.
The
operational calendar for 2003 has scheduled 6552 hours of operation of which
4920 hours dedicated to User operation. Beam energy for the calendar year is
2.0 GeV for 74% of the time and 2.4 GeV for the remaining time. The overall
User uptime to date has been 90.4% (92.1 excluding storms) with the main
causes of downtime due to storms, the commissioning of the third harmonic
cavity, linac and difficulties with refills. Of the many activities performed
during the machine shutdowns the most notable has been the putting into
operation of the third harmonic cavity that has significantly improved
operational behaviour and, together with the fast multi-bunch feedbacks, the
quality of the beam. A further important shutdown activity, to be performed
during the last quarter of the year, is the measurement and re-alignment of
the storage ring magnets.
Many
improvements have also been made to accelerator systems during the year. On
the side of control electronics and software there has been the continued
upgrade to a two level architecture that adopts new CPU boards for the
front-end computers. The upgrade renews control hardware that is becoming
obsolete and adds new features. Two complete subsystems, insertion devices and
the radio-frequency (RF) plants, have been equipped with the new controllers
and an additional seven vacuum controllers will be installed by the end of the
year. In the control room the high-level software program 1bm (one button
machine) has been redesigned and rewritten. 1bm automates and optimises the
long sequence of operations required during a refill, that includes, magnet
cycling, injection, energy ramping, orbit correction and insertion device
management, to mention a few. The new version has improved performance and
robustness. The electronics controlling the RF phase and higher order mode
(HOM) shifters have been upgraded. The RF plants have also been equipped with
mains stabilisers that increase the stability of the amplitude and phase of
the RF output power. An upgrade of the phase loop electronics has started that
allow an increase of the correction factor of the loop, permit increased
bandwidth and the possibility to perform phase modulation of the RF signals
for beam manipulation. An important improvement of the effectiveness of the
correction of residual closed orbit distortions from insertion devices has
been initiated. For this the correction coils, associated power supplies and
feedforward control hardware for section 2, 3 and 6 insertion devices will be
upgraded. Moreover, the upgrade will permit correction of individual modules
of the full insertion device.
For what
regards mechanical upgrades, the vacuum chamber in straight section 7 was
replaced during the June shutdown. Together with the new thinner three-meter
long NEG-coated aluminium vacuum chamber the straight section includes two new
low-gap beam position monitors (BPM) for orbit feedback systems, two
additional BPMs dedicated to the multi-bunch feedback systems and the machine
scrapers. The latter were removed from straight section 11 following the
installation of the superconducting wiggler.
Activities
on photon sources have principally concentrated on the insertion devices for
the second X-ray and IUVS beamlines and modifications to the bending magnet
chamber for the infra-red beamline. During the year the installation and final
commissioning of the second Figure-8 undulator module for the IUVS beamline
took place. No significant perturbation is observed on storage ring beam
dynamics when closing the insertion device to the minimum gap of 19 mm and
undulator control is freely allowed to beamline users. Radiation spectra
measured at the experimental station show good agreement with the predicted
peak wavelength and intensity.
The
superconducting wiggler (manufactured in BINP, Novosibrisk) will produce 14
times more photon flux at 25 keV compared to the present permanent magnet
device for the second X-ray diffraction beamline. The wiggler installed in the
autumn of 2002 has been studied under differing operational conditions. Both
the power mode (where the magnet is permanently connected to its power
supplies) and the persistent current mode (where a stationary current is
circulating in the superconducting coils) were successfully tested. An upgrade
to the vacuum chamber (modifications to the tapers and copper liner) will be
performed during the next quarter to lower the consumption of liquid helium.
The wiggler has been installed in section 11 of the storage ring next to the
superconducting third harmonic cavity. A future upgrade to both cryogenic
systems foresees to deliver liquid Helium from the cavity liquefier to the
wiggler dewar and a combined helium recovery scheme.
The
installation of the new infrared beamline, which is foreseen in the early
2004, has required the development of new type of exit port for the beamline
itself. Modification to machine components has centred on the bending magnet
vacuum chamber, the photon absorber and the photon shutter. These
modifications will allow a horizontal acceptance angle of 70 mrad and 25 mrad
in the vertical plane. The horizontal acceptance allows both edge and main
magnet infrared radiation. The requirements of the new beamline, in particular
the vertical acceptance, have also required a new vacuum chamber design based
on previous experience with aluminium constructs. While the photon absorber
was just modified, the shutter component has been completely redrawn for the
layout requirements of the beamline.
.
| figure
1 |
|
|
|
.
an
exploded view of the vacuum chamber assembly for the infrared
beamline
showing the new beam shutter and photon absorber;
the chamber is constructed
of two aluminium half shells
.
|
.
