Latest Developments at Daresbury Laboratory · Edinburgh, Scotland . Chilbolton Observatory ....
Transcript of Latest Developments at Daresbury Laboratory · Edinburgh, Scotland . Chilbolton Observatory ....
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Latest Developments at Daresbury Laboratory
Joe Herbert Vacuum Science Group Leader
- Daresbury Laboratory
OLAV IV April 1 – 4, 2014 – NSRRC, Hsinchu, Taiwan
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Outline •Introduction (STFC; Cockcroft Institute; ASTeC)
•Activities of ASTeC (main accelerator projects) •ALICE; EMMA •VELA/CLARA •UK FEL •ELI-NP-GB
•ASTeC Vacuum Science Group R&D Highlights (general description) •NEG Coatings •SRF Coatings •SEY Studies •Photocathode development
•Topics to address during OLAV
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Science and Technology Facilities Council
One of Europe’s largest multi-disciplinary
scientific research organisations
~£600 million
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Joint Astronomy Centre Hawaii
Isaac Newton Group of Telescopes
La Palma Isaac Newton Group of Telescopes La Palma
UK Astronomy Technology Centre Edinburgh, Scotland
Chilbolton Observatory Stockbridge, Hampshire
Rutherford Appleton Laboratory Harwell Science and Innovation Campus Didcot, Oxfordshire
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ALICE & EMMA
ASTeC & Cockcroft Institute
Old SRS Facility
VELA (CLARA)
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“Its purpose is to research, design and develop particle accelerators, machines that can be used to reveal the nature of matter, to probe what happened at the instant the universe was born and to develop new materials and medicines to improve our quality of life.” – Swapan Chattopadhay (Director CI)
Significant increase in Activity in Accelerator Science and Technology in the UK (e.g. No’s of students)
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Background
Centre of excellence with a flexible skill base. Play strategic role in shaping accelerator based projects in the UK (Internationally).
SRS 2001
20 Staff (now 50 + 15) RF (& Cryo) Vacuum (SS & MS) Magnets (Rad.S) Acc. Phys. Intense Beams (Lasers & Diagnostics)
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ALICE & EMMA – Test Facilities (2003)
IR FEL
EMMA – FFAG
Photoinjector Laser Energy Recovery LINAC
Super Conducting RF
Beam Dump
THz Dipole Chicane
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ALICE
• Grant to fund science using IRFEL & THz through Liverpool University. (Cancer)
• Demonstrate 20 um FEL output to enhance future funding opportunities.
• Use as a training facility for staff/students, e.g. LHeC test facility.
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EMMA
• Understanding non-scaling FFAG
• Explore potential uses/applications (e.g. protons, muon accelerator, compact accelerators)
• Physics – Verify effects of resonance crossing.
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VELA (Versatile Electron Linear Accelerator)
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VELA – The Facility
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VELA Beam Energy 4 - 6 MeV Bunch Charge 10 - 250 pC Bunch length (σt,rms) 1 - 10 ps Normalised emittance
1 - 4 µm
Beam size (σx,y,rms) 1 - 5 mm Energy spread (σe,rms) 1 - 5 %
Bunch repetition rate
1 - 10 Hz (with ALPHA-X gun) 1 - 400 Hz (with high rep. rate gun in the future; klystron and laser specified for 400 Hz)
£2.5 million capital investment from UK government Projects with clear IMPACT (Economic) Applications in Medicine; Health; Security; Energy Allow development of new accelerator technologies specifically through partnership with Industry. Industrial and Scientific support Required VELA, it is hoped will form the injector for CLARA (Compact Linear Advanced Research Accelerator) – Next generation particle accelerators.
Beam Energy 250 MeV Undulator Minimum
Gap 6 mm
Undulator Period 29 mm FEL Wavelength 400 – 100 nm Bunch Charge 20 – 250 pC Normalised Emittance 0.2 – 2.0 mm-mrad Seed Sources 800 nm TiSa + Mid-IR
OPA + 100 nm HHG Afterburners 50 nm Novel
Technology
CLARA
S-band RF Gun (2 ½ Cell) developed for the ALPHA-X laser-wakefield accelerator. Photoinjector uses a Cu photocathode Laser source – 400Hz amplified Ti:S laser at 800nm. Peak Intensity ~1 TW/cm^2
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VELA – Industrial Interest Novel security scanning techniques
Performance testing of components for RF power delivery
Testing of novel beam position monitors
Evaluation of beam diagnostic technologies
Testing and evaluation of beam stabilisation equipment
Applications in using electron beams for industrial processes (Health & Environment e.g. Water Purification)
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Shie
ld W
all
Shield Wall
Shield Wall
Electron Beam Test Facility
2m
4m
6mSh
ield
Wall
Shie
ld W
all
0m 10m
Gun
4m 6m2m 8m 12m
2.5 cell, S – band RF π-mode SWCu photocathode100 MV/m peak6 MeV
14m 16m 18m
Load – locksystem
Beam stay clear increase from φ34 mm to φ100 mm
Beam stay clear From ICT1 to YAG11minimum φ34 mm
Beam stay clearminimum φ34 mm
BPM 8 : Mechanics in placeCan be instrumented later.
