Laboratory for Underground Nuclear Astrophysics

Slides:



Advertisements
Similar presentations
Proposal for the Establishment and Funding of the Cluster of Excellence Origin and Structure of the Universe The Cluster of Excellence for Fundamental.
Advertisements

NuPECC - Milan Present and future of Laboratory Underground Nuclear Astrophysics Alba Formicola - Status of the D(, ) 6 Li measurement -Status of.
1 MSci Astrophysics 210PHY412 Stellar structure and evolution Dr. Stephen Smartt (Room S039) Department of Physics and Astronomy Online.
Introduction to nuclear physics Hal. Nucleosynthesis Stable nuclei.
Time dependence of SM parameters. Outline Dirac´s hypothesis SM parameters Experimental access to time dependence  laboratory measurements  Quasar absorption.
Status of TACTIC: A detector for nuclear astrophysics Alison Laird University of York.
The neutrons detection involves the use of gadolinium which has the largest thermal neutron capture cross section ever observed. The neutron capture on.
I NSTITUTE FOR S TRUCTURE AND N UCLEAR A STROPHYSICS N UCLEAR S CIENCE L ABORATORY Research:Stellar Burning – nuclear reactions with stable beams Explosive.
Stuttgart Dynamitron at Bucharest - Perspectives and New Activities
E.Chiaveri on behalf of the n_TOF Collaboration n_TOF Collaboration/Collaboration Board Lisbon, 13/15 December 2011 Proposal for Experimental Area 2(EAR-2)
Text optional: Institutsname Prof. Dr. Hans Mustermann Mitglied der Leibniz-Gemeinschaft Direct measurement of the d( α, γ ) 6 Li cross-section.
The FAIR Chance for Nuclear Astrophysics Elemental Abundances Core-collapse Supernovae The neutrino process The r-process nuclei in -Wind Neutron Stars.
The LUNA experiment: direct measurement of thermonuclear cross sections of astrophysical interest Alessandra Guglielmetti Universita’ degli Studi di Milano.
Stellar Fuel, Nuclear Energy and Elements How do stars shine? E = mc 2 How did matter come into being? Big bang  stellar nucleosynthesis How did different.
Lecture 2: Formation of the chemical elements Bengt Gustafsson: Current problems in Astrophysics Ångström Laboratory, Spring 2010.
I NSTITUTE FOR S TRUCTURE AND N UCLEAR A STROPHYSICS N UCLEAR S CIENCE L ABORATORY CASPAR An underground Accelerator Laboratory for Nuclear Astrophysics.
-NUCLEUS INTERACTIONS OPEN QUESTIONS and FUTURE PROJECTS Cristina VOLPE Institut de Physique Nucléaire Orsay, France.
 -capture measurements with the Recoil-Separator ERNA Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum HRIBF Workshop – Nuclear.
Nuclear structure and fundamental interactions Solid state physics Material irradiation Micrometeorite research and study Astrophysics Nuclear astrophysics.
I. Introductory remarks and present status II. Laboratory experiments and astrophysics III. Future options scenarios status and challenges new developments.
Kopylov A.V. Erice School/Workshop 2009 on Neutrinos in Cosmology, in Astro, in Particle and in Nuclear Physics in Erice/Trapani/Sicily/Italy on September.
Lesson 13 Nuclear Astrophysics. Elemental and Isotopic Abundances.
Underground Laboratories and Low Background Experiments Pia Loaiza Laboratoire Souterrain de Modane Bordeaux, March 16 th, 2006.
ALNA- Accelerator Laboratory for Nuclear Astrophysics Underground Heide Costantini University of Notre Dame, IN, USA INFN, Genova, Italy.
Physics Colloquium Ⅱ Shibata Laboratory OKA, Hiroki Nucleosyntheses studied with a Van de Graaff Accelerator [Contents] 1. Objective.
 ( E ) = S(E) e –2   E -1 2      m  m   m   m   Reaction Rate(star)    (E)  (E) dE Gamow Peak  Maxwell Boltzmann.
 ( E ) = S(E) e –2   E -1 2       m  m   m   m   Reaction Rate(star)    (E)  (E) dE Gamow Peak  Maxwell Boltzmann.
Forschungszentrum Karlsruhe in der Helmholtz-Gemeinschaft Neutron cross sections for reading the abundance history Michael Heil Forschungszentrum Karlsruhe.
Experimental Nuclear Astrophysics: Key aspects & Open problems Marialuisa Aliotta School of Physics University of Edinburgh Nuclear Physics Autumn Retreat.
Low Background Studies at the Soudan Underground Laboratory-9/20/ Low Background Studies at the Soudan Underground Laboratory The Soudan Underground.
Selected Topics in Astrophysics. Solar Model (statstar) Density Mass Luminosity Temperature Nuclear Reaction Rate Pressure.
Cristina VOLPE BETA-BEAMS The beta-beam concept The baseline scenario The physics potential Conclusions LOW ENERGY BETA-BEAMS A N D The idea Motivation.
© 2003 By Default! A Free sample background from Slide 1 JINR SCIENTIFIC COUNCIL 102 nd Session, September 2007, Dubna.
1/38 Laboratory Underground Nuclear Astrophysics The D( 4 He,  ) 6 Li reaction at LUNA and the Big Bang Nucleosynthesis Carlo Gustavino For the LUNA collaboration.
High Energy Observational Astrophysics. 1 Processes that emit X-rays and Gamma rays.
NUCLEAR REACTIONS OF ASTROPHYSICAL INTEREST AT LUNA D. Trezzi (for the LUNA collaboration) Università degli Studi di Milano | INFN – New Vistas in Low-Energy.
The LUNA experiment at Gran Sasso Laboratory: studying stars by going underground Alessandra Guglielmetti Università degli Studi di Milano and INFN, Milano,
 -capture measurements with a Recoil-Separator Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum Int. Workshop on Gross Properties.
LBNF/DUNE Update Public Meeting Sanford Lab Update
 s s 2ph = Z1Z2 m/E m = m1m2 / (m1+m2), E in keV
Nuclear Astrophysics at LUNA and the Big Bang Nucleosynthesis
L’esperimento LUNA- CdS MI giugno 2013
Prompt Gamma Activation Analysis on 76Ge
Why going underground g-background
The scientific program for the first five years of LUNA-MV
the s process: messages from stellar He burning
The nucleosynthesis of heavy elements in Stars: the key isotope 25Mg
Simulation for DayaBay Detectors
status and perspectives
Alessandra Guglielmetti Universita’ degli Studi di Milano and
György Gyürky Institute of Nuclear Research (Atomki) Debrecen, Hungary
The D(4He,)6Li reaction at LUNA and the Big Bang Nucleosynthesis
Stato dell’esperimento LUNA e del progetto LUNA MV- CdS MI giugno 2015
Carbon, From Red Giants to White Dwarfs
Nucleosynthesis 12 C(
EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH
Making Carbon and Oxygen in Stars
Introduction to Bubble Chamber: Ops Training
BBN, neutrinos and Nuclear Astrophysics
Pauli´s new particle * nt nm ne e m t Beta-Decay Pa 234 b (electron)
From small to big scales
(g,z) Breakup Experiments Charged Particles in the Final State
 s(E) = S(E) e–2ph E-1 s Nuclear Burning in Stars s(Estar) s
Starting Points (Collaboration ; Laboratory ; Magnetic Moment Results)
Lecture 11: Age and Metalicity from Observations
Fusion Reactions in Stars
7. Internal structure. II.
Astrophysical implications of the (n,
Institut de Physique Nucléaire Orsay, France
1930: Energy conservation violated in β-decay
Presentation transcript:

