In Progress T-Rex TAMUTrap SASSYER Active Target Det RTC + chemistry Radioisotope production.

Slides:

Advertisements

Similar presentations

GEANT4 Simulations of TIGRESS

Advertisements

4/29/20151Cosenors - BentleyOverview Physics of Proton-rich Nuclei in the UK Mike Bentley (Univ. of York, UK) Physics of Proton-rich Nuclei in the UK Mike.

Γ spectroscopy of neutron-rich 95,96 Rb nuclei by the incomplete fusion reaction of 94 Kr on 7 Li Simone Bottoni University of Milan Mini Workshop 1°-

An Association of Florida State University Accelerator Lab Hope College Ion Beam Laboratory Ohio University Accelerator Lab Texas A&M Cyclotron Lab TUNL.

Contributions to Nuclear Data by Radiochemistry Division, BARC

W. Udo Schröder, 2004 Instrumentation 1. W. Udo Schröder, 2004 Instrumentation 2 Probes for Nuclear Processes To “see” an object, the wavelength of the.

Outlook towards future Polish participation in the new Accelerator Facility Tomasz Matulewicz Warsaw University.

For more information about the facility visit: For more information about our group visit:

Using GEMINI to study multiplicity distributions of Light Particles Adil Bahalim Davidson College Summer REU 2005 – TAMU Cyclotron Institute.

Adil Bahalim Davidson College Dr. Joseph Natowitz (Advisor), Dr. Seweryn Kowalski (Mentor) Summer REU 2005 – TAMU Cyclotron Institute Reconstruction Main.

© 2003 By Default! A Free sample background from Slide 1 JINR SCIENTIFIC COUNCIL 106 nd Session, 24 September 2009, Dubna.

29:006 FINAL EXAM FRIDAY MAY 11 3:00 – 5:00 PM IN LR1 VAN.

ANASEN - Array for Nuclear Astrophysics Studies with Exotic Nuclei Silicon-strip detector array backed with 2-cm-thick CsI Gas proportional counter for.

The Roadmap on Nuclear Physics at the JINR M.G.Itkis.

Radioactivity php.

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.

Future Penning Trap Experiments at GSI / FAIR – The HITRAP and MATS Projects K. Blaum 1,2 and F. Herfurth 1 for the HITRAP and MATS Collaboration 1 GSI.

A facility for Nuclear, Atomic, Material and Radiobiology Sciences. Delivering stable (from C to U) and radioactive ions (from He to Xe) in the energy.

Nuclear physics input to astrophysics: e.g.  Nuclear structure: Masses, decay half lives, level properties, GT strengths, shell closures etc.  Reaction.

Nuclear Chemistry Nuclear chemistry is the study of the structure of atomic nuclei and the changes they undergo.

NUCLEAR CHEMISTRY QUIZ.

Nuclear Astrophysics with the PJ Woods, University of Edinburgh.

FAIR/SFRS meeting at HIPHeikki Penttila Oct 6, 2008 Facility for Antiproton and Ion Research FAIR is An international accelerator facility of the ”next.

Decay Spectroscopy Working Group Nuclear Structure Theory Morten Hjorth-Jensen – Shell Structure and Interactions Ivan Borzov – Theory of  Decay Applications.

NUSTAR Nuclear Structure, Astrophysics, Reactions NUSTAR is the biggest collaboration in FAIR The collaboration unites 450 scientists from 98 institutions.

Spin-isospin studies with the SHARAQ Spectrometer Tomohiro Uesaka & Y. Sasamoto, K. Miki, S. Noji University of Tokyo for the SHARAQ collaboration Aizu2010.

Lawrence Livermore National Laboratory Nicholas Scielzo Lawrence Fellow Physics Division, Physical Sciences LLNL-PRES Lawrence Livermore National.

CERN NuPAC meeting Dec 2005 The future of ISOLDE: accelerated radioactive beams Peter Butler 1.HIE-ISOLDE 2.EURISOL.

