Institute of Accelerator Technologies of Ankara University and TARLA Facility



Similar documents
Towards large dynamic range beam diagnostics and beam dynamics studies. Pavel Evtushenko

K O M A C. Beam Commissioning of 100-MeV KOMAC Linac. Korea Multi-purpose Accelerator Complex 양 성 자 가 속 기 연 구 센 터

10 Project Costs and Schedule

ULTRAFAST LASERS: Free electron lasers thrive from synergy with ultrafast laser systems

Results: Low current ( ) Worst case: 800 MHz, GeV, 4 turns Energy oscillation amplitude 154 MeV, where

Damping Wigglers in PETRA III

Project X: A multi-mw Proton Source at Fermilab. Steve Holmes Extreme Beam Lecture Series

Activities at the University of Frankfurt (IAP)

Reliability and Availability Aspects of. the IPHI Project

Comb beam for particle-driven plasma-based accelerators

Status of Radiation Safety System at

AUTOMATION OF OPERATIONS ON THE VEPP-4 CONTROL SYSTEM

Status of High Current Ion Sources. Daniela Leitner Lawrence Berkeley National Laboratory

source at CERN G.McMonagle AB/RF

FLASH Commissioning and Startup

Status of the Diamond Storage Ring RF Systems. Morten Jensen on behalf of Diamond Storage Ring RF Group

Status of the Free Electron Laser

OVERVIEW OF PROTON DRIVERS FOR NEUTRINO SUPER BEAMS AND NEUTRINO FACTORIES*

Cathode Ray Tube. Introduction. Functional principle

Short overview of TEUFEL-project

Content. > How to ensure sustainability of RIs? > RIs generate knowledge > Socio-economic impact of RIs

BEPC UPGRADES AND TAU-CHARM FACTORY DESIGN

Development of a Low Frequency Superconducting RF Electron Gun. September 2010

THE ALIGNMENT STRATEGY FOR THE SPIRAL2 SUPERCONDUCTING LINAC CRYOMODULES

Cleaning Methods of SRF Power Couplers. Mircea Stirbet

DEMONSTRATION ACCELERATOR DRIVEN COMPLEX FOR EFFECTIVE INCINERATION OF 99 Tc AND 129 I

THE DUKE FEL LIGHT SOURCE FACILITY

BEAM OPERATION OF THE PAL-XFEL INJECTOR TEST FACILITY

HIGH CURRENT OPERATION OF THE ACSI TR30 CYCLOTRON

THE TESLA TEST FACILITY AS A PROTOTYPE FOR THE GLOBAL ACCELERATOR NETWORK

Industrial Involvement in the Construction of Synchrotron Light Sources

Systems, Inc. Energy Advanced

A. Martinez, A. L. Klebaner, J. C. Theilacker, B. D. DeGraff, M. White and G. S. Johnson

Experiment 5. Lasers and laser mode structure

Status of the SOLEIL project Commissioning from Linac to beamlines

Data-analysis scheme and infrastructure at the X-ray free electron laser facility, SACLA

Zero Degree Extraction using an Electrostatic Separator

STAR: State of the art

Development of on line monitor detectors used for clinical routine in proton and ion therapy

Status Overview The Australian Synchrotron. Steven Banks Control Systems Group

LEReC Engineering. J. Tuozzolo, C-AD Chief Mechanical Engineer (LEReC Project Engineer)

11th International Computational Accelerator Physics Conference (ICAP) August 19 24, 2012, Rostock-Warnemünde (Germany)

Status And Future Plans. Mitsuyoshi Tanaka. AGS Department.Brookhaven National Laboratory* Upton NY 11973, USA INTRODUCTION

FIVE PROJECTS OF HIGH RF POWER INPUT COUPLERS & WINDOWS FOR SRF ACCELERATORS*

The European X-ray Free-Electron Laser Facility European XFEL Massimo Altarelli.