An
important result of the last few months is the successful operation of the
storage ring free electron laser (FEL) in the so-called Q-switching mode. This
is performed by periodically modulating the main RF oscillator in such a way
that laser pulses are generated with a regular time structure (following the
RF signal modulation) and with increased output intensity. This is believed to
be particularly useful for the planned time-resolved experiments that would
benefit from the more predictable macro-temporal structure compared to the
natural regime. A procedure to energy down-ramp the storage ring was also
tested and enabled to lase for the first time at 750 MeV. The advantage of low
beam energy consists in a corresponding reduction of synchrotron radiation
power that is responsible for the fast degradation of mirrors used in the
optical cavity.
On-going
synchrotron radiation tests of different single and multi-layer mirror samples
are an important part of the European collaboration (EUFELE contract). The
characterization of these samples before and after exposure allows a
significant database of material properties to be built up. The database is
then used to optimise the production process and the choice of materials that
lead to FEL compliant mirrors for the VUV spectral region.
.
| figure
2 |
 |
.
FEL signal in
standard (figure a) and Q-switched operation mode (figure b); beam
energy:
900 MeV, beam current (four bunches) 10 mA, laser wavelength 250 nm,
optical gain 7%,
cavity losses 10 to 5%
. |
.
A
common problem of all intermediate energy third generation light sources is
the short beam lifetime that arises from a small beam emittance. Such machines
have high bunch densities and correspondingly increased elastic intra-beam
collisions that lead to particle loss, i.e., the Touschek effect. To
circumvent this effect the bunch is diluted by increasing its length while
maintaining the all-important transverse emittance. A cavity operating at a
higher harmonic of the main RF system, when appropriately phased, will
lengthen the bunch without introducing increased energy spread. A
superconducting third harmonic cavity was chosen and put into operation during
the year. The system provides both an increase in lifetime, through bunch
lengthening, and the Landau damping of longitudinal multi-bunch instabilities.
The system installed during the later half of 2002 underwent a series of
adjustments by the manufacturer followed by a period of commissioning early
this year. The cavity is now in routine operation at 2.0 GeV and 320 mA, where
the improvement in beam lifetime attains to more than a factor of three and a
full damping of longitudinal beam instabilities is provided. The cavity has
been activated also during user’s run at 2.4 GeV, 140 mA, where it provides
an increase in lifetime up to 50% of the nominal value.
.
| figure
3 |
 |
| effect
of the third harmonic cavity on the beam lifetime when the cavity is
tuned for bunch lenthening (red) and parked (blue); the stored current
after 20 hours is roughly twice that without the cavity in operation |
.
Activities
with the transverse multi-bunch feedback system have progressed with the
putting into operation of the second system acting in the horizontal plane.
Prior to this system, horizontal instabilities were suppressed by acting on
the harmonic sextupoles to provide Landau damping. The sextupole settings,
however, were not optimal for a long beam lifetime. The two transverse
multi-bunch feedback systems have enhanced the effectiveness of User operation
through a considerable gain in beam lifetime. Machine operation with the
systems allows nominal optics to be used with a consequent increase also in
dynamic aperture. In this configuration together with the operation of the
third harmonic cavity, a beam free of coupled-bunch instabilities is delivered
to Users also at 2.0 GeV. Since installation, the operational behaviour of the
two systems has been effective and reliable. They are integrated into the
control system with initialisation, run and standby routines that are fully
automatic and easily activated from standard control room panels.
.
First extensive
tests of the longitudinal multi-bunch feedback were performed during the start
of the year. The longitudinal feedback digital processing electronics take
advantage of the same kind of hardware developed for the already operating
transverse feedback, so that individual digital filters are executed for each
of the 432 2-ns spaced bunches. Principal differences exist on the front end
(detector electronics) and the back end (RF modulator, RF amplifier and
kicker). Commissioning results have been positive and by activating the system
from the beginning of the injection process up to 280 mA of longitudinally
stable beam at 0.9 GeV have been accumulated. At present the system is not
used for User operation since the third harmonic cavity naturally damps
longitudinal instabilities when operating in bunch lengthening mode. The
system has, however, been effectively operated for the suppression of
longitudinal instabilities of the 4-bunch beam used by the storage ring FEL.
