The Genesis of the LCLS

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The Genesis of the LCLS

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... the first X-ray free-electron laser (X-FEL), in the wavelength range 1.5 to 15 ngstrom, ... while reducing the bunch length to the sub-picosecond range. – PowerPoint PPT presentation

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Title: The Genesis of the LCLS


1
The Genesis of the LCLS
  • Herman Winick
  • SLAC National Accelerator Laboratory
  • Presented at
  • ICFA Workshop on Future Light Sources (FLS2012)
  • Newport News VA
  • March 8, 2012

Draft Mar. 6, 2012 2pm
2
The history of X-ray free-electron lasers. C.
Pellegrini, UCLA
  • Dear Colleagues, Feb. 27, 2012
  •  
  • I am sending you a link to read or download a
    paper that I have recently written and is in
    course of publication in European Physical
    Journal H (EPJH, Historical perspective on
    Contemporary Physics).
  •  
  • The file is too large to be attached to this
    message because of the many figures. I hope you
    might find it interesting and welcome your
    comments.
  •  
  • files.me.com/claudiusmixcxxxv/qzap0j
    lthttps//files.me.com/claudiusmixcxxxv/qzap0jgt
  •  
  • Best regards
  •  
  • Claudio Pellegrini

3
The history of X-ray free-electron lasers C.
Pellegrini, UCLA
  • Abstract
  •  
  • The successful lasing at SLAC of LCLS, the first
    X-ray free-electron laser (X-FEL), in the
    wavelength range 1.5 to 15 Ã…ngstrom, with pulse
    duration from 50 to a few femtoseconds, and a
    number of coherent photons per pulse ranging from
    1013 to 1011, is a landmark event in the
    development of coherent electromagnetic radiation
    sources. Until now the best X-ray source was
    provided by an electron beam traversing an
    undulator magnet in a storage ring, usually
    referred to as a synchrotron radiation source.
    The LCLS has set a new standard. Its X-ray
    brightness is higher than that of the best
    synchrotron radiation source by ten orders of
    magnitudes. For the first time, the X-ray beam
    generated by LCLS gives us the capability of
    exploring matter at the atomic and molecular
    level, with wavelength and pulse duration as
    short as the atomic scales of length and time.
    Creating matter from the vacuum, taking an atomic
    scale motion picture of a chemical process in a
    time of a few femtoseconds or less, and
    unraveling the structure and dynamics of complex
    molecular systems, like proteins, are some of the
    exciting experiments made possible by this novel
    X-ray source. LCLS, and the other X-ray FELs now
    being built in Europe and Asia, will open a new
    chapter in the biological and physical sciences.
    What has made this success possible, and what
    will be the likely future developments for X-ray
    FELs? In this paper, we describe the history of
    the many theoretical, experimental and
    technological discoveries and innovations,
    starting from the 1960s and 1970s, leading to the
    first X-ray FEL, and consider what can be the
    next steps in their developments.

4
https//news.slac.stanford.edu/features/20th-anniv
ersary-great-idea-building-lcls-slac
  • 20th Anniversary of a Great Idea Building the
    LCLS at SLAC
  • February 23, 2012 by Herman Winick
  • The spectacular success of the Linac Coherent
    Light Source (LCLS), the worlds first hard X-ray
    free-electron laser, has put SLAC National
    Accelerator Laboratory at the frontier of photon
    science. Although relevant work was done by many
    scientists 30 or more years ago, the idea for the
    LCLS at SLAC really got started 20 years ago this
    month, when 146 scientists from around the world
    gathered here in 1992  from Feb. 24 to Feb. 27
     for the Workshop on Fourth Generation Light
    Sources.
  • At this workshop Claudio Pellegrini of the
    University of California-Los Angeles stood up to
    propose that a powerful new free-electron laser,
    operating in the previously unattainable short
    X-ray wavelength range of 4 nanometers to 0.1
    nanometers, could produce an astonishing 10
    gigawatts of peak power, and that it could be
    built at relatively low cost by making use of
    part of SLACs 2-mile-long linear accelerator.