Cryogenic Current Comparator Status at GSI/FAIR -

High Brightness Photo Injectors for Brilliant Light Sources

Figure 1: Lattice drawing for the APS storage ring.

FCC JGU WBS_v0034.xlsm

FLS 2010 Storage Ring Working Group Session 4: Future ring technology and design issues

& Tunnel Cross Section

ESS Proton Linac Accelerator Project Leader: Mats Lindroos Roland Garoby Technical Director Ankara - October 6, 2015

Projects and R&D activities

Radiant Dyes Laser Accessories GmbH

EUROPEAN ORGANIZATION FOR NUCLEAR RESEARCH Laboratory for Particle Physics SUPERCONDUCTIVITY AND CRYOGENICS FOR FUTURE HIGH-ENERGY ACCELERATORS

ELECTRICAL ENGINEERING ASPECTS OF RADIOTHERAPY ACCELERATORS *

Development and Experimental Performance Evaluation of a Dose-Rate meter for Pulsed Beam.

Beam Instrumentation Group, CERN ACAS, Australian Collaboration for Accelerator Science 3. School of Physics, University of Melbourne 4


Instrumenter til E-XFEL. Martin Meedom Nielsen Section for Neutrons and X-rays for Materials Physics

The STAR Project: Southern european Thomson source for Applied Research

CLS Beamline Remote Control Project. E. Matias Canadian Light Source University of Saskatchewan

The IR FEL at the Fritz Haber Institute Berlin: A Tool for IR Spectroscopy of Molecules, Clusters, and Solids

A Quick primer on synchrotron radiation: How would an MBA source change my x-ray beam. Jonathan Lang Advanced Photon Source

A c tiv itie s in Ita ly and at E u r o p e a n S y n c h ro tro n R a d ia tio n S ou rces. S. Tazzari INFN-LNF Frascati, Italy

LLRF. Digital RF Stabilization System

Real-world applications of intense light matter interaction beyond the scope of classical micromachining.

Relativistic kinematics basic energy, mass and momentum units, Lorents force, track bending, sagitta. First accelerator: cathode ray tube

ESS Cost Book Affiliation Authors Johan Brisfors ESS Reviewers EPG, EMT ESS Approver James Yeck ESS

Large Systems Commissioning

Speed Network Marketing, Energy Selection and Optimal Timetable

DIODE PUMPED CRYSTALASER

Should SMTF Include RIA?

Shielding and Radiation Measurements at ESRF

THE TAIWAN LIGHT SOURCE AND SUPERCONDUCTING CAVITY

CLIC accelerator and detector

RF SYSTEM FOR VEPP-5 DAMPING RING

MYRRHA Injector Design

Experimental Particle Physics PHYS6011 Southampton University Lecture 1

Les Accélérateurs Laser Plasma

SOLEIL Current Performances. And. Futur Developments

ASACUSA: Measuring the Antiproton Mass and Magnetic Moment

3 Main Linac. 3.1 Introduction. 3.2 Beam Dynamics II-63

Introduction to Superconducting RF (srf)

Development of Virtual Accelerator Environment for Beam Diagnostics *

TTF OPERATIONS STATISTICS

Libera at ELETTRA: prehistory, history and present state

Recent Measurements and Plans for the SLAC Compton X- Ray Source

Solutions Manufacturing Performance

The BESSY HOM Damped Cavity with Ferrite Absorbers. Review of prototype cavity test results, taperedwaveguidesvshomogenouswaveguides

World-first Proton Pencil Beam Scanning System with FDA Clearance

A Beam Halo Monitor Based on Adaptive Optics. Courtesy of Dr Carsten P. Welsch AB/BI/PM

- thus, the total number of atoms per second that absorb a photon is

Linac RF Commissioning with the SNS HPRF Systems

NUCLEAR MAGNETIC RESONANCE. Advanced Laboratory, Physics 407, University of Wisconsin Madison, Wisconsin 53706

