cathi and the hie-isolde design study richard catherall isolde technical coordinator isolde users...
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CATHI and the HIE-ISOLDE Design Study
Richard CatherallISOLDE Technical Coordinator
ISOLDE Users Workshop15th – 17th December 2014
CATHI:Cryogenics, Accelerators and Targets for HIE-ISOLDE
HIE-ISOLDE PROJECT
High Energy
Upgrade
Design Study
CATHI
• A European funded Initial Training Network Program• 20 Marie Curie Fellows• A project within a project• Design Study
– Address the issues associated with an increase in p-beam intensity and energy– Investigate upgrades for an improvement in beam quality
Who was doing what?Marie Curie Fellow
Michal Czapski Pol Target material developments
Mathieu Augustin Fra HRS layout and magnet design, Off-line 2
Carla Babcock Can RFQ Cooler
Jacobo Montano Ven Target and Frontend Developments. Off-line 2
Serena Cimmino Ita Target design
Mario Hermann Ger Vacuum: RFQ Cooler, Dry pumps, Fast gate valves
Andrea Polato Ita Ventilation
Andrej Shornikov (ER) Rus EBIS upgrade
Leonel Morejon Cub Fluka Calculations
Martino Colciago Ita HRS Magnet controls
Martin Breitenfeld Ger HRS magnet design and MRTOF
Maddalena Maietta Ita Radioisotope propagation
Roger Barlow Eng HT modulator
Valentina Venturi Ita Beam dumps
Outline• Infrastructure
– Baseline Parameters– Beam dumps– Shielding– Vacuum– Ventilation
• Targets and FE– Target materials– Target design– Frontend– Off-line separator
• Beam quality– New RFQ Cooler– MR-TOF for ISOLDE– HRS Separator
• Magnet Design and layout
– EBIS electron gun
Base line parameters
• Linac 4– Linac 4 will be able to provide 5 x 1013 ppp = 1.25
x 1013/ring• Based on 40mA from the ion source
– Could possibly go beyond this value with a combination of different options
• Increase in source current output• An increase in pulse length• Chopping factor
– All need to be in place for testing
Protons/pulse Intensity(µA)
Energy(GeV)
Cycle(s)
Power(kW)
3.3x1013 2.2 1.4 1.2 3.1
1x1014 6.7 1.4 1.2 9.3
1x1014 6.7 2.0 1.2 13.3
Protons/pulse Intensity(µA)
Energy(GeV)
Cycle(s)
Power(kW)
5.0x1013 3.33 1.4 1.2 4.67
6.4x1013 4.3 1.4 1.2 6.0
1x1014 6.7 2.0 1.2 13.3
• Booster RF upgrade– CO2/CO4 upgrade would limit
protons to 1.4 x 1013/ring• Could be increased with a power
amplifier upgrade after LS2– Finemet upgrade (+MOSFET
amplifiers) = 2.5x1013/ring• Depends on the upgrade solution
chosen
Beam dumps
• Estimations made for different heat transfer coefficients• New design based on PSB design
Valentina Venturi
Shielding and activation
• Simulations and Design of further shielding
• Simulations for the implementation of extended target storage within the same building
Figure 5 : Views from the target storage geometry. Top 2D (left) and top 3D (right).
Figure 9 : Dose in µSv/h on target storage and surrounding areas. 108 stored targets situated in shelves next to opposite walls inside the storage as shown. View from top.
Leonel Morejon
Dry-pump stand and test
Substitution of normal, oil sealed pumps with dry pumps and pre-filtering before storage
Selective filtering between primary pump and dummy gas storage
Spectroscopy on filters in progress
M. Hermann, G. Vandoni
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VentilationPurpose of the airlocks:• Create a volume between Tunnel and Class A Laboratory in such a way to:
– Avoid activated air backflows from the Tunnel to the Class A Laboratory;– Prevent the Class A Laboratory evacuation in case of Tunnel ventilation stop (and vice versa);– Enhance a more flexible pressure regulation in the two buildings;
• Increase the leaktightness of the structure• Ventilation separation in progress
NOT FEASABLE
Andrea Polato
Progress on Infrastructure
• Supplementary shielding has already been installed…mainly to reduce radiation levels in neighbouring MEDICIS lab.
• Validation and implementation of extra storage will eliminate the need for unnecessary transport in the long term.
• Ventilation modifications are already in progress and will contribute to a reduction in activated air release as from next year.
• Still awaiting results on spectroscopy of filters from the dry pump tests.
• Beam dumps are a critical item for any increase in intensity and energy and should be upgraded during LS2 – 2018-2019.
