Nuclear Physics Institute ASCR, p.r.i. V.Kroha Nuclear Reactions Dept. -Nuclear Astrophysics -Neutron Physics -Exotic Nuclei.

Slides:



Advertisements
Similar presentations
Small Scale Facilities in EUROPE ( not included in the Large Scale Facilitity Network) Belgium: 1IKS KU Leuven Czech Republic: 2Nucl. Phys. Inst. Acad.
Advertisements

Meeting – Prague, June 2011 Jaromir Mrazek, NPI ASCR Rez Nuclear Astrophysics in NPI ASCR Rez, Czech Republic Outline: Hardware Indirect methods Experiments.
Nuclear Astrophysics Experiments in ATOMKI Gy. Gyürky Institute of Nuclear Research (ATOMKI) Debrecen, Hungary.
Marina Barbui Trento, Italy, April 7-11, 2014
Nara, June 03 Solar neutrino production rates by heavy ion reactions T. Motobayashi (RIKEN) 7 Be(p,  ) 8 B reaction pp chain in the sun direct measurement.
Alpha Stucture of 12 B Studied by Elastic Scattering of 8 Li Excyt Beam on 4 He Thick Target M.G. Pellegriti Laboratori Nazionali del Sud – INFN Dipartimento.
Contributions to Nuclear Data by Radiochemistry Division, BARC
(p,g) reaction via transfer reaction of mirror nuclei and direct measurement of 11C(p,g)12N at DRAGON Bing Guo For nuclear astrophysics group China Institute.
Spectroscopic factors and Asymptotic normalization coefficients Oak Ridge, Oct 2006 F.M. Nunes NSCL, Michigan State University in collaboration with D.
Low energy radioactive beams Carmen Angulo, CRC Louvain-la-Neuve, Belgium FINUPHY meetingLouvain-la-Neuve, Belgium3-4 May 2004 Recent highlights on nuclear.
S. Sidorchuk (JINR, Dubna) Dubna Radioacive Ion Beams DRIBsIII: STATUS and PROSPECTS S. Sidorchuk (JINR, Dubna) 9-16 May 2013, Varna, Bulgaria 1.
Astrophysical Reaction Rate for the Neutron-Generator Reaction 13 C(α,n) in Asymptotic Giant Branch Stars Eric Johnson Department of Physics Florida State.
Astrophysical S(E)-factor of the 15 N(p,α) 12 C reaction at sub-Coulomb energies via the Trojan-horse method Daniel Schmidt, Liberty University Cyclotron.
15 N Zone 8 Zone 1 Zone 28 p Zone 1 Zone O Zone 1 Zone 4 Zone 8 Zone N 16 O p Reaction rates are used to determine relative abundance of elements.
Status of TACTIC: A detector for nuclear astrophysics Alison Laird University of York.
12C(p,g)13N g III. Nuclear Reaction Rates 12C 13N Nuclear reactions
Astrophysical S(E)-factor of the 15N(p,α)12C reaction at sub-Coulomb energies via the Trojan-horse method Daniel Schmidt, Liberty University Cyclotron.
Reaction rates in the Laboratory Example I: 14 N(p,  ) 15 O stable target  can be measured directly: slowest reaction in the CNO cycle  Controls duration.
Reaction rates in the Laboratory Example I: 14 N(p,  ) 15 O stable target  can be measured directly: slowest reaction in the CNO cycle  Controls duration.
Nuclear Physics for Astrophysics with Radioactive Beams Livius Trache Texas A&M University EURISOL Workshop ECT * Trento, Jan
Pierre Descouvemont Université Libre de Bruxelles, Brussels, Belgium The 12 C(  ) 16 O reaction: dreams and nightmares theoretical introduction.
ANASEN - Array for Nuclear Astrophysics Studies with Exotic Nuclei Silicon-strip detector array backed with 2-cm-thick CsI Gas proportional counter for.
DAF Distributed Accelerator Facility (DAF) Transnational Access Nodes: 1.Tandem Accelerator Laboratory, Rudjer Boskovic Institute (RBI), Zagreb, Croatia.
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.
Coupled-Channel Computation of Direct Neutron Capture and (d,p) reactions on Non- Spherical Nuclei Goran Arbanas (ORNL) Ian J. Thompson (LLNL) with Filomena.
Studying alpha-cluster structure using low-energy RI beam Nuclear astrophysics group (CRIB supporting members) in Center for Nuclear Study, Univ. of Tokyo:
Recoil Separator Techniques J.C. Blackmon, Physics Division, ORNL RMS - ORNL WF QT QD Q D Target FP ERNA - Bochum WF Target D QT FP DRS ORNL QD VF D VAMOS.
New methods to measure the cross sections of 12 C+ 12 C fusion reaction Xiao Fang Department of Physics University of Notre Dame.
Recent Results for proton capture S-factors from measurements of Asymptotic Normalization Coefficients R. Tribble Texas A&M University OMEG03 November,
Nuclear Astrophysics with the PJ Woods, University of Edinburgh.
Vladimír Wagner Nuclear physics institute of CAS, Řež, Czech Republic, E_mail: for collaboration “Energy plus transmutation RAW”
Facilities at the Nuclear Physics Institute Academy of Sciences of the Czech Rep., Řež.