Radioactive ion beam facilities How does they work ? 2012 Student Practice in JINR Fields of Research 9.oct.2012 I. Sivacekflerovlab.jinr.ru.

10-Year Vision: expanded RIB program with: three simultaneous beams increased number of hours delivered per year new beam species increased.

The Belgian Research Initiative on eXotic nuclei – BriX network BriX Days Liege, May 27-28, 2015 Funded by the Interuniversity Attraction Poles Programme.

FINUPHY Instrumentation for radioactive nuclear beam facilities Rauno Julin FINUPHY Madeira, February 9, 2005.

Mass measurements using low energy ion beams -1- C. Thibault 31 mars 2004 Motivations to measure masses Present status Experimental methods for direct.

International Workshop on Nuclear Dynamics and Thermodynamics Honoring the achievements of Joseph B. Natowitz Robert E. Tribble Texas A&M University August.

106 th Session of the JINR Scientific Council September 24-25, 2009, Dubna Perspectives of JINR – ORNL Collaboration in the Studies of Superheavy Elements.

Ln(R 12 ) N Alan McIntosh, Yennello Research Group, TAMU-CI. Nuclear Physics Town Meeting, Aug 2014, College Station, TX Asymmetry Dependence of Thermodynamic.

Sep. 2003CNS Summer School Feb 分 => Talk なら 35 枚だが、 lecture だと少なめ？ 50 分 => Talk なら 35 枚だが、 lecture だと少なめ？

 Atomic Number  Protons + Neutrons = Atomic Mass.

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.

Alpha Decay A Helium- 4 nucleus (two protons and two neutrons). Is produced by nuclear fission Massive nucleus breaks apart into two less-massive nuclei.

Lawrence Livermore National Laboratory Nicholas Scielzo Lawrence Fellow Physics Division, Physical Sciences LLNL-PRES Lawrence Livermore National.

Fundamental Interactions Physics & Instrumentation Conclusions Conveners: P. Mueller, J. Clark G. Savard, N. Scielzo.

European Isotope Separation On-Line Radioactive Nuclear Beam Facility A preliminary design study of the next- generation European ISOL RNB facility GANIL,

Accelerator Physics, JU, First Semester, (Saed Dababneh). 1 Electron pick-up. ~1/E What about fission fragments????? Bragg curve stochastic energy.

Nuclear Radiation 9.2. The Nucleus Protons and neutrons Charge of electrons and protons – x C = e –Proton +e –Electron -e.

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

W. Nazarewicz. Limit of stability for heavy nuclei Meitner & Frisch (1939): Nucleus is like liquid drop For Z>100: repulsive Coulomb force stronger than.

L-35 Modern Physics-3 Nuclear Physics

1 Programme Advisory Committee for Nuclear Physics 29 th meeting, January 2009 Programme Advisory Committee for Nuclear Physics 29 th meeting,

1 CNS summer school 2002 The RI-Beam Factory and Recent Development in Superheavy Elements Search at RIKEN ◆ Brief introduction to the RI Beam Factory.

February 12-15,2003 PROCON 2003, Legnaro-Padova, Italy Jean Charles THOMAS University of Leuven / IKS, Belgium University of Bordeaux I / CENBG, France.

NUCLEAR CHANGES What is Radioactivity?. What happens when an element undergoes radioactive decay? During radioactive decay an unstable nuclei of an isotope.

© 2003 By Default! A Free sample background from Slide 1 JINR SCIENTIFIC COUNCIL 102 nd Session, September 2007, Dubna.

NSCL Nuclear Research at MSU A world-class facility for nuclear experimentation and theory ISO 9001, ISO 14001, OHSAS registered NATIONAL SUPERCONDUCTING.

NSCL Nuclear research at MSU National Superconducting Cyclotron Laboratory A world-class facility for nuclear experimentation and theory ISO 9001, ISO.

Nuclear Stability and Decay 1500 different nuclei are known. Only 264 are stable and do not decay. The stability of a nucleus depends on its neutron-to-

The NSCL is funded in part by the National Science Foundation and Michigan State University. Results: the neutron source was located 19.9 inches from the.

