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Janurary 12, 200 5 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

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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

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Page 1: Why is this important?

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

Page 2: Why is this important?

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

Page 3: Why is this important?

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

Page 4: Why is this important?

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

Page 5: Why is this important?

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

Page 6: Why is this important?

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

Page 7: Why is this important?

Janurary 12, 2005 Dave Johnson RR Dept Meeting 7

Corrector Currents for Smoothed Orbit

.027*117 ur/A = <3.1 ur> inside

Page 8: Why is this important?

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

Page 9: Why is this important?

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

Page 10: Why is this important?

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

Page 11: Why is this important?

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

Page 12: Why is this important?

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

Page 13: Why is this important?

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

Page 14: Why is this important?

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

Page 15: Why is this important?

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