1 New horizons for MCAS: heavier masses and α-particle scattering Juris P. Svenne, University of Manitoba, and collaborators CAP 15/6/2015.
Nuclear Level Density 1.What we know, what we do not know, and what we want to know 2.Experimental techniques to study level densities, what has been done.
Studies of Deuteron and Neutron Cross-sections Important for ADS Research Vladimír Wagner Nuclear physics institute of CAS, Řež, Czech Republic,
Neutral pion photoproduction and neutron radii Dan Watts, Claire Tarbert University of Edinburgh Crystal Ball and A2 collaboration at MAMI Eurotag Meeting.
-NUCLEUS INTERACTIONS OPEN QUESTIONS and FUTURE PROJECTS Cristina VOLPE Institut de Physique Nucléaire Orsay, France.
Zagreb IP: Experimental nuclear physics inputs for thermonuclear runaway - NuPITheR Neven Soić, Ru đ er Bošković Institute, Zagreb, Croatia EuroGENESIS.
Single nucleon transfer between p- shell nuclei around 10 MeV/u - for nuclear astrophysics Livius Trache Cyclotron Institute, Texas A&M University ATLAS.
Progress of Experimental Nuclear Astrophysics in CIAE Wei-ping Liu China Institute of Atomic Energy (CIAE) CCAST symposium on physics.
Some aspects of reaction mechanism study in collisions induced by Radioactive Beams Alessia Di Pietro.
ANC Techniques and r-matrix analysis Santa Fe, April 2008 ANC Techniques and r-matrix analysis Grigory Rogachev.
In Progress T-Rex TAMUTrap SASSYER Active Target Det RTC + chemistry Radioisotope production.
Study of unbound 19 Ne states via the proton transfer reaction 2 H( 18 F,  + 15 O)n HRIBF Workshop – Nuclear Measurements for Astrophysics C.R. Brune,
 2-proton emission  experimental set-up  decay results  2p emission from 45 Fe  perspectives Jérôme Giovinazzo – CEN Bordeaux-Gradignan – France PROCON’03.
 ( E ) = S(E) e –2   E -1 2      m  m   m   m   Reaction Rate(star)    (E)  (E) dE Gamow Peak  Maxwell Boltzmann.
Nucleosynthesis in AGB Stars: the Role of the 18 O(p,  ) 15 N Reaction Marco La Cognata.
Institute for Structure and Nuclear Astrophysics Nuclear Science Laboratory E381: Search of potential resonances in the 12 C+ 12 C fusion reaction using.
The concept of compound nuclear reaction: a+B  C  d+F The particle transmission coefficients T are usually known from cross sections of inverse reactions.
FLUORINE DESTRUCTION IN STARS: FIRST EXPERIMENTAL STUDY OF THE 19 F(p,α 0 ) 16 O REACTION AT ASTROPHYSICAL ENERGIES Marco La Cognata INFN-LNS Catania.
Nuclear Astrophysics ARUNA Workshop, Notre Dame, IN Carl R. Brune Ohio University, Athens Ohio June 12-13, 2014.
THEORETICAL PREDICTIONS OF THERMONUCLEAR RATES P. Descouvemont 1.Reactions in astrophysics 2.Overview of different models 3.The R-matrix method 4.Application.
Nuclear Physics Institute ASCR, p.r.i. V.Kroha Nuclear Reactions Dept. Nuclear Astrophysics Workshop on ESSAF Aghios Nikolaos Sept. 7-8,2007.
Tariq Al-Abdullah Hashemite University, Jordan Cairo 2009 Problems and Issues in Nuclear Astrophysics.
Effects Of Distortion On Trojan Horse Applications Rosario Gianluca Pizzone INFN – Laboratori Nazionali del Sud Catania.
Experimental Nuclear Astrophysics: Key aspects & Open problems Marialuisa Aliotta School of Physics University of Edinburgh Nuclear Physics Autumn Retreat.
Nuclear and Radiation Physics, BAU, First Semester, (Saed Dababneh). 1.
Indirect Techniques ( I) : Asymptotic Normalization Coefficients and the Trojan Horse Method NIC IX R.E. Tribble, Texas A&M University June, 2006.
Indirect measurements of the -3 keV resonance in the 13 C(α, n) 16 O reaction: the THM approach Marco La Cognata.
Studies on alpha-induced astrophysical reactions using the low-energy RI beam separator CRIB Studies on alpha-induced astrophysical reactions using the.
 -capture measurements with a Recoil-Separator Frank Strieder Institut für Physik mit Ionenstrahlen Ruhr-Universität Bochum Int. Workshop on Gross Properties.
Exploring the alpha cluster structure of nuclei using the thick target inverse kinematics technique for multiple alpha decays. The 24 Mg case Marina Barbui.
the s process: messages from stellar He burning
L. Acosta1, M. A. G. Álvarez2, M. V. Andrés2, C. Angulo3, M. J. G
Giant Monopole Resonance
gamma-transmission coefficients are most uncertain values !!!
Study of the resonance states in 27P by using
Study of the resonance states in 27P by using
Elastic alpha scattering experiments
Catalin Borcea IFIN-HH INPC 2019, Glasgow, United Kingdom
Presentation transcript:

