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Title: Alessandro Variola


1
ESGARD OMNIA Meeting10/09/2007
  • JRA
  • Polarised Positron Sources

2
Polarised Positron Sources
  • Framework Future lepton colliders need positron
    sources !!!
  • The important requirements in peak currents imply
    extremely high performances that are much more
    demanding
  • SLC 0.6 mA - 4 kW deposited in the target
  • LEP (LIL) 3 mA - 0.6 kW deposited in the
    target ILC 40 mA -
    5 kW deposited in the target
  • DAFNE 2 mA - 0.5 kW deposited in the target
    ILC (conventional) gt
    28 kW
  • KEKB 0.5 mA - 2 kW deposited in the target
    CLIC new 10 mA gt
    Conventional 16 kW
  • LAL 0.8 mA - 0.8 kW deposited in the target
  • Positron source performances lt electron sources
    Many parameters of the collider (also in the
    electron arm) are imposed by the quality of the
    positron source !!
  • Positron production efficiency e electron
    driver e conversion e capture need for
    extremely performing electron beams, high thermal
    dissipation in converters, optimised capture
    section (linked with the whole machine)
  • Physics case for polarised positrons already
    illustrated (see for example Moortgat-Pick, G. et
    al The role of polarized positrons and
    electrons in revealing fundamental interactions
    at the Linear Collider. ArXiv High Energy Physics
    - Phenomenology e-prints arXivhep-ph/0507011).
  • Advantage of polarised positron source vs
    conventional pair creation in the converter
    only by high energy gammas. No charged particles.
    Thermal constraints strongly reduced.
  • Disadvantage need for a lot of gammas.and RD
    too
  • Most components of the colliders project are
    based on established technologies (need for D
    only). Polarised positron sources imply
    completely innovative schemes (undulators at 150
    GeV, Compton scattering _at_ 1-2 GeV with MW class
    optical devices) that need important RD programs
    to be validated.
  • I hope that I managed to convince you that
    positron sources are critical for future lepton
    colliders projects and that polarised is better !!

3
Two main lepton collider projectsCLIC ILCAnd
two different techniques to produce polarised
positrons Undulator and Compton
CLIC 2007 (3 TeV) ILC (Nominal)
Energy E GeV 9 150
Bunch population N 109 4 - 4.1 20
Nb bunches / train nb - 311 2625
Bunch spacing Dtb ns 0.667 (8 RF periods) 369.2
Train length tpulse ns 207 968625
Emittances gex , gey nm, nm.rad 600, 10 8400, 24
rms bunch length sz mm 43 - 45 300
rms energy spread sE 1.5 - 2 1.5
Repetition frequency frep Hz 50 5
Beam power P kW 91 130
ILC (Already in EDR phase) Baseline solution
undulator Alternative Solution
Compton CLIC Preferred solution
Compton Analysed Solution Undulator
Both schemes are based on a drive high energy
beam (undulator 150 GeV Compton 1-2 GeV)
producing the gammas. These are
subsequently converted in polarised pairs in a
spinning target
4
Critical aspects JRA for Polarised positron
sources
  • Undulator Comptongt Instantaneous Energy
    deposition. Heating Target technology
  • Undulator Length gt Prototype of new materials SC
    undulator. Higher B field
  • Undulator mass production
  • Compton High power, high frep fiber laser
  • CW warm cavity for the capture section thermal
    dissipation
  • Polarimetry and polarisation transport
  • This JRA aims at solving these issues, at least
    the most important ones on this list (or even
    betterall of them).

5
ESGARD feedback and present situation
  • 1st Proposal presented on Compton Sources
  • 2nd phase join also of the Undulator request. A
    big effort was spent in integrate the different
    activities.
  • Feedback from the Directors meeting to be
    postponed (or fully included in Optional
    activities)
  • Also if in Optional activities strong budget
    reduction requested (4.1 M total _at_ 33 refunding)
  • We find unfair both decisions and
  • We try to convince the community that the program
    is indispensable
  • We will present our Priority (4.1 MEuros) and
    Option (1.5 MEuros) activities. We feel that,
    since we have already been penalised once (fully
    optional), the budget cut is not justified
    compared with other programs that have maintained
    a fraction of CORE activities. In the case that
    we will still remain in the Optional we want to
    go with our 5.6 MEuros Program.
  • It is difficult for us to set up a clear scenario
    (JRA/WP) since it depends on the decision on
    funds availability

6
JRA WP0 Management
  • Managing the JRA program, work, reports and
    milestones
  • Coordinate the communication between different
    institutes
  • Ensuring the communication with the FP7 IA
    management and with the EU representatives.

7
JRA WP1
  • Priority
  • Develop a high-power fiber laser and its
    associated digital feedback to be locked on a
    Fabry Perot resonator 564.500 (EU-funded). On a
    basis of the 33 EU refunding the total cost is
    1,693,500 .
  • The expected outcomes are to develop a 200W
    continuous pulsed laser (Min. repetition
    frequency 40 MHz) and to lock it to a Fabry Perot
    cavity (Min. finesse 10000). This system should
    subsequently be installed in an accelerator
    complex (ATF/FLASH/CTF3/DAFNE Linac/ERLP) to test
    the gamma/x production.
  • Participating labs LAL Orsay, IPN Lyon, LNF
    Frascati

8
JRA WP2
  • Priority
  • Develop prototype of ILC positron source target
    consisting of a rapidly spinning wheel of
    titanium alloy in a strong magnetic field, with
    integral water cooling. Demonstrate mechanical
    stability under strong eddy current braking,
    reliability, and thermal control. The prototype
    would be developed jointly by STFC and University
    of Liverpool at Daresbury Laboratory.
  • Cost to EU 420,000 with matching funds of
    1,310,000 giving a total cost of 1730,000 .
  • Participating labs Liverpool, Daresbury
    Laboratory

