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Site Details ATF Newsletters |
2000 ATF NewslettersJan | Feb | March | April | May | June | July | Aug | Nov | DecJuly 26
Fast Detector Group Progress in June/July 2000. The two runs we had in this period were dedicated to detailed
studies of beam effects in electro-optical (E-O) crystals while a new
vacuum chamber containing the optical detection system was being prepared
for rise time measurements with the streak camera. The E-O setup is shown in
http://www.picosec.bnl.gov/ITEMS/tt0007266.ps
where a polarized laser light goes through an E-O crystal (LiNbO3) and
then through a quarter wave plate and finally an analyzer. The ATF electron beam is directed through the hole between
the LiNbO3 crystal and the ceramic support.
The rise time of the E-O signal caused by the electron beam E-field
is shown in http://www.picosec.bnl.gov/ITEMS/tt0007261.ps
(red). This is to be compared
to the rise time of the signal due to a pulsed laser of 10ps width (blue)
obtained at the lab using the same photodiode, amplifier and oscilloscope.
The E-O signal rise time of 90ps is therefore limited by the detection
electronics and particularly the oscilloscope BW.
This BW limitation we plan to overcome by using the streak camera
in order to take full advantage of the method. The dependence of the electro-optical signal on the beam
charge and the distance between the electron beam and the beam light path
in the detector were well measured as shown in http://www.picosec.bnl.gov/ITEMS/tt0007265.ps
and http://www.picosec.bnl.gov/ITEMS/tt0007264.ps.
The dependence on the beam charge is linear as expected, and the
dependence on the distance goes as 1/r again according to theory.
The last point comes from the fact that the E-O effect is proportional
to the electric field (1/r^2 dependence) times the length of the crystal
the laser light travels during the presence of the electron beam pulse
duration (r dependence) which is typically 10ps at the ATF.
In addition to the electro-optical modulation of the light
beam and the previously observed beam induced opacity, signals with time
structure of hundreds of nsec were observed when the crystal intercepted
the beam several millimeters from the light path and when the beam struck
the ceramic holder. Most
signals were the sum of the several effects with the electro-optical component
the fastest and the only one that changes sign with reversal of the light
polarization or the position of the beam relative to the polarization
direction. The very slowly decaying signal may result from ionization
of material with an electro-optical effect produced by local charge density
resulting from the difference in charge mobility between electrons and
ions as the neutral equilibrium is re-established. The new vacuum chamber was designed and built in order to
increase detection sensitivity by increasing significantly the polarization
extinction. A large degradation of the extinction was observed when the
analysis was done near the control room rather than locally. A remotely
controlled analyzer and photodiode are now in the vacuum and under test. The proofs for our Nuclear Instruments and Methods article
on the original detection by this method were returned to the publisher
along with the copyright waver forms.
Run of June 9th: Data taken from the last runs indicate little correlation to the proposed correct trajectories sent out by Robert. This could indicate the presence of other uncertainties in the fiducialization numbers. The trajectory data taken also shows a huge kick, 12.5mrad, near the beginning of Section 3. This kick is on the order of a missing dipole magnet. (A steering magnets at full strength gives a kick of ~4.5mrad.) Heinz-Dieter has done simulations showing that the proposed correct trajectory by Robert could not fix this kick. Also, a kick of this magnitude would have to be a gross mis-alignment of the undulator. For results please view the pdf file: Run of June 13th: We performed more systematic and accurate studies in the x-direction, and also briefly recorded a couple of y-trajectories. The attached PDF file has all the relevant details: Run of June 20th: The
important result of this run is that we can straighten the trajectory
with the intra-undulator magnets. By using three magnets (before, after and at junction 2-3)
we compensated the kick and brought the trajectory down to a few hundred
microns walk-off. As Vitaly suggested, we simulated with MathCad the undulator
sections offset and its effect on the trajectory.
