|
|
|
|
|
C-band is a name of RF frequency band. Various
bands of the microwave frequency are
named
as the figure. 
We use 5712 MHz as the drive frequency. It is
twice higher than S-band (2856 MHz) frequency,
which has been widely used in conventional
electron accelerators.
The reason why we chose C-band is,
(1) Since the shunt-impedance (a measure of
power efficiency in the accelerating structure)
becomes higher at higher rf frequency,
we can obtain a very high accelerating gradient
such as 35 MV/m using 50 MW-class
klystron.
(2) A 50 MW-class klystron can be developed
by scaling from the existing S-band
high power klystrons, and the power level is
technically feasible. We have already
developed 50 MW C-band klystrons.
(3) Since the wavelength becomes shorter, thus
the size of various components in RF
system becomes smaller as proportional to
the wavelength, resulting in reducing
size and cost of the accelerator system.
This is important for the large scale Linear
Collider project, as well as industrial applications
including the medical oncology electron accelerator,
and compact sterilization machine.
|
|
|
|
One unit of the C-band accelerator system
is shown here, which is designed to generate
35 MV/m accelerating gradient for the multi-bunch
beam of 200 nsec width, and 40 MV/m
for single-bunch.
In the case of the Linear Collider project,
to reach 500 GeV c.m. (center-of-mass energy),
we need 2000 units of C-band accelerator
unit in total for electron and positron beams.
In the case of SCSS X-ray FEL project, four
units of the same system will be used to
generate 1 GeV beam within 30 m long C-band
accelerator.


|
|
|
|
Traditionally, the modulator is the most
troublesome component, while it was expensive.
In the Linear Collider project, it is
one of the most important R&D items to
develop a reliable and low-cost modulator.
To do this, we C-band group is currently
developing the "Smart Modulator", in which a high-voltage inverter-switching
power supply is used to charge the PFN capacitors,
which simplified the modulator circuit and
reduced its size, drastically. It also contributed
to reduce cost.
In order to reduce modulator size further,
we are developing "oil-filled
modulator".
All of PFN unit, thyratron switch and
protection
circuit will be installed in one tank,
and
filled with the insulation oil. First
model
will be developed in 2001 and tested
in the
SCSS project at SPring-8.

|
|
|
|
C-band high-power pulse-klystron was developed
by collaborating with TOSHIBA Co.
The developed klystron is already on the
product list on TOSHIBA klystron tube, the
catalog number is E3746.
The developed C-band klystron is designed
to generate 50 MW peak power for pulse
width
2.5 micro-sec, and repetition rate
50 pps.
In the R&D, we have developed three
C-band
klystrons, and tested life-time for
5000
hours on each tubes. Test results were
acceptable
for the Linear Collider project at
500 GeV
energy stage.
The next generation high-power klystron will
use PPM (Periodic Permanent Magnet) focusing,
instead of solenoid focusing. We are
currently developing C-band PPM klystron,
and the first tube generated 40 MW peak power.


|
|
|
|
In order for generating very high accelerating
gradient in the accelerating structure, the
RF power from the klystron is compressed
and its peak power is multiplied in
the RF pulse compressor. It firstly
stores the klystron output power in the high-Q
energy storage cavity, then reversing
the RF phase at the klystron input. By mixing
the emission power from the high-Q storage
cavity with klystron output power at
the hybrid-combiner, 3.5 times higher peak
power in generated at the hybrid-combiner
and fed into the accelerating structures.
C-band group developed a special RF pulse
compressor "Three-cell Coupled-Cavity
Pulse Compressor", which generates a
flat output pulse, which is very important
for the multi-bunch beam acceleration in
the Linear Collider.

|
|
|
|
C-band accelerating structure uses "Choke-Mode
cavity" inside, which damps unwanted
noise power (wakefield) from the beam and
stalely accelerate multi-bunch beam.
The first C-band accelerating structure (left
figure) was developed and its HOM (Higher
Order Mode) damping performance was tested
in the ASSET beam line at SLAC, in 1998.
Test result proved the Choke-mode cavity
damped the HOM power as designed. 

|