gsi future facility walter f. henning march 2003, leap03 introduction facility layout and...
TRANSCRIPT
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GSI Future Facility
Walter F. HenningMarch 2003, LEAP03
• Introduction• Facility Layout and Characteristics• Scientific Areas and Goals• Research with Antiprotons• Summary
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GSI Future Facility
UNILACSIS
FRS
ESR
100 m
SIS 100/200
HESRSuperFRS
NESR
CR
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Present GSI Facility
UNILAC
SIS
FRS
ESR
Energies:Unilac < 20 MeV/uSIS 1-2 GeV/uESR < 0.8 GeV/u
Accelerator Parameters Parameters
3 Injectors
HSI: 8 mA Ar1+
18 mA Ar10+
15 mA U4+
2,5 mA U28+
0,5 mA U73+
Upgrade towards the Future FacilityFreqency (power): 0.3 Hz 3 HzSpace charge reduction (vacuum): U73+ U28+
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GSI Facility Characteristics
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Primary Beams
•1012/s; 1.5 GeV/u; 238U28+
•Factor 100-1000 over present in intensity•2(4)x1013/s 30 GeV protons•1010/s 238U73+ up to 25 (- 35) GeV/u
GSI Facility Characteristics
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Primary Beams
•1012/s; 1.5 GeV/u; 238U28+
•Factor 100-1000 over present in intensity•2(4)x1013/s 30 GeV protons•1010/s 238U73+ up to 25 (- 35) GeV/u
Secondary Beams
•Broad range of radioactive beams up to 1.5 - 2 GeV/u; up to factor 10 000 in intensity over present •Antiprotons 3 (0) - 30 GeV
•Cooled beams•Rapidly cycling superconducting magnets
Key Technical Features
Storage and Cooler Rings
•Radioactive beams•e – A collider
•1011 stored and cooled 0.8 - 14.5 GeV antiprotons
GSI Facility Characteristics
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SIS 100/200
2T, 4T/s 4 (6)T, 1 (2)T/s
FuE:Pulsed superconducting magnets
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Collector (CR) and
Storage Rings (NESR)
for Ions and Antiprotons
Storage Rings
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HESR - High Energy Storage Ring
1011 stored antiprotons0.8 - 14.5 GeVL = 2 x 1032
p/p ≥ 10-5
x/x ≥ 100m
Characteristics
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electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
electron collector electron gun
high voltage platform
magnetic field electron beam
ion beam
Storage Rings: Cooled Ion Beams
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electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
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electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
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electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
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electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
0.97 1 1.03
rel. ion velocity v/v0
ion
inte
nsity
before cooling
after cooling
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electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
0.97 1 1.03rel. ion velocity v/v0
ion
inte
nsi
ty
before cooling
after cooling
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electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
0.97 1 1.03rel. ion velocity v/v0
ion
inte
nsi
ty
before cooling
after cooling
![Page 17: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/17.jpg)
electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
0.97 1 1.03rel. ion velocity v/v0
ion
inte
nsi
ty
before cooling
after cooling
![Page 18: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/18.jpg)
electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
0.97 1 1.03rel. ion velocity v/v0
ion
inte
nsi
ty
before cooling
after coolingfrequency [Hz]
no
ise
po
wer
den
sity
a.u
.
