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NuSTAR – An Overview
Reiner KrückenTechnische Universität MünchenNuSTAR
Nuclear STructure, Astrophysics and Reactions
Annual NUSTAR Collaboration Meeting
> 800 members from 37 countries and 146 institutions
2Reiner Krücken - NuSTAR
Chair of the NuSTAR Board: Thomas Nilsson (Chalmers)
Low-energy QCD using chiral dynamics
Chiral extrapolation
Relativistic Nuclear Energy Density Functional constraint by low-energy QCD • isospin dependent forces from chiral dynamics
• natural inclusion of
• 3-body interactions
• tensor and spin-orbit forces
• pairing interaction
• Low-energy QCD is non perturbative no analytical ab-initio calculations possible
• Chiral Pertubation Theory offers possibility to study Structure and Phases of QCD
3Reiner Krücken - NuSTAR
Nuclei – towards a unified theoretical framework
Vlow-k, VUCOM (+3N)
AV18, CD Bonn + 3N EFT
Greens Function Monte CarloNo Core Shell Model
Coupled Cluster
Large Scale Shell Model
Density Functional TheoryRelativistic Mean Field Theory
4Reiner Krücken - NuSTAR
New shell gaps through residual interaction
Nuclear structure at the extremes of isospin
New shell gaps through residual interaction
Halos
11Li
9Li
2n
δrRn-Rp
Neutron Skins Neutron stars
EOS
Shell quenching bydiffuse surface
Interplay
sdr
dUUU lss
Soft collective modes(Pygmy Resonance)
5Reiner Krücken - NuSTAR
40
39 41
32
31
302928
27
262524
23
18 O (1970)
F (1999)
Ne (2002)
24
4038
37
36
36
35
3433
544644434240 48
50
45
49484746
32
Na
Mg
Al
Si
P
S
Cl
Ar
K
Ca
Sc
Ti
36
43
44
19 31
222120
47
51
Classic shells
New shells
island of inversion
deformed ground state
34
16 17
15 N (1985)
Na (2002)
Mg (2007)
Si (2007)
Al (2007)
new doubly magic nucleiN=16
N=34N=28
N=20
N=8
Changing shell structure in light nuclei
6Reiner Krücken - NuSTAR
Nuclear Astrophysics at FAIR
rp-, p-process:• masses at & beyond the proton drip-line• (p,), (,p) rates
r - process
7Reiner Krücken - NuSTAR
r-process:• masses, half-lives• -delayed neutron emission• (,n), (n,) rates• shell structure
FAIR will provide unique access to many nuclei relevant in explosive nucleosynthesis
rp- p
roce
ss
Shell structure and the r-processNuclear shell structure- defines r-process path- imprinted in abundance pattern- maybe modified for exotic nuclei
r - process
Pfeiffer et al.
J.J. Cowan, C. Sneden, Nature 440 ( 2006)
robust r-process pattern
Combine accurate nuclear physics and precision astronomy to constrain astrophysical scenarios
8Reiner Krücken - NuSTAR
Central Topics for NuSTAR at FAIR
• Quest for the limits of existence
• Halos, Open Quantum Systems, Few Body Correlations
• Changing shell structure far away from stability
• Skins, new collective modes, nuclear matter, neutron stars
• Phases and symmetries of the nuclear many body system
• Understanding the origin of the heavy elements
unified theory (ab-initio, density functional, shell model)
9Reiner Krücken - NuSTAR
The Super-FRS
Central instrument for the NuSTAR program!!
