The two last weeks in May were dedicated to the bake out of the last four cells, the finalization of cabling of vacuum automats, the connection of cooling circuits of the vacuum chambers, crotches, and front-ends, the improvement of the command controls, and finally RF conditioning of the supraconductive cavities which, it must be indicated, was carried out in record time (less than one week). An initial period of three uninterrupted weeks organized in 3 shifts of 8 hours was scheduled. In reality, following problems with the blocking of water circuits by resins (see the paragraph problems encountered) the effective time with beam was reduced for this first part to around 14 days.
An initial beam of 0.3 mA could be stored on June 2, 2006 at 2:00 a.m. for 15 minutes. Below is a photo, everybody smiling, taken during the storage of the first beam (figure 3). The first accumulation 4, up to 8 mA, occurred on June 4, 2006, near 3:00 a.m. The image of radiation synchrotron photons is given in figure 4.
| |
 |
| Figure 3: Photo taken during storage of first beam. |
| |
 |
| Figure 4: Image of synchrotron radiation at the exit of a dipole of the Ring. |
The increasing of the current progressed rapidly after that: 20 mA on June 7; 30 mA on June 10; 50 mA on June 16; and 85 mA on June 17, 2006. At the end of this initial period, on June 19, the integrated current reached 2.7 A.h, as shown in figure 5 below. The filling method used most often,due to its being the most favorable, was ¾ of the bunches filled. We would like to point out that as with the injector, all of the equipment operated with remarkable stability from the very first day.
| |
 |
| Figure 5: Intensity of current (red) and integrated dose (blue) after 14 days of the beam. |
As planned, two weeks of shutdown followed this first part of the commissioning with beam. They were dedicated to equipment maintenance, the completion of various cablings, and the cleaning of the cooling circuits in the power supplies racks and in all the storage ring magnets, and in all vacuum chambers. The final vacuum chamber of dipole D1 of the C02 cell was also installed to prepare the assembling of the IR beamline, SMIS.
Tests with beam were resumed on July 3, 2006, and proved to be extremely reproducible. Systematic measurements of different parameters of the optic were carried out and analysis of the results is in progress. The final objective is to bring the real machine and the design as close together as possible to reach our objectives in terms of performance.
On July 11, 2006, the dose of integrated current was increased to 5 A.h. The maximum current reached values passing 100 mA (~123 mA) but the current intensity decreased in an extremely abrupt way to 50 mA, subsequently showing an exponential decrease characteristic of lifetime corresponding to various known mechanisms. Following several observations and appropriate measurements, it would seem that the trapping of positive ions by the5 potential electron beam combined with the presence of obstacles in the vacuum chamber explains this dramatic drop in beam lifetime at the end of this initial phase.
During the following 8 weeks of shutdown, numerous interventions were conducted on the machine. The HU256_PLÉIADES and U20_SWING undulators were installed, as well as the final vacuum chamber for the IR_AILES line. The vacuum chambers crossing the shielding wall for the SMIS, AILES, CASSIOPÉE and DÉSIRS lines were installed, as well as all the corresponding shielding and the cabling of the safety system of the first lines and front ends was completed. Finally, a systematic gammagraphy campaign was launched on all straight sections bellows to check for possible obstacles in the vacuum chambers.
On September 5, 2006, tests with the beam resumed, and the results have been even more promising. As before, the reproducible adjustment of the storage ring is excellent, and the drastic drop in high-intensity current has disappeared. This improvement has followed the disappearance of obstacles in the vacuum chamber subsequent to the intervention that took place during the month of August (see the paragraph entitled problems encountered). Figure 6 below shows the diminution of the electron beam during a night dedicated to the conditioning of the vacuum chamber. The maximum current achieved was 100 mA, limited by the significant increase of temperature in one of the crotches where cooling flow was still very low. As shown in figure 6, we see a decrease in current near an exponential behavior.
On September 11 the current reached a value of 201 mA and finally on September 20, 300 mA were stored, the maximum current available with the current RF system (the second cryomodule necessary to reach 500 mA is under construction and will be installed on the machine mid 2007).
Note: Radiation measurements are regularly taken all around the tunnel (with beam) and inside the tunnel after a beam shutdown. The maximum intensity of the current authorized at the moment during working hours is 80 mA, probably limited by the Bremsstrahlung6 radiation created in straight sections. This limitation of current should be able to be increased rapidly thanks to the improvement of the vacuum by conditioning7.
| |
 |
Figure 6: Natural diminution of current intensity in mA (in red) and integrated dose in A.h (in blue) during conditioning sessions at 100 mA. |
The goal of this second part of the commissioning is to continue the characterization of the storage ring optics and the conditioning of the vacuum chambers, to investigate the stability of the beam position, and to study the effects of the first insertion devices and their compensations.