Upload
gram
View
40
Download
0
Tags:
Embed Size (px)
DESCRIPTION
Defining a “Golden” Closed Orbit (smoothed ‘n centered). beams doc 1540. Why is this important? We want average corrector current to be zero (not contribute to central trajectory) Reduce feed down from quad and sextupole in gradient magnet - PowerPoint PPT Presentation
Citation preview
Janurary 12, 2005 Dave Johnson RR Dept Meeting 1
• Why is this important?– We want average corrector current to be zero (not contribute to central
trajectory)– Reduce feed down from quad and sextupole in gradient magnet
• Determine true tune/chromaticity/coupling from Recycler permanent magnets
– Match complex to true Recycler energy (w/o corrector contribution to average dipole field)
– Reduce/eliminate dependency on DC magnetic elements, use magnet moves to reduce corrector strength (0.2A max) and install PM quad trims in phase trombone
• Some statements– The Recycler central trajectory should be “as defined by the design lattice”.
– The BPM’s were specified to lay on the central trajectory with dp/p as zero
– The BPM’s/beam pipe were installed to centered on this central trajectory
– The gradient magnets were installed with a specific sagatti (and longitudinal offset) correction to minimize feeddown and maximize aperture.
Defining a “Golden” Closed Orbit (smoothed ‘n centered) beams doc 1540
Janurary 12, 2005 Dave Johnson RR Dept Meeting 2
• Factors in absolute BPM readings– Data for individual channels
• Survey offset • Electrical center of plates• Electronic offset (cables+electronics)
– Data for BPM type• Gain (mm/volt)
• In process of verifying gains/offsets installed in front end
• Rechecked lattice specification and survey technique
– Magnets survey w/ Laser tracker (not shown)
• Radial = 0.001mm , = 0.041 mm• V = 0.002 mm, = 0.022 mm• Roll = -0.024mr , = 0.201 mr
– BPM/beam pipe optical survey • PLOTS to the right ->• Parallel offset to mini straight as
defined by up/down stream gradient magnets/quads (using sagatti corrected offsets)
Horizontal BPM Set- Ideal
0
5
10
15
20
25
30
35
B P M Off s et [mm]
Recycler BPM’s (do we trust them?)
Vertical BPM Set- Ideal
0
5
10
15
20
25
30
35
40
45
B P M Off s et [mm]
+/- 1.6 mm
+/- 1 mm
Horizontal
Vertical
OBPM Survey Offsets installed in front end
Results of global BPM survey 2001
Janurary 12, 2005 Dave Johnson RR Dept Meeting 3
rms 7.3 mmdp/p 0.0013Xmax ~16 mm
rms 1.38 mmaveg -.174mmXmax ~16 mm
Our Current Operational Orbit
After Stan’s vertical aperture scan
Centering in physical aperture
Janurary 12, 2005 Dave Johnson RR Dept Meeting 4
Corrector Settings for Current Operational Orbit
.157*117 ur/A = <18.4 ur> inside
corr / dipole ~ 0.001
-.305*73 ur/A = <22.3 ur> down
Janurary 12, 2005 Dave Johnson RR Dept Meeting 5
Closed injection to same effrms 3.7 mmdp/p 0.0002Xmax ~ 2 mm*
Smoothed* and Centered* Orbit
S•Centered Orbit by Rfreq•Smoothed using R50 to select dipole/region for smooth•Not smoothed MI30 or MI60•Avoided LEP corr (for now)•Fixed positions thru known apertures
First pass at adj tunes
Admittance > 90
* First pass
Coupling/chromaticity NOT adjusted
KnownOffsets
Janurary 12, 2005 Dave Johnson RR Dept Meeting 6
• RF freq: 52809500 -> 52809000 (only approximate now) • Revolution freq: reduced by ~0.85 Hz (89812.0748 Hz -> 89811.2244 Hz) • Revolution period: reduced by ~ 105 ps• dp/p (RR) = -0.0011 (
• Impact on MI and complex– MI/complex energy reduced by ~ 8 Mev
• Impact on RR BPM– only 89 kHz and narrow band – Minor impact
• Schottkies– Mixdown frequencies
• Stochastic Cooling – delay times between pickup and kicker change by ~20 ps
• Electron Cooling• RF (low level wave forms)
Recycler frequency change
Janurary 12, 2005 Dave Johnson RR Dept Meeting 7
Corrector Currents for Smoothed Orbit
.027*117 ur/A = <3.1 ur> inside
Janurary 12, 2005 Dave Johnson RR Dept Meeting 8
TM-2134 Meiqin, et.al.