~1m space required for cavity BPMsThree in a row, each with ~30 cm (Information from S. Boogert)
LaserRoom
SynchronisationRoom
NEG
Vacuum baked section
Beam stay clearminimum φ34 mm
NEG
Optical Table
Vacuum Pressure Zone 2
Vacuum Pressure Zone 1
Sputter Ion Pump (SIP)
NEG Pump
Pneumatic All metal gate valve
Inverted Magnetron Gauge (IMG)
Pirani Gauge (PIRG)
Residual Gas Analyser (RGA
Pumping Port
Key for Vacuum Symbols:
NEG
EBT-
INJ-MA
G-DI
P-01
EBT-
INJ-MA
G-QU
AD-0
1
EBT-
INJ-MA
G-QU
AD-0
2
EBT-
INJ-MA
G-QU
AD-0
3
EBT-
INJ-MA
G-QU
AD-0
4
EBT-
INJ-MA
G-QU
AD-0
7
EBT-
INJ-MA
G-QU
AD-0
8
Tran
sver
se D
efle
ctin
g Ca
vity
S -b
and
EBT-
INJ-VA
C-VA
LV-0
1
EBT-
INJ-MA
G-HC
OR-0
2/VCOR
-02
EBT-
INJ-DI
A-WC
M-01
EBT-
INJ-DI
A-HB
PM-0
1/VBPM
-01
EBT-
INJ-DI
A-YA
G-01
EBT-
INJ-MA
G-HC
OR-0
1/VCOR
-10
EBT-
INJ-MA
G-BS
OL-0
1
EBT-
INJ-MA
G-SO
L-01
EBT-
INJ-DI
A-HB
PM-0
2/VBPM
-02
EBT-
INJ-DI
A-YA
G-03
EBT-
INJ-MA
G-HC
OR-0
6/VCOR
-06
EBT-
INJ-DI
A-YA
G-05
EBT-
INJ-MA
G-HC
OR-0
4/VCOR
-04
EBT -
INJ-MA
G-HC
OR-0
3/VCOR
-03
EBT-
INJ-DI
A-YA
G-02
EBT-
INJ-VA
C-VA
LV-0
2
EBT-
INJ-MA
G-DI
P-02
EBT-
INJ-MA
G-QU
AD-1
1
EBT-
INJ-MA
G-QU
AD-1
5
EBT-
INJ-DI
A-IC
T-01
EBT-
INJ-DI
A-HB
PM-0
4/VBPM
-04
EBT-
INJ-MA
G-HC
OR-0
8/VCOR
-08
EBT-
INJ-DI
A-HB
PM-0
5/VBPM
-05
EBT-
INJ-DI
A-YA
G-08
Win
dow
EBT-
BA1-DI
A-HB
PM-0
1/VBPM
-01
EBT-
BA1-DI
A-YA
G-01
EBT-
INJ-MA
G-QU
AD-0
9
EBT-
INJ-MA
G-QU
AD-1
0
EBT-
INJ-DI
A-YA
G-06
EBT -
INJ-MA
G-HC
OR-0
7/VCOR
-07
EBT-
INJ-DI
A-YA
G-07
EBT-
INJ-MA
G-HC
OR-0
9/VCOR
-09
EBT-
INJ-VA
C-SH
UT-0
3
Tem
pora
ry V
alve
Loc
atio
n
EBT-
BA1-VA
C-VA
LV-0
1
EBT-
INJ-DI
A-IC
T-03
EBT-
INJ-DI
A-BA
M-01
LC T
est B
PM
EBT-
INJ-VA
C-SH
UT-0
2
EBT-INJ-MAG-QUAD-13
EBT-INJ-MAG-QUAD-14
EBT-INJ-DIA-YAG-09
EBT-INJ-MAG-VCOR-11
EBT-INJ-VAC-SHUT-01
EBT-BA2-DIA-YAG-01
EBT-BA2-DIA-HBPM-01/VBPM-01
EBT-BA2-VAC-VALV-01
EBT-INJ-DIA-ICT-02
EBT-INJ-DIA-HBPM-06/VBPM-06
Window
EBT-INJ-VAC-IONP-01
EBT-INJ-VAC-NEG-01
EBT-INJ-VAC-IMG-01
EBT-INJ-VAC-PIRG-01
EBT-INJ-VAC-RGA-01
EBT-INJ-VAC-IONP-03
EBT-INJ-VAC-IONP-04
EBT-INJ-VAC-IONP-05
EBT-INJ-VAC-NEG-02
EBT-INJ-VAC-IMG-02
EBT-INJ-VAC-PIRG-02
EBT-INJ-VAC-RGA-02
EBT-BA1-VAC-IONP-01
EBT-BA1-VAC-IMG-01
EBT-BA1-VAC-PIRG-01
EBT-BA1-VAC-RGA-01
EBT-BA2-VAC-IONP-01
EBT-BA2-VAC-IMG-01
EBT-BA2-VAC-PIRG-01
EBT-BA2-VAC-RGA-01
EBT-INJ-VAC-IONP-06
EBT-INJ-VAC-IONP-07
EBT-INJ-VAC-IONP-08
EBT-INJ-VAC-IONP-09
EBT-INJ-VAC-IONP-10
EBT-INJ-VAC-IONP-11
EBT-INJ-VAC-IMG-03
EBT-INJ-VAC-PIRG-03
EBT-INJ-VAC-RGA-03
EBT-INJ-VAC-IMG-04
EBT-INJ-VAC-PIRG-04
EBT-INJ-VAC-RGA-04
EBT-INJ-VAC-IMG-05
EBT-INJ-VAC-PIRG-05
EBT-INJ-VAC-RGA-05
EBT-INJ-VAC-IMG-06
EBT-INJ-VAC-PIRG-06
EBT-INJ-VAC-RGA-06
EBT-INJ-VAC-IONP-02
VELA - Schematic
