- Overlap Integral Fits done using 20130205_1627/fit_parameters_input.dat on shift - the previous week's M2.
- Overlap Integral Fits done using 20130210_1637/fit_parameters_input.dat for post shift analysis of quad scan
20130207 Shift
Plans
Accelerator
- SAVE OPTICS!!!!
- Increase charge to ideally between 0.7 and 1.0
- Spend a little time to optimise linac / transport for higher charge and stability
Optics
- Load Lw optics
- Upstream steering to minimise background (before FF)
- Vertical Dispersion measurement / correction at LWIP - using Glen's FS tool. Measure after correction as well to verify - sometimes takes more than once
- Coupling correction - using upstream OTRs?
- Steer to centre of QM16FF
- BBA QM16,15,14,13 and 12FF - manual or using Glen's FS tool
- Most importantly 14, then 15, but ideally both.
- Reduce ipangle to < 100urad in both dimensions
- Check background
OTR
- Verify vertical beam size
- Quick quad scan to optimise QM14FF strength
- Update horizontal size in EDM
CBPM Resolution Logs
- Move chamber until MFB2FF not saturated - ie at minimum ADC counts - use CBPM panel
- Log 5 sets of CBPM data using CBPM EDM - 500 pulses per set - for resolution measurements
- Vertical Dispersion measurement / correction at LWIP - using Glen's FS tool. Measure after correction as well to verify - sometimes takes more than once
Laser-wire Startup
- Spatial Alignment
- Temporal Alignment
- Optimise, Vertical, Phase, Horizontal; repeat.
- Charge ramp - Log 1000 pulses on collisions
- Laser ramp - Log 1000 pulses on collisions
- Charge ramp - Log 1000 pulses off collisions (ie laser off but same position)
PLIC Detector
- Turn up vertical scale on PLIC and compare laser on laser off on collisions - anything at all?
Data Synchronicity
- While on collisions, block laser beam upstairs for a couple of pulses; repeat about 10 times in 500 pulse log
- Use single shot mode of accelerator to fire one electron bunch during say 500 pulse log; repeat about 10 times
- Check syncrhonicity of refc1amp, cherenkov, laserenergy, photodiode
Laser-wire Angular Dependence
- Back on collisions
- Move QM14FF on movers slightly to affect angle at LWIP - need to make large steps in angle +- 200urad in angle
- Compare laser on, laser off signal to background ratio at each point with two separate logs
Scans
- check optimisation of laser-wire via
- Phase scan
- Long range horizontal -2200 -> +2200 chahor, 80 steps, 15 samples at each
- Vertical scan - usual - 70 points, 20 samples
- Vertical scans at +- 25um, 50um, 75um, 100um horizontally - may need to use linear scan for larger ones at sides as nonlinear too narrow
MFB2FF Alignment
- Save positions for optimal laser-wire position - 100 pulse log (for bpm information)
- Move chamber for best MFB2FF position
- Save positions here - 100 Pulse Log
The Almighty LW Quad Scan
- NOTE quad scan should go in order - NOT middle first, then out, to avoid hysteresis or drift of accelerator effects in results
- Save accelerator set file at beginning!!! for e beam modelling purposes!
- 11 point quad scan
- Centre +- 1,2,3,5,7A on QM14FF
- At each point:
- Horizontal scan -2000 -> + 2000, 50 points, 10 samples -> move to centre at end
- Small linear vertical scan to centre properly
- Nonlinear vertical scan - 70 points, 15 samples
The Almighty OTR Quad Scan
- Repeat above quad scan, but with OTR images
- 3 samples at each magnet current
RELOAD OPTICS
- Save our optics!
- Quads
- Steering
- Optics save again
On Shift
The Best Laid Plans...
Laser build up time had increased yesterday, but not significantly. I have avoided using the laser due to damage on the etalon and this only gets worse with use. Today, the build up time was much longer again. The maximum output from the regen is 4mJ, which is very low. Slight tweaks really didn't improve it at all. Tried various pockel's cells timing, but no improvement. Removed etalon and unseeded regen output is 17mJ, which is down from last week's 24mJ. So, likely cavity is also degrading, but still expect around 12/24mJ (with etalon / without etalon - last week) out, which would be around 8.5mJ with etalon.
Further damage is evident on the etalon in the new position and there isn't much space to move the laser beam anywhere else.
So, current regen output around 4.2mJ. Maximum output from laser around 70mJ upstairs.
Took access and checked alignment downstairs - corrected slightly. Tweaked green upstairs on energy meter.
Optics
Loading set file
***.dat. Changing magnets QM15,14,13,12FF.
- Laser-wire signal attenuation was 9dB last week to take best advantage of ADC range. Typical background level was 8800 ADC counts.
- Changed attenuation to 14dB - aim for 5000 ADC counts background with this attenuation or lower.