5
Claudio pointed to developments in three areas of
accelerator technology that enabled his proposal
  • 1. High-brightness electron sources  In the
    1980s a group at Los Alamos National Laboratory
    showed that so-called radiofrequency (rf)
    photocathode guns, which shine ordinary laser
    light onto a copper cathode to generate
    electrons, could produce very high-brightness
    electron beams. An advanced version of this type
    of gun now provides the electrons for LCLS.
  • 2. Preserving electron beam brightness during
    acceleration, transport and compression  To
    achieve collisions in the SLAC Linear Collider
    (SLC) project in the late 1980s, bright electron
    and positron beams from the SLAC damping rings
    had to be accelerated to 50 billion electronvolts
    (GeV), compressed and transported to the
    interaction point while preserving their initial
    brightness. To accomplish this, SLAC developed
    much relevant instrumentation (diagnostics,
    controls, feedback systems, etc.). Claudio
    pointed out that the success of SLC gave
    confidence that this could also be done for an
    even brighter electron beam from an rf
    photocathode gun at the LCLS.
  • 3. Undulator technology  Undulators are arrays
    of magnets that are used to bend the paths of
    electrons back and forth. This causes the
    electrons to emit X-ray light for use in
    research. The first permanent-magnet undulator, a
    2-meter-long device conceived by Klaus Halbach at
    Lawrence Berkeley National Laboratory, had been
    tested in SLACs SPEAR storage ring in 1979.
    Since then, longer undulators built with the
    higher precision required for the LCLS had been
    developed at SLAC and many other synchrotron
    radiation labs around the world. The LCLS now
    uses up to 108 meters of undulator magnets.

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Date Tue, 03 Mar 1992 123232 -0700 (PDT)From
WINICKSSRL01_at_SSRL.SLAC.STANFORD.EDUSubject
1-40A FELs using the SLAC LinacTo
A_at_SSRL.SLAC.STANFORD.EDU, HODGSON_at_SSRL.SLAC.STANFO
RD.EDU
  • Art Together with John Seeman of SLAC and
    Claudio Pellegrini at
  • UCLA, we are working on the basic design
    parameters and layouts of
  • 1-40A FELs that would use parts or all of the
    SLAC linac equipped with
  • a low emittance gun such as is being developed
    at several places. I
  • hope to have something to show you about this
    soon, possibly by the
  • end of this week. Pellegrini has agreed to come
    to Stanford on March
  • 18 for a follow up meeting. I briefed Keith on
    this today and also told
  • him about Burt's request that we convene a
    meeting with Paul Berg to
  • discuss biological applications of such a source.
    Is it possible to
  • arrange for a first meeting at the end of this
    week? I am gone most of
  • next week. Herman

9
Monthly meetings starting 4 weeks after
Pellegrini presentation at 4th Generation Light
Source Workshop
  • A remarkable feature of these meetings was that
    all the participants had major responsibilities
    in their regular day jobs. I merely sent out an
    email announcing the topics to be discussed at
    the next meeting and they came, often from a
    great distance, out of interest and eagerness to
    contribute their special skills and experience to
    what we all perceived to be an exciting venture.
    Not only did they come to the monthly meetings,
    but many also presented the work they had done
    between meetings.
  • At SLAC, their participation in the early and mid
    1990s was tacitly approved, and even encouraged,
    by Burt Richter, then director of SLAC, and
    Arthur Bienenstock, then director of the Stanford
    Synchrotron Radiation Lightsource. Later in the
    1990s, SLAC Director Jonathan Dorfan and SSRL
    Director Keith Hodgson continued this support.
    Apparently, the bosses of scientists from other
    labs also encouraged their participation.
  • Claudio, who is now at SLAC, was the driving
    figure in these meetings, engaging specialists in
    all the relevant areas and pointing out where
    more detailed study and experimental RD was
    needed. By November 1992, work done at these
    meetings led to an outside review of a
    preliminary proposal for a 4-nanometer FEL at
    SLAC.
  • This first proposal called for equipping the last
    part of the SLAC linac with a new rf photocathode
    gun, compressing and accelerating the electron
    beam to about 7 GeV, putting this beam through a
    34-meter-long undulator located in an existing
    shielded enclosure then in use for the SLAC Final
    Focus Test Beam, and deflecting the X-ray beam
    emerging from this undulator into an experiment
    station in a modified existing building in the
    SLAC research yard.

