April 4, 2006 New orbit testing for
X25-suite
When the beam came
back after studies, I realigned the beamline. The merit for 300 um
collimator (2 dots) at 1.0A= 422.
I moved the ladder slit back to it
original value (46.16) and the merit got better. I move the pitch on
the mirror; merit =560.
I optimize the v-slit.
I optimized the bending on the
mirror, tested the yaw on the table. I need to test the pitch better.
I started a data collection to
examin the stability on the beam
stability/1/html
This is really stable!
Lets test a xtal.
April
3, 2006 New orbit testing for X25
Since March 8 there has been a new
orbit for X25 without any announcement. We are officialy testing it
today. This might impact people in between X25 and X29 in particular.
The beam is injected with the "old"
orbit for an hour and the new one will follow for an hour. I started a
dummy data collection 15 sec exposure time in order to follow the io.
(counter on the tip of the collimator).
The sweep reports can be accessed at
old/1/html
old-suite/1/html
new-25-orbit/1/html
Picture
1 (old)
1-So the beam is injected and the beamline is warming up while
collecting
2-alignment of the beamline around frame #30.
It seems like the monochromotor finally reach its temperature after 20
minutes. That's what we would expect.
Picture
2( called new but it's actually
the continuation of old)
I realign after frrame #2. It doesn't make a difference in the counts.

Picture
3 newest (the new X25 orbit)
I left the data collection go for about 8 frames before realigning. The
count are about 15% down from the previous orbit. The realign did not
improve the counts.
X26A is also seeing a 20% decrease in their intensity. Their beam has
moved by 120 microns. They get their intensity back by moving their
slits.
Realign around frame # 67.
I tested a little moving the ladder slit and it seems like I am getting
back the intensity. I need to wait for ops in order the adjust the slit.
May
24, 2005 spring shutdown
The vme crate running the motors has
been updated
The computers are now running
Fedora 3.0. There is a problem while trying to FTP. This should
be taken care of in the near future.
The computers have a new naming
scheme consistent with the other beamlines.
x26c-c is where you start CBASS (old
folgers)
x26c-d is the octane which
interfaces with the diffractometer. The users are not use this machines.
x26c-b is the new linux machines. It
has the HKL2000 license installed.
Dec 15, 2004
winter shutdown
Berilium window
A new berilium window is in place in the hutch. This window is narrower
but longuer than the previous one. This will give us more freedom to
move the mirror when optimizing the beam. We will not have to move the
pipe when we change the experimental setup for 3-beam experiment. We
will need to make sure the beam goes thru!
Resulting from this upgrade, the IG controller didn't want to
come back up. It's being sent back for repair. The vacuum in the last
segment of the beamline is stable and in the 10^-9.-done
X26C-w
The SGI Octane x26c-w is being replace with a new Linux machine with
dual head monitor. The Octane did not perform anymore compared to
a simple Linux machine. It is also less burden on our computer staff as
far as maintenance and upgrades to slowly get rid of all the SGI
machines. The users also really appreciate having a dual head monitors.
goniometer head
We are in the process of implementing auto-centering on this beamline.
We need to install and optimize the parameters for a motorized
goniometer head-- The goniometer
head is too long and can't be accomodated on this beamline.
Dryer line
Replacement of the dryer line unit for the cryostream with exhaust line
of liquid nitrogen from the Light Source--
Detector's controller
Unit back form ADSC. We need to swap controller to make sure it's
working properly-- This controller is on X12b now.
Nonius phi spindle
A service call is in place for Andy Gangloff to come and service the
phi spindle. We observed signs that it is not as reliable as the omega
motor.
camera
We are having a new mount position for the camera at the working
station. This will enable a view of the monitor, of the control panel,
and all the computers including the detector's computer and
controllers. This is critical for the staff when troublshooting from
off site.
-- work in progress
HV panel
The in hutch panel for all the HV cables of the IG and ionization
chamber is being modified to be staff friendly!
