Difference between revisions of "SHMS Optics Working Group"
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! SHMS angle !! HB Bdl (As built) !! HB Bdl ( with wedges) | ! SHMS angle !! HB Bdl (As built) !! HB Bdl ( with wedges) | ||
|- | |- | ||
− | ! 5.5!! 117 Tm !! | + | ! 5.5!! 0.117 Tm !! 0.070 |
|- | |- | ||
− | ! 10 !! | + | ! 10 !! 0.035 !! 0.0109 |
|} | |} | ||
Revision as of 09:27, 31 March 2016
Weekly Meetings
- Meetings will be held on Thursdays 11:30-12:30 in F228.
- Next meeting March 31st.
- Join by Bluejeans by phone and computer +1.888.240.2560 (US Toll Free) Enter Meeting ID: 653182486
Notes from March 10th meeting
- Need to check whether the beam pipe will allow one to go to 8-9.5 degrees. (Dave Gaskell will look into this.)
- Using the 2nd plan configuration of the initial beam pipe ( SHMS to about 10, HMS to 10.5) it was checked by Dan Young that SHMS could go to 9 degrees drawing of beam pipe region.
- Get the Q1 mapping information from Steve Lassiter.
- See SHMS Q1 Section
- Need to keep track of detector surveys. Contact Bert Metzger.
- Put code for setting field on wiki.
- Double check to understand why there is a 0.7% difference between field at +3900A and -3900A.
- The probe readings had not been corrected for non linearity in probe. Plot with correction shows less than 0.2% difference over all currents that drops to .02% at 3900A.
- Change the effective length of HB by 4% to see effects on the optics. Look at sieve.
- Need table for conversion of all magnet currents to momentum.
- See HB and Q1 sections
- Check with Steve Lassiter about what is exactly thinking of using to mitigate the HB stray fields. Wedges + C-section + iron pipe?
- See [] . C-section has a minimal impact on field.
- Work on run plans. (Rolf and Tanja)
Preparation plans
- Magnets.
- Determination of B versus I curve. Develop new code for setting SHMS. Revise HMS field setting codes.
- Cycling procedure especially for HB. Look what is done for the HMS.
- Double check that the magnet field between magnets are superpositions.
- Survey of the positioning of magnets.
- Carbon elastics at 2 pass.
- Survey of collimators, detectors and beamline components.
- Survey of HMS/SHMS pointing at different angles. Look into what was done in the past for HMS commissioning. Determine a list of angles for survey.
- Need to come up with the sieve pattern as a function of quad settings.
- Need to look at use of ideal dipole versus TOSCA field map for HB in COSY.
- Checked with Howard about the quad field centering. The idea that Howard had didn't work. Need to rely on mapping data.
- Integration of detector checkout and optics.
Carbon elastics
- Results from Dipangkar for 1 pass- 2.2 GeV, and 2 pass -4.4 GeV). Measurements at 8-9.5 are doable.
- Using the 2nd plan configuration of the initial beam pipe ( SHMS to about 10, HMS to 10.5) it was checked by Dan Young that SHMS could go to 9 degrees drawing of beam pipe region.
SHMS HB mapping
- A Lakeshore Hall probe was used for the mapping measurements. The probe has a linearity error as a function of magnetic field which was measured by the company ( Table of data). This linearity error is different for positive and negative field directions. In the data table, the Error = abs(Measured Field)-abs(True Field). So for positive fields True Field = Measured Field - Error. For negative fields True Field = Measured filed + Error.
- Document and plots about mapping of B versus I at center of HB bore and the fringe fields in the beam region.
- B/I versus I plot.
- Measurements of B at bore center versus I when ramping magnet from 0 to +3900 and back to 0. Then switch polarity and ramp from 0 to -3900 and back to zero.
- plot of absolute difference between B when ramping magnet up and down versus I when going to +3900 and -3900.
- plot of relative difference between B when ramping magnet up and down versus I when going to +3900 and -3900.
- Plot of difference in B between ramping up to +3900 and ramping up to -3900 versus current.
- When ramping to negative currents there was a trip at I= -3139A. Plot of difference between first ramp to -3139A and the second.
- Document and plots about mapping Of B versus z for five different x,y locations (center,top,bottomleft and right) for I = 2000, 3000, 3500 and 3900A.
- Table of momentum versus current:
Momentum (GeV) | Current (A) |
---|---|
3.687 | 1200 |
6.110 | 2000 |
8.967 | 3000 |
10.283 | 3500 |
11.277 | 3900 |
SHMS HB Fringe fields
- NIM article on the TOSCA calculations of SHMS fringe fields effects on the ebam and mitigation.
- Drawing of beam pipe region. Presentation with more drawings of beam pipe configurations.
- The integral Bdl along the beam line for different angles of SHMS set at 3900A with and without wedges.
SHMS angle | HB Bdl (As built) | HB Bdl ( with wedges) |
---|---|---|
5.5 | 0.117 Tm | 0.070 |
10 | 0.035 | 0.0109 |
- At 10 deg the fringe field from Q1 and Q2 is very small. theta_b = .299*.0109/11. = 0.0003 and displacement at the beam dump (50m upstream) is
SHMS Q1 mapping
- Report on the analysis of the Q1 mapping data.
- Plot of B versus I compared to OPERA.
- Table of momentum versus current:
Momentum (GeV) | Current (A) |
---|---|
6 | 1228 |
8 | 1672 |
10 | 2169 |
11 | 2454 |
HMS and SHMS Dipoles
- Pdf version of the HMS field setting program.
SLITS and COLLIMATORS
SHMS Detector Positions
- Detector_Locations_in_SHMS location
SHMS Characteristics
SHMS Drawings of magnets
Study of the SHMS resolution
- Study of the SHMS resolution.
Old HMS information
- HMS Detector survey information,Magnet location surveys
- File with B/I data and plots for dipole and quads.
- Document about dipole field measurements.
- Dipole Transfer Function which compares Tosca and measurements at probe and center.
- Q1 Transfer Function plots and data
- Q2 Transfer Function plots and data
- Q3 Transfer Function plots and data
- Note by Dave Mack on dipole current regulation.
- Plot of Q2 predicted waist versus momentum for effects of zero offset.
- Plots of quads effective field length.
- Plots of quad fringe field.
- Plot X_fp versus momentum.
SNAKE
Moved Snake section here.