ARIEL at TRIUMF: science, status and opportunities

Similar documents
Recirculating Electron Beam Photo-converter for Rare Isotope Production CYC2016

Highlights and Status from TRIUMF: ISAC & ARIEL

Study of Photo-Production of Radioactive Ion Beams

Inves&ga&on of neutron- rich isotopes: Understanding the r process

Actinide Target Station & 238

Pushing the boundaries of Penning trap mass spectrometry

Report on Nuclear Physics activities in Canada

An Electron Linac Photo-Fission Driver for the Rare Isotope Program at TRIUMF

RI-Beam Graduate studies and research opportunities in Canada. R. Kanungo Saint Mary s University, Halifax

Molecular and Materials Science

Benchmarks from high-precision mass measurements at TITAN

Long Range Planning in Canada

Charge State Breeding for the. at TRIUMF

Searching for SUSY at the upgraded LHC

Decay spectroscopy of neutron-rich isotopes for astrophysics at GSI, IGISOL, TRIUMF, and RIKEN

Introduction to REX-ISOLDE concept and overview of (future) European projects

The SPIRAL2 Project and experiments with high-intensity rare isotope beams

Review of ISOL-type Radioactive Beam Facilities

Isotopes: atoms with the same Z but different A s (number of neutrons varies)

Multiple Choice Questions

Neutron induced reaction and neutron sources

[2] State in what form the energy is released in such a reaction.... [1]

b-delayed neutron emission and its role in the r-process

What s going on and why people care

The Facility for Rare Isotope Beams

There are 82 protons in a lead nucleus. Why doesn t the lead nucleus burst apart?

Information Nuclide = is an atomic species characterized by the specific constitution of its nucleus (protons and neutrons) Neutron

K.U.Leuven. : an Application of the MYRRHA Accelerator for Nuclear Physics. Piet Van Duppen IKS, KUL, Leuven (BE)

Laser Spectroscopy on Bunched Radioactive Ion Beams

Capabilities at the National Superconducting Cyclotron Laboratory. Sean Liddick NDNCA workshop, May 26-29, 2015

Developments of the RCNP cyclotron cascade

Spallation, multifragmentation and radioactive beams

Chapter 3. Radioactivity. Table of Contents

Status & Plans for the TRIUMF ISAC Facility

A Simple Estimate of Production of Medical Isotopes by Photo-Neutron Reaction at the Canadian Light Source

The PIENU Experiment a sensitive probe in the search for new physics

Delivering on the Promise

Nuclear Chemistry. Decay Reactions The most common form of nuclear decay reactions are the following:

Alta Chemistry CHAPTER 25. Nuclear Chemistry: Radiation, Radioactivity & its Applications

PREX and CREX. R N from Electroweak Asymmetry in Elastic Electron-Nucleus Scattering. Neutron Skin.

PRODUCTION OF RADIOISOTOPES FOR IMAGING AND THERAPY AT LOW ENERGY

GANIL / SPIRAL1 / SPIRAL2

NSCL and Physics and Astronomy Department, Michigan State University Joint Institute for Nuclear Astrophysics

Chapter. Nuclear Chemistry

Radioactive Ion Beams for Astrophysics

Neutron skin measurements and its constraints for neutron matter. C. J. Horowitz, Indiana University INT, Seattle, 2016

Nuclear research and education at the Australian National University

Nuclear Physics. PHY232 Remco Zegers Room W109 cyclotron building.

Nuclear Radiation. Natural Radioactivity. A person working with radioisotopes wears protective clothing and gloves and stands behind a shield.

Extreme Light Infrastructure - Nuclear Physics ELI - NP

D) g. 2. In which pair do the particles have approximately the same mass?

Nuclear Reactions Homework Unit 13 - Topic 4

Why Make Rare Isotopes?

Opportunities with collinear laser spectroscopy at DESIR:

Advisory Committee on

Efficient inter-trap transfer of cold francium atoms

Physics with Exotic Nuclei

Fiesta Ware. Nuclear Chemistry. 2009, Prentice-Hall, Inc.