OTR
- Horizontal (otr switch) scan with focus scan at each location
- Focus Scan
initial position ip:otrlens:z 14.25000, scan range: 12.4 - 14.4, step: 0.1 mm, best position - 13.4000
- OTR Focus Scan:
scan range QM14FF: -80 - -100 A, step 2.5 A, best position: -89.37171
- quad.jpg:
01:30 LW
- Positions saved after OTR and before LW alignment - 20130208_0126_pos.dat
02:00 Alignment
- Set manipulator to 8820 (where laser was before)
- Vertical & Horizontal scans with chamber -> look at wire-scanner detector
- Set V:185, H:250
- Timing ok - Set voltage to 5.0V
Horizontal Alignment |
Vertical Alignment |
|
|
- Initial scan - collisions!
- Within 20um of aligned position.
- Signal:Background ~ 1:8 so not great, but visible
- Laser energy downstairs is estimated to be 33mJ post-ip although this is a slight underestimate
- Comparing to previous shift, signal to background is approximately the same accounting for lower laser energy
Phase Scan
Initial Collision Scan
Laser-wire Vertical Scan
Laser-wire Horizontal Scan
Laser-wire Phase Scan
Phase scan suggested a voltage of 4.47V and we set to that. Then repeated vertical scan, but signal vastly reduced. Setting back to original 5.0V and rescanning vertical.
- Charge dropping off - Mod #2 very sensitive. Alex retuning linac
- Signal was dropping off despite returning to same position - not clear what's happening
- Laser energy the same both before and after LWIP (photodiode & laseren)
Things got worse...
- Phase, Horizontal, Vertical again...
- Phase set to 4.74V, Horizontal set to 62. Vertical scan nonlinear about chaver:151, 60 points, 20 samples
- Vertical scan quite good!!! Shows 1.7 +- 0.23um. Larger size before must have been due to horizontal offset.
- Amplitude 0.72 vs background 4.2
Re-aligned Proper Vertical Scan |
Apparently small... |
|
|
More Sensible... |
Pretty Good |
|
|
Horizontal Slicing
- Centre is chahor:62
- Using cherenkovcnbgslen
ChaHor |
Filename |
Size |
62 (centre) |
20130208_0418_lws |
1.71 +- 0.26um |
72 |
20130208_0437_lws |
0.73 +- 0.23um |
82 |
20130208_0453_lws |
1.73 +- 0.25um |
92 |
20130208_0504_lws |
1.23 +- 0.18um |
* Not showing clear dependence -> step size too small. Also better to take a few scans at each location.
* 62, +-50, +-100 -> 3 scans as each location
ChaHor |
Filename |
Size |
62 |
20130208_0418_lws |
1.71 +- 0.26um |
62 |
20130208_0517_lws |
2.35 +- 0.16um |
62 |
20130208_0527_lws |
2.63 +- 0.18um |
72 |
20130208_0536_lws |
1.50 +- 0.2um |
*set file: set13feb080608.dat
LW Quad Scan
- Vertical Linear - 20 steps - 10 samples - +-20um
- Horizontal Linear - 30 steps - 20 samples - +-700um
- Vertical Nonlinear - 50 steps - 20 samples - default range
- Repeat above pattern for each quad setting.
- After each scan, set that axis to its centre
- Do quads in order to avoid hysteresis or beam wander effects
QM14FF |
FilenameV |
FileNameH |
FileNameNL |
80 |
20130208_0614_lws |
20130208_0618_lws |
20130208_0631_lws |
84 |
20130208_0639_lws |
20130208_0643_lws |
20130208_0653_lws |
86 |
20130208_0701_lws |
20130208_0712_lws |
20130208_0723_lws |
88 |
20130208_0730_lws |
20130208_0732_lws |
20130208_0742_lws |
89 |
20130208_0750_lws |
20130208_0752_lws |
20130208_0802_lws |
90 |
20130208_0810_lws |
20130208_0812_lws |
20130208_0822_lws |
91 |
20130208_0829_lws |
20130208_0832_lws |
20130208_0842_lws |
92 |
20130208_0849_lws |
20130208_0852_lws |
20130208_0902_lws |
94 |
20130208_0910_lws |
20130208_0913_lws |
20130208_0923_lws |
96 |
20130208_0930_lws |
20130208_0939_lws |
20130208_1010_lws |
100 |
20130208_1019_lws |
20130208_1021_lws |
20130208_1031_lws |
Reanalysis post shift in table below
QM14FF |
Vertical Fit |
Horizontal Fit |
NonLinear Using s_ex = 235.0 |
Nonlinear using s_ex = horizontal |
80 |
5.21 +- 0.84 |
202.2 +- 9.1 |
6.1 +- 0.3 |
6.27 +- 0.33 |
84 |
2.29 +- 0.6 |
138.1 +- 9,3 |
5.0 +_ 0.3 |
6.25 +- 0.32 |
86 |
5.39 +- 0.44 |
162.0 +- 6.3 |
4.26 +- 0.3 |
5.21 +- 0.34 |
88 |
1.23 +- 0.27 |
192.5 +- 6.2 |
3.0 +- 0.4 |
3.39 +- 0.38 |
89 |
1.38 +- 2.02 |
161.7 +- 12.6 |
1.3 +- 0.6 |
2.18 +- 0.47 |
90 |
1.5 +- 1.05 |
174.4 +- 13.1 |
3.1 +- 0.5 |
3.67 +- 0.44 |
91 |
1.14 +- 1.44 |
304.4 +- 43.1 |
3.2 +- 0.5 |
2.59 +- 0.58 |
92 |
1.86 +- 0.83 |
150.3 +- 9.0 |
0.74 +- 0.5 |
1.91 +- 0.31 |
94 |
2.35 +- 1.05 |
184.2 +- 9.5 |
2.11 +- 0.4 |
2.64 +- 0.40 |
96 |
1.38 +- 2.02 |
200.8 +- 13.1 |
5.12 +- 1.24 |
5.54 +- 1.37 |
100 |
4.96 +- 1.53 |