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electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
0.97 1 1.03rel. ion velocity v/v0
ion
inte
nsi
ty
before cooling
after cooling
![Page 20: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/20.jpg)
electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
0.97 1 1.03rel. ion velocity v/v0
ion
inte
nsi
ty
before cooling
after cooling
![Page 21: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/21.jpg)
electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
0.97 1 1.03rel. ion velocity v/v0
ion
inte
nsi
ty
before cooling
after cooling
![Page 22: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/22.jpg)
electron collector electron gun
high voltage platform
magnetic fieldelectron beam
ion beam
Storage Rings: Cooled Ion Beams
0.97 1 1.03rel. ion velocity v/v0
ion
inte
nsi
ty
before cooling
after cooling
![Page 23: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/23.jpg)
0% 50% 100%
Radioactive Beams
Nucleus-NucleusCollisions
Antiprotons
Plasma-Physics
100 Tm Ring
200 Tm Ring
Collector & Storage Ring
High-Energy Storage Ring
Nucleus-Nucleus 100 sec
RadioactiveBeams
PlasmaPhysics
Antiprotons
Duty-Cycles of the Accelerator RingsDuty-Cycles of the Accelerator Rings Duty-Cycles of the Physics ProgramsDuty-Cycles of the Physics Programs
Parallel Operation
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Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Proton-rich nuclei•Proton radioactivity•Proton - neutron pairing•Isospin symmetry•Tests of standard model and symmetries•Nucleosynthesis
Neutron-rich nuclei•Neutron drip line•Shell quenching•Skins and halos•Loosley bound systems•Soft collective modes•Nucleosynthesis
Superheavy elements•Shell stabilization•Long-lived nuclei
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Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Pro
ton
nu
mb
er
Z
Accreting white dwarf
Nova Cygni 1992
Sun
Elements in our solar system
Neutron number N
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Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
![Page 27: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/27.jpg)
Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Hadron Structure and Quark-Gluon Dynamics - AntiprotonsNon-pertubative QCDQuark-gluon degrees of freedomConfinement and chiral symmetry
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Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Hadron Structure and Quark-Gluon Dynamics - AntiprotonsNon-pertubative QCDQuark-gluon degrees of freedomConfinement and chiral symmetry
![Page 29: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/29.jpg)
Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Hadron Structure and Quark-Gluon DynamicsNon-pertubative QCDQuark-gluon degrees of freedomConfinement and chiral symmetry
Nuclear Matter and the Quark-Gluon Plasma - Relativistic HI - BeamsNuclear phase diagramCompressed nuclear/strange matterDeconfinement and chiral symmetry
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Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Hadron Structure and Quark-Gluon Dynamics - AntiprotonsNon-pertubative QCDQuark-gluon degrees of freedomConfinement and chiral symmetry
Nuclear Matter and the Quark-Gluon Plasma - Relativistic HI - Beams Nuclear phase diagramCompressed nuclear/strange matterDeconfinement and chiral symmetry
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Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Hadron Structure and Quark-Gluon Dynamics - AntiprotonsNon-pertubative QCDQuark-gluon degrees of freedomConfinement and chiral symmetry
Nuclear Matter and the Quark-Gluon Plasma - Relativistic HI - Beams Nuclear phase diagramCompressed nuclear/strange matterDeconfinement and chiral symmetry
Physics of Dense Bulk Matter - Bunch CompressionProperties of high density plasmasPhase transitions and equation of stateLaser - ion interaction with and in plasmas
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Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Hadron Structure and Quark-Gluon Dynamics - AntiprotonsNon-pertubative QCDQuark-gluon degrees of freedomConfinement and chiral symmetry
Nuclear Matter and the Quark-Gluon Plasma - Relativistic HI - Beams Nuclear phase diagramCompressed nuclear/strange matterDeconfinement and chiral symmetry
Physics of Dense Plasmas and Bulk Matter - Bunch CompressionProperties of high density plasmasPhase transitions and equation of stateLaser - ion interaction with and in plasmas
SIS 18
Ion BeamHeating
Jupiter
Sun Surface
Magnetic Fusion
solid statedensity
Tem
pera
ture
[eV
]
Density [cm-3]
LaserHeating
PHELIX
Ideal plasmas
Strongly coupled
plasmas
Sun Core
InertialCofinement
Fusion
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Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Hadron Structure and Quark-Gluon Dynamics - AntiprotonsNon-pertubative QCDQuark-gluon degrees of freedomConfinement and chiral symmetry
