nuclear astrophysics luna-mv – the next underground ... · luna-mv – the next underground...
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
Frank StriederRuhr‐Universität Bochum, GermanySeconda
Universita
di Napoli, Caserta, Italy
EuroGENESIS
Workshop – Origin of the
ElementsBarcelona, Catalunya14.06.2013
LUNA-MV – The next UndergroundAccelerator Facility
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
Outline
of this
Presentation
LUNA-MV – The next Underground Accelerator Facility
•
History
and Status of the
LUNA-MV project
• Site preparation
at the
Laboratori
Nazionali
del Gran Sasso
• Astrophysical
Motivation and Advantage going
Underground
• Holy Grail
of Nuclear
Astrophysics
–
12C(α,γ)16O
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
History
of LUNA‐(MV)
in 2000: LUNA-400kV was installed → talk
by
G. Imbriani
(Wednesday)
in April 2007: a Letter of Intent was presented to the LNGS Scientific Committee about key reactions in He burning and the s-process neutron sources:12C(α,γ)16O, 13C(α,n)16O, and 22Ne(α,n)25Mgas well as (α,γ) reactions on 14,15N and 18O
→ 3.5 MV single ended positive ion accelerator
→
… 2013 …
something moved forward (finally)
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
A suitable place inside LNGS has been found (Node B), far away from other experiments. A real feasibility study started!
LUNA‐MV
LUNA
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
Single ended accelerator: •with Ion source for H and He beams → high intensity α
beams
• robust, commercially available • reliable time line, reliable costing• 2 beam lines, accessible independently
LUNA‐MV
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
LNGS is a low background laboratory: a shielding solution has been developed and validated by Monte Carlo simulations
Just‐outside the wall the n‐flux is less than 1% of the LNGS natural flux!
LUNA‐MVLUNA‐MV
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
LNGS is a low background laboratory: a shielding solution has been developed and validated by Monte Carlo simulations
Just‐outside the wall the n‐flux is less than 1% of the LNGS natural flux!
LUNA‐MVLUNA‐MV
Constrains for neutron background
Natural Neutron flux in LNGS: appr. 1 -
2×10-6
cm-2
s-1
→
LUNA MV has been asked to verify compatibility with existing experiments→
Maximum neutron rate acceptable at LUNA-MV: 2000 n/s
→
Maximum neutron energy: 5.6 MeVLUNA has presented a shielding concept which allows to respect these constraintsThe concept is approved by LNGS.
Constraints due to drinking water abstraction
LUNA MV location is close to springs used for drinkable water→ special requirements to assure preservation of water qualityLNGS technical division has engineered a project to protect springs
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
60 participants mainly from Europe but also Asia and USA
• Status of LUNA MV•
Physics cases with round table on
specific technical aspects•
Discussion on the
collaboration structure
• Request for adhesions"adhesion should be intended as the
willingness of the involved group to apply soon to the financing agency of the respective country....“
process is still open, please contact: [email protected]
LUNA‐MV Workshop and status
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
60 participants mainly from Europe but also Asia and USA
• Status of LUNA MV•
Physics cases with round table on
specific technical aspects•
Discussion on the
collaboration structure
• Request for adhesions"adhesion should be intended as the
willingness of the involved group to apply soon to the financing agency of the respective country....“
process is still open, please contact: [email protected]
LUNA‐MV Workshop and status
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
4000 5000 6000 7000 8000 9000 10000 110001
10
100
1000
spectrum 25Mg(p,γ)26Al (Geant4) environmental backgr. beam induced backgr. total
25Mg (p,γ)25Al
11B
C
ount
s pe
r 40
keV
Eγ [keV]
13C
Ep = 100 keV
Motivation for
Underground measurement
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
Motivation for
Underground measurement
4000 5000 6000 7000 8000 9000 10000 110001
10
100
1000
spectrum 25Mg(p,γ)26Al (Geant4) environmental backgr. x5 beam induced backgr. total
25Mg (p,γ)25Al
11B
C
ount
s pe
r 40
keV
Eγ [keV]
13C
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
William A. Fowler (1911 –
1995)
Nobel Prize
for
Physics
(1983) for
„his theoretical
and experimental studies
of thenuclear
reactions
of importance
in the
formation
of the
chemical
elements
in the
universe“. (shared
with
S. Chandrasekhar)
noble prize
lecture, 1983
„…
the
holy
grailof nuclear
astrophysics“
LUNA‐MV Physics
‐
12C(α,γ)16O almost 40 years
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
Carbonwe are made of !
Oxygenwhich we breath !