Chapter 21. Chemistry, The Central Science, 10th edition Theodore L. Brown; H. Eugene LeMay, Jr.; and Bruce E. Bursten

Unit 3: Chemistry in Society Nuclear Chemistry Summary Notes

4 Nuclear Stability And Instability

Chemistry Unit 5 Exam Study Guide Nuclear Chemistry

Utilization of Intense Rare Isotope Beam at KoRIA

Atomic Parity Non-Conservation in Francium: The FrPNC Experiment

Chapter 12: Nuclear Reaction

NSCL Operations and ReAcclerator Facility at MSU. Daniela Leitner Michigan State University

The FrPNC Experiment, weak interaction studies in Francium at TRIUMF

Radiochemistry and Nuclear Methods of Analysis

High efficiency 3 He neutron detector TETRA for DESIR.

Notes: Unit 14 Nuclear Chemistry

Experimental Nuclear Astrophysics: Lecture 1. Chris Wrede National Nuclear Physics Summer School June 19 th, 2018

Opportunities to study the SHE production mechanism with rare isotopes at the ReA3 facility

SPIRAL-2 FOR NEUTRON PRODUCTION

u d Fig. 6.1 (i) Identify the anti-proton from the table of particles shown in Fig [1]

Unit 12: Nuclear Chemistry

The Gamma Factory proposal for CERN

Understanding the proton radius puzzle: Nuclear structure corrections in light muonic atoms

L-35 Modern Physics-3 Nuclear Physics 29:006 FINAL EXAM. Structure of the nucleus. The atom and the nucleus. Nuclear Terminology

Reactions of neutron-rich Sn isotopes investigated at relativistic energies at R 3 B

Isotope Production for Nuclear Medicine

Recent Results from ISOLDE and new Opportunities with HIE- ISOLDE

Operation of the Coupled Cyclotron Facility at Michigan State University

Nuclear Chemistry. Mass Defect. E=mc 2. Radioactivity. Types of Radiation. Other Nuclear Particles. Nuclear Reactions vs. Normal Chemical Changes

FAIR. Reiner Krücken for the NUSTAR collaboration

RADIOACTIVITY. Nature of Radioactive Emissions

Nuclear Astrophysics with DRAGON at ISAC:

L 36 Modern Physics [3] The atom and the nucleus. Structure of the nucleus. The structure of the nucleus SYMBOL FOR A NUCLEUS FOR A CHEMICAL X

D.H. Ryan. Centre for the Physics of Materials and Physics Department, McGill University, Montreal, Quebec CANADA

The Accelerator System for ReA3 the New Re-accelerated RIBs Facility at MSU

Introduction to Accelerator Physics Part 1

Nuclear Chemistry. In this chapter we will look at two types of nuclear reactions.

Chapter 18. Nuclear Chemistry

Nuclear and Radiation Physics

RDCH 702 Lecture 8: Accelerators and Isotope Production

Yongseok Oh Kyungpook National University

Nuclear Chemistry. Radioactivity. In this chapter we will look at two types of nuclear reactions.

Section 2: Nuclear Fission and Fusion. Preview Key Ideas Bellringer Nuclear Forces Nuclear Fission Chain Reaction Nuclear Fusion

Status of the EBIT in the ReA3 reaccelerator at NSCL

SOURCES of RADIOACTIVITY

Planning and preparation approaches for non-nuclear waste disposal

Transcription:

Canada s National Laboratory for Particle and Nuclear Physics ARIEL at TRIUMF: science, status and opportunities Jens Dilling Associate Laboratory Director TRIUMF - Physical Sciences Division September 15 2016 International Nuclear Physics Conference 2016, Adelaide

TRIUMF was founded in 1968 and has delivered nearly 50 years of accelerator-based science and innovation for Canada, and is engaging the World. TRIUMF: Canada s National Laboratory