10
March 6, 1992 To Roberto Coisson, Heinz-Dieter
Nuhn, Claudio Pellegrini, John Seeman and Roman
Tatchyn From H. Winick Subject Summary of FEL
plans using SLAC Linac
  • I spoke with Claudio just before he left for a
    week in Italy. Claudio is in agreement
  • with our plan to calculate a series of possible
    FEL examples as Heinz-Dieter, Roberto and
  • I discussed yesterday. This includes refining the
    examples Claudio gave in his draft report
  • for 1A and 40A FELs with normalized emittance
    guns of 2.5 mm-mrad and a range of
  • other examples such as the following
  • 1. Use of the SLC damping rings with normalized
    emittance of 30 mm-mrad when they operate at 1.2
    GeV and about 4 mm-mrad at 0.6 GeV. I assume that
    these are uncoupled emittances so that they could
    be reduced by a factor of 2 with full coupling as
    Roberto has suggested.
  • 2. Use of presently available photocathode guns
    with 4 mm-mrad normalized emittance.
  • 3. Use of future photocathode guns with 1.5
    mm-mrad.

11
Participants in first LCLS monthly meeting March
18, 1992
  • Ali Amiry, Karl Bane, Roberto Coisson, Jeff
    Corbett, Albert Hofmann, Phil Morton,
    Heinz-Dieter Nuhn, Claudio Pellegrini, Tor
    Raubenheimer, John Seeman, Roman Tatchyn, Herman
    Winick

12
Date Wed, 18 Mar 1992 163757 -0700 (PDT)From
WINICKSSRL01_at_SSRL.SLAC.STANFORD.EDUSubject
Meeting on Scientific Applications of Short
Wavelength FELsTo A_at_SSRL.SLAC.STANFORD.EDUCc
HODGSON_at_SSRL.SLAC.STANFORD.EDU,
WINICK_at_SSRL.SLAC.STANFORD.EDU
  • Art
  • We had a very good meeting today on linac-based
    short wavelength
  • FELs. I am very encouraged and excited about this
    project.
  • Thirteen people from SLAC, UCLA, and SSRL were at
    the meeting. We
  • reviewed work that has been done and outlined the
    tasks that remain
  • along with the people who will carry out this
    work. We agreed to meet
  • again on the afternoon of April 13 at SSRL. We
    are planning a paper at
  • an international FEL meeting in Osaka in August
    and will be working
  • toward a proposal.

13
March 25, 1992 To Distribution From H.
Winick Subject Notes on Linac-based FEL Meeting
of 3/18/92
  • This was a meeting to discuss the use of the SLAC
    linac equipped with a low emittance photocathode
  • gun to drive short wavelength FELs as described
    in the note by Pellegrini. It was agreed that we
  • would adapt three standard wavelengths at which
    calculations will be made. These are 140 A, 40 A
  • and 1 A. It was agreed that the tasks listed
    below will be pursued by those indicated. The
    lead person
  • is indicated in CAPITAL LETTERS. That person
    will coordinate activities on that task and give
    a
  • progress report at the next meeting. The next
    meeting is on Friday, April 10 at 1 PM in the
  • large third floor conference room at SSRL.