Dynamic Aperture
25.5 mm
38.25 mm
Dp/p = +0.003
Current central orbit p/p +.0014Typical p/p(90%) +/-.0015
Working point (.425, .415)for this calculation
Chromaticity = -2 units
Janurary 12, 2005 Dave Johnson RR Dept Meeting 9
x
Working point
Current Operating PointQh ~ .414-.415Qv ~.412
For = -10,And p/p ~.0015v = +/-0.015 each plane(into 5th and 7th)
For = -2,And p/p ~.0015v = +/-0.003 each plane(into 12th)
Approx. tune spread for = -10shown on plot
For p/p of .0015 maximum to avoid 5th and 7th order resonances
Janurary 12, 2005 Dave Johnson RR Dept Meeting 10
5280
9500
5281
0250
5280
8750
1250 Hz
Data taken by Stan… Extinguish points are 52805750 and 52813300 for momentumaperture of +/- about 3800 Hz. MI is not ramping for this data, H and V chromaticityis about -2.5 unit.
p/p>0 < 0
p/p>0 > 0
2500 hz 3000hz
Current Momentum Aperture12/3/04
Janurary 12, 2005 Dave Johnson RR Dept Meeting 11
Tunes
Current Orbit Smoothed OrbitCurrents: 0.427, 0.040, 0.489, -0.679, 0.172
Currents: 0.808, -0.239, 0.919, 0.016, 0.395
*No attempt to adjust coupling or chromaticity
Trims: 2/half-cell @ 0.027 T/A PM quad: 4/half-cell @ .85 T trims contribute 1.6% of focusing at 1 amp
Qh ~ .414Qv ~ .415
Janurary 12, 2005 Dave Johnson RR Dept Meeting 12
“Bare Machine” Tunes
Qh .4099Qv .4310
Qh .4131Qv .4393
Qh .4216Qv .4349
Schottky
VSA (uncorrected)
Nov 30, 2004
January 11, 2005
Design.425/.415
Measured Harm.4269 / .4022
Janurary 12, 2005 Dave Johnson RR Dept Meeting 13
Horizontal Admittance
22.3 mm
21.7 mm
Operational orbit
Smoothed orbit
A = 0.02232*9.52/52A > 90 -mm-mr
Janurary 12, 2005 Dave Johnson RR Dept Meeting 14
Our Current Operational Orbit
•Smoothed orbit with freq at 52809000 Hz •Increased freq back to 52809500 Hz•Orbit difference shows dp/p +0.0014•Contribution +0.0011 from freq change
Dp
p/p = -(1/)f/f
=(1/tr2 – 1/2)
= -0.00851
tr = 19.968
Janurary 12, 2005 Dave Johnson RR Dept Meeting 15
• Include all offsets in BPM front end (in progress) • Smooth orbit (reduce average corrector strength)• Determine quad moves to reduce largest correctors (MI30 and MI60)• Adjust freq to get a zero dp/p with average corr current zero.• Investigate apertures in MI60 and MI30 Center beam in phase trombone quads (H & V rms < .1mm / 5A) - Jan 11• Adjust coupling (what’s the source)• Adjust chromaticity • Determine momentum aperture • Determine source of “bare machine” tune shift (X =-.0034 , y =+.02)• Measure sensitivity of lifetime due to tunes• Re-tune injection/extraction (may require adjustments to closed orbit/counter-
wave in MI)• Re-adjust cooling/instrumentation to centered Recycler frequency• Match MI (and eventually the complex) to this new frequency/energy• Revisit MI ramp compensation
What Needs to be Done