10Reiner Krücken - NuSTAR
Z
Super-FRS
FRS30X
10X
Two-stage separation yields isotopic nuclear beams
Fission
Fragmentation
I II
I II
• High acceptance for projectile fragments and fission products
• Two-stage separation for îsotopically clean beams
• More than one order of magnitude transmission gain relative to FRS
SC MultipletsRemote HandlingTarget & Beam Catcher
SC Dipoles
Cryogenics
Radiation Resistant Magnets
Technical Challenges
11Reiner Krücken - NuSTAR
NuSTAR Experiments in Modularized Start Version
• ILIMA in CR: Masses and Half-lives for short-lived ions
•R3B: (full capability) Reactions with Relativistic Radioactive Beams in complete kinematics
Primary Beams
• 1012/s; 1.5-2 GeV/u; 238U28+
• Factor 100-1000
Secondary Beams
• up to factor 10 000
Accommodate LEB experiments at available Super-FRS focal points
• HISPEC: In-Flight Spectroscopy
• DESPEC: Decay Spectroscopy
• MATS: Penning trap system (Masses, Trap Assisted Spectroscopy)
• LASPEC: LASER Spectroscopy (Spins, Moments, isotope shifts)
SIS 100
12Reiner Krücken - NuSTAR
NuSTAR provisional experimental areas (discussion)
13Reiner Krücken - NuSTAR
NuSTAR Experimental areas (full version)
14Reiner Krücken - NuSTAR
SF Magnets for the EB / MS (LoI by India)
Dipole (unit): = 4.35 m = 22.5° Bmax = 1.6 T
W = ±350 mm G = ±100 mm
Quadrupole: Leff = 0.8/1.2 m
RWarm = 300 mm
gmax = 4.7/5.2 T/m
• Energy buncher cost is covered in Module 3• Missing building (~ 5 MEuro) in Module 4• Can be built immediately when extra funds available• has high priority within NuSTAR and FAIR no delay in construction expected
15Reiner Krücken - NuSTAR
NuSTAR Experiments in Modularized Start Version
• R3B will have its full capability for rates > 1pps
• High energies (> 1AGeV) world-wide unique experiments
Neutrons
Heavy fragments
Large acceptancedipole magnet
• Target• Tracker• Calorimeter
RIB from Super-FRS
Protons
16Reiner Krücken - NuSTAR
R3B: Reaction studies at the highest energies in complete kinematics
• Few body correlations (halo nuclei, open quantum systems)
• Dipole response (Pygmy resonance, n-skins, neutron matter, EOS)
• Single-particle structure (shell-evolution, r-process path)
• Fission & fragmentation dynamics (large scale collective motion, symmetry energy, EOS)
• (gamma,n) reactions (r-process path)
DiamondTracker
Indian proposalCALIFAreadoutelectronics Indian proposal
NeuLANDRPC construction
NeuLAND – Neutron Detector for R3B
Detector development at SINP, Kolkata
MRPC detectors between iron convertors
Dipole Excitations of Neutron-Rich Nuclei- Symmetry Energy, Neutron Skin, and Neutron Stars -
neutron skin core vibration
LAND collaboration A. Klimkiewicz, PRL subm. P. Adrich, PRL 95 (2005)
124Sn
132Sn
Photoabsorption
Coulomb excitation
130SnP. Ring et al.
18Reiner Krücken - NuSTAR
excitation of the neutron skin
Dipole Excitations of Neutron-Rich Nuclei- Symmetry Energy, EOS and Neutron Stars -
Pyg
my
stre
ngth
Asymmetry a4 [MeV]
N. Paar
RQRPA
19Reiner Krücken - NuSTAR
NuSTAR Experiments in Modularized Start Version
DESPEC: decay spectroscopy using gamma-ray spectroscopy and neutron detection following isomeric or beta-decay of very exotic nuclei • Gamow Teller strength (short range correlations, nucleosynthesis, supernovae)
• Structure along the proton drip-line (proton radioactivity, rp-process)
• Structure of r-process nuclei (shell evolution, r-process path)
• g-factors and lifetimes of isomers (evolution of shells and collectivity, nuclear shapes)
• Experiments possible with stopped beams & production rates down to 1 isotope per hour • farthest reach towards the drip lines
100Sn (1 per hour)
A/Q
Z
20Reiner Krücken - NuSTAR
Indian proposals:• Planar Ge• Neutron Detectors• Silicon Detectors
RISING on the way towards DESPEC
Reiner Krücken - NuSTAR 21
A. Jungclaus et al.,
PRL (2007)
S.J. Steer et al., PRC (2008)