UK Resources from STFC (LCABD, CI,
ASTeC) Approved by UK Project Manager, CI
Director, ASTeC Director
9
JRA WP3
  • Priority
  • Develop short undulator prototype (40 cm) using
    more advanced materials (eg Nb3Sn) with the goal
    of generating significantly higher on-axis
    magetic fields and so reducing the overall length
    of the full ILC undulator by several tens of
    metres.
  • Cost to EU 180.000 with matching funds of
    970,000 giving a total cost of 1,150,000 .
  • Participating labs Daresbury Laboratory, RAL

UK Resources from STFC (LCABD, CI,
ASTeC) Approved by UK Project Manager, CI
Director, ASTeC Director
10
JRA WP4
  • Priority
  • Polarization studies for alternative
    helicity-flipping schemes
  • Spin tracking through targets (including magnetic
    and electric fields) and capture section
  • Polarization studies on possible systematic
    uncertainties in the machine design
  • Theoretical uncertainties from higher order
    corrections including spin effects
  • Construction and test of a prototype for a low
    energy positron polarimeter (Bhabha polarimeter).
    It will be developed and tested jointly by DESY,
    Humboldt University, Tel Aviv University and
    NCPHEP Minsk
  • Cost to EU 200,000 with matching funds of
    400,000 giving a total cost of 600,000 .
  • Participating labs DESY, IPPP Durham, Humboldt
    University Berlin, Liverpool (?)

11
JRA WP5
  • Option
  • Design and construction of a CW RF warm cavity
    with high gradient (100 kW dissipation). Study
    prototyping 250,000 (EU Funded) gt Total cost
    750,000 .
  • This cavity is needed in the capture section
    since after the target and in a strong solenoidal
    field we cannot envisage the use of a SC CW
    cavity. The expected outcomes are to design and
    realise a CW warm cavity (frequency ranging from
    600 to 1500 MHz) with a gradient higher than 1.5
    MeV/m with 100 kW max dissipation. The cavity
    will be tested in (DAFNE/ATF).
  • Participating labs LAL Orsay, IPN Lyon, LNF
    Frascati

UK Resources from STFC (LCABD, CI,
ASTeC) Approved by UK Project Manager, CI
Director, ASTeC Director
12
JRA WP6
  • Option
  • For the ILC approximately fifty undulator modules
    will be required. It is essential that the
    present design is taken forward to a position
    where a contract can be placed with an industrial
    partner for this large quantity. The undulator
    concept will be value-engineered and the revised
    design prototyped and tested.
  • Cost to EU 250,000 with matching funds of
    500,000 giving a total cost of 750,000 .
  • Participating labs Daresbury Laboratory, RAL

13
At present (hoping in positive evolutions)
  • JRA Priority Activities

  • EU funding request Total
  • -WP1 fiber laser
    564000 1693000
  • -WP2 converter target prototype
    420000 1730000
  • -WP3 undulator prototype
    180000 1150000
  • -WP4 polarisation studies
    200000 600000

  • 1364000 5173000
  • JRA Option Activities
  • -WP5 CW cavity
    250000 750000
  • -WP6 undulator engineering 250000
    750000

  • 500000 1500000
  • TOTAL gt
    1864000 6673000

14
Commitments of the funding agencies
  • LAL-IN2P3 CNRS 4.6 FTE/year 4 Years. Approved
    by LAL Director
  • IPN Lyon 0,5 FTE/year 4 Years (TBC)
  • INFN 0,5 FTE/year 2 Years (TBC)
  • LCABD (UK) UK Resources from STFC (LCABD, CI,
    ASTeC)
  • Approved by UK Project Manager, CI Director,
    ASTeC Director
  • STFC 3 FTEs/year 4 years
  • U of Liverpool 2 FTEs /year 4 Years
  • DESY 1FTE /year 4 years (tbc)
  • Durham 0.1 FTE /year, TBA

15
Apart form the colliders program medical and
industrial fallout
  • Compton
  • Low energy Compton scattering application by
    the others gt
  • in the static and dynamic imaging (like 3D
    compressionless mammography and broncography),
  • In K-edge radiography and therapy and in the
    catheterless coronary arteries angiography
  • gadolinium based cancer therapy and blood imaging
    .
  • x-ray diffraction protein crystallography
  • The possibility to identify the atomic number of
    different materials with hard x rays open the
    way also for nuclear application of the Compton
    scattering.
  • High penetration photons are also suitable for
    security and aerospace applications like for
    example the radiography of shielded material
    investigating the presence for small quantities
    of a particular nuclei.
  • Undulator
  • Knowledge exchange with industrial partner will
    enhance superconducting magnet manufacturing
    within EU
  • Superconducting undulators could have major
    impact on all light sources and FELs

16
Conclusions
  • Positron sources are one of the most critical
    issues for the future generation of lepton
    colliders
  • An international community is working to give an
    answer to the most delicate aspects
  • We planned to suggest a JRA to have the
    possibility to develop, in this framework,
    important advancements.
  • Work is essentially based on Undulator, Laser and
    Target tech.
  • We estimate to have been penalised twice. 1)
    Optional activities 2) budget cut.
  • We are asking to get back into the game trying to
    take into account as much as possible the
    suggested work plan
  • In principle we would like to be considered at
    least in the Priority activity. Also the
    Option activities are important for the
    completeness of the program.

17
  • Thanks to all the collaborators that provide
    material for this presentation
  • Thank you for your attention
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