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VELA - Layout
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Laser Transport Path – Differential Pumping System
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VELA - Vacuum Requirements
• 1 x 10-10 mbar in the RF photoinjector • 5 x 10-8 mbar in the remainder of the beam transport path
• ~10-6 mbar in the laser transport system
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CLARA
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Why CLARA?
Dedicated Flexible FEL test facility Demonstrate advanced FEL concepts
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Operating Modes
Parameter Seeding SASE Ultra-short Multibunch
Max Energy (MeV) 250 250 250 250 Macropulse Rep Rate (Hz) 1–100 1–100 1–100 1–100 Bunches/macropulse 1 1 1 16 Bunch Charge (pC) 250 250 20–100 25 Peak Current (A) Bunch length (fs)
125–400 850–250 (flat-top)
400 250 (rms)
∼1000 <25 (rms)
25 300 (rms)
Norm. Emittance (mm-mrad) rms Energy Spread (keV)
≤ 1 25
≤ 1 100
≤ 1 150
≤ 1 100
Radiator Period (mm) 27 27 27 27
CLARA CDR Parameters
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UK FEL - ? (4GLS/NLS….)
• Next large scale user facility for the UK? • Significant prototyping required – CLARA • Many possible options:-
– Hard X-rays at low rep rate – Soft X-rays at high rep rate – OR a combination (multiple source)
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3x Basic Accelerator Technologies
CW Superconducting RF (equi-spaced e- pulses)
Pulsed superconducting RF (non equi-spaced e- pulses, “burst mode”)
Normal conducting RF (equi-spaced e- pulses)
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• There are many possibilities. • Need input from the UK FEL user community on priorities.
Key parameters determining technology and cost are: – maximum photon energy – energy per pulse – repetition rate – regularly spaced pulses or burst mode and also: – number of FELs – tuneability (energy range of each FEL) – fixed/variable polarization – attosecond schemes – seeding schemes Choice of technology will also determine how much R&D is needed and hence overall timescales …
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Possible Target Parameters ? • Energy ~ 8.7 GeV • Peak photon energy ~ 18.6 keV • Gap tuneable e.g. ~ 5.5 -16.5 keV • Repetition rate ~ 100 Hz • Initial no. of FELs ~ 2 • Possible no. of FELs ~ 4+ • Length ~ 840 m • Power ~ 6.6 MW • Cost < £450m
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Extreme Light Infrastructure (ELI)
Nuclear Physics (NP)
Gamma Beam (GB)
3x Co-ordinated ELI projects – Hungary (ELI – Attosecond), Czech Republic (ELI – Beamlines) and Romania (& perhaps more to come?).