Nuclear Physics Institute ASCR, p.r.i. V.Kroha Nuclear Reactions Dept. -Nuclear Astrophysics -Neutron Physics -Exotic Nuclei

Facilities used by Nuclear reactions department of NPI Řež Cyclotron : protons 12 – 24 MeV deuterons 12 – 17 MeV 3 He – ions 20 – 52 MeV 4 He – ions 20 – 40 MeV posibility of axial injection Planned use : Tandem : 4 MV, ECR source, heavy ions available exploatation during next two years for nuclear physics research

Aparatus : - achromatic magnetooptical system AMOS for „zero-angle measurements ( up to 20 deg ) - target chamber for angular cross sections measurements - gas target chamber -  E – E telescopes with semiconductor detectors - spectroscopical electronic for multiparameter registration - fast on-line CAMAC system for multiparameter easurements - neutron generators NG 1 and NG 2 for activation xperiments and application research - neutron spectrometers

Nuclear astrophysics The most important results for the period 1999 – 2006 Development of the new method for indirect determination of the astrophysical S – factors Method of Asymptotic Normalization Coefficients was developed in cooperation with Texas A&M University The main test of ANC method was realized in INP at Řež using 16 O( 3 He,d) 17 F reaction. Publications : Phys.Rev.C56(1997)1302 Phys.Rev.C59(1999)1149 Few-Body Syst.Suppl.12(2000)102 Czech.J.Phys.54(2001)

Determination of astrophysical S – factor for 8 B synthesis This work was implemented on 7 Be radioactive beam in TAMU as a joint experiment. Reactions 10 B( 7 Be, 8 B) 9 Be and 14 N( 7 Be, 8 B) 13 C were studied. The necessary complementary measurements of the 9 Be( 3 He,d) 10 B and 13 C( 3 He,d) 14 N reactions were performed on the 3 He beam of cyclotron NPI. The most important published results : Phys.Rev.Lett.82(1999)3960 Phys.Rev.C60(1999) Phys.Rev.C62(2000) Phys.Rev.C63(2001) Phys.Rev.C66(2002) Phys.Rev.C73(2006)025808

Determination of the reaction rate for 14 N + p  15 O synthesis The reaction 14 N( 3 He,d) 15 O was studied on cyclotron NPI at beam energy 26.3 MeV.The direct capture to the subthreshold bound state of 15 O dominates in this key reaction of all CNO cycle. Up to now,the most accurate value of the total S – factor for the 14 N(p,  ) 15 O radiative capture was obtained. The main published results : Phys.Rev.C67(2003) Nucl.Phys.A718(2003)147 Nucl.Phys.A725(2003)279

S factor for 14 N(p,  ) 15 O ANC’s  14 N( 3 He,d) 15 O NRC to subthreshold state at E x = 6.79 MeV Q cm (deg) d s /d W( mb/sr ) 3/2 +, 6.79 MeV

S factor for 14 N(p,  ) 15 O C 2 (E x  6.79 MeV)  fm -1 [non-resonant capture to this state dominates S factor] S(0)  1.41 ± 0.24 keV·b for E x  6.79 MeV S tot (0)  1.62 ± 0.25 keV·b Subthreshold resonance width from Bertone, et al. R-Matrix fits to data from Schr ö der, et al.