C. Hinke, K. Eppinger et al.
NuSTAR Experiments in Modularized Start Version
LYCCAReaction product identification
Fragmentbeam
HISPEC: high resolution in-flight gamma-spectroscopy
• Excited states in exotic nuclei
• Inelastic excitation (EM, hadronic), secondary fragmentation, knock-out
• Lifetimes and g-factors of short-lived excited states
(evolution of shells and collectivity)
(phase-/shape-transitions & shape coexistence)
(isospin symmetry, pn-pairing)
• Experiments possible with medium-energy beams (50-100 AMeV)• Broad program for nuclei with A up to ~100
22Reiner Krücken - NuSTAR
Coulex sample spectrum (RISING)
NuSTAR Experiments in Modularized Start Version
MATS and LASPEC: ground state properties using high-precision techniques• Penning trap system (MATS)
• High-precision masses for highly charged ions
• Trap-assisted and in-trap spectroscopy
• Laser spectroscopy (LASPEC)
• Ground state spins, moments, isotope shifts from laser spectroscopy
(evolution of shells and nuclear shapes)
(nuclear astrophysics input: masses, EC rates, GT strength)
(test of fundamental symmetries: CKM unitarity, CVC)
• Stopping in and extraction from gas-cell
• charge breeding & non-destructive techniques
• half-life limit ~10ms
• Access to refractory elements, highest precision
23Reiner Krücken - NuSTAR
NuSTAR Experiments in Modularized Start Version
• Masses with precision ~50 keV
• Many masses at same time
• access to nuclei with half-lives shorter than cooling times
24Reiner Krücken - NuSTAR
ILIMA in CR: mass measurements of nuclei with half-lives in the ms region • Masses of very exotic nuclei using isochronous mode & TOF technique
• Half-lives via detection of decay products with particle detectors
• Study of isomeric states
(shell evolution, effective interaction)
(nuclear astrophysics input: masses, half-lives)
ILIMA in CR
Reiner Krücken - NuSTAR 25
Super-FRS+CR enables unique program for mass and lifetime measurements of very short lived, few-electron ions
In particular large areas of the r-process path can be covered
Low-energy cave and Energy Buncher
Dedicated Low-Energy-Branch experimental area more efficient experimental program:
• no loss of time through set-up work• access during other experimental runs (R3B)
26Reiner Krücken - NuSTAR
NuSTAR programme at the NESR (Module 4)
Experiments with stored, electron cooled ion beams• World-wide unique• Conceptionally new experiments
ILIMA• electron cooled beams needed for
• higher precision and separation(ground and isomeric states)• time-resolved studies (unique decay modes, e.g. bound beta decay)
• studies with pure isomeric beams
EXL: Elastic and inelastic scattering, reaction with low-momentum transfer• matter distributions, monopole resonances, capture reactions, charge exchange reactions, transfer, knock-out
(n-skins, compressibility, GT-strength, shell evolution, nucl. astrophysics reactions)
27Reiner Krücken - NuSTAR
Vigorous R&D program and development of demonstration experiments at ESR
Electron Ion Collider (ELISe) (Phase B)
fromRESR
NESR
e-LI
NAC
Future Extension: Antiproton-Ion Collider (AIC)• neutron-skin thickness• antiproton-neutron interaction• antideuterons ?
• charge densities from (e,e) scattering• multipolarities of collective modes via (e,e’) scattering • single-particle structure from (e,e’N) reactions
28Reiner Krücken - NuSTAR
The aims of NuSTAR @ FAIR
Nuclear Structure Physics: Isospin dependence of effective nuclear interaction
Modification of shell structure far off stability (role of tensor, 3-body interactions)
New effects in weakly bound & open quantum systems (halos, skins, soft modes)
Relevant symmetries, structural evolution, role of phase transitions
Nuclear Astrophysics Studies: Nuclear properties and reaction rates in explosive nucleosynthesis
Nuclear Reaction Studies: Investigate reaction dynamics for RIB production, spallation, ADS Dynamics in systems with weakly bound nucleons (halos, correlations, continuum,
low density nuclear matter)
Towards a unified description of nuclear structure and dynamics Towards and understanding of the origin of the heavy elements