Nuclear Chemistry. Radioactivity  Nuclear Reactions – reactions in which the nuclei of unstable isotopes (radioisotopes) gain stability by undergoing.

FAST IN-MEDIUM FRAGMENTATION OF PROJECTILE NUCLEI

6th Grade Life Science Miss Sauer

Studies of Pear Shaped Nuclei using rare isotope beams

Nuclear Chemistry Physical Science.

CNS Active Targets for Missing Mass Spectroscopy with RI beams Tomohiro Uesaka CNS, University of Tokyo ・　Missing Mass Spectroscopy ・ Two different.

Nuclear Chemistry: Radioactivity & Types of Radiation

Nuclear Chemistry Chapter 21.

CNS Active Targets for Missing Mass Spectroscopy with RI beams Tomohiro Uesaka CNS, University of Tokyo ・　Missing Mass Spectroscopy ・ Two different.

Nuclear Chemistry The energy of life.

Atomic Structure.

Presentation transcript:

In Progress T-Rex TAMUTrap SASSYER Active Target Det RTC + chemistry Radioisotope production

16 Faculty 32 students 14 Postdocs 26Staff ( Research + Ops) 6 TAMU undergraduates 13 REU students

NSCL - ANASEN TRINET decays) SAMURAI collaboration at RIKEN Jyvaskyla (mass measurements w/ penning trap) STAR

Future research directions Studies of survival of excited nuclei in the actinide region with SaSSYER. Study the complexation of transactinide homologs with cryptands and crown ethers in "online" experiments Studying beta-delayed proton decays of pure Fermi Transitions with TAMUTrap Nuclear astrophysics with stable and rare isotope beams. Structure of light exotic nuclei. Clustering phenomena in light and medium mass nuclei. Studies of the EOS and Esym Pionic Fusion Superallowed  decay studies on Tz=-1 nuclei GMR as probe of structure and asymmetry Develop and apply nuclear theory of HI rxn and GR to determine the next generation energy density functional for nuclei.

1. facility & equipment 2. people (faculty staff, postdoc, students) 3. future research directions 4. connections to programs elsewhere

MDM SPECTROMETER (1993, 2000) High-resolution, broad-range spectrometer. Beam analysis system provides beams for the MDM Spectrometer. FORWARD ARRAY USING SILICON TECHNOLOGY – QUADRUPOLE TRIPLET (FAUST-QT) (2013) Detection of light charged particles and intermediate mass fragments in the FAUST multi- detector array, while simultaneously collecting the heaviest fragment in the QT. K500 SUPERCONDUCTING CYCLOTRON (1987) The Cyclotron Institute at Texas A&M University operates one of only five K500 superconducting cyclotrons in the world. MARS RECOIL SPECTROMETER (1992) Spectrometer for production and separation of radioactive ions PRECISION ON-LINE g-DECAY FACILITY (1999) Isolates pure samples of short-lived isotopes for high-precision decay measurements. ELECTRON CYCLOTRON RESONANCE (ECR) ION SOURCES ( ) Two ECR sources inject beam into the K150 and K500 Cyclotrons. A third acts as a charge breeder for radioactive beams. NEGATIVE-ION SOURCE (2010) For the production of high intensity proton and deuteron beams from the K150 Cyclotron. K150 CYCLOTRON(1967) Following 20 years off line this facility is now operational and is an integral part of the facility upgrade to make the Cyclotron Institute a dual-cyclotron facility providing accelerated secondary beams. NIMROD (1999) High efficiency detection of both neutrons and charged particles. RADIATION EFFECT FACILITY (1994, 2000) Available for commercial, governmental and educational use, the testing facility is installed on a dedicated beam line with complete diagnostic equipment and controls. With the modern K500 superconducting cyclotron and the advanced ECR ion source, a diverse range of particle beams and energies is available for radiation-effects testing. TARGET & ION SOURCE FOR RADIOACTIVE BEAMS (2011) Exotic isotopes produced by the K150 Cyclotron will be conveyed to the K500 for re- acceleration.