Outline• Infrastructure
– Baseline Parameters– Beam dumps– Shielding– Vacuum– Ventilation
• Targets and FE– Target materials– Target design– Frontend– Off-line separator
• Beam quality– New RFQ Cooler– MR-TOF for ISOLDE– HRS Separator
• Magnet Design and layout
– EBIS electron gun
Study of prototype refractory ceramics (SiC and Al 2O3 ) with open unidirectional porosity
Michal Czapski
Uncouple container and heating functions
Ta container
Graphite heater
Graphite insulation
Graphite rigid connectors
Graphite flexible connectors
• Utilization of graphite pieces• Reduction of Tantalum weight 50%=> nuclear waste reduction
Serena Cimmino
Prototype
Thermocouple
• Insertion of a thermocouple between the heater and the container
=> Direct Temperature measurement (without calibration)
Serena Cimmino
Two stage extraction
For determining the optimum intermediate electrode configuration:• Thermal tests and simulations with ion
source @2000°C• HV insulation tests up to 5kV with
respect the ion source• Extraction efficiency measurements• Ionized air conductivity measurements• Acceleration gap pressure measurements
60 kV57 kVGround
Few geometrical parameters are studied in order to find an optimum electrode design:• Aperture• Acceleration gap• Tip shape
Jacobo Montano
Two stage extractionThermal characterization
Jacobo Montano
Charge pump modulator3. A new modulator concept
Advantages
• Modulation recovery time adjustable
• Requires a single low current high precision power supply (High power supply not necessary)
• A single HV switch is required (compared to C modulator which uses 3)
1) In this circuit a 400 nF buffer capacitor (C1) and the target capacitance (C2) are charged to 60 kV by a low power, high precision d.c. power supply (HVPS)
2) Immediately prior to beam impact the HVPS is disconnected from the target and the buffer capacitor using a 90 kV rated semiconductor switch (HV_Switch1). During beam impact the target capacitance is rapidly discharged to 54 kV. Then the buffer capacitor begins to re-establish voltage on the target to 99,4% of its initial value.
3) After 1 ms a feedback loop controlling an auxiliary high voltage amplifier is switch on and increases the buffer capacitor potential. This additional voltage brings the target voltage back to the required +/- 0.6 V tolerance within 5 ms.
4) Finally, when the target has recovered to a sufficient high impedance, the feedback loop is opened and the HVPS is re-connected to the target to maintain the stable 60 kV voltage.
Roger Barlow
Charge pump modulatorAssembly / Tank housing
• Custom built tank enclosure
• Tank is filled with dielectric oil
• Has a second ‘skin’ for oil leak protection
• Contains the modulator system, buffer capacitor bank, HV precision divider, static and dynamic load
Tank housingCapacitor bank0.05uF 75kVdc (hivoltcapacitors)
75kVdc high precision dividerVD75-20Y-BDSC-KC-BEA/PB/F (RossEngineering)
Viewing window
Essex HV connector
Oil temp gauge
Pressure sensor Oil filter
Filler cap
EAPPC2014: A charge-pump 60kV modulator for the ISOLDE target extraction voltage , R. A. Barlow1, B. Bleus1, A. Fowler*1, H. Gaudillet1, T. Gharsa1, J. Schipper1
1800mm
Roger Barlow
Off-Line separator 2
• Built and operated in B.275 earlier this year• Now being moved to B.3• To be used for FE modification tests, beam optics for RFQ Cooler, new
magnet design tests…• Can also be used for target production/prototype testing
M. Augustin, J. Montano
Progress on target and FE• Post-irradiation analyses is required of the remaining irradiated
samples• Graphite heat shields need to be tested further but show promising
results already– Step in the right direction uniform heat distribution and for waste
treatment• Further testing required for the two-stage extraction
– However any modifications incur:• Modifications of the FE’s (LS2 during their replacement?)• Amendments to the target production contract• Modifications to OL separators and production protocol
• HT modulator design looks promising. Implementation could be in 2016/2017– Note that new HT power supplies (compatible with the modulator design)
will be delivered in October 2015
Outline• Infrastructure
– Baseline Parameters– Beam dumps– Shielding– Vacuum– Ventilation
• Targets and FE– Target materials– Target design– Frontend– Off-line separator
• Beam quality– New RFQ Cooler– MR-TOF for ISOLDE– HRS Separator
• Magnet Design and layout
– EBIS electron gun
RFQ Cooler1. Alignment
– Internal and external alignment possibilities and done externally
2. Pressure monitoring– Possibility to measure gas pressure inside
the electrodes– Modification of conductance
3. Mechanical and electrical design– Investigating mechanical support to
maintain electrodes in place– Improved wiring and insulation to avoid
short-circuits
4. Laser pumping1. Modification of apertures to allow lasers
to interact with ions in the bunched region
Carla Babcock
MR-TOF for ISOLDE
Can it replace a magnetic separator? • Surely not with state of the art, too small
current: • 1000 ions per cycle (~4ms for
RFWHM=20000) • 3e5 ions per 1.2s, but usually a huge
fraction is contamination!
But the performance could be improved: • Higher energy inside the MR-ToF • Bigger device to reduce density • Investigations are still ongoing to improve
throughput
Ion-beam composition analysis • direct feedback for target/line
optimization • sampling of release curve possible • single ion sensitivity to detect
lowest yields • no upper limit on half-life as with
decay station • not hindered by decay branching
ratio
Martin Breitenfeld
HRS Separator LayoutBeam emittance ε=3π.mm.mrad R = 20 000for more than 99% transmission of pure beam R ~ 23 000 for 90% transmission of pure beam
Mathieu Augustin
New Magnet Design
Schematic view in cross section of the new HRS magnet (H-type), and partial view in 3D, featuring the pole face windings technology (picture credit to M. Breitenfeldt)
• H type magnet, mechanically more stable, possibility of better pole face machining • Yoke made of laminated steel reduction of eddy currents, allowing an increase in cycling
speed (~1min VS 15min) • Poleface windings allow the adjustment of the magnetic field along the beam axis.