The best fit to the non-steered trajectories occurs when we assume
a sudden offset of about 300-400 microns at the junction of section 2
and 3. Visual observations
confirm such a possibility. In
addition, the simulated steering scheme to compensate for the offset was
implemented during today’s run, and worked fairly well. Also, for the first time since the shut down we turned on the detector. We measured a steady spontaneous emission of 300 pJ at 400 pC charge. Run of July 13-17: We had run days last Thursday, Friday, Sunday, Monday, and
Tuesday. Not much noticeable gain was seen, but interesting trajectory
measurements were done. Heinz-Dieter from SLAC came out and through his
simulations we were able to analyze the trajectories. We horizontally
moved the undulator and with the monitoring system were able to move the
undulator to <15um of the desired position. At first the peak-peak
trajectory was >1.5mm and after several iterations of undulator movement
(using Heinz-Dieter’s simulation) it was down to <500um. The agreement
between simulation and undulator movement/ trajectory measurement is quite
encouraging. This shows we believe that the undulator was not straight
for this last set of runs, but we do have the ability to accurately move
the undulator in the horizontal plane. This week the undulator was pulled and moved to the magnetic
measurements lab. Robert and his team arrived and with George’s help are
setting up the pulsed-wire measurement and will teach Alex and Aaron to
re-fiducialize and interferometrically align the undulator sections. If
all goes well the fiducialization should be finished the last week in
August at which time it will be moved back to the ATF.
Summary of Smith-Purcell Experiment Running of June 26-28,
2000: Principle goals of this running period: 1) Exercise
our new data acquisition system. Confirm that software protection prevents
stages from traversing beyond limits. Prolific data taking. 2) Operate
a BaF2 prism dispersion spectrometer in order to identify the spectrum
of the radiation emitted in the forward direction as a result of the e-beam
grazing the face of the grating. Great progress has been realized for goal 1) Goal 2) will require more work. Our LABVIEW environment now permits stage manipulations
and concurrent data acquisition so that stage scans can be done automatically
and quickly. The data is based on the waveform analysis of the ATF Tektronix
644B scope. Results of this data taking can be reviewed at http://pubweb.bnl.gov/people/kirk/atf/sp_exp/jun26_00 http://pubweb.bnl.gov/people/kirk/atf/sp_exp/jun27_00 http://pubweb.bnl.gov/people/kirk/atf/sp_exp/jun30_00 Principle results: I) Our
beam profile consisted of E = 45 MeV, Q = 400 pc, Width = 3 ps, Emittance ~ 1 pi mm-mrad II) We
have determined the cause for previous differences in angular mirror scan
profiles. The detector position
along the optical collection axis gives different profiles and signal
strengths by 1 order of magnitude for 2 cm axial translations. See: http://pubweb.bnl.gov/people/kirk/atf/sp_exp/jun27_00/2_mscans.ps III) We
have confirmed an angular dependency to the wavelength of the emitted
radiation. See: http://pubweb.bnl.gov/people/kirk/atf/sp_exp/jun27_00/mscan_none_sapphire_I.ps IV) We see evidence
that the longer wavelength radiation has a larger coupling length to the
grating. See: http://pubweb.bnl.gov/people/kirk/atf/sp_exp/jun28_00/pyrex_sapphire_7um.ps Fitted Gaussian to the xscan distributions yield: Pyrex-- Sigma
= 56 +/- 0.2 Sapphire—Sigma = 56 +/- 0.3 > 7um -- Sigma = 76 +/- 0.8 V) Spectral content
for our observed radiation is approximately: Less than 3 um
-- 60% 3 um - 5um
-- 20% > 7 um
-- 20% Our goal for the next run is to implement the BaF2
prism spectrometer and perform a spectrum analysis of the detected radiation. June 23: Over the past two weeks we have been able to move our people into the new offices of 820-M. We now have all of the ATF staff under one roof. Mechanical assistance was offered to HGHG on the realignment of the three camera’s that were moved to access the new liquid crystal CO2 beam display. I believe this saved a lot of time and frustration. All three camera’s were being powered by a single power supply, loading down the system, Marc has ordered additional supplies and will install them as soon as they arrive. We also provided electrical help with the HGHG pneumatics for the pop-in monitors and video switching system. The remaining two UPS