Flerov Laboratory of Nuclear Reactions, JINR, Dubna, Russia

Slides:



Advertisements
Similar presentations
SYNTHESIS OF SUPER HEAVY ELEMENTS
Advertisements

Invariant-mass spectroscopy of neutron halo nuclei Takashi Nakamura 中村隆司 Tokyo Institute of Technology 東京工業大学 中日 NP 06, Shanghai.
Fission Readings: Modern Nuclear Chemistry, Chapter 11; Nuclear and Radiochemistry, Chapter 3 General Overview of Fission Energetics The Probability of.
The peculiarities of the production and decay of superheavy nuclei M.G.Itkis Flerov Laboratory of Nuclear Reactions, JINR, Dubna, Russia.
Microscopic time-dependent analysis of neutrons transfers at low-energy nuclear reactions with spherical and deformed nuclei V.V. Samarin.
Multinucleon Transfer Reactions – a New Way to Exotic Nuclei? Sophie Heinz GSI Helmholtzzentrum and Justus-Liebig Universität Gießen Trento, May ,
The Dynamical Deformation in Heavy Ion Collisions Junqing Li Institute of Modern Physics, CAS School of Nuclear Science and Technology, Lanzhou University.
S. Sidorchuk (JINR, Dubna) Dubna Radioacive Ion Beams DRIBsIII: STATUS and PROSPECTS S. Sidorchuk (JINR, Dubna) 9-16 May 2013, Varna, Bulgaria 1.
Estimation of production rates and secondary beam intensities Martin Veselský, Janka Strišovská, Jozef Klimo Institute of Physics, Slovak Academy of Sciences,
Fusion-Fission Dynamics for Super-Heavy Elements Bülent Yılmaz 1,2 and David Boilley 1,3 Fission of Atomic Nuclei Super-Heavy Elements (SHE) Measurement.
Higher Order Multipole Transition Effects in the Coulomb Dissociation Reactions of Halo Nuclei Dr. Rajesh Kharab Department of Physics, Kurukshetra University,
1 Role of the nuclear shell structure and orientation angles of deformed reactants in complete fusion Joint Institute for Nuclear Research Flerov Laboratory.
Heavy Element Research at Dubna (current status and future trends) Yuri Oganessian Flerov Laboratory of Nuclear Reactions Joint Institute for Nuclear Research.
7-1 CHEM 312 Lecture 7: Fission Readings: Modern Nuclear Chemistry, Chapter 11; Nuclear and Radiochemistry, Chapter 3 General Overview of Fission Energetics.
Opportunities for synthesis of new superheavy nuclei (What really can be done within the next few years) State of the art Outline of the model (4 slides.
106 th Session of the JINR Scientific Council September 24-25, 2009, Dubna Perspectives of JINR – ORNL Collaboration in the Studies of Superheavy Elements.
II. Fusion and quasifission with the dinuclear system model Second lecture.
1 Reaction Mechanisms with low energy RIBs: limits and perspectives Alessia Di Pietro INFN-Laboratori Nazionali del Sud.
Presentation by T. Gogami 2015/6/15 (Mon). Equation state of neutron matter.
Nuclear Structure Studies South of 208 Pb Using Multi-nucleon Transfer Reactions BNL - U. Maryland - Oregon State U. Nuclides south of 208Pb can be reached.
Yu. Oganessian FLNR (JINR) PAC–meeting, June 22, 2009, Dubna Experimental activities and main results of the researches at FLNR (JINR) Theme: Synthesis.
© 2003 By Default! A Free sample background from Slide 1 JINR SCIENTIFIC COUNCIL 104 th Session, 25 September 2008, Dubna.
10-1 Fission General Overview of Fission The Probability of Fission §The Liquid Drop Model §Shell Corrections §Spontaneous Fission §Spontaneously Fissioning.
Some aspects of reaction mechanism study in collisions induced by Radioactive Beams Alessia Di Pietro.
Results of the de-excitation code ABLA07 GSI Darmstadt, Germany Aleksandra Kelić M. Valentina Ricciardi Karl-Heinz Schmidt.
W. Nazarewicz. Limit of stability for heavy nuclei Meitner & Frisch (1939): Nucleus is like liquid drop For Z>100: repulsive Coulomb force stronger than.
Structure of Super-Heavy Elements Andreas Heinz A. W. Wright Nuclear Structure Laboratory Yale University ATLAS Workshop, August 8-9, 2009.
Study on Sub-barrier Fusion Reactions and Synthesis of Superheavy Elements Based on Transport Theory Zhao-Qing Feng Institute of Modern Physics, CAS.