Digital vs. Analogue Control Systems

Calculation of Eigenmodes in Superconducting Cavities

Atomic and Nuclear Physics Laboratory (Physics 4780)

Beam Position Monitoring at CLIC

Transcription:

Institute of Accelerator Technologies of Ankara University and TARLA Facility Avni Aksoy Ankara University avniaksoy@ankara.edu.tr On behalf of IAT & TARLA Team

Contents Brief history of TAC project Institute of Accelerator Technologies of Ankara University TARLA facility Potential of facility Main Components Proposed FEL applications TAC proton accelerator facility Conclusion 2

TAC was born The Turkish Accelerator Center (TAC) project was first proposed in 2000 s linac-ring type e-e+ collider with center of mass energy of 1 GeV as Φ factory. as Additionally in the proposal ; Electron linac of the complex maybe used to drive SASE undulators Positron ring of the complex may be used as SR source. 1st phase Preliminary phase (1997-2001) Outcome: A preliminary report Report in 2001 Accelerator Center (TAC) Project was proposed 2nd phase Feasibility Report (2002-2005) Outcome : A Feasibility Report in 2005, Change from Ф-factory to Charm factory Main parameters of the proposed facilities Types and technologies of accelerators Research potential of proposed facilities of TAC are explained A. K.Çiftçi, O. Gürkan, T. Olgar, E. Recepoğlu, S. Sultansoy, M. Yılmaz, Ö. Yavaş 06.10.2015 avniaksoy@ankara.edu.tr 3

Current phase 3rd phase (current phase) (2006-20..) First Facility, Institute, Conceptual and Technical Design Reports of Proposed TAC Facilities Started in 2006 as collaboration of 12 Turkish universities under the coordination of Ankara University (~155 people) Goal of the phase TAC Project TARLA SR PA SASE 40 MeV 3 GeV 2 GeV 6 GeV Oscillator Establishment FEL Synchrotron of The Institute of Accelerator Proton Technologies SASE (IAT) FEL Establishment of Radiation Accelerator test facility (Oscillator mode IR FEL & Bremsstrahlung) (TARLA, founded and installation continueing). Installation and commissioning phase Detailed Design Report phase Conceptual Design Report phase Feasibility Report phase Completing the Design Report of Synchrotron Radiation facility PF 1 GeV - 3.5 GeV e - - e + collider Completing the Conceptual Design Reports of SASE FEL, Proton accelerator and TAC Particle Factory 06.10.2015 avniaksoy@ankara.edu.tr 4

Institute of Accelerator Technologies IAT is proposed to To train people about accelerators To host and construct the Test facility of TAC To establish collaborations with international communities Institute of Accelerator Technologies has been established in Ankara University in 2011 The institute which is located in Gölbası (15 km south of Ankara) housing the TARLA facility It is the first institute established in Turkey as research in the fields of accelerators and related topics We have 16 full-time employee in the institute (11 technical, 5 administrative) About 5 part time collaborator from different universities 06.10.2015 avniaksoy@ankara.edu.tr 5

Scope of the test facility, TARLA Constructing accelerator based research facility in order to serve our country and our region within the frame of Turkish Accelerator Center Project. In TARLA facility we propose; To generate Free Electron Laser between 3-250 µm using 15-40 MeV electron beam and two different optical resonator system housing two different undulators with 25 mm and 90 mm period length To generatre Bremsstrahlung radiation using 0-30 MeV electron beam and three different radiator-colimator setup and study nuclear physics To use 0-40 MeV electron directly in order to make fixed target experiments 06.10.2015 avniaksoy@ankara.edu.tr 6

TARLA layout E = 250 kev σ = 500 E = ps 250 kev σ = 10 E ps =10-20 MeV E =10-40 MeV E =10-20 MeV σ = 2 ps σ = 0.4-5 ps σ = 0.4-5 ps FEL-1 λ= 3-19 µm Bremmstrahlung FEL-2 Eγ =1-30 MeVλ= 19-250 µm 7 ~60m