ANC’s  9 Be( 3 He,d) 10 B and 9 Be( 10 B, 9 Be) 10 B R-Matrix fit to ground plus excited states (includes interference) Data from Zahnow,..., Rolfs et. al (1995) Uses known values for E r and   S factor for 9 Be(p,  ) 10 B

S factor for 13 C(p,  ) 14 N total S(0) = 7.7 ± 1.1 keV ·b (R keV ·b; D – 1.5 keV ·b; INT – 1. 9 keV ·b)

Determination of ANC from 20 Ne( 3 He,d) 21 Na reaction and S factor for 20 Ne(p,  ) 21 Na The ANCs for 20 Ne(p,  ) capture were obtained on cyclotron of NPI at laboratory energy 25 MeV. Measurements were realized on gas target of isotopic 20 Ne. Analysis was given for all bound states up to the threshold. The main results were published at international meetings : Catania, March 20,2003,Italy Conf. of American Physical Society,Oct.29,2003,Tuscon,Arizona and in Phys.Rev.C73(2006)035806

ANC’s via transfer reactions using radioactive (rare isotope) beams 7 Be + p  8 B [ 10 B( 7 Be, 8 B) 9 Be] {TAMU} [ 14 N( 7 Be, 8 B) 13 C] {TAMU} [d( 7 Be, 8 B)n] {Beijing} 11 C + p  12 N [ 14 N( 11 C, 12 N) 13 C] {TAMU} 13 N + p  14 O [ 14 N( 13 N, 14 O) 13 C] {TAMU} 17 F + p  18 Ne [ 14 N( 17 F, 18 Ne) 13 C] {ORNL (TAMU collaborator)} beams  MeV/u

Texas A&M University

ANC’s for 11 C + p  12 N reaction: 14 N( 11 C, 12 N) 13 C K500: 11 B beam  144 MeV MARS: 11 C beam  110 MeV

Measurement of the S – factor for 11 C(p,  ) 12 N reaction S – factor was determined by the ANC method using the 14 N( 11 C, 12 N) 13 C reaction. Effect of the distant resonances was analysed in R – matrix approach. It was shown that value of the S – factor is much higher than the present theoretical predictions. It increases the probability of successive generating of the CNO cycle in supermassive stars and their stabilization against the gravitational collapse into a black hole. Such stars explode in the final stage of their evolution as supernovae. The main published result : Phys.Rev.C67(2003)015804

14 N( 11 C, 12 N) 13 C angular distribution Normalization(beam&target)6.5% Optical Model8% ANCs of 14 N6.4% Statistical Error3% MC parameters2% Total12.7%

S factor for 11 C(p,  ) 12 N Solid TAMU Dashed GANIL

3/12/2005 TAMU GANIL Wiescher et al. Updated Reaction rates

Trojan-Horse Indirect method Validity test of the T–H method on cyclotron 3 He beam Coincidence measurements of 7 Li +p     reaction via the 3 He break – up Published : Intern. Conf. Debrecen, Hungary, 2005 Intern. Conf.FINUSTAR 2005, Kos, Greece, 2005 Accepted in European Phys. Journal

S – factor for 13 C( ,n) 16 O reaction S(0) = [ 2.5  0.2(stat)  0.2(syst)  0.5(theor)]  10 6 MeVb

Research program until the year proton transfer reactions of the CNO and NeNa cycles will continue on the NPI cyclotron. The main goal – to find out intensities of reactions leading to synthesis of heaviest nuclei -transfer reactions will be studied also at TAMU with heavy ions 8 B, 12 N, 13 N and 22 Ne to determine the direct components of the capture reactions important for evolution of the supermassive stars and for relation between reactions in standard and „hot“CNO cycles -the other indirect technique, Trojan-Horse method, was developed by Catania group. Using a 3 He beam of our cyclotron and in cooperation with LNS we study the possibility of absolutization of this method by its combination with ANC one. -in LNS Catania we realized a study of alpha transfer reactions on the Li– beam to test our ANC method for the case of alpha particle capture processes. -Results of 12 C( 6 Li,d) 16 O are under way

The research will be supported by the newly accepted project of MŠMT(CR) – NSF(USA) ME902(2007) : Indirect Methods in Nuclear Astrophysics principal investigators V.Kroha (NPI),R.E.Tribble (TAMU) by grant of GAČR 202/05/0302 Astrophysical Reactions and Method of Asymptotic Normalization Coefficients principal investigator V.Burjan (NPI) and by Centrum of Nuclear astrophysics and Nuclear Physics (MED) Principal investigators A.Kugler and V.Kroha

Collaborators INP (CR) : P.Bém, V.Burjan, Z.Hons, V.Kroha, J.Novák, Š.Piskoř, E.Šimečková, J.Mrázek TAMU (USA) : A.Azhari, C.A.Gagliardi, A.M.Mukhamedzhanov, A.Sattarov, X.Tang, L.Trache, R.E.Tribble INFN-LNS (Italy) : M.LaCognata, L.Lamia, R.G.Pizzone, S.Romano, C.Spitareli, S.Tudisco, A.Tumino INF Debrecen(Hungary):S.Fulop,E.Somorjai,G.Kiss

Publications 1999 – 2007 I nternational journals : 46 International conferences : 61 Preprints and Reports : 24 Citations 1999 – 2007 International journals : 178