Martin Breitenfeld, Mathieu Augustin
Beam Quality Summary• The new RFQ Cooler is (almost) built
– To be coupled to the Off-Line 2 for testing and characterization with beam• MR-TOF is a promising tool for both experiments requiring high
resolution and target characterization– Already discussed in the ISCC but WG required to further pursue design
and integration• Could well be an out-of-beam device
• HRS: A long way from being implemented– New magnet design looks very promising– Would like to see a 90 deg “compact version” built and tested on Off-line
2 as a pre-requisite to any further decisions• REXEBIS developments should be strongly encouraged
– For HIE-ISOLDE and for possibly the TSR.
CATHI Final Review
• Held on 22nd to 26th September in Barcelona• Wrap-up of all the HIE-ISOLDE – CATHI activities• https://indico.cern.ch/event/316392/page/5• The CATHI Fellows have made excellent
contributions to the HIE-ISOLDE project• They will be missed!
Spare Slides
Target simulations• The use of borated polyethelyne to reduce activation
Figure 11 : Views 3D of the target wrapped ina borated polyethylene box of 10-30 cm thickness.
|Table 1 : Values of activity of the air for the cases when the target is at GPS and when it is at HRS. Wrapped and Unwrapped stand for the case when the target is not covered by the polyethylene and when it is respectively. The values are normalized to a proton (ppp: per primary particle)
• The research leading to these results has received funding from the European Commission under the FP7-PEOPLE-2010-ITN project CATHI (Marie Curie Actions - ITN). Grant agreement no PITN-GA-2010-264330.
On-line Sampling :• Realized along the primary pumping system, with active carbon and
cellulose filters installed downstream of the turbomolecular pumps;
• Spectroscopy Analysis.
Use of a tape station to• analyze ACTIVITY and evaluate the TIME OF
FLIGHT of different gas species (spectroscopy);
• TEST the accuracy of Monte Carlo model (time dependent mode).
Sampling and measurement of radioactive species
Maddalena Maietta M. Hermann, G. Vandoni
Cold Line Study…
• Additional 4th cooled finger assembled by EB welding
• Cooled line screwed on it• Thermal contact by pressure
Actual design Proposed design
=> This solution has still to be tested and validated by a prototype
Serena Cimmino
Two stage extractionExtraction optics
Particle tracking (second gap)
The low energy first extraction produces large beams. The second gap focalizes the beam
Jacobo Montano
3. Charge pump modulatorHardware assembly
• C modulator topology / Charge pump topology (Reconfigurable prototype)
• Design can support up to 3 (90kV) Belkhe switches
• Structure all Vetronite • Static charge for ‘on-board’ testing• Compact design
HV supplies/Amplifier
Signal feedtroughs
HV switch
Diode
Hall effect
CTStatic charge
Roger Barlow
ISOLDE Beam DumpsOption 2
• Replace existing beam dumps• Advantages
– Low dose rate for installation– Take advantage to improve shielding (see next slides)– Reduction in air activation through new design
• Disadvantages– Removal, storage and replacement of ~3500m3 of earth,
about half of which is activated.– Handling and storage of radioactive beam dump– Still require cooling and its associated disadvantages
ISOLDE Beam Dumps Option 1
• Insert a PSB like water-cooled beam dump in front of existing beam dumps.– Advantages:
• Cheaper option• Based on known design• “easier” access
– Disadvantages• Implementation and maintenance of a cooling system
– Activated water
• Contribution to target area air activation and consequent release to atmosphere.
• High dose rate for installation
Shielding
• Further shielding required to attenuate dose rates observed during operation and under certain conditions:– 2uA of p-beam on thick ISOLDE targets (>50gcm-2)– Identified by RP in https://edms.cern.ch/document/1142606/1
CERN-DGS-2010-006-RP-SN– Impact of p-beam intensity and energy increase on radiation
dose rates outside the CERN perimeter to be assessed• Can be combined with an upgrade of the ISOLDE beam
dumps• Requires major excavation work of activated earth
Shielding
39
REX-EBIS: Electron Beam Ion Source for HIE-ISOLDE
Design values for EBIS (HIE-ISOLDE/TSR@ISOLDE application ) / available now with REXEBIS
Electron energy [kV] 150 / 5
Electron current [A] 2-5 / 0.2
Electron current density [A/cm2] 1-2x104 / 100
New EBIS – High Energy Compression and Current (HEC2) EBIS
Main challenge – produce the high compression electron beam
Goal – have a reliable design of the HEC2 electron gun on earliest possible stage
Priorities and the goal setting
Realization – in a joint effort with BNL, based on BNL design and infrastructure (BNL Test-EBIS), funded and manned by CERN
See presentation by A. Shornikov