Tuesday, May 29, 2007
Highest RF peak power - 29th of May
RF pulse from 2157A Klystron - 25th of May
We have driven the input of the klystron at a low power (estimated at 2.5 W peak power, which is a tenth of the optimal power).
The output level measured by the RF diode detectors corresponds to 2.5 MW peak power. This corresponds to a small signal gain of +60 dB.
Friday, May 25, 2007
High Power RF Test - 23th of May
The RF setup is orginized in the following way:
- The output of the RF source, Phase-Locked Loop (PLL) Synchroniser, is fed to the 100-W continuous RF amplifier, MAL tld..
- Inside the PLL a RF switch is integrated at the output, so that we can produce a low power (13 dBm) RF pulse of tens of microsecond in duration.
- The MAL amplifier (type AM82-3S-45-50R) has a small signal gain of 41 dB and has a output maximum of 50.2 dBm.
- The output of the MAL amplifier is fed to the input of the Klystron Tube. The klystron tube has a small signal gain of 57 dB.
- At the output of the Klystron Tube the waveguide section (WR284) is mounted, which contains a circulator with load (Ferrite SC3-118), bi-directional coupler and RF pressure window (CPI VWX-1053) at the accelerator cavity.
- To the bi-directional coupler RF diode detectors (Agilent 423B) are connected to monitor the forward and reflected RF power.
In this test phase the RF pressure window is replaced by a reflection plate, so that all the RF power is dissipated in the RF load on the circulator.
In the control room we have placed all the measurement equipment: two puls generators to supply the trigger pulse for the modulator and RF switch inside the PLL Synchronizer. The signals are displayed on a oscilloscoop.
For the computer in the control room the modulator can be controlled and all the operating parameters can be monitored.
Upper: PLL Synchronizer, Lower: MAL RF Amplifier | N-type Coax cable connected to RF input of Klystron Tube. |
Bi-directional coupler in waveguide section. RF diode detectors connected to forward and backward outputs. | Trigger signal generation and signal analyzing in control room. |
Control computer in control room. | Red warning light indicates accelerator operation. |
Friday, February 23, 2007
Assembly of Laser Transport System - 23th of Februari 2007
The Laser Transport System consists of 4 boxes containing turning mirrors. Between the boxes vacuum tubes are mounted to transport the beam. The entrance and exit tubes are closed by vacuum windows (anti-reflection coated). Two complete laser beam lines can be hosted in the Laser Transport System. For the time being only one line will be used to transport the high-power fundamental beam (800 nm) from the femtosecond laser system.
Test assembly of Cavity Container with RF input coupler - Half Februari 2007
Secondly, we can also start the assembly of the vacuum components.
(a) Stainless Steel container with flange on one side and RF input coupler (copper) on the other side. The flange will host cooling water feedthroughs and vacuum pump connector. | (b) The RF waveguide (black) is connected to the RF input coupler. Between a RF window is placed to isolate the vacuum side (10-9 mbar) from the pressure side (2 bar SF6). |
(c) This is the side on with the electron beam line will be constructed. |
Monday, February 12, 2007
Repair of azimuthal orientation - 7th of Februari
The solution was to replace the fitting pin with a new one having an offset. Last week we installed this new pin. The last photo shows that the replacement was successful. Now both the cooling channel and all the bolts fit correctly.
Wednesday, January 3, 2007
Friday, December 22, 2006
Current status just before Christmas
Test assembly of RF waveguide section - 22th of December
Below you see a small impression.
Total waveguide section | Circulator directly behind klystron tube |
Bridging section | Section to Cavity with bi-directional coupler |
RF input coupler with RF window | 4-port Circulator |
Wednesday, December 20, 2006
Modulator test 28th of November 2006
From the BNC output connectors the current and voltage pulses were obtained and recorded by an oscilloscope:

Note: The tension pulses are multiplied by a factor 2, because they were recorded using 50Ω termination, which causes the measured tension to be half of the proper value.