TASKS 1. FEL design, performance and
optimization Coisson, Corbett, Morton, Nuhn,
PELLEGRINI, Tatchyn 2. Gun and acceleration to
70 MeV Morton, Pellegrini, Raubenheimer, SEEMAN
3. Beam transport and acceleration from 70 MeV
including compression Bane, RAUBENHEIMER, Seeman
4. Wiggler Coisson, Halbach, TATCHYN 5.
Layout SEEMAN, Winick 6. Scientific
applications Tatchyn, WINICK Distribution
Meeting attendees, M. Cornacchia, K. Halbach
14
Date Thu, 16 Apr 1992 183803 -0700 (PDT)From
WINICKSSRL01_at_SSRL.SLAC.STANFORD.EDUSubject
Notes on 4/10/92 FEL meeting send
comments/corrections to H. Winick
  • Attendees Karl Bane, Max Cornacchia, Klaus
    Halbach, Kwang-je Kim, Phil Morton, Heinz-Dieter
    Nuhn, Claudio
  • Pellegrini, Don Prosnitz, Tor Raubenheimer, David
    Robin, Ted Scharlemann, John Seeman, Roman
    Tatchyn, Herman
  • Winick, Dandan Wu
  • This was a follow up meeting to the meeting of
    March 18. The next meeting will be at noon on
    Tuesday, May 19.
  • Lunch will be provided.
  • The following was discussed at this meeting
  • 1. Several examples of 40 A and 1 A FELs were
    presented by Kim, Pellegrini, and Tatchyn. Each
    of these was
  • requested to send a write-up on their work,
    particularly on the 40 A case, to Winick for
    distribution to others.
  • 2. Seeman showed layouts and photographs of the
    possible locations for the FEL and experimental
    area.
  • 3. Morton gave information about measurements
    taken at Los Alamos with their photocathode gun.
  • 4. Raubenheimer reviewed the work done by him
    Bane on pulse compression, wake fields
    emittance degradation.
  • 5. It was agreed that we would prepare a paper on
    this project for the International FEL meeting in
    Japan, Aug. 24-28.
  • SUMMARY OF TASKS
  • Write-up examples of cases for a 40 A FEL at
    different electron energies and different long
    undulators. HALBACH, KIM, TATCHYN.
  • Based on above, decide on one example of a 40 A
    FEL to be detailed and costed based on trade-offs
    among output power, beam energy, and undulator
    length. PELLEGRINI, WINICK
  • Carry out one detailed example of beam
    compression and transport. BANE, SEEMAN,
    RAUBENHEIMER
  • Do full simulation with additional focussing and
    including error analysis using FRED. PELLEGRINI,
    SCHARLEMANN
  • Do a design for the photocathode gun. HALBACH,
    KIM, PELLEGRINI
  • Do a layout of a facility at sector 10. Can we
    bend 3-40A light by large angles using
    multilayers? PIANETTA, SEEMAN, TATCHYN, WINICK
  • Describe possibilities for using several bunches
    within one linac macropulse. SEEMAN. Implications
    for laser gun. PELLEGRINI
  • Distribution Attendees, Jeff Corbett, Albert
    Hofmann, Piero Pianetta

15
First LCLS Project Schedule April 1992
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ABSTRACT FOR THE INTERNATIONAL FEL CONFERENCE IN
JAPAN IN AUGUST, 1992
  • A 4 nm High Power FEL on the SLAC Linac
  • C. Pellegrini, J. Rosenzweig, UCLA
  • A. Bienenstock, K. Hodgson, H.-D. Nuhn, P.
    Pianetta, R. Tatchyn, H. Winick, SSRL
  • K. Bane, P. Morton, T. Raubenheimer, J. Seeman,
    SLAC
  • K. Halbach, K.-J. Kim, LBL
  • J. Kirz, SUNY Stony Brook
  • We discuss the characteristics and performance of
    a 4 nm SASE FEL, using a photoinjector to
  • produce the electron beam, and the SLAC linac to
    accelerate it to an energy up to 10 GeV. One
  • longitudinal bunch compression at an intermediate
    energy will increase ten fold the peak
  • current to a value of 2 kA, while reducing the
    bunch length to the sub-picosecond range. The
  • saturated output power of the FEL is in the
    multi-gigawatt range, producing about 1014
  • coherent photons with a bandwidth of about 0.5
    (1 standard deviation) in a radiation pulse of
  • several millijoules. At a 120 Hz repetition rate
    the average power is about 1 W. The system
  • performance is optimized for x-ray microscopy in
    the water window around 4 nm, and will
  • permit imaging a biological sample in a single
    sub-picosecond pulse. Details of biological
  • applications and the planned experimental layout
    will be presented.

