Title: Nuclear Astrophysics
1Nuclear Astrophysics
- Roland Diehl
- Nuclear Astrophysics Science Issues
- Specific Sub-Topics Status, Challenges,
Requirements - Next Steps for Gamma-Ray Astronomy Missions
2The Key Science Questions of Nuclear Astrophysics
- How are the elements and isotopes formed, which
we see throughout the universe? - How do nuclear transmutations affect the sites
where they occur?
3Key Science Question 1 The Cosmic Abundance
Pattern
- How are the elements and isotopes formed, which
we see throughout the universe?
4Key Science Question 1 (current-day frontier)
Cosmic Nuclear Reaction Dynamics
- How are the elements and isotopes formed, which
we see throughout the universe? - Nuclear-Reaction Dynamics
- Specific Isotopic Abundances as Calibration
Marks
Cas A _at_ 1.157 MeV 44Ti (T1/259y)
5Key Science Question 2 (e.g.) Stellar
Evolution
- How do nuclear transmutations affect the sites
where they occur?
Stars are gravitationally- confined
thermonuclear reactors Stellar structure lt-gt
Nuclear-reaction physics
6Key Science Question 2 (current-day frontier)
Cosmic Explosions
- How do nuclear transmutations affect the sites
where they occur?
500 msec (fast!) R10000km)
- SNIa - HOW?
- Explosive C Burning
- Flame Propagation Dynamics
- Issues
- Rapid Time Scales
- Huge Range in Spatial Dimensions
7Key Science Question 1 The Present Status
- How are the elements and isotopes formed, which
we see throughout the universe? - Basics known (processes)
- Details poorly understood (e.g.)
- SNIa Fe yield 0.5 0.4 Mo
- Unknown sites for r-process(es), p nuclei
synthesis - Unknown relevant nuclear-reaction rates
- Uncertain relevance of neutrino reactions (ccSN)
- Stability of heavy nuclei (deformations, skin,?)
- Cosmic-ray nucleosynthesis (LiBeB) contribution
uncertain
8Nuclear Reaction Uncertainties in Astrophysics
- New Effects
- EC in initial cc-SN n shells partly occupied
at finite (SN) temperature
Experimentally-Unaccessible Reactions Target and
Projectile areRadioactive/shortlived
9Key Science Question 2 in Nuclear Astrophysics
- How do nuclear transmutations affect the sites
where they occur? - Basics known (stellar phases, explosions)
- Details poorly understood
- SNIa lightcurves vs. composition and GCE
- Shell burnings in massive stars and AGB
- Explosive C burning in SNIa
- Explosive shell burnings in SNII
- Burried C burning in Type-I XRB Superbursts
10Key Science Question 2 (current-day frontier)
Cosmic Explosions, Stars
- How do nuclear transmutations affect the sites
where they occur?
- SNIa
- Nuclear-Burning Front
- CC-SN
- pe-gtn initial collapse
- Stars
- Stellar Core Sizes lt-gt
- 12C(a,g)16O
11Key Science Question 2 (current-day frontier)
Stellar Structure in Late Phases
- Episodes of Core and Shell Burning
- Impacts on Pre-SN Core Size Composition
- Nucleosynthesis Products
12Key Science Questions Interested?
- If we want to go beyond empirical models of the
effects of - Sources of nucleosynthesis -gt chemical
evolution - Stellar structure explosions -gt object/event
frequencies - then we need to proceed investigating the
nuclear physics in cosmic environments - MeV Gamma-rays are a natural messager
- (nuclear binding energies)
13Key Science Questions Relevant?