Consequenceslate stellar evolutioncomposition of C/O White dwarfsSupernova type I explosionSupernova type II nucleosynthesis
Stellar Helium burning in Red Giant Stars
the
He burning
is
ignited
on the
4He und 14N ashes
of the preceding
hydrogen
burning
phase
(pp
und CNO)
LUNA‐MV Physics
‐
12C(α,γ)16O
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
relevant questions:Energy production and time scaleof Helium burning:4He(2α,γ)12C(α,γ)16O(α,γ)20Ne
Neutron sources for s process:
14N(α,γ)18F(β+ν)18O(α,γ)22Ne(α,n)22Ne(α,γ) Oxygen-16
Stellar Helium burning in Red Giant Stars
the
He burning
is
ignited
on the
4He und 14N ashes
of the preceding
hydrogen
burning
phase
(pp
und CNO)
LUNA‐MV Physics
‐
12C(α,γ)16O
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
example: Stellar model for a 20 Msolar SternS factor(CF85) = 2 ×
S factor(CF88)
0
0,2
0,4
0,6
0,8
1
0,E+00 3,E+05 6,E+05 9,E+05t(yr)
XHe
(ΔtHe /tHe )CF85-88 ≤
10%
CF88
CF85
0
0,2
0,4
0,6
0,8
1
0,E+00 3,E+05 6,E+05 9,E+05t(yr)
X (ΔX12C /X12C )CF85-88 ≈
50%
12C
16O
CF85
CF88
12C/16O ratio
at the
end of Helium burning
G. Imbriani
et
al., ApJ
558 (2001) 903
& O. Straniero
private communication
CF88S300 = 100 keV b
CF85S300 = 200 keV b
in Gamow window
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
example: Stellar model for a 20 Msolar SternS factor(CF85) = 2 ×
S factor(CF88)
0
0,2
0,4
0,6
0,8
1
0,E+00 3,E+05 6,E+05 9,E+05t(yr)
XHe
(ΔtHe /tHe )CF85-88 ≤
10%
CF88
CF85
0
0,2
0,4
0,6
0,8
1
0,E+00 3,E+05 6,E+05 9,E+05t(yr)
X (ΔX12C /X12C )CF85-88 ≈
50%
12C
16O
CF85
CF88
12C/16O ratio
at the
end of Helium burning
G. Imbriani
et
al., ApJ
558 (2001) 903
& O. Straniero
private communication
CF88S300 = 100 keV b
CF85S300 = 200 keV b
in Gamow window
Why is the 12C(α,γ)16O so important?
The energy generation interferes with the structural dynamics of the stellar evolution!
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
M. Fey, Stuttgart, Ph.D. thesisEγ
[MeV]9.0 9.5 10.0
expected. Eγ
= 8.05 MeV
Direct
Methods
–
γ‐ray
Experiments
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
M. Fey, Stuttgart, Ph.D. thesisEγ
[MeV]
7.5 8.0 8.5
expected. Eγ
= 8.05 MeV
Direct
Methods
–
γ‐ray
Experiments
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
Phaseshift
fixed
through
elastic
scattering
data
Measurements
at low
energies
are
very
difficult
!!
Direct
Methods
–
γ‐ray
Experiments
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS12C(α,γ)16O –
towards
LUNA-MV12C(α,γ)16O –
State of the
Art
Influ
ence
of tw
osu
bthr
esho
ld s
tate
s (total)
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS12C(α,γ)16O –
Open Issues
Influ
ence
of tw
osu
bthr
esho
ld s
tate
s (total)
poor
statistic
of low-energy
data
E1 ExtrapolationReliability
of 16N β-delayed
α-decay
E2 Extrapolation largely
unconstrained
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS12C(α,γ)16O –
Open Issues
Influ
ence
of tw
osu
bthr
esho
ld s
tate
s (total)
E1 destructive
interferenceStot
(0.3) → 50 % lower
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
Work in Progress:a Working Group between LUNA and ERNA was established→ ERLUNA Working GroupLUNA: direct kinematics -
α
beam, 12C solid target, γ-ray detection
→ measure angular distribution with E1 and E2ERNA: inverse kinematics -
12C beam, 4He gas target, γ-ray detection & recoil mass separator
→ measure Stot
(E) and cascade transitions
Objectives of Working Group:•
determination of Stot
(0.3) with sufficient precision for stellar models
•
identify and exploit synergies between two different approaches
• coordinate efforts and strategy
• solve common experimental issues, e.g. γ-ray detection system• develop improved techniques for target preparation/characterization
12C(α,γ)16O –
towards
LUNA-MV
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
Influ
ence
of tw
osu
bthr
esho
ld s
tate
s (total)
12C(α,γ)16O –
Aims
LUNA-MV/ERNA
LUNA-MV: low-energy
E1/E2 measurementlowest
feasible
energy
to be
defined
by
WG
ERNA: higher energy Stot
measurement & cascadesconstraint on
total S factor
extrapolation
and E2 (through
6.92 MeV state
ANC)
improved
extrapolationto astrophysical
energy
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
12C(α,γ)16O –
ERLUNA practical workGEANT4 simulation
of γ-ray
array
example: GASP 4π
BGO array
12C target preparation at SIDONI (France)contact established preliminary studies in progress
target characterization at LNLtest studies in progress
high homogeneity
higher
separation
power
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
0 50 100 150 20010-5
100
105
1010
isot
opic
abu
ndan
ce
mass number A
cosmic rays
stellar burning phases,supernovae
s processHe burning in AGB stars,massive stars
r processsupernovae type II
p processsite disputed
- processes of nucleosynthesis
LUNA‐MV Physics
‐
– Origin of the
Elements
n source
reactions: 13C(α,n)16O and 22Ne(α,n)25Mg
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NUCLEAR ASTROPHYSICSNUCLEAR ASTROPHYSICS
Summary
of Presentation
LUNA-MV – The next Underground Accelerator Facility
• The LUNA-MV project has been launched.
•
Funding (through INFN, Italy) for accelerator and site preparation seems to be available
• Site preparation started (e.g. removal of the interferometer)
•
12C(α,γ)16O –
at low energies with sufficient statistical uncertainty will be one of the corner stones of the LUNA-MV project
• other reactions are: 3He(α,γ)7Be, 13C(α,n)16O, and 22Ne(α,n)25Mg