--
work
in progress
Control rack
The control rack where all the VME crate and Origon cards are, in the
back of the experimental station, has new electrical outlets on each
side. This was implemented after the NSLS Tier I electrical rewiew
found we were using power strips powered via electrical extensions.
This as been clean up i.e, no more electrical extensions.
-done
August 5, 2004
New CBASS
A
new version a CBASS is now running on X26C and X12C. This will be
implemented on the other beamlines in a short time.
In order to start
CBASS you still
have to ssh or telent to the x26c-h
as pxuser.
telnet
pxuser@x26c-h
password:
{same as the pxuser on all the machines}
cd
/img06/data1/x26c/your_directory
1 June 2004
Beam
Alignment
28
may 2004
Maintenance
The ring has been in conditioning for
several days. We could not enable the beamline since there was an
interlock trip on the mirror proteus. Joe started to work on it and
Shai and Annie finished it. The flow was not sufficient for the setting
on the proteus. We changed the setting to BC (inter flow).
The beamline was still yellow tagged. There wasn't any yellow tag on
Valve 2. This valve is not interlocked. You have to feel on the top of
it with your hand to know if it's open or closed. We enable the
beamline so that the mono can be cooked. The vacuum was
in the low 10-7.
There was beam all the way in the hutch but after "realign" the merit
was only 10% of what it should be. We wait for the real user beam on
Tuesday
24 march 2004
Ladder
slit Optimization
I want to optimize the vertical
position of the beam on the
mono. We
want to have the ladder slit position aligned with the peak of
intensity of the incoming beam is. Of course this is an iterative
process since the height of the mono has to follow were the best ladder
slit position is.
I am starting with the 2 dots collimator (300 µm) at lambda 1.1A.
I moved the slit by a small increment (0.2 mm) and waited a
minute or two. Then I collected 7-10 frames in order to see how
reproducible the counts were.
The exposure time is only 10 sec.
The data I collected last night were for the ladder slit at 44.945 mm.
On the graph that correspond to light blue series. This position is
right at the edge of the plateau (44.745 mm to 43.945 mm). This plateau
is fairly larger and a slight change in the orbit should not influence
too much the counts observed. I will leave the ladder slit at 44.345
mm. This is a lower position than used previously.
Stability of the beam

Each data point is for 90 sec frames with the
pause on dump ( CBASS detects
when the beam has dumped, pause the data collection, wait 15 minutes
after the beam is enable again, realign, backs up one frames and
recollect) and
automax
(realign macro activated) every 30 minutes. We can locate where the
automax occurred since we have a point with a counts of zero where a
dark was taken.
First observation the
automax slightly
improves the counts during a normal data collection within the first
hour after a fill.
Second observation
the counts are slowly dropping from the beginning of the injection to
the dump of the beam. We do not have more intensity at the end of a
fill than at the beginning.
Third observation
the next fill gives about the same count as for the previous fill.
Forth Observation
On the C2 counts (blue), we can
see a slight fluctuation that seems to be periodic and doesn't
correspond to the
automax.
This is not really seen in the C4 counts (pink). That was also present
in the previous graph but at a lesser extent. We believe this is due to
a slight change in the orbit of the beam. The smaller collimator can
pick it out better than the 300 µm collimator. This should not
affect the scaling of data.
Next project; Monochromator's height.
The bourgandy line is what we are getting now. We can see that the
values for the small lambdas (0.9-1.1) are in the range of what we
expect. The Merit for the longer lambdas are not good at all.
To be done: The
mono
needs to be lowered.
23 March 2004
John Skinner has implemented CBASS
with
a supplementary harvesting
feature. When CBASS is started a file called i0.dat
is created in the main
directory. Every time a frame is collected the counts at C2, C3 and
C4, the ring current and the MERIT are harvested. These counts are for
1/10 sec as opposed to the usual 1 sec in the Optix window.
The HTML logger also will have the counts in.
Optimization of the slits
We are dealing with two issues:
intensity and stability. The Vslit and
the ladder slits have not been moved since the new orbit. This could
account for the lost of intensity on the beamline. The fact that I
don't get the right counts suggest that I am not in an optimum position
which could be responsible for the abnormal behavior of the intensity.