Laboratory for Underground Nuclear Astrophysics The LUNA experiment Laboratory for Underground Nuclear Astrophysics Reunion prospective: Univers et Rayons Cosmiques

Why studying nuclear fusion reaction cross sections? - Stars are powered by nuclear reactions They determine: stellar evolution and dynamics elements origin and abundances neutrino production Reunion prospective: Univers et Rayons Cosmiques 1

Heavy elements nucleosynthesis LUNA MV The scientific program: 12C(a,g)16O: Carbon/Oxygen in the universe SN Type II, Type Ia… 13C(a,n)16O: 22Ne(a,n)25Mg: 3He(4He,g)7Be: Solar neutrinos Heavy elements nucleosynthesis Reunion prospective: Univers et Rayons Cosmiques 2

12C(,)16O Holy Grail of Nuclear Astrophysics Oxygen-16 12C(,)16O Most important reaction in He-burning phase Determines Carbon-Oxygen abundance in the universe Influences late stellar evolution nucleosynthesis of heavy elements Carbon/Oxygen determines: dynamics of SN type II end of heavy stars (Black Hole, Neutron star) peak-luminosity and shape of SN type Ia (standard candles in measurements of cosmological distances) Reunion prospective: Univers et Rayons Cosmiques 3

nucleosynthesis of heavy elements Heavy elements are produced in neutron capture processes 13C(a,n)16O neutron sources 22Ne(a,n)25Mg Reunion prospective: Univers et Rayons Cosmiques 4