22
Nov. 1992 First review of design for a
water-window FEL
  • Charge to the Committee
  • Critically review the plans for short
    wavelength coherent light sources using the SLAC
    linac with particular regard to the following
  • Assess the basic feasibility of the project
  • Indicate the particular areas in which individual
    work needs to be done to reach the level of a
    comprehensive conceptual design report
  • Where more than one option is presented (e.g.
    high or low energy electron beams) give your
    opinion of the relative merits

23
LCLS Technical Review Nov. 20-21, 1992
Reviewers Ilan Ben-Zvi (BNL) - Chairman Joseph
Bisognano (CEBAF) Luis Elias (CREOL - Univ. of
Central Florida) John Goldstein (Los
Alamos) Brian Newnam (Los Alamos) Kem Robinson
(STI Optronics) Ross Schlueter (LBL) Andrew
Sessler (LBL) Richard Sheffield (Los Alamos)
24
  • Nov, 1992 First review of design for a
    water-window FEL Ilan Ben-Zvi Chair members.
    Bjorn Wiik was observer.
  • Recommendations need gun rd, need demonstration
    that SASE works at short wavelengths shorter than
    cm, which was done in an LLNL/LBL collaboration.

25
TECHNICAL REVIEW REPORT (excerpts) LINAC COHERENT
LIGHT SOURCE SLAC, November 20-21 1992
The LCLS wavelength of 40Ã… is a big jump beyond
that of any FEL that has been built and tested.
We believe that the LCLS is feasible, but only a
careful R and D program and a phased approach
will give confidence that it will perform as
expected. Very few comparisons of theory and
experiment exist for a SASE amplifier which is
the basic design of the LCLS project. In view
of the paucity of such comparisons from previous
FEL experiments, and in view of the large
extrapolation in wavelength from those
experiments to 40Ã…, the wavelength of the LCLS
device, it is strongly recommended that
26
TECHNICAL REVIEW REPORT (continued) LINAC
COHERENT LIGHT SOURCE SLAC, November 20-21 1992
Further experiments should be developed at
intermediate wavelengths (at least two widely
spaced wavelengths). In this way theory and
simulation can be benchmarked and
verified. Furthermore, we believe that a credible
path for this project requires a phased approach,
and preliminary thoughts of a possible path are
presented - Experiments with 10 MeV
photoinjector. - Acceleration to 100 MeV
preserving the emittance and energy spread. -
Pulse compression without significant emittance
degradation. - Construction of a short undulator,
measurement of spontaneous emission. -
Realization of the full soft x-ray FEL
facility. In closing, we would like to state
emphatically that If no resources are provided
for the development of the Conceptual
Design Report and the benchmarking experiments,
important scientific opportunities may be missed.
27
TECHNICAL REVIEW REPORT (continued) LINAC
COHERENT LIGHT SOURCE SLAC, November 20-21 1992
In summary, some demonstration experiments are
required to ameliorate the concerns of the
performance of the photoinjector. In particular,
the following demonstrations would reduce the
uncertainty considerably 1) lt3 mm-mrad
emittance, 2) 4 ps FWHM pulses from a
photoinjector with less than the required jitter,
and 3) a reliable laser system.
Since the compression process depends on a
delicate balance between wakefields and applied
fields (with strongly off-crest operation),
maintaining a low level of both current and phase
fluctuations are critical elements in
successfully reaching the desired peak current.
The LCLS design team has discovered this problem
in its modeling, and has set specifications of
current fluctuations at less than 1 and phase
fluctuations at less than 0.2 degrees. These will
be difficult numbers to achieve for the laser
that illuminates the photocathode.
In conclusion, the Review Panel feels that there
are no show-stopping issues that prevent the
realization of a 50 meter undulator for the LCLS
Project. The main concerns are ones of proceeding
with deliberate care during the design of the
device.
A concerted attempt should be made to carefully
design and carry out a program of comparison of
theory and simulation predictions with
experiments on the UCLA 10µm experiments.
It is highly recommended that experimental data
be obtained to substantiate mirror survival at
the predicted intensities at sub-ps pulsewidths
and for irradiation areas comparable to the mm
spot sizes anticipated for this application.
28
Workshops to build the scientific case
Paraphrased comment by a prominent biologist We
have no interest in an expensive x-ray laser in
the water window. We get all we need by
examining cells with cryo-electron microscopy.
29
An order by SSRL Director Art Bienenstock
  • If biologists dont appreciate a water window
    (30-40 Ã…) FEL, go to 1 Ã….
  • I know that material scientists will find good
    uses for such a source.

