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Why is this important

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Reduce feed down from quad and sextupole in gradient magnet ... After Stan's vertical aperture scan. Centering in physical aperture. Janurary 12, 2005 ... – PowerPoint PPT presentation

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Title: Why is this important


1
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
  • 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 BPMs were specified to lay on the central
    trajectory with dp/p as zero
  • The BPMs/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.

2
Recycler BPMs (do we trust them?)
  • Factors in absolute BPM readings
  • Data for individual channels
  • Survey offset
  • Electrical center of plates
  • Electronic offset (cableselectronics)
  • 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 m 0.001mm , s 0.041 mm
  • V m 0.002 mm, s 0.022 mm
  • Roll m -0.024mr , s 0.201 mr
  • BPM/beam pipe optical survey
  • PLOTS to the right -gt
  • Parallel offset to mini straight as defined by
    up/down stream gradient magnets/quads (using
    sagatti corrected offsets)

Results of global BPM survey 2001
/- 1.6 mm
Horizontal
/- 1 mm
Vertical
BPM Survey Offsets installed in front end
O
3
Our Current Operational Orbit
rms 7.3 mm dp/p 0.0013 Xmax 16 mm
rms 1.38 mm aveg -.174mm Xmax 16 mm
After Stans vertical aperture scan
Centering in physical aperture
4
Corrector Settings for Current Operational Orbit
-.30573 ur/A lt22.3 urgt down
.157117 ur/A lt18.4 urgt inside Q corr / q
dipole 0.001
5
Smoothed and Centered Orbit
  • 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

S
Known Offsets
  • Closed injection to same eff

rms 3.7 mm dp/p 0.0002 Xmax 2 mm
  • First pass at adj tunes
  • Admittance gt 90 p
  • Coupling/chromaticity
  • NOT adjusted

First pass
6
Recycler frequency change
  • RF freq 52809500 -gt 52809000 (only approximate
    now)
  • Revolution freq reduced by 0.85 Hz (89812.0748
    Hz -gt 89811.2244 Hz)
  • Revolution period reduced by 105 ps
  • dp/p (RR) -0.0011 (h -0.00851)
  • 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)

7
Corrector Currents for Smoothed Orbit
.027117 ur/A lt3.1 urgt inside
8
Dynamic Aperture
Working point (.425, .415) for this calculation
Chromaticity -2 units
D
dp/p 0.003
25.5 mm
Current central orbit dp/p .0014 Typical
dp/p(90) /-.0015
38.25 mm
TM-2134 Meiqin, et.al.
9
Working point
Current Operating Point Qh .414-.415 Qv .412
For x -10, And dp/p .0015 Dv /-0.015 each
plane (into 5th and 7th)
x
For x -2, And dp/p .0015 Dv /-0.003 each
plane (into 12th)
Approx. tune spread for x -10 shown on plot
For dp/p of .0015 maximum x to avoid 5th and 7th
order resonances
10
Current Momentum Aperture
12/3/04
52809500
52810250
52808750
1250 Hz
2500 hz
3000hz
dp/pgt0 dn lt 0
dp/pgt0 dn gt 0
Data taken by Stan Extinguish points are
52805750 and 52813300 for momentum aperture of
/- about 3800 Hz. MI is not ramping for this
data, H and V chromaticity is about -2.5 unit.
11
Tunes
Qh .414 Qv .415
Current Orbit
Smoothed Orbit
Currents 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 _at_ 0.027 T/A PM quad
4/half-cell _at_ .85 T ? trims contribute 1.6 of
focusing at 1 amp
12
Bare Machine Tunes
Design .425/.415
Measured Harm .4269 / .4022
Nov 30, 2004
Qh .4099 Qv .4310
January 11, 2005
VSA (uncorrected)
Qh .4131 Qv .4393
Schottky
Qh .4216 Qv .4349
13
Horizontal Admittance
A 0.022329.52/52 A gt 90 p-mm-mr
21.7 mm
22.3 mm
Operational orbit
Smoothed orbit
14
Our Current Operational Orbit
gtr 19.968
  • 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 -(1/h)Df/f
Dp
h(1/gtr2 1/g2) h -0.00851
15
What Needs to be Done
  • 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 lt .1mm / 5A) - Jan 11
  • Adjust coupling (whats the source)
  • Adjust chromaticity
  • Determine momentum aperture
  • Determine source of bare machine tune shift
    (DnX -.0034 , Dny .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
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