Nuclear Matter and the Quark-Gluon PlasmaNuclear phase diagramCompressed nuclear/strange matterDeconfinement and chiral symmetry
Physics of Dense Plasmas and Bulk Matter - Bunch CompressionProperties of high density plasmasPhase transitions and equation of stateLaser - ion interaction with and in plasmas
Ultra High EM-Fields and Applications - Ions & Petawatt LaserQED and critical fieldsIon - laser interactionIon - matter interaction
SIS 18
Ion BeamHeating
Jupiter
Sun Surface
Magnetic Fusion
solid statedensity
Tem
pera
ture
[eV
]
Density [cm-3]
LaserHeating
PHELIX
Ideal plasmas
Strongly coupled
plasmas
Sun Core
InertialCofinement
Fusion
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Summary of Research Areas at the GSI Future Facility
Structure and Dynamics of Nuclei - Radioactive BeamsNucleonic matterNuclear astrophysicsFundamental symmetries
Hadron Structure and Quark-Gluon Dynamics - AntiprotonsNon-pertubative QCDQuark-gluon degrees of freedomConfinement and chiral symmetry
Nuclear Matter and the Quark-Gluon Plasma - Relativistic HI - Beams Nuclear phase diagramCompressed nuclear/strange matterDeconfinement and chiral symmetry
Physics of Dense Plasmas and Bulk Matter - Bunch CompressionProperties of high density plasmasPhase transitions and equation of stateLaser - ion interaction with and in plasmas
Ultra High EM-Fields and Applications - Ions & Petawatt LaserQED and critical fieldsIon - laser interactionIon - matter interaction
SIS 18
Ion BeamHeating
Jupiter
Sun Surface
Magnetic Fusion
solid statedensity
Tem
pera
ture
[eV
]
Density [cm-3]
LaserHeating
PHELIX
Ideal plasmas
Strongly coupled
plasmas
Sun Core
InertialCofinement
Fusion
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HESR - High Energy Storage Ring
1011 stored antiprotons0.8 - 14.5 GeVL = 2 x 1032
p/p ≥ 10-5
x/x ≥ 100m
Characteristics
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Quark-Gluon Structure of Hadrons
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Confining potentiales
Quark-Gluon Structure of Hadrons
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Confinement
Quark-Gluon Structure of Hadrons
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadronsp - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
Chiral symmetry and quark condensate
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
|<qq>|
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
|<qq>|
Glueballs Hybrids
qqg ggg
Hybrid Glueball
Normal meson: 2 fermionsP = (-1)L+1
C = (-1)L+S
Excited glue: bosonic degree of freedom→ exotic quantum numbers eg. JPC=1-+, 0--, 0+-, 2+-…→ normal quantum numbers
Signal:exotic quantum numbers:
partial wave analysisnormal quantum numbers:
model comparison (LGT)
mixing with normal mesonscharm sector: few resonances
with small widths
Meson
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
|<qq>|
Glueballs / Hybrids
qqgqq
![Page 45: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/45.jpg)
Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
|<qq>|
Glueballs / Hybrids
qqgqq
Double Strangeness
![Page 46: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/46.jpg)
Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
|<qq>|
Glueballs / Hybrids
qqgqq
Double Strangeness
![Page 47: GSI Future Facility Walter F. Henning March 2003, LEAP03 Introduction Facility Layout and Characteristics Scientific Areas and Goals Research with Antiprotons](https://reader031.vdocuments.us/reader031/viewer/2022013012/56649e905503460f94b94e20/html5/thumbnails/47.jpg)
Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
|<qq>|
Glueballs / Hybrids
qqgqq
Double Strangeness
Two-bodyThresholds
Molecules
Gluonic
Excitation
Mesons
Light MesonsCharmonium
p momentum [GeV/c]
Mass [GeV/c2]
Energy (mass) range covered by new GSI facility
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
|<qq>|
Glueballs / Hybrids
qqgqq
Double Strangeness
Two-bodyThresholds
Molecules
Gluonic
Excitation
Mesons
Light MesonsCharmonium
p momentum [GeV/c]
Mass [GeV/c2]
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
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Glueballs / Hybrids
qqgqq
Double Strangeness
Two-bodyThresholds
Molecules
Gluonic
Excitation
Mesons
Light MesonsCharmonium
p momentum [GeV/c]
Mass [GeV/c2]
HESR - High Energy Storage Ring
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
|<qq>|
Glueballs / Hybrids
qqgqq
Double Strangeness
Two-bodyThresholds
Molecules
Gluonic
Excitation
Mesons
Light MesonsCharmonium
p momentum [GeV/c]
Mass [GeV/c2]
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Confinement
Quark-Gluon Structure of Hadrons
Mass of hadrons
Chiral symmetry
p - beams
SIS 18
SIS 200T [MeV]
300
LHC
RHIC
SPS
|<qq>|
Glueballs / Hybrids
qqgqq
Double Strangeness
Two-bodyThresholds
Molecules
Gluonic
Excitation
Mesons
Light MesonsCharmonium
p momentum [GeV/c]
Mass [GeV/c2]
HESR Detector
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Storage Rings
Positron-Antiproton Scattering(~1 GeV c.m.)