ELI-NP-GB
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Gamma Beam System
700 MeV high brightness e- beam, scatter intense high power optical laser photons into energetic gamma ray photons 2-20 MeV – Very High Quality Gamma Beams
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Roof & Crane support steel columns
33 ELI-NP-GS Overall Accelerator & Building Layout – 3D
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BPM 2 Screen 2
Ion pump
RF Acc. Structure S-band 2
(Solenoid omitted)
RF Acc. Structure C-band 1
M1 M2
M3
M4
M5
C2 C3
RF Acc. Structure S-band 1
RF Gun
Corrector 1
RF Acc. Structure S-band 1
RF Acc. Structure S-band 2
RF Acc. Structure C-band 1
QUA 01,2,3-C
SPECT-C Dipole Dump 1
M2 M3 M4 M5 Corrector 2
Laser
Solenoid coils
M1 Screen 6
Ion Pump
RF Acc. Structure C2
RF Acc. Structure C3
BPM 4 Screen 4
Ion pump
Solenoid coils
RF Gun
Screen 1 Ion pump
Current monitor 1
Corrector 3, 4 Corrector 5
Vacuum valve 2
Vacuum valve 1
BPM 3 Screen 3
Ion pump Corrector 6
BPM 5 Screen 5 Ion pump
BPM6 Ion pump
Transverse Deflecting
Cavity 1
Screen 7 Ion pump
BPM 1
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Vacuum Science Group Programmes Major Work Programmes
Novel Coatings including NEG Photoinjector development SRF – Coatings SEY – Measurements (inc. morphology and surface structure effects on SEY) Vacuum System Design
Underpinning Activities Characterisation of materials for vacuum (Outgassing/Surface Analysis) Gauge Calibration (TPG & RGA/QMS) Pump Speed Measurements Cleaning/Processing Developments for UHV/XHV
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NEG Developing Coating Techniques
Planar, Tubular, Complex shapes Magnetron Sputtering (PVD) Twisted wire & Alloy Wire (target for coating) CVD (plasma assisted)
Studying properties of films with different compositions. Using Ti; Zr; V; Hf (comparison of ternary and quaternary films) Using additional barrier layers e.g. Dense Aluminium, Nitrides Developing low SEY coatings e.g TiN, DLC. Reducing Activation Temperature (extends range of materials,
reduces energy consumption)
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Development of Photoinjector for ALICE (complete)
Conceptual design of photoinjector for NLS/UK-FEL (complete)
Design/build upgrade ALICE gun to include load-lock wafer transfer and offline cathode activation. (Complete)
Understanding the requirements for XHV for GaAs cathode operation and the techniques to achieve XHV. (Complete)
Investigation of various cathode materials (Copper, GaAs; alkali metals) (Ongoing)
Investigating activation procedures/techniques (including fundamental understanding of surface properties) (Ongoing)
Photoinjectors
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Loading chamber
Preparation chamber Surface analysis chamber
Cleaning chamber
RGA
Hydrogen cracker source
Hemispherical analyser for XPS
X-ray source
Caesium dispenser
LEED
Used to investigate surface properties of wafers under different conditions
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XPS spectra of the GaAs for (a) un-cleaned sample, (b) after heating to 550° C and (c) after depositing Cs and O layers.
O1s
OKLL
Cs3d5
Cs3d3 CsMNN
Ga2p1 Ga2p3
As2p3
As2p1
(a)
(b)
(c)
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3-Stage Loadlock Vacuum & Transfer Wafer Replacement System Wafer replacement time reduced from ~1 month to ~30 min
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Metal Photocathodes - Highlights
• Surface preparation of variety metal photocathodes to be used in an RF Gun ( Cu, Ag, Mg, Ti, Pb, Zr, Nb).
• Determination of QE, Work Function and Transverse Energy Spread for different Bulk metals ( single crystal and polycrystalline) and thin metal film as a function of surface preparation, surface chemical state and residual gas absorbate.
• Theoretical modelling of photoemission and validation of calculations using experimental data.
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Surface Science Facilities
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SRF Thin Films- Highlights • PVD and ALD deposition of SRF thin film ( Nb, NbN and
NbNC) on flat surfaces and 3D structures.
• Study of SRF properties and Microstructure of the film as function of deposition parameters.
• Study of Superconducting properties of these films such as RRR, Hc, AC susceptibility.
• More than 40 Nb samples with RRR ranging from 3 to 30 has been deposited so far.
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SRF-Films
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Last 2 slides - OLAV IV
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OLAV IV
• ELI – NP Project – Ion Pump PSU as TPG – Experience with VACOM, EVAC and Slotted
CF flanges (where space is restricted) – Contamination risk from mobile vacuum
diagnostic systems (rather than permanent) – Extended Warranty Options (vacuum
equipment)
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Special Issue ‘VACUUM’ –OLAV? • Oleg Malyshev (ASTeC)
– Associate editor of journal ‘Vacuum’ – Tasked specifically to develop ‘Special Issues’. – Suggested Topic - OLAV – Literature doesn’t contain Operational Wisdom. – Is there a desire to document significant
learning/experience/wisdom? – A few volunteers to coordinate articles (perhaps
3 - US, Asia, Europe)
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ASTeC activation procedure
O.B. Malyshev, K.J. Middleman, J.S. Colligon and R. Valizadeh. J. Vac. Sci. Technol. A 27 (2009), p. 321.