Vslit Optimization

I want to optimize the size of the
horizontal beam on the mono. The
idea
is to get as wide a beam as the mono can take without over heating the
xtal.
I am starting with the 2 dots collimator (300 µm) at lambda 1.1A.
I closed down the slit by a small increment (0.2 mm) and waited a
minute or two. Then I collected 4-5 frames in order to see how
reproducible the counts were. Considering that the mono takes
about 20-30 minutes to stabilize and that those points are separated by
about 20 sec, we should not see a big variation. We observe at first
that the counts go up as I close the Vslit down.
The four blue line are for the same Vslit value. The difference is just
a waiting period between taking the measurements. By the third
measurement, as I was looking at the shape of the beam on a phosphorus
paddle, realignment of the collimator in the hutch was clearly
needed. That gave the forth blue series with better counts. I continued
closing the slit until the counts start going down again. That mean
that I am cutting the beam smaller than the width of the xtal (last
yellow series). I will keep this last value.
Stability of the beam

Each data point is for 90 sec frames with the
pause on dump ( CBASS detects
when the beam has dumped, pause the data collection, wait 15 minutes
after the beam is enable again, realign, backs up one frames and
recollect) and
automax
(realign macro activated) every 30 minutes. We can locate where the
automax occurred since we have a point with a counts of zero where a
dark was taken.
First observation the
automax doesn't
improve the counts during a normal data collection. The hutch setup
doesn't need to be realigned.
Second observation
the counts are slowly dropping from the beginning of the injection to
the dump of the beam. We do not have more intensity at the end of a
fill than at the beginning.
Third observation
the next fill gives about the same count as for the previous fill.
22 March 2004
It seems like some PRT users are
unhappy about the
stability of the beam.
The frames were taken at 500 mm and show about 5-6 spots at very low
resolution, ~17 A. The background is ~300 for the first frames
while ~250 for the last frame of the data collection.
I called Tony
Lenhard and he says that’s possible that the Ir/Ga coating in between
the xtal and the copper block reacted over time. The contact would then
be less efficient and affect the cooling of the xtal. This phenomenon
has been seen happens over
a long
period of time. This mono is old and it would be a more plausible thing
than the Ir/Ga dripping off as Bob suggested.
Howard, Tony Lanzirotti and I went in the hutch to see if we had any
problems with the cooling. We can see water flowing from the
gravity tank and both proteus (cooling loop of the tank and mono) are
turning.
The slits are also water cooled and the proteus are turning.
19 March 2004
Photon
shutter
Howard had problems centering
his xtal. They were so small that there was no diffraction in one
direction (the side view of the loop as oppose to the flat view. He
finally was able to center the xtal and collected (1 dot collimator).
His scaling shows that the intensity went up over a period of 10 hours.
Howard thinks that there is a cooling problem with my mono.
Monochromator’s height:
trying
to get the Merit to expected values
Since the last maintenance period, I
sometimes get ½ to ¾
of the MERIT I expect according to my standard curves. It varies
from one injection to the other.
I troubleshoot the mono’s height with Ming. We had the 1 dot
collimator. We watched the counts stabilize on C2 (collimator). We did
some realign but no tilt scans. We moved lambda from 0.9 to 1.6A to see
if the MERIT followed the calibration curves. The merit looked ok but
not great for short lambdas. It followed the shape of the curve but
with smaller values. We lowered the mono by ¼ turn and it made
things worst. We raised the mono back to its position plus ¼
turn. It marginally
improved the merit at 1.2 A and didn’t make it worst at 1.0 A. We
raised it again by ¼ turn and it barely made any difference. We
let it in that position. Howard will collect (px04-082).
18 March 2004
Photon shutter
The photon shutter is sluggish to
respond since
coming out of maintenance. It finally died.
John Gallagher from interlock was called and he diagnosed a faulty
solenoid. It was replaced during normal operation within an hour after
lunch.