30
More workshops on the scientific case
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Collaboration to Produce Improved RF Photocathode
Guns August 1993
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Next Version Photocathode RF gun
Laser Port
Photocathode
Electron Beam Exit
Full Cell
Half Cell
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Linac and Diagnostics
J. Schmerge Gun Test Facility at SLAC/SSRL
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SLAC/BNL/UCLA 3 photocathode rf gun (left)
symmetrized by a vacuum pump-out port installed
directly opposite the RF feed-in port and a
PARMELA simulation of its minimal attainable
emittance (right) using a solenoidal magnetic
compensation scheme. The discontinuous drop
results from energy-tail halo scraping of the
electron beam.
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A 2-4 nm Linac Coherent Light Source (LCLS) Using
the SLAC LinacPresented at PAC 93
H. Winick, K. Bane, R. Boyce, G. Loew, P. Morton,
H.-D. Nuhn. J. Paterson, P. Pianetta, T.
Raubenheimer, J. Seeman, R. Tatchyn, V. Vylet
SLAC C. Pellegrini, J. Rosenzweig, G. Travish
UCLA D. Prosnits, E.T. Scharlemann LLNL K.
Halbach, K.-J. Kim, M. Xie LBNL
  • Abstract
  • We describe the use of the SLAC lilac to drive a
    unique, powerful, short
  • wavelength Linac Coherent Light Source (LCLS).
  • Operating as an FEL, lasing would be achieved in
    a single pass of a high peak
  • current electron beam through a long undulator by
    self-amplified spontaneous emission (SASE).
  • The main components are
  • a high brightness rf photocathode electron gun
  • pulse compressors
  • about 1/5 of the SLAC linac
  • and a long undulator with a FODO quadrupole
    focusing system
  • Using electrons below 8 GeV, the system would
    operate at wavelengths down to about
  • 3 nm, producing 210 GW peak power in sub-ps
    pulses.
  • At a 120 Hz rate the average power is 1 W.

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  • Presenting the conclusions of the working group
    on X-rays at the ''4th Generation Light Sources
    Workshop, held at Grenoble in 1996, the
    chairman, J. Als-Nielsen, made a ''Wish List for
    4th Generation Sources''.
  • He listed lower emittance, shorter pulses,
    higher average brightness, much higher peak
    brightness, circular polarization, tunability
    from 0.15 to 0.05nm, multiple beams, fundable
    construction and operational cost. His final
    conclusion was ''
  • The Hard X-ray group is unanimously excited
    about the FEL project as a 4th generation light
    source''.

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SASE demonstration experiments at shorter
wavelengths
58
An Important SASE Demonstration Experiment
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LEUTL lases 0.53 microns at APS/Argonne Oct. 2000
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DOE Review Committee (Birgeneau/Shen) recommends
3M for FEL rd in FY 98
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Leone Panel, 1999 Need stronger scientific case
68
The first five experiments G.K. Shenoy and J.
Stöhr (edts.), SLAC-R-611, (September 1, 2000)
Atomic Physics Experiments Plasma and Warm
Dense Matter Studies Structural Studies on
Single Particles and Biomolecules
Femtochemistry Studies of Nanoscale Dynamics
in Condensed Matter Physics
DOE takes notice!!
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Claudio in the LCLS Tunnel
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  • End of Presentation
  • Thank you
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