1 Synthesis of superheavy elements with Z = in hot fusion reactions Wang Nan College of Physics, SZU Collaborators: S G Zhou, J Q Li, E G Zhao,
CHEMICAL IDENTIFICATION of the element Db as decay product of the element 115 in the 48 Ca Am reaction CHEMICAL IDENTIFICATION of the element Db.
Fusion of light halo nuclei
Observation of new neutron-deficient multinucleon transfer reactions
Knyazheva G.N. Flerov Laboratory of Nuclear Reactions Asymmetric quasifission in reactions with heavy ions TAN 11, Sochi, Russia.
Dynamical Model of Surrogate Reaction Y. Aritomo, S. Chiba, and K. Nishio Japan Atomic Energy Agency, Tokai, Japan 1. Introduction Surrogate reactions.
Production mechanism of neutron-rich nuclei in 238 U+ 238 U at near-barrier energy Kai Zhao (China Institute of Atomic Energy) Collaborators: Zhuxia Li,
Feng-Shou Zhang College of Nuclear Science and Technology Beijing Normal University, Beijing, China Collaborators: Long Zhu, Bao-An Bian, Hong-Yu Zhou,
2 nd SPES Workshop Probing the Island of Stability with SPES beams.
Lecture 4 1.The role of orientation angles of the colliding nuclei relative to the beam energy in fusion-fission and quasifission reactions. 2.The effect.
Systematic Investigation of the Isotopic Distributions Measured in the Fragmentation of 124 Xe and 136 Xe Projectiles Daniela Henzlova GSI-Darmstadt, Germany.
Asymmetric quasifission in reactions with heavy ions
Entry distributions for fragments produced in deep-inelastic collisions with stable and radioactive beams For the PARIS collaboration W. Królas, M. Kmiecik,
Study of Heavy-ion Induced Fission for Heavy Element Synthesis
Fusion of 16,18O + 58Ni at energies near the Coulomb barrier
Extracting β4 from sub-barrier backward quasielastic scattering
Two-body force in three-body system: a case of (d,p) reactions
HEAVY ELEMENT RESEARCH AT THE FLNR (DUBNA)
Limits of stability: halo nuclei
Structure and dynamics from the time-dependent Hartree-Fock model
Fusion reactions with light stable and neutron-rich nuclei:
Nuclear excitations in nucleon removal processes
Triple-Humped Fission Barrier and Clusterization in the Actinide Region A. Krasznahorkay Inst. of Nucl. Res. of the Hungarian Acad. of Sci. (ATOMKI) Debrecen,
Peripheral collisions Hans-Jürgen Wollersheim
GSI-Darmstadt, Germany
Satoshi Adachi Research Center for Nuclear Physics (RCNP),
CHEM 312 Lecture 7: Fission Readings: Modern Nuclear Chemistry, Chapter 11; Nuclear and Radiochemistry, Chapter 3 General Overview of Fission Energetics.
Isomers and shape transitions in the n-rich A~190 region:
Sensitivity of reaction dynamics by analysis of kinetic energy spectra of emitted light particles and formation of evaporation residue nuclei.
NEUTRON EMISSION FROM SPONTANEOUS FISSION OF HEAVY ELEMENTS
Nuclear Stability.
Introduction Calculations for the N=7 isotones Summary
Production of heavy neutron-rich nuclei around N=126 in multi-nucleon transfer (MNT) reactions Long ZHU (祝龙) Sino-French Institute of Nuclear Engineering.
Flerov Laboratory of Nuclear Reactions, JINR, Dubna, Russia
Flerov Laboratory of Nuclear Reactions, JINR, Dubna, Russia
Fangataufa atoll French Polynesia
Institut de Physique Nucléaire Orsay, France
New Transuranium Isotopes in Multinucleon Transfer Reactions
Production Cross-Sections of Radionuclides in Proton- and Heavy Ion-Induced Reactions Strahinja Lukić.
V.V. Sargsyan, G.G. Adamian, N.V.Antonenko
Comparison of the isotopic distributions measured in the fragmentation of 136Xe and 124Xe projectiles with the EPAX parameterization Daniela Henzlova GSI-Darmstadt,
Catalin Borcea IFIN-HH INPC 2019, Glasgow, United Kingdom
Presentation transcript:

Flerov Laboratory of Nuclear Reactions, JINR, Dubna, Russia Application of multinucleon transfer reactions to the synthesis of neutron-rich nuclei Alexander Karpov Flerov Laboratory of Nuclear Reactions, JINR, Dubna, Russia 47th meeting of the PAC for Nuclear Physics, JINR, Dubna