TARLA Electron Beam Spacing between bunches will be adjusted with grid modulation installed on gun. CW Beam 1 ma, 0-40 MeV Coherent IR Laser 3 250 µm materials research biophysics biochemistry environment Polarized Gamma 0 30 MeV Nuclear physics Nuclear astrophysiscs Radiation physics Macropulse time structure is manipulated with macropulsed installed on injector. Electrons 0 40 MeV radio biology detector studies materials research 8/20

Research Potential of TARLA Superconducting accelerator based electron beam 0-40 MeV, 0-1 (1.5) ma 40 (60) kw pulsed/ CW Free Electron Laser Radiator Foil (Al,Nb) Direct Use W Moderator Christal cannelling Compton Back Scattering Lead Target Bending Magnet Coherent IR Radiation 3-250 µm Material, (bio)physics, (bio)chemistry, medical.. Polorized Gamma 0-30 MeV Nuclear Physics, Astrophysics, Radiation hardness Gamma induced positron spectroscopy Electron Beam 0-40 MeV Radyobiolgy, Detector study, Thomson scattering Electron difraction, plasma studies Mono Chromatic Positron Semiconductors, material, Quasi Monochromatic X-ray Radiation physics, Radiobiology.. Notron Source Fission, material, nuclear physics THz Radiation Material research, detector study 9

TARLA Superconducting accelerating module Super conducting RF accelerating modules is being manufactured by Research instruments (Contract in 2012 Oct) This module is compact and houses two TESLA cavities It is designed for continuous operation with accelerating gradient up to 15 MV/m. The cryostat design has been developed by ELBE team (HZDR) and is used under a license agreement. Modules will be delivered by beginning of 2016 10

TARLA RF System, Block Diagram RF control is DESY design digital LLRF (μtci4) Each structure will be fed by individual power amplifiers Each amplifier will have its own driver / LLRF controller RF amplifiers are solid state power amplifiers 11

TARLA Electron Beam Parameters Parameter Unit Base Upgrade Beam Energy MeV 5-40 5-40 Max average beam current ma 1 1.5 Max bunch charge (@ 13 MHz) pc 77 115 Horizontal emittance mm.mrad < 15 < 16 Vertical emittance mm.mrad < 12 <13 Longitudinal emittance kev.ps < 85 <100 Bunch lenght Ps 0.4-6 0.4-6 Bunch repetition MHz 13 13-26 Macropulse duration μs 50 CW 50CW Macropulse repetition Hz 1 CW 1 CW 12

Electron gun test setup Experience and problems solved High Voltage 250 kv High vacuum 3 10 10 mbar Relativelly high frequency < 20 ps jitter, σ=500 ps @13 MHz High radiation >2000 μs/h Remote control EPICS & LabView, PLC. BPM FCT Beam charge 13

Free Electron Laser Section We propose to use 2 different optical resonator in order to scan all wavelengths between 3-250 μm. The beam is injected to undulators with achromatic beamlines (dipole-quadrupole triplet-dipole). U90 undulator with 90 mm period length and U25 undulator with 25 mm period length Besides the length of the periods of the undulators, the waveguide structure of U95 is another main difference between resonators. Preliminery design for undulators NbFe pole material, vanadium permandur blocks Roll off filed for max field is 0.04 NbFe pole material, vanadium permandur blocks Roll off filed for max field is 0.1 14

FEL Simulations in progress Time depended simuiation for FEL with 3 µm wavelength E=38:2 MeV K u = 0.35 Z r =0.75 σ b = 0.5 ps No detunning R 1 =R 2 =5.86 Mirror Reflection ratio=%98 Transverse beam sizes 15