Maintaining
a transversely stable closed orbit is of fundamental importance. Towards this
goal high resolution and high accuracy beam position monitors (low gap
BPM’s) have been developed for insertion device straight sections. The
installation of these monitors is being systematically pursued. At the same
time upgraded detector electronics are being tested on both the standard
rhomboidal and low gap BPM’s to be used in either local or global orbit
feedback systems. One such complete feedback sub-station is being used for the
local orbit correction tests in sections 1 and 2, where both the
‘old-type’ rhomboidal and low-gap BPMs are respectively installed. In
section 2, in particular, the feedback has been positively closed on both the
horizontal and vertical planes using a PID (Proportional, Integral,
Derivative) controller. Beam noise induced by the mains at 50 Hz and at higher
harmonics is removed by specific harmonic suppressors. The feedback software,
which runs on a PowerPC CPU board under the Linux operating system with a
real-time extension, can manage system saturation and periodically transfers
the accumulated DC correction contribution to the already existing DC orbit
correction schemes.
The
upgrade of the storage ring RF system is necessary to handle the RF power
requirements of the full set of insertion devices and to allow operational
overhead. The first phase of the upgrade is the substitution of one of the
original 60 kW amplifiers with a 150 kW plant. The substituted plant will be
used to power the booster RF system. The detailed evaluation of the offers
received in reply to the call for tender has been completed. The upgrade,
based on Inductive Output Tubes (IOT’s), will use two 80 kW tubes combined
by means of a switchless combiner and allows the operation of each IOT in
stand-alone mode if necessary. This option has been preferred compared to the
use of three 50 kW tubes for reasons of cost and space. The cooling and
electrical supplies for the new plant will also be upgraded. The RF cavity, an
improved version of the original and already power conditioned, will replace
the one in section 9. The new cavity features an upgraded cooling system that allows operation
at a higher gap voltage corresponding to 60 kW wasted power on the cavity
walls. The newly designed input power-coupler also doubles the RF power to the
cavity from the present 60 to 120 kW.
Finally also the HOM frequency shifter is of the new concept, free of RF
contacts, which will allow use of the full shifting range, at full cavity
power (60 kW). Installation will be performed during the last quarter of 2003.
The full energy
injector for the storage ring is composed of a 100 MeV pre-injector linac and
a 2.5 GeV booster synchrotron with a repetition frequency of 3 Hz. The 100 MeV
pre-injector linac for the booster is presently being assembled using two 50
MeV accelerating sections donated by CERN. The in house construction of the
modulator for the klystron of the pre-injector has been completed and
undergoing tests. Specifications and signal handling for the pre-injector
control system are well established and will adopt a voltage-to-frequency
conversion technique. After the successful test of the prototypes series
production has started. Progress is also well underway for the electronics of
the gun.
The
system for beam injection into the booster is composed of a septum magnet and
a fast kicker magnet, while extraction is performed by a set of bumper
magnets, kickers and an extraction septum. The call for tender for the septum
magnets for injection and extraction from the booster and those for the
upgrade of injection into the storage ring was made early this year. Delivery
of all three systems is foreseen in the coming six months. The booster will be
built to operate in top-up mode necessitating reliable operation of all parts.
In view of this, tests to identify critical components of the septum magnet
power circuit were performed on a prototype and the six units of the series
production are now being assembled.
The
design of the fast kicker magnets, based on in-vacuum ferrite magnets, is
progressing A prototype will then be constructed along with a prototype of the
kicker high voltage pulsed power supply to perform tests on a complete unit.
The booster synchrotron is a two-fold symmetric lattice with long straight
sections for injection and extraction. The lattice is composed of bending
magnets, two types of quadrupoles and sextupoles. Specifications for the
bending and quadrupole magnets have been reviewed and are now available in
their final version together with the specification for the steerer magnets.
The RF system for the booster is composed of a DESY type five cell cavity
powered by one of the storage ring amplifiers that will be available after the
RF upgrade. The cavity was delivered at the end of May and is currently being
measured in the RF laboratory and will soon undergo full RF power tests.
Development activities for other systems, such as power supplies, controls,
interlocks, access control, diagnostics and vacuum have also advanced. For the
diagnostics a new version of the fluorescent screen is being developed and a
prototype constructed, with a combined thermal and mechanical design, for use
in both transfer lines and the booster. The associated image acquisition and
analysis system after being tested in the laboratory is being installed on the
storage ring synchrotron radiation profile monitor where it will upgrade the
existing system. The first detectors adopted for the booster BPMs have been
installed on the ELETTRA linac and transfer line for characterisation with
beam.
Civil
engineering activities are going ahead with the construction of the second
part of the new injector building that is scheduled in the coming months. This
part of the building includes the electrical service area, the bridge
connecting the existing control room and a part of the booster tunnel in the
injection area.
.
| figure
4 |
|
 |
|
.
the
five cell booster cavity undergoing power tests in the RF bunker
. |
.
|
figure
5 |
 |
|
.
the
complete modulator and klystron tank for the booster pre-injector
. |
.
|
figure
6 |
 |
|
.
view
of the high voltage power supply of the pre-injector linac
. |
.