GSI Future Facility Walter F. Henning March 2003, LEAP03

GSI Future Facility

Walter F. HenningMarch 2003, LEAP03

• Introduction• Facility Layout and Characteristics• Scientific Areas and Goals• Research with Antiprotons• Summary

GSI Future Facility

UNILACSIS

FRS

ESR

100 m

SIS 100/200

HESRSuperFRS

NESR

CR

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+

GSI Facility Characteristics

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


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


SIS 100/200

2T, 4T/s 4 (6)T, 1 (2)T/s

FuE:Pulsed superconducting magnets

Collector (CR) and

Storage Rings (NESR)

for Ions and Antiprotons

Storage Rings

HESR - High Energy Storage Ring

1011 stored antiprotons0.8 - 14.5 GeVL = 2 x 1032

p/p ≥ 10-5

x/x ≥ 100m

Characteristics

electron collector electron gun

high voltage platform

magnetic fieldelectron beam

ion beam



magnetic field electron beam

ion beam

Storage Rings: Cooled Ion Beams




ion beam





ion beam





ion beam





ion beam


0.97 1 1.03

rel. ion velocity v/v0

ion

inte

nsity

before cooling

after cooling




ion beam


0.97 1 1.03rel. ion velocity v/v0

ion

inte

nsi

ty

before cooling

after cooling




ion beam



ion

inte

nsi

ty

before cooling

after cooling




ion beam



ion

inte

nsi

ty

before cooling

after cooling




ion beam



ion

inte

nsi

ty

before cooling

after coolingfrequency [Hz]

no

ise

po

wer

den

sity

a.u

.




ion beam



ion

inte

nsi

ty

before cooling

after cooling




ion beam



ion

inte

nsi

ty

before cooling

after cooling




ion beam



ion

inte

nsi

ty

before cooling

after cooling




ion beam



ion

inte

nsi

ty

before cooling

after cooling

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

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



Pro

ton

nu

mb

er

Z

Accreting white dwarf

Nova Cygni 1992

Sun

Elements in our solar system

Neutron number N





Hadron Structure and Quark-Gluon Dynamics - AntiprotonsNon-pertubative QCDQuark-gluon degrees of freedomConfinement and chiral symmetry






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




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





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




Nuclear Matter and the Quark-Gluon PlasmaNuclear phase diagramCompressed nuclear/strange matterDeconfinement and chiral symmetry


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






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


1011 stored antiprotons0.8 - 14.5 GeVL = 2 x 1032

p/p ≥ 10-5

x/x ≥ 100m

Characteristics

Quark-Gluon Structure of Hadrons

Confining potentiales


Confinement


Confinement


Mass of hadrons

Confinement


Mass of hadrons

Confinement


Mass of hadronsp - beams

SIS 18

SIS 200T [MeV]

300

LHC

RHIC

SPS

Chiral symmetry and quark condensate

Confinement


Mass of hadrons

Chiral symmetry

p - beams

SIS 18

SIS 200T [MeV]

300

LHC

RHIC

SPS

|<qq>|

Confinement


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

qq

Meson

Confinement


Mass of hadrons

Chiral symmetry

p - beams

SIS 18

SIS 200T [MeV]

300

LHC

RHIC

SPS

|<qq>|

Glueballs / Hybrids

qqgqq

Confinement


Mass of hadrons

Chiral symmetry

p - beams

SIS 18

SIS 200T [MeV]

300

LHC

RHIC

SPS

|<qq>|

Glueballs / Hybrids

qqgqq

Double Strangeness

Confinement


Mass of hadrons

Chiral symmetry

p - beams

SIS 18

SIS 200T [MeV]

300

LHC

RHIC

SPS

|<qq>|

Glueballs / Hybrids

qqgqq

Double Strangeness

Confinement


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

Confinement


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


p momentum [GeV/c]

Mass [GeV/c2]

Confinement


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


p momentum [GeV/c]

Mass [GeV/c2]


Confinement


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


p momentum [GeV/c]

Mass [GeV/c2]

Confinement


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


p momentum [GeV/c]

Mass [GeV/c2]

HESR Detector

Storage Rings

Positron-Antiproton Scattering(~1 GeV c.m.)

Structure Functions etc. CPT Invariance

Storage Rings

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

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

Concept for Staged Construction of the International Facility for Beams of Ions and Antiprotons

Total Costs: 675 Million Euro

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)

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“

Contributors to the CDR

GSI - Future Facility

Physics of Hadrons and NucleiFuture Facilities in Europe

ERA

European Research Area

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GSI Future Facility Walter F. Henning March 2003, LEAP03

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