Helyum Plant The plant is used to cool down superconducting structures down to 1.8 K Our plant has been manufactured by Air Liquide and delivered by the end of 2014. Installation is still continueing The system will consist of Capacity Helium refrigerator (4 K box) Distribution Box (2 K box, housing cold compressors) Two compressors Warm vacuum pump station Oil remover, transfer lines, vaporizer etc.. 210 W @1.8K 16 mbar ± 0.2mbar Installation and commissioning tests will be finished in by beginning of 2016 16

Auxiliary systems Water cooling, (installation completed for non-radioactive areas) 24±1 C o, 850.000 kcal/h Nitrogen Cooling (installation completed) 500 l/day LN2 will be provided by storage system. The shielded lines are installed arround facility.. Power network 2+1 (main + backup) MW Transformer, 2+1 (main + backup) MW Generator, 6 300 kw UPS EPICS and PLC based Control system EPICS Machine control PLC Control of auxialiry systems PSS Cooling Building control 17

Proposed FEL Stations Proposed FEL stations are: IR spectroscopy lab. SFG-PP lab. Bio-Micro Spectroscopy lab. Material research lab. Main FEL parameters are available for these labs wavelength range: 3-250 m Average FEL power: 1-100 W Each room will be equipped with table-tab laser sources with 700 1000 nm wavelength Ti-sapphire laser Nd:Yag laser FEL and external lasers will be synchronized Δσ<100 fs The rooms will have class 1000 standard 18

TAC Proton Accelerator Facility (PAF) http://tac.ankara.edu.tr/paf TAC Proton Accelerator is proposed as a multipurpose, multi GeV energy and MW power machine (Low enery 3-65 MeV & 65-250 MeV, High energy up to 2 GeV) The project is planned progress in three stages: Stage 1: ion-source, Low Energy Beam Transport and a RFQ (up to 3 MeV); Stage 2: 250 MeV linear accelerator, which could be built in two step Step 1- a 3-65 MeV Drift Tube Linac (DTL) step 2 - a Medium energy beam transport and 65-250 MeV SC-spoke cavity and SC-elliptical cavity Stage 3: a 1 MW proton facility up to 2 GeV probably a SC-Elliptical cavity Ö.Yavaş (omer.yavas@ankara.edu.tr) L. Şahin (latife.sahin@istanbul.edu.tr) 19

TAC Proton Accelerator Facility This proton accelerator facility could serve as a neutron source, a radioactive ion beam facility as well as a number of lower energy facilities for use in nuclear, material, biological, and medical sciences. Coordinators of TAC PAF: B. Akkuş, L. Şahin (Istanbul U.) E. Algin (ESOGU) M. Yılmaz (Gazi U.) Ö.Yavaş (omer.yavas@ankara.edu.tr) 20

Conclusion TARLA is the first step of TAC project and will be the first accelerator based user facility in Turkey and around our region. The facility will give opportunity to scientists and industry to make research about material, biotechnology, optics, semiconductors, medicine, chemistry and nanotechnology as well.. The infrastructure has almost been completed The milestones of TARLA is The helium plant will be ready by the beginning of 2016, The injector will to be ready by the end of 2016. First cyromodule will be delivered by June of 2016. We expect to get first beam from SRF1 by 1st Q of 2017, and beam from SRF2 is expected in 2018. Purchasing components of laser station(s) will be started by next year and parallel to TARLA construction experiments with traditional laser sources will start by 2018 We expect to get first lasing by the end of 2019. 21

Conclusion Besides constructing TARLA, one of the scope of IAT is proposed to train people in accelerator related technologies We established first accelerator technogies post-graduate education program in our university.. Law for Research Infrastructure and legislations of related law has been published in July 2014 and September 2015, respectively. The objective is to define issues related to support to ensure a more effective use of research infrastructure and their sustainability. IAT is candidate to be a research center. To lead accelerator related projects in Turkey To establish proposed facilities of TAC To prepare accelerator based research infrastructure to the researches in our region. 22

Thanks for your attention!