201.6 +- 45.5 |
3.74 +- 1.30 |
2.52 +- 1.40 |
- 20130208_0701_lws - problem with this file
The uncertainty on the sigma from the initial vertical scans is obviously very high (and even unphysical), however, the purpose of this scan is purely to determine the centre vertically for the best horizontal scan and although there is insufficient data for an accurate vertical vertical measurement, the reduced data provides a quick scan and sufficient data to ascertain the vertical centre to within a few microns - adequate for both the horizontal scan and the subsequent non-linear vertical scan.
QM14FF |
Vertical Fit |
Horizontal Fit |
Nonlinear using s_ex = horizontal |
80 |
|
|
|
84 |
|
|
|
86 |
|
|
|
88 |
|
|
|
89 |
|
|
|
90 |
|
|
|
91 |
|
|
|
92 |
|
|
|
94 |
|
|
|
96 |
|
|
|
100 |
|
|
|
- quad_LW.png:
- Log on collisions with charge varied
- Log on collisions with laser energy varied
- Log with no laser for background
OTR Quad Scan
Corresponding OTR quad scan to LW scan. Three samples at each point. Repeat in same order as laser-wire.
- quad_OTR.png:
- Laser-wire optics saved - set13feb08_1102.dat
- Restored previous ATF2 optics set13feb07_19
Quad Scan / Shift Analysis
Firstly, having a look at the vertical sigma from both the quick linear vertical scans for centring and the full resolution nonlinear vertical scans. There isn't the clear parabola that one would ideally expect from a quad scan. However, there is an approximate minimum. From the scans above it is clear that the signal to noise ratio is too low near the end of the quad scan - due to degraded laser energy at the end of the shift as well as the accelerator conditions changing as the machine heats up in the day.
Next, the horizontal sigma. This shows no clear pattern and changes quite dramatically through the quad scan.
Having a look at the centre of the horizontal and vertical scans, the vertical has a clear and linear sweep in centre throughout the quad scan, however, the horizontal centre shows no clear trend.
From this quad scan it is clear that the time for scans must be minimised. The quick vertical scans for alignment produce reasonable results due to the short time they are recorded over and therefore the consistency of experimental conditions. The high resolution nonlinear scans obviously have a lower uncertainty, but this could be even lower if the beam / conditions were more consistent throughout the scan. Swings in charge normalised background can be seen in the raw data for the quad scans (above ones are background subtracted - linear model between first and last 5% of data). This is linked directly with tuning of the linac. The linac energy is unstable on the timescale of about 5 - 15 minutes, which is the approximate timescale for a detailed laser-wire scan. The horizontal laser-wire scans are the longest purely due to the distance required for the chamber to travel. It is unlikely that we can change the behaviour of the linac so therefore we must shorten scan times.
All of this is because there is some dispersion at our location. Changes in the energy affect the size and the position of the beam. Therefore, even without touching the linac during a scan, it will still drift and we'll be sensitive to it. Dispersion must be at least measured and ideally corrected. Furthermore, the beam based alignment wasn't performed so there was a clear drift in position with change in magnet strength.
It is also possible that the beam is coupled coming into the LWIP area. In this case, the quad scan would rotate the beam as well. If the rotation angle is on the order of about 20mrad, the projected beam size by the laser-wire will be almost double its original value - dependent on proportions of electron beam of course and the unknown angle between the laser-wire axis and the nominal electron beam axis.
Analysis files were put in 20130213_1436_qwd in ana directory manually.
Improvements to be made
- Software to automatically analyse the quad scan from a list of files for each scan type
- ControlPlot2 showing cherenkov, cherenkovcn, cherenkovcnbgs, cherenkovcnbgslen
- Increase horizontal chamber speed to 50um/s - currently 20um/s to at least halve horizontal scan time
- Don't tune linac during any scan - if transmission drops off - stop scan, fix, repeat scan
- Perform Dispersion measurement and correction
- Perform BBA on magnets around us
- Perform coupling measurement and correction