Structure Functions etc. CPT Invariance
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Storage Rings
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Electroweak Force
Electromagnetic ForceQED
Weak ForceStandard Model
Strong Force
QCD
Gravitational ForceGeneral Relativity
galaxy1021 m
matter10-1 m
crystal10-9 m
atom10-10 m
atomic nucleus10-14 m
electron
nucleon10-15 m
<10-18 m
quark
DNA10-8 m
Structure of Matter
Research with Beams of Hadrons and Ions
Ion-Matter Interactions
Dense Plasmas
Ultra High EM FieldsNuclei at the Extremes
Quark Gluon Structure of Hadrons
Quark Matter
quark-gluon plasmaexcited vacuum
HI Beams 12 TW/g
RIBs 1.5 - 2 GeV/u
Antiprotons 0-15(30) GeV
Relativ. HI 35 GeV/u
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COSTS
Building and infrastructure: 225 Mio. € Accelerator: 265 Mio. €
Experimental stations / detectors: 185 Mio. €
Total: 675 Mio. €
SCHEDULE
0 100 200 300 400 500 600 700
Nuclear structurephysics
Antiproton physics
Nuclear matterresearch
Atomic physics
Plasma research
Materials research
Radiation biology
Accelerator physics New facilityGSI today
Users interest
Users, Costs and Schedules
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Concept for Staged Construction of the International Facility for Beams of Ions and Antiprotons
Total Costs: 675 Million Euro
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Major Milestones of the GSI Future Facility
1996 - 1999 Workshops and Working Groups
2001 Conceptual Design Report
2001 Review of Project by the Science Council (Wissenschaftsrat)
of the German Government
2002 Recommendation for Realization by the Wissenschaftsrat
2001 - 2002 Workshops and Formation of the Proto-Collaborations
2003 Cabinet Decision of the Federal Government to Fund the Project
(with: a) staging and b) 25% external contributions)
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Activities in Connection with the GSI Plans
Working Groups on Long-Term Perspectives of GSI
Deep-inelastic electron-nucleon and electron-nucleus scattering at s = 20 – 30 GeVConveners: V. Metag (GSI), D. v. Harrach (Mainz),A. Schäfer (Frankfurt)
X-ray spectroscopy and radiation physicsConveners: J. Kluge (GSI), H. Backe (Mainz), G. Soff (Dresden)
Nuclear collisions at maximum baryon densityConveners: P. Braun-Munzinger (GSI), R. Stock (Frankfurt),J. P. Blaizot (Saclay)
Physics with secondary beamsConveners: U. Lynen (GSI), D. Frekers (Münster),J. Wambach (Darmstadt)
Nuclear structure with radioactive beamsConveners: G. Münzenberg (GSI), D. Habs (LMU München),H. Lenske (Gießen), P. Ring (TU München)
Plasma physics with heavy ion beamsConveners: R. Bock (GSI), D.H.H. Hoffmann (Erlangen),J. Meyer-ter-Vehn (IPP München)
Accelerator studies (electron-nucleon/nucleus collider)Conveners: K. Blasche (GSI), J. Maidment (DESY),B. Autin (CERN), N. S. Dikansky (Novosibirsk)
Accelerator studies (high intensity option)Convener: D. Böhne (GSI)
Short Pulse/High Power LasersConvener: J. Kluge (GSI)
Letter of Intent: "Construction of a GLUE/CHARM Factory at GSI"
Editorial Board: B. Franzke (GSI)P. Kienle (Munich)H. Koch (Bochum)W. Kühn (Giessen)V. Metag (Giessen)U. Wiedner (CERN & Uppsala)
Contributions from W. Cassing (Giessen), S. Paul (Munich), J. Pochodzalla (Heidelberg), M. Soyeur (Saclay) and J. Wambach (Darmstadt) and many members of the Hadron Working Group for GSI.
25 Workshops on science and technical aspectsof the GSI future facility
Evaluation of the German Wissenschaftsrat
“Stellungnahme zu neun Großgeräten der naturwissenschaftlichen Grundlagenforschung und zur Weiterentwicklung derInvestitionsplanung von Großgeräten“
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Contributors to the CDR
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GSI - Future Facility
Physics of Hadrons and NucleiFuture Facilities in Europe
ERA
European Research Area