supplies were installed in the MCR to protect the CAMAC control system and the repair of various Darlington transistor power supply channels were needed for the continuation of operations. Last week the workload consisted of installing the main discharge chamber at the Terawatt pre-ionizer along with an alignment that sets the gap on the electrode screen. Clamping rings were installed and torqued to hold the pre-ionizer in place and the connection was made up to allow for vacuum testing. Unfortunately, the vacuum control interlock network is not finalized and we cannot continue with the system check-out. Scott Buda will be back from vacation on Wednesday and hopefully we can complete the interlock chain and resume testing. The new hardware has arrived to replace the Russian stock and is being installed. In addition to all this activity, the technical staff of the ATF continues to support the control room operations on a daily basis. June 30: The majority of the week was spent assisting the HGHG experiment with the ordering, design and construction of tv monitor power supplies and power distribution for the lamps used in the experiment. Assistance was also given in the trouble-shooting of the failed power supplies for the trim magnets within the undulator. Luckily, these supplies are not needed at this time but will have to be repaired as soon as possible for future experimentation. We attempted to install a replacement power supply for the focusing into the undulator but were unable to attain the manual from NSLS to wire it in properly. Hopefully, we can find the information needed to make the changeover as our loaned supply is needed badly for another function. Time was spend inventorying possible PCB equipment. A test for high levels remain on the old high voltage transformer inside the gun modulator, after which, we are PCB free. The Failed UPS power system in the control Room was replaced and at this time, all CAMAC crates are now protected. The mechanical team has achieved high vacuum on the terawatt pre-ionizer at a pressure of 5x10-5 and the vacuum control system appears to be working properly. Before closing the main pressure vessel, we will leak-check all components. Aside from all these responsibilities, the technical staff of the ATF continues to support the control room and experimental operations on a daily basis. July 21: The high voltage Maxwell pulse generator was sent out for repair and has arrived in time for installation for the HGHG run next week. Don Davis and Bob Harrington have been installing the gas lines for the main discharge cell of the terawatt laser and securing the parts needed for the exhaust line for the pre-ionizer. The heater assembly for the YAG amplifier has been installed and the bracket for the active mirror relating to the YAG oscillator has been machined. Electrically, Marc replaced a bad triode in the third stage on the linac 1 kw driver. The unit has been retuned and is running to ATF specifications. The CO2 pulser has been electrically tested and installed back in the CO2 room. The high voltage contactor needed for the gigawatt has been built and is in the process on installation. June 9:
June 16
June 23
Have a nice holiday. July 7:
5. Solid state modulator: I was impressed
by the progress of the solid state modulator technologies, now MIT and
NLC are adopting this technology, I suggest we should also consider this
for our energy upgrade. July 14: 1.
ATF schedule: Next week ATF maintenance day is on Wednesday, and
Friday beam studies time experimental hall will open for access. 2.
GW CO2: Igor has shipped the pulser to Maxwell last Friday, Bill
and Mark are now following the status. We were told the unit will
be fixed and ship back to BNL next Tuesday after the test if they get
paid. 3.
Wednesday jobs: Mark will check the RF system, including 1 KW and
modulator. Bob will help to install the heater for the YAG laser. 4.
YAG laser: next week’s Friday beam studies will be used for cathode
cleaning and crystal testing. 5.
VISA: Visa is planning to remove the magnet for testing, Sam agreed
to provide one day help from vacuum group and Mike. Don will also
help on that day. 6.
TW CO2: Bob and Don will work on the TW CO2 except next Wednesday. 7.
Fast detector: new equipment installed and surveyed, I told them
they must have better than 5x10-8 vacuum for operation. July 21:
Last Modified: December 3, 2007 |
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