Motivation 3-4 neutron-rich nuclei were added during last years based on the fragmentation reactions Cross section is 4.4±2.0 pb for 202Os J. Kurcewicz et al., PLB (2012) Only lower limit of half-life values were identified Other efficient methods of production of these nuclei are still of great value Multi-nucleon transfer reactions are thought to be an efficient method of synthesis of new neutron-rich heavy and superheavy nuclei

Model A.V. Karpov and V.V. Saiko, Phys. Rev. C 96, 024618 (2017)

Potential energy A.V. Karpov, EXON (2006) V.I. Zagrebaev, A.V. Karpov, et al. PEPAN (2007) Double-folding potential with Migdal forces Two-center shell model

Equations of motion (R, d1, d2, hA, hZ, q1, q2, q)

136Xe+208Pb experiment: E.M. Kozulin, et al., PRC (2012)

experiment: Y. X. Watanabe, et al., PRL (2015) 136Xe+198Pt @ 643 MeV

136Xe + 198Pt Production of neutron-rich Os-isotopes 102 N=126 101 100 185 190 195 200 205 210 102 101 100 10-1 10-2 10-3 10-4 10-5 10-6 10-7 10-8 10-9 107 Mass number Cross section, mb last stable last studied last known N=126 fragmentation of 238U massive transfer 136Xe + 198Pt J. Kurcewicz et al.,(2012) fragmentation of 208Pb T. Kurtukian-Nieto et.al (2014)

Production of N=126 nuclides Optimal reaction and detection angles experiment: Y. X. Watanabe, et al., PRL (2015)

Production of N=126 nuclides Optimal energy

Production cross section

Production of neutron-rich heavy and SH nuclei in actinide-actinide collisions (U+smth.) Strong shell effects may lead to increased cross section for formation of a Pb-like fragment as one of the reaction products and a heavy or SH fragment as another one e.g. U+Cm→Pb*+Sg*

Collisions of actinides Collisions of actinides. Potential energy @ contact point: 238U+254Es case 254Es 238U 208Pb A1 A2 286Mt A1 A2

Orientation effects in nucleus-nucleus collisions 462 MeV 502 MeV 860 MeV 160Gd + 186W (b2=0.22) (b2=0.28) 412 MeV 447 MeV 454 MeV 492 MeV exp exp A>200 A>200 A>200

Orientation effects 160Gd + 186W exp: E.M. Kozulin, et al. (2017) Ec.m.=462 MeV A>200 A>200 Ec.m.=502 MeV A>200 A>200

Collisions of actinides. A way to superheavies? large production cross sections for primary reaction products 298114* (double magic) can be produced with the cross section ~100 nb

Collisions of actinides. Comparison with existing data: U+Cm cross sections for Z>103 are below 1 pb but… new isotopes of elements with Z<103 can be produced with sufficiently large cross sections exp: M. Schädel et al., PRL (1982)

Collisions of actinides. Comparison with existing data: U+U cross sections for heavy products are lower than in the U+Cm case no significant influence of shell effects (parabola-like shapes) one should use the heaviest available target (254Es) exp: M. Schädel et al., PRL (1978)

Collisions of actinides. Comparison with existing data: U+U SH nuclei up to isotopes of Mt can be produced with cross sections larger than 1 pb pronounced influence of shell effects on the production cross sections

Conclusions and Outlook PRODUCTION OF NEUTRON-RICH HEAVY NUCLEI (N=126) Large cross sections (>100 nb) for yet-unknown nuclei. Weak energy dependence of the production cross sections of neutron-rich nuclei, but strong sensitivity of the angular distributions to the collision energy. (collisions of spherical nuclei) ORIENTATION EFFECTS IN NUCLEUS-NUCLEUS COLLISIONS Strong influence on the production cross sections as well as on the angular and energy distributions. PRODUCTION OF SH NUCLEI IN COLLISIONS OF ACTINIDES Production cross sections drop down very quickly with increasing nucleon transfer due to small survival probabilities. One should use the heaviest available target (254Es) to increase the production cross section of heaviest nuclei. Strong shell effects may give a real chance to produce new isotopes of heavy actinides. In spite of a long history of studies of heavy-ion nucleus-nucleus collisions, systematic high-quality experiments are of great demand. A.V. Karpov and V.V. Saiko, Phys. Rev. C 96, 024618 (2017) Co-author: Vyacheslav Saiko