- If we want to go beyond current nuclear astronomy
data of - Gamma-ray observatories (survey _at_10-5 ph cm-2
s-1 E/dE500) - Indirect methods (e.g. inferred abundances from
meteorites, recombination) - then we must identify the uniqueness of cosmic
gamma-rays in nuclear-astrophysics topics
14Cosmic Vision in Nuclear Astrophysics
- We seek understanding of cosmic phenomena in
terms of nuclear-physics - We want to add new qualities to existing astronomy
15Gamma-Ray Lines for Nucleosynthesis Study
- Radioactive Trace Isotopes as Nucleosynthesis
By-Products - For Gamma-Spectroscopy We Need
- Decay Time gt Source Dilution Time
- Yields gt Instrumental Sensitivities
16Status and Issues, in more detail
- Thermonuclear Supernovae (56Ni)
- Core Collapse Supernovae (56Ni, 44Ti)
- Novae (22Na, 7Be, e)
- Cumulative Nucleosynthesis
- Cosmological (56Ni)
- Massive Stars (26Al, 60Fe)
- Supernovae and Novae (e annihilation)
17Thermonuclear Supernovae (SNIa)
- Rarely SNIa 56Ni Decay Gamma-Rays are Above
Instrumental Limits (10-5 ph cm-2 s-1) - 2 Events captured / 9 Years CGRO
- Signal from SN1991T (3s) (13 Mpc)
- Upper Limit for SN1998bu (11 Mpc)
- 2 Candidate Events / 2 Years INTEGRAL
- Gamma-Ray Results
- Controversial
- Exceptional Events (1991T)?
- Systematic Uncertainty too Large!
18Thermonuclear Supernovae (SNIa)
Close Binary System
SN IaProgenitor Models
Giant
WD
White Dwarf Merger
Binary Mass Transfer
He Layer
C/O Layer
- Issues
- The 56Ni Power Source 0.5 Mo of 56Ni??
- Which Progenitor Path?
- Which Explosion Model?
WD at MCh
He Shell Flash
SN Ia
Central C Ignition
19Core Collapse-Supernovae Model
Empirical / Parametrized Models for
Explosion(Explosion Energy, Mass Cut)
- Explosion Mechanism Competition Between Infall
and Neutrino Heating - 3D-Effects Important for Energy Budget AND
Nucleosynthesis
20Core Collapse Supernovae 56Ni and 44Ti
- Consistency of cc-SN Model Cas A vs.
- 44Ti from Models/SN1987A/g-Rays
- 44Ti Correlation to
- Large Explosion Energy
- Large Mass of 56Ni (Bright Supernova)
Aspherical explosions?? (-gtGRB) Need Event
Statistics, 44Ti Spectra
21Core Collapse Supernovae 60Fe
- Neutron Capture on 56,58Fe
- n Sources
- 13C(a,n)16O (He Burning)
- 20Ne(a,n)23Na (O/Ne Burning)
- Sites/Locations
- CC-Supernova O/Ne Shell and Bottom of He Shell
- Giant Phase of Massive Star He Shell, C Shell
- Astrophysical Significance
- Clarify SN Nuclear-Reaction Parameters
(multi-paramter issue!) - CC-SN Shell Structure
- n Capture from Fe-Group Elements-gt r-process
feeding
22Novae
- Brief Annihilation Flash
- b Decay Continuum (before optical nova!)
- 22Na Radioactivity (O-Ne Novae)
- None SeenYet
- Need ltlt2kpc
- 511 keV Flash survey
23SNIa Cosmology with Gamma-Rays
- Cosmological SN Fill in MeV Emission to Diffuse
Background (gap between AGN and Blazars SN
lines redshift-gt characteristic cont) - SN rate (zgt5), SNIa/cc-SN ratio (z SNIa delay)
24Massive Stars 26Al
- Nucleosynthesis in the Current Galaxy (t106y)
- Massive Stars are dominating sources
- COMPTEL imaging
- Massive-Star clusters of right age are
26Al-bright - Population synthesis
- Nucleosynthesis products from massive-star
clusters ejected into ISM cavities - COMPTEL Orion
- SPI Line Shapes
- Astronomical window to massive-star activity
2526Al Astronomy
- ISM Properties Near 26Al Sources
- 26Al Ejected into Hot Cavities (WR Winds, ) -gt
ISM Turbulence lt-gt Line Width-gt 26Al Source
Offset from Clusters - 26Al Condensed on Dust, Re-accelerated -gt
High-Velocity Tail?
