Beam Tune and Beam-position Monitoring
Beam position monitoring task list:
- Check averaged BPM readings every 15 minutes ( this does not show 60 Hz noise).
IPM1H03B, at 1.1m from the Hall A target, is the closest one to the HAll A target.
X and Y absolute positions measured by this BPM are good approximations
to the x , y positions of the beam at the target.
Both vertical and horizontal readings from this BPM should be below +/- 0.2 mm
IPM1HO3A, at 7m from the Halla target, is the next closest BPM we have . X and Y
absolute positions measured by this BPM should also be small (<0.3 mm) enough so
that the beam has no slope at the target. Which will give rise to a Scattering angle
(Theta note) change <0.5mr.
- BPM strip chart ( spikes ) (Example) - expect to get a better tune than
this.
- Find the Accelerator main
menu (monticello screen) on the HAC x-terminal. If it is not there, you
have to call the MCC and request it.
- Go to BPM >> BPM overview >> Hall A >> Hall A Absolute
- BPM position summary window (Example)
- as above
- Go to BPM >> BPM position summary >> BSY-experiemntal halls >> Hall A
- BPM x-y plots (Example)
- as above
- Go to Hall A >> Hall A BPM position plots
- When the beam is turned on and
at the beginning of every shift, request a Bscope from MCC to check the
60 Hz noise. Check both the horizontal and vertical noise corresponding
to IPM1H03B BPM. Both offset and the amplitude should be < 0.2 mm.
For a detailed discussion on the Beam position monitoring and the effects
of Beam position on the spectrometer resolution please see below.
Beam Tune
This is done by the accelerator.
Currently, we have no control over the tune. The accelerator division will
nominally check the tune once in every shift. At these times , we should
verify that the beam spot is centered on the cross wires , and have the
operators look fon any Halo.
The nominal tune calls for:
- Point focus at the target.
- Zero dispersion.
>
- The Emitance is ~10E-7 m.rad so that the nominal beam spot size is very small.
- A description of the beam line is available in the counting house.
Beam Position Monitoring
There is a four wire stripline
antenna system to monitor the beam motion .This is documented in one of
the beam line documents. What is important is to monitor the shifts in
x and y positions of the beam. IPM1H03B, at 1.1m from the Hall A target,
is the closest one to the HAll A target. X and Y absolute positions measured
by this BPM are good approximations to the x , y positions of the beam
at the target. To make sure their is no angular dispersion of the beam,
should look at the IPM1HO3A.
Snapshot of Hall A BPM window
How to get the BPM window :
1) Find the Accelerator main menu (montecello screen) on the HAC x-terminal.
If it is not there , you have to call the MCC and request it.
2) Go to BPM >> BPM position Summary >> BSY/Experimental Halls
>> Hall A
Important Information about the Beam position:
1) Accelerator BPM's give a coordinate
system z along the beam ,y vertically upwards, x horizontal making an orthogonal
system. In the spectrometer coordinate system
, at the target, z along the beam, x is the dispersive direction ( vertically
down) , y is horizontal making a right handed system.
2) Magnification factor in the
spectrometer along the x (dispersive) direction = 2.5
(A distance of 1 mm at the target
in x correspond to 2.5 mm at the focal plane).
3) Dispersive constant of the
spectrometer = 8 x10-2 m-1.
(1m of x at the focal plane correspond
to dp/p =8 x 10-2 = 8 %)
Both x_acc, and y_acc beam positions
are important to us because :
1) Y_acc < 0.5 mm (remember 0.2mm sigma corespond to a fwhm of 0.5mm)
( Momentum Resolution)
X_target < 0.5 mm , X_fp < 0.5 x 2.5 = 1.25 mm
dp/p < 12.5 x 10-4 x 8 x 10-2 = 1x 10-4
2) X_acc < 0.5 mm
Angular resolution in phi if the beam has just an offset or shift in X_acc
dx_acc < 0.5 mm = 5x 10-4 m
Distance between the target and the spectrometer ~ 1.1 m
dphi < 5x 10-4 / 1.1 = 0.5 mrad
3) Differencd between IPM1HO3B and IPM1HO3A beam
positions < 3 mm
Distance between the Two BPms = 6 m.
d (Theta-note) = 3 x 10-3 / 6 = 0.5 mr
Determination of the Scattering angle Theta
(if the beam has a slope in X_acc)
1) Instantaneous values of monitors should be read out in the data stream.
This can be used in the offline analysis to correct the data.
2) As far as the visual monitoring
is concerned, we should keep the relative offsets of the xy monitors to
below +-0.2 mm( This will ensure fwhm. of dp/p < 10-4 and fwhm. of dphi
< 0.5 mrad.
3) Since the visual monitors
are locked at 60 Hz , we do not see the 60 Hz motion of the beam . Up to
now the accelerator does not know the source of this 60 Hz noise. We should
run Bscope
once in every shift to make sure that this 60 Hz noise in not large . Peak
to peak < 200micrometers.
To get the Bscope :
4) Beam halo should normally
be small . If it is too large , it will hit the magnet poles or other objects
like iron-chamber , and will automatically shut the beam off. The accelerator
is installing a halo monitor at the point of maximum despersion in the
arc , and this is the best place to check for the halo, since it is likely
to be energy dependent. When the accelerator is doing system checks once
every shift , they can check whether the Crest of the wave coinsides with
the RF kick.