![]() |
![]() |
|
Site Details ATF Newsletters |
2001 ATF NewslettersJan | Feb | March | April | May | June - July | Aug | Sept | Oct | Nov - Dec
Greetings, In this update we see some of the facility development work as well as some accelerator physics. The ATF new computer control system make great strides towards operations. The CO2 laser and capillary plasma channel promise to shape up the future of x-ray production and laser acceleration. Photoinjector R&D continues at the ATF as usual. Results from experimental work-in-progress show the effects of laser uniformity on the emittance of the photoinjector. Ilan Ben-Zvi. The long awaited 100 MHz Ethernet CAMAC crate controllers have
arrived, replacing the 10 MHz units which were on loan from the manufacturer
pending final delivery of the 100 MHz components.
Initial tests uncovered a communications glitch which ocurred 5
times in 2^24 iterations. It is suspected that a network switch, which was not properly
filtering traffic from the BNL campus network, caused this problem.
BNL’s Information Technology Division will be reprogramming the
switch to isolate the CAMAC communications.
Otherwise, the performance has been excellent and we feel comfortable
with this new communication hardware which will eventually replace the
CAMAC serial highway and associated controllers. As with the 10 MHz controllers, the new units are
presently operating as auxiliary crate controllers, sharing the CAMAC
crates with the old VAX/serial highway system.
This shared operational mode will continue until all VAX software
has been ported successfully to the new system and the VAX retired. ·
The new IBM control system host has been upgraded to the
latest Linux kernel, version 2.4.3.
The new kernel more reliably supports multiple CPUs and large memory
systems. Although things
are now well-behaved and stable, the upgrade required a number of telephone
calls and e-mails to both IBM and Red Hat to iron out configuration, compiler
and RAID subsystem issues. · First server program successful: The server program which handles Darlington magnet power supplies has been completed and tested successfully. This is an important event since it marks the first integrated test of separate components (operator displays, databases, low level drivers and new CAMAC controllers) working together in the new control system. Many of the software libraries needed for this server are common to other programs yet to be ported to the new system, so the success of this first program gives confidence about the work remaining to be done. (Note: Since the data communication rate is relatively slow for magnet power supplies, the Ethernet switch problem described above was not an issue during this test.)
Meeting attendees:
All the above recommendations are built into the ATF implementation plan that is scheduled for completion in summer 2002.
Figure 1 shows a 3-cm long capillary cylinder with the electrical components forming the discharge circuit assembled at the tip of translation/tilt manipulator.
Preliminary optical tests performed with a Nd:YAG laser (8 mJ, 200 ps) demonstrate proper functioning of the device. Figure 3 shows the laser beam profile observed after the 1 mm diameter capillary without discharge (left picture) and at a proper timing after discharge (right). The effect of the channeling is clearly seen by the fact that the laser spot-size is reduced significantly.
A study is under way to measure experimentally the emittance of a photoinjector as a function of the uniformity of the laser distribution on the cathode. In this study we generate various laser intensity distributions by masking part of the laser light, measure the laser distribution and the emittance under various conditions and compare the results to simulation done with the PARMELA code. This study is at a very preliminary stage, but it is worth looking at some of the results. Some preliminary results can be seen in the figures below. Figure 1 shows the measured values of five laser intensity profiles (shown here as a function of radius, the distribution has a cylindrical symmetry). Figure 2 shows the emittance for these five distributions holding the total gun charge constant at 0.5 nC. The agreement with the simulation results is satisfactory. Figure 3 shows the emittance as a function of charge for one of the laser types (profile 5). The agreement with simulation is good, as above, except that PARMELA seem to overestimate the emittance when it is very small.
Last Modified: December 3, 2007 |
||||||||||||