ
3
4
Mass [GeV/c2]
conventional
charmonium
5
6
Comparison e+e- versus pp
Crystal Ball
e+e- interactions:
only 1-- states formed
other states populated in
secondary decays
(moderate mass
resolution)
production of 1,2
e  e   '
1,2
 J / 
 e  e 
E 760 (Fermilab)
pp reactions:
all states directly formed
(very good mass
resolution)
formation of 1,2
pp  1,2
 J/
 ee
sm (beam) = 0.5 MeV
Charmed Hadrons @ PANDA
Antiproton momentum [GeV/c]
0
2
4
ΛΛ
ΣΣ
ΞΞ
Two body
thresholds
DD
DsDs
nng,ssg
Hybrids
ΛcΛc ΩcΩc
ΣcΣc
ΞcΞc
ccqq
ccg
nng,ssg
Hybrids+Recoil
ccg
ggg,gg
Glueball
exotic
charmonium
ggg
Glueball+Recoil
qq Mesons
8 10 12 15
qqqq
Quark molecules
Gluonic
excitations
ΩΩ
6
light qq
π,ρ,ω,f2,K,K*
1
2
cc
J/ψ, ηc, χcJ
3
4
Mass [GeV/c2]
conventional
charmonium
5
6
PANDA Physics Program
Charmonium spectroscopy
Exotics: charmed hybrids &
heavy glueballs
Time-like
form factors
Medium
modifications
of charmed mesons
Drell-Yan
processes
Hard
exclusive
processes
CP-violation
(D &  - sector)
Hypernuclei
Drell-Yan processes
• Cross section depends
on elementary process
qq   *
• Measured as a function of
polar angle  and
azimuthal angle 
• Direct access to quark
distribution functions
(no fragmentation
function involved)
• Complementary to DIS
Drell-Yan processes and parton distributions
• Unpolarised DY 
Boer-Mulders DF
h1┴ (PANDA @
HESR)

Single or double
polarisation DY 
transversity h1
(PAX @ HESR)
Hard exclusive processes  GPDs
Crossed channel (time-like)
Wide Angle Compton Scattering and DVCS:
p p  
(*)
• Hard scale:
large s ~ 10 GeV2 and │t│~
s, or large pT
• Soft part can be separated
and parameterised by
generalised distribution
amplitudes
• Experimental problem:
large hadronic background
(e.g. 00)
Time-like proton form factors
Crossed channel p p  ee:
• Goals:
– To measure time-like FF from
threshold up to high s = q2 in
one experiment
(reduced systematic error)
– To compare with space-like
FFs (pQCD at large s?)
• PANDA:
– Wide kinematical range
– Large solid angle coverage
– Large statistics
 High-quality measurement
of both GE and GM
PANDA Physics Program
Charmonium spectroscopy
Exotics: charmed hybrids &
heavy glueballs
Time-like
form factors
Medium
modifications
of charmed mesons
Drell-Yan
processes
Hard
exclusive
processes
CP-violation
(D &  - sector)
Hypernuclei
The phase diagram of strongly interacting matter
RHIC, LHC: high temperature, low baryon density
FAIR:
moderate temperature, high baryon density
Mapping the QCD phase diagram
“Trajectories” from 3 fluid hydrodynamics
Hadron gas EOS:
Y. Ivanov, V. Russkikh, V.Toneev
nucl-th/0503088
early phase not in
thermodynamic
equilibrium !
Compressed Baryonic Matter:
physics topics and observables
Location of the deconfinement phase transition at high B
 enhanced strangeness production ?
Observables: K, , , , 
 anomalous charmonium suppression ?
Observables: charmonium (J/ψ, ψ'), open charm (D0, D)
 Search for the critical point
Observable: event-by-event fluctuations (K/π, pT, ...)
 Search for the softest point
Observable: collective flow of hadrons
Chiral symmetry restoration at high B
 search for in-medium modifications of hadrons
Observables: , ,   e+e- , open charm, .....
Strangeness/pion ratios from central Au+Au (Pb+Pb) collisions
C. Blume for the NA49 collaboration, nucl-ex/0409008
Strangeness Production in Au+Au / Pb+Pb
SPS (NA 49)
AGS
RHIC
The CBM Experiment
 Radiation hard Silicon (pixel/strip) Tracking System in a magnetic dipole field
 Electron detectors: RICH & TRD & ECAL: pion suppression better 104
 Hadron identification: TOF-RPC
 Measurement of photons, π, η, and muons: electromagn. calorimeter (ECAL)
 High speed data acquisition and trigger system
CBM
8 – 45 AGeV
HADES
2 – 8 AGeV
Experimental challenges
Central Au+Au collision at 25 AGeV:
URQMD + GEANT4
160 p
400 400 +
44 K+
13 K-
 107 Au+Au reactions/sec
(beam intensities up to 109 ions/sec, 1 % interaction target)
 determination of (displaced) vertices with high resolution ( 50 m)
 identification of electrons and hadrons
J. Randrup and J. Cleymans, hep-ph/0607065
The critical point: can we locate it?
RM
NJL/inst
CJT
LSM
NJL
NJL/I
2
Meson production in central Au+Au collisions
W. Cassing, E. Bratkovskaya, A. Sibirtsev, Nucl. Phys. A 691 (2001) 745
SIS18
SIS100/
300
Annual yields at RHIC II & LHC
(from Tony Frawley
RHIC Users mtg.)
FAIR
at LHC: (10-50) x s
~10% of L
25% running time
• Phase Diagram
• EOS
• matter & constit. prop.
Quark Matter
• N-Hyperon Int.
Nuclear Matter • n-skin & beta
matter
• n-star & Q-matter
• thermal prop. ofQGP
charmonium states...
SPS
RHIC
LHC
Condensate
Nuclei
• spectral functions
(vector mesons) Hadrons
QCD
Vacuum
Nucleon-Nucleon / Meson
• SRC & PD
• 3NF
• p (N) structure
in-medium
Master Schedule
FAIR Baseline Technical Report 2006
Volume 1: Executive Summary
Volume 2: Technical Report Accelerators and Scientific Infrastructure
ca. 700 pages
Volume 3: Techn. Experiment Proposals on QCD physics (Volume 3A und 3 B;
ca. 450 pages
Volume 4: Techn. Experiment Proposals on Nuclear Structure and Astrophysics
ca. 700 pages
Volume 5: Techn. Experiment Proposals on Atomic Physics, Plasma Physics and
Applied Physics ca. 500 pages
Volume 6: Techn. Report Civil Constructions
a. Supplies
b. Electrical systems
c. Civil Engineering (Bung)
d. Radiation Safety
Supplement 1: Cost, Schedule, Manpower
Supplement 2: Costbook (5000 entries; 3500 WPs))
FAIR – Facility for Antiproton and Ion Research
Thank You !
CN
DE
ES
FI
FR
GB
GR
IN
IT
PL
RO
RU
SE