Neutrino production in the Sun p + p  d + e+ + ne d + p  3He + g 3He +3He  a + 2p 3He +4He  7Be + g 7Be+e- 7Li + g +ne 7Be + p  8B + g 7Li + p  a + a 8B 2a + e++ ne 84.7 % 13.8 % 13.78 % 0.02 % pp chain ONLY if the cross sections of the involved reactions are accurately known Neutrino flux from the Sun can be used to study: Solar interior composition Neutrino properties ONLY if the cross sections of the involved reactions are accurately known Reunion prospective: Univers et Rayons Cosmiques 6

Why going in an underground laboratory? Energy range in stars ~ kTstar ( ~ 10 keV for H-burning ; ~ 100 keV for He-burning) Due to Coulomb barrier, cross section ~ pbarn-fbarn …even less!! Extremely low measured reaction rate 12C(a,g)16O It is mandatory to have very low background Surface Underground Perform measurements in an underground laboratory Reunion prospective: Univers et Rayons Cosmiques 7

Laboratory for Underground Nuclear Astrophysics LUNA site LNGS (1400 m rock shielding  4000 m w.e.) LUNA MV (2018->...) 3.5 MV LUNA 1 (1992-2001) 50 kV LUNA 2 (2000…) 400 kV Radiation LNGS/surface Muons Neutrons 10-6 10-3 7

Key nuclear reactions studied with LUNA1, LUNA2 LUNA 1: 3He(3He,2p)4He ; first direct measurement at solar energies (neutrino problem) LUNA 2: 14N(p,g)15O: determination of age of the globular clusters (age of the universe) 3He(4He,g)7Be: precise determination of 8B and 7Be neutrino flux d(4He,g)7Li: Li –problem in BBN LUNA 1 accelerator: 50 kV LUNA 2 accelerator : 400 kV At the moment unique accelerator facility underground Reunion prospective: Univers et Rayons Cosmiques 9

Heavy elements nucleosynthesis LUNA MV The scientific program: 3He(4He,g)7Be: solar neutrinos 13C(a,n)16O: 22Ne(a,n)25Mg 12C(a,g)16O: C/O ratio in the universe SN Type II, Type Ia… Heavy elements nucleosynthesis 3.5 MV accelerator LUNA-MV LUNA-MV existing meas. existing meas. Reunion prospective: Univers et Rayons Cosmiques 10

Experimental challenges 12C(a,g)16O : - extremely pure (10-7) and stable solid carbon target - high efficiency, high resolution and bck-free gamma-detector 13C(a,n)16O, 22Ne(a,n)25Mg : - dense and pure 22Ne gas target - high efficiency and bck-free neutron detector (Possible) French contribution Carbon target (CSNSM-Orsay) Sidonie implanter at CSNSM: consolidated expertise in high pure implanted targets Neutron detector (CPPM) Expertise in : detector simulation and characterization - low background environment Proximity of neutron facility (Cadarache) good occasion to develop new expertise (neutron detection) Reunion prospective: Univers et Rayons Cosmiques 11

Status of the LUNA-MV project February 2013 the “Starting up the LUNA MV Collaboration” workshop was organized at the LNGS September 2013: different WG were formed Neutron detector (F. Cassol) Solid carbon targets (A. Formicola) Gamma detector (R. Menegazzo) LUNA-MV has been financed with a total of 5.3 Meuro by Italian Research Ministry: Accelerator Site preparation Shieldings Beam-lines Reunion prospective: Univers et Rayons Cosmiques 12

Schedule 2014-2015 Site definition -Tender for the accelerator- Beam lines and detectors R&D 2016 beginning of Site preparation - Infrastructures 2017 Accelerator arrival at LNGS – Shielding – beam lines construction 2018 Calibration of the apparatus and first beam on target Competitive project A USA project (CASPAR) is aiming to install a 1 MV machine at the SURF lab (Homestake): time schedule similar to LUNA-MV Collaboration has started with CASPAR project Reunion prospective: Univers et Rayons Cosmiques 13

“ We are made of star-stuff” Interested people at CPPM: J. Busto, F. Cassol, H. Costantini preliminary work: Feb. 2013-Dic. 2013 present status: frozen participation due to: 2 years delay of the project (change of location at LNGS) at present no French critical mass (CPPM, CSNSM only) ...... Something to keep in mind for 2015-2020 LUNA-MV looks for collaborators Connected to the Cosmology, Astrophysics and Particle physics Small scale experiment: small investment for good quality physics Short time needed for physics results Ideal experiment for students (from experimental work to data analysis and astrophysical implications) “ We are made of star-stuff” (Carl Sagan 1973)