TRIUMF s accelerator complex 40 MV SRF Heavy Ion Linac Advanced Rare Isotope Laboratory (ARIEL) Cyclotron 500 MeV 350 ma ISAC-II >10 AMeV ISAC-I 60 kev, 1.7 AMeV Particle Physics Pienu Ultra Cold Neutrons ISAC (Isotope Separator and ACcelerator) Rare Isotope Facility - Nuclear Structure - Nuclear Astrophysics - Fund. Symmetries - CMMS (bnmr) Nordion commercial medical isotope production 3 cyclotrons CMMS Centre for Molecular and Material Science (msr)

ISAC rare isotope facility Programs in ISAC II: 10 AMeV for A<150 16AMeV for A<30 ISAC I: 60 kev & 1.7 AMeV Nuclear Structure & Dynamics Nuclear Astrophysics Electroweak Interaction Studies Material Science 18 permanent experiments ISOL facility with high primary beam intensity (100 ma, 500 MeV, p) Operational since 1998.

Experimental facilities and programs @ ISAC Material Science DESCANT GRIFFIN

The Advanced Rare IsotopE Laboratory will triple TRIUMF s isotope beam capacity Uses state-of-the-art, made-in-canada superconducting electron linear accelerator technology; targets are designed to allow medical isotopes to be extracted alongside the experimental program Represents ~$100 million investment by federal and provincial governments; supported by 19 university partners from across Canada Project to occur in two phases: ARIEL-I completed in Fall 2014; ARIEL-II funded by Canada Foundation of Innovation, funding announcement imminent. Will provide more and new isotopes ARIEL: The future of isotopes at TRIUMF

ARIEL expand isotope program at TRIUMF with: 3 simultaneous beams ( 1 ISAC + 2 ARIEL) e-linac and proton beams Increased number of hours delivered per year New isotope species Time for beam developments Clean beam using HRS and new EBIS Enable long beam times Nucl. astrophysics, Fundamental sym. Tests ARIEL is a project in 2 phases ARIEL-1 completed on time and on budget (2014) ARIEL-2 is starting up

The goal of ARIEL: science and opportunities What we can do at ARIEL: isotopes for characterizing new materials: 8 Li as a sensitive probe for interfaces medical isotopes for nuclear imaging and tumor treatment: alpha-emitters like 211 At isotopes for developing and refining theory for nuclear physics Proton- and electron-induced rare isotopes at the extremes isotopes as laboratories to search for new symmetries in nature Heavy proton-induced isotopes, like Fr, Rn and some light electron-induced isotopes: Li isotopes: how and where the heavy elements were produced in the universe Very neutron rich isotopes from photo-fission Triple the available beam time: more time for beam developments

Isotopes for characterizing new material Putting new materials together and investigate their behavior: magnetism, superconductivity, semiconductors, batteries + LaAlO3 = non-magnetic insulator LAO STO LAO STO Magical Multilayers What happens at the interface? Studies to investigate behavior at the conjunction that is responsible for new effects or features: Need a very sensitive probe for thin layers (~5-10 nm). LAO STO βnmr: uses beta-decay of polarized 8 Li to probe for changes in the electric and magnetic fields. βnmr has unique sensitivity to probe very thin layers (~5-10 nm) to see what happens at the interface by adjusting the implantation depth of the heavy ion.

Alpha emitting isotopes: powerful way for direct tumor treatment Isotopes for medical application: tumor treatment and imaging Clustered DNA damage due to heavy particle stopping power, short range. 211 At particularly well suited for applications Study surrogate functionality of 209 At for imaging 211 At is generated via 211 Rn at ISAC and ARIEL via protons and could be exported across Canada.