Orion OB1 Plüschke et al. 2001
- Massive-Star Clusters
- Characteristic 26Al Lightcurve 3-7 My,
WR-gtSNe-gt Cluster Ages
26Galactic Astronomy of 26Al Sources
- Galaxy Nearby Groups of Stars
27The 60Fe Puzzle
Model Predictions
- No Source Would Bring the 60Fe/26Al Gamma-Ray
Intensity Ratio Close to Measurement Constraints!
(Factor 5!) - Nuclear Physics?
- Model Sample Statistics?
- Uncertainties
- n Capture Cross Sections for Fe Isotopes
- b Decay Rate for 59Fe
- Development of Hot-Base He Shell, C Shell
- n Source Activation
28Annihilation of Positrons in the Galaxy
- Positron-Source Variety
- Nucleosynthesis Sources (SNIa, )
- Pulsars, Binaries, Jet Sources
- Light Dark Matter Annihilations
- Annihilation in Diluted ISM (t105y)
- Status (INTEGRAL / SPI)
- Annihilation Rate (_at_GC) 1.4 1043 s-1
- Annihilation in Warm ISM Phase
- Extended 511 keV Line Emission
- Extended, bulge-like Emission (dl8o,db7o)
- Weak Disk Emission No Fountain
- -gt Young Stars make Minor Contribution
- Old stellar population!
- Dark-Matter Annihilations?
29Positron Annihilation Prospects
- After INTEGRAL
- Annihilation emission mapped throughout the
Galaxy - Inner-Galaxy 511 keV line shape well-measured
- Issues
- Other galaxies?
- Point sources?
- Specific regions with known sources?
- Dark matter constraints?
30Unique Nuclear-Astrophysics Info from Gamma-Rays
- SNIa
- Absolute Amount of 56Ni Radioactivity
- Progenitor Type
- Inner Explosion Kinematics
- CC-SNe
- Inner Core of SN Explosion (near mass cut)
- Shell Structure and Explosive Burning
- n Capture on Fe-Group Nuclei
- Novae
- Progenitor Evolution, Burning-Zone Mixing
- Cumulative Nucleosynthesis
- Cosmic SNIa Rate
- Massive-Star Group Nucleosynthesis
- ISM Around Massive Stars at 106y Time Scale
- Positron Transport in ISM/Galaxy
31Future Telescopes for Gamma-Ray Lines
- Advanced Compton Telescope
- Steve Boggs et al. -gt Elemental Origins Probe
- Laue Lens Photon Concentrator
- P. von Ballmoos et al. -gt MAX
32Instrumental Sensitivities for Gamma-Ray Lines
Advanced Compton Telescope
Courtesy S. Boggs, 2003
33Unique Nuclear-Astrophysics Info from Gamma-Rays
- SNIa
- Absolute Amount of 56Ni Radioactivity
- Progenitor Type
- Inner Explosion Kinematics
- CC-SNe
- Inner Core of SN Explosion (near mass cut)
- Shell Structure and Explosive Burning
- n Capture on Fe-Group Nuclei
- Novae
- Progenitor Evolution, Burning-Zone Mixing
- Cumulative Nucleosynthesis
- Cosmic SNIa Rate
- Massive-Star Group Nucleosynthesis
- ISM Around Massive Stars at 106y Time Scale
- Positron Transport in ISM/Galaxy
34Key Science in Nuclear Gamma-Ray Astrophysics
- Understand Supernova Explosions
- Exploit Line Astronomy in 26Al and e
Annihilation
35Unique Nuclear-Astrophysics Info from Gamma-Rays
- SNIa
- Absolute Amount of 56Ni Radioactivity
- Progenitor Type
- Inner Explosion Kinematics
- CC-SNe
- Inner Core of SN Explosion (near mass cut)
- Shell Structure and Explosive Burning
- n Capture on Fe-Group Nuclei
- Novae
- Progenitor Evolution, Burning-Zone Mixing
- Cumulative Nucleosynthesis
- Cosmic SNIa Rate
- Massive-Star Group Nucleosynthesis
- ISM Around Massive Stars at 106y Time Scale
- Positron Transport in ISM/Galaxy