Title: The Genesis of the LCLS
1The 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
2The history of X-ray free-electron lasers. C.
Pellegrini, UCLA
- Dear Colleagues, Feb. 27, 2012
- Â
- 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). - Â
- 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. - Â
- files.me.com/claudiusmixcxxxv/qzap0j
lthttps//files.me.com/claudiusmixcxxxv/qzap0jgt - Â
- Best regards
- Â
- Claudio Pellegrini
3The history of X-ray free-electron lasers C.
Pellegrini, UCLA
- Abstract
- Â
- 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.
4https//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 Â 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.
5Claudio 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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8Date 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
9Monthly 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.
10March 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.
11Participants 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
12Date 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.
13March 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
14Date 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
15First LCLS Project Schedule April 1992
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21ABSTRACT 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.
22Nov. 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
23LCLS 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.
25TECHNICAL 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
26TECHNICAL 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.
27TECHNICAL 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.
28Workshops 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.
29An 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.
30More workshops on the scientific case
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32Collaboration to Produce Improved RF Photocathode
Guns August 1993
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38Next Version Photocathode RF gun
Laser Port
Photocathode
Electron Beam Exit
Full Cell
Half Cell
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40Linac and Diagnostics
J. Schmerge Gun Test Facility at SLAC/SSRL
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42SLAC/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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45A 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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55- 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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57SASE demonstration experiments at shorter
wavelengths
58An Important SASE Demonstration Experiment
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60LEUTL lases 0.53 microns at APS/Argonne Oct. 2000
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64DOE Review Committee (Birgeneau/Shen) recommends
3M for FEL rd in FY 98
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67Leone Panel, 1999 Need stronger scientific case
68The 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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70Claudio in the LCLS Tunnel
71- End of Presentation
- Thank you