Nuclear Astrophysics: how and where are the heavy elements produced In a normal star, only elements up to iron are produced via nuclear fusion. How do you generate the heavier elements? 126 S p =0 82 82 National Research Council (US) Question 3 How and where were the elements from iron to uranium made? Z 28 20 8 2 2 8 20 28 N 50 S n =0 50 MPA Garching

Isotopes to search for new symmetries in nature Nature is governed by symmetry principles Use synthesized isotopes with special features to carry out precision experiments to search for new symmetries. There are multiple symmetry test programs planned (or on-going) at ISAC / ARIEL: Fr atomic parity non-conservation, anapole moment 212 Fr Fr permanent electric dipole program 208 Fr Rn permanent electric dipole program 221 Rn MTV (Mott polarimetry for time violation): 8 Li TRINAT electro weak symmetry tests 39 K

ARIEL-1: e-linac completed and commissioned ARIEL e-linac: completed and operational

5 cm ARIEL-2: developments Target developments for p- and - fission targets with 238 UC x (100kW) New target removal and exchange concept (internat. review) Test stand for e-hall vertical 50 cm 3 BaO / UC x target e - 8 x 45 mm high-z primary converter

Photo-fission isotopes Photo-fission isotopes: cleaner n-rich isotopes Limited to 100kW targets initially (10 12 fission) Can be achieved with conventional technologies Factory model for three beams developed Target exchanges every 3 weeks Storage of targets for up to 3 years New target production capabilities Modular target system, hermetically sealed units

ARIEL-II Schedule Science Phases 8 Li via 9 Be(,p) using e-linac isotopes via U(,f) using e-linac isotopes from ISAC, new EBIS and HRS isotopes via p-induced from ARIEL 2016 2017 2018 2019 2020 2021 2022 Phase Will deliver isotopes for... 1 Materials science with β-nmr + light beams for Fund. Symmetries. ( 8 Li) 2 Photo-fission of uranium from e-linac 3 Purified accelerated high mass beams 4 Fundamental Symmetries w/ new proton beamline (BL4N) ARIEL user consultation ongoing: town-hall meeting in January 2017

ARIEL/ISAC will enable the delivery of three parallel radioactive beams to users: Two cyclotron-beams for proton-induced reactions, up to 100 kw Heavy elements for test of symmetries in Nature p-rich beams for fundamental nuclear physics/astrophysics Developments of isotopes for nuclear medicine One electron linac beam, up to 100 kw, 35 MeV Photo-fission elements of n-rich beams, astrophysics, nuclear physics Li-beams for material sciences Extra time for beam developments ARIEL will be the first multi-user radioactive beam facility in the world Up to three independent experiments More time for beam developments Conclusions Excellent progress, project is on track: Photo-fission target developments under way e-beam lines on track, first beam 2019/20 Proton beam line in preparation User consultation on-going

Canada s national laboratory for particle and nuclear physics Laboratoire national canadien pour la recherche en physique nucléaire et en physique des particules Thank you! Merci! TRIUMF: Alberta British Columbia Calgary Carleton Guelph McGill Manitoba McMaster Montréal Northern British Columbia Queen s Regina Saint Mary s Simon Fraser Toronto Victoria Western Winnipeg York Follow us at TRIUMFLab

Proton number Z The Future: Science enabled by ARIEL Actinide proton beam-line: High intensity, clean beams for electroweak precision experiments using hundreds of days of beam per year - Francium PNC - Atomic EDM in Rn - Electron EDM using Fr fountain 126 S p =0 50 50 20 28 28 20 8 2 S n =0 2 8 Neutron number N 82 82 Multi-user operations: More beam time for - Beam development - Nuclear astrophysics - Precision experiments e-linac and photo-fission Delineating the r-process path with fission fragment beams from the e-linac - masses, charge radii, decay properties - transfer reactions mapping shell structure - studies of neutron capture and photo dissociation rates

FLUKA Production Map from 35 MeV Electrons ARIEL Current Concept Design In-Target Production Yields [10 kw-1 s-1] In-target production rates [10 kw-1 s-1]: from BeO: 8Li: 5 1010 from UCx: 78Ni: 1 105 98Kr: 8 107 100Rb: 1 108 98Sr: 5 109 132Sn: 5 108 146Xe: 2 107 144Ba: 5 109 150Cs: 4 105 FLUKA: A. Gottberg (TRIUMF and results verified independently with GEANT4 (Marla Cervantes Smith, University of Victoria)