Outline Stability Requirements Feedback Implementation 1 Slow Orbit - - PDF document

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Outline Stability Requirements Feedback Implementation 1 Slow Orbit - - PDF document

Orbit Control at the SLS Storage Ring 26th Advanced ICFA Beam Dynamics Workshop on Nanometre-Size Colliding Beams (September 2-6, 2002, Lausanne) T. Schilcher Outline Stability Requirements Feedback Implementation 1 Slow Orbit Feedback


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SLIDE 1
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

Orbit Control at the SLS Storage Ring

  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop

  • n

Nanometre-Size Colliding Beams (September 2-6, 2002, Lausanne)

Outline

  • Stability Requirements
  • Feedback Implementation

1 Slow Orbit Feedback

  • Results of Slow Orbit Feedback
  • Upgrade to Fast Orbit Feedback
slide-2
SLIDE 2
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

SLS Parameters Stability Requirements

! ! !

Energy: 2.4 GeV RF frequency: 500 MHz Circumference: 288 m Emittance (horizontal): 5.0 nm·rad Vertical Beamsize @ ID (short straights): X10 µm (1% coupling) Beta functions @ short straights: horizontal: 1.4 m vertical: 0.9 m Source fluctuations < one order of magnitude below resolution of experimental stations angular stability: position stability: ∆Θ < 1 µrad

beam

1/10th of vertical beam size at location of insertion devices 1 suppress oscillations up to 100 Hz by factor of 10 1 µm in vertical plane

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SLIDE 3
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

72x72

A =

  • 1

1 72 1 72 bpm corr.

Feedback Strategy

! using all 72 BPMs and all 72 corrector magnets in each plane ! ! RF frequency as independent control parameter global orbit feedback based on SVD algorithm

Slow Orbit Feedback Fast Orbit Feedback

BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station

100 Mbit/s Ethernet

SLS Storage Ring beam dynamics server

central processing unit:

!

calculate inverted response matrix (SVD)

!

all BPM values

!

calculate correction

!

new corrector settings

!

use control system network read set

! !

processing and in the 12 BPM stations (6 BPMs and 6 corrector magnets per station) decentralized integrated

BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station BPM / Corrector Station

100 Mbit/s Ethernet

SLS Storage Ring beam dynamics server

40 Mbyte/s point-to-point fibre optic links

slide-4
SLIDE 4
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

Slow Orbit Feedback: Properties

! ! ! ! ! ! ! stroboscopic position readings with a rate of (BPM resolution < 0.5 µm) BPM server sends data to feedback client with a rate of sliding average of BPM data over a predefined no. of successive samples (default: 3) correction calculated on TRACY server toggle correction between x & y plane full correction cycle < 3 s ( ) running since Aug. 2001 3 Hz 2 Hz X0.4 Hz

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SLIDE 5
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

177 179 178 181 180

Results of Slow Orbit Feedback

beam current:

Example: 3 days run, 13 Aug 2002 - 16 Aug 2002

70 14 28 42 56 84

time [h] current [mA] 180 mA top-up

−3

∆I / I = 3.3E10

! top-up operation 1 thermal equilibrium of machine 1 nearly no drifts 1 no beam current dependencies of BPMs 1 constant heat load on experiments ! correct orbit to “golden orbit”

  • minimum coupling (beam based

alignment)

  • requested local bumps at ID
slide-6
SLIDE 6
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

Global Orbit Stability

70 14 28 42 56 84

time [h]

5 10 15 20 25 30 35

x (rms) [µm]

70 14 28 42 56 84

time [h]

5 10 15 20 25

y (rms) [µm]

number of samples @ 0.4 Hz

1 2 3 4 y (rms) [µm]

1 orbit globally stabilzed to micron level

1 2 3 4

x (rms) [µm]

number of samples @ 0.4 Hz

RF freq. corrections

Global RMS Values:

slide-7
SLIDE 7
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

Global Horizontal Mean Position:

70 14 28 42 56 84 time [h] x mean [µm]

5

  • 5
  • 50
  • 10
  • 45
  • 15
  • 20
  • 25
  • 30
  • 40
  • 35

RF frequency corrections

RF frequency corrections: if path length changes correspond to > 5 Hz frequency changes

  • number of samples @ 0.4 Hz
  • 3e-05

3e-05

  • 2e-05

2e-05

  • 1e-05

1e-05

  • 4e-05

4e-05

dp / p

  • 5

Energy Stability: G2E10

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SLIDE 8
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

RF Frequency Change:

1 day 1 day 70 14 28 42 56 84 time [h]

  • utside temperatures [deg C]

10 30 12 14 16 18 20 22 24 26 28

Outside Temperatures:

1 day 1 day 70 14 28 42 56 84 time [h]

∆f [Hz] ∆f = 5 Hz 1 ∆U Z 3 µm (circumference)

  • 1630
  • 1540
  • 1550
  • 1560
  • 1570
  • 1580
  • 1590
  • 1600
  • 1610
  • 1620
slide-9
SLIDE 9
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

x position:

RF BPM @ Insertion device 6S (protein crystallography beamline):

upstream BPM x position [µm]

5

  • 5

10

  • 10

15

  • 15
  • 20

70 14 28 42 56 84

time [h] y position [µm]

5

  • 5

10

  • 10

15

  • 15
  • 20

70 14 28 42 56 84

time [h] upstream BPM

y position [µm]

number of samples @ 0.4 Hz

  • 2

2

  • 4

4

σ = 0.65 µm

y

downstream BPM horizontal:

σ = 0.98 µm

x

vertical:

σ = 0.64 µm

y

y position:

x position [µm]

number of samples @ 0.4 Hz

  • 2

2

  • 4

4

σ = 1.04 µm

x

slide-10
SLIDE 10
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

Angular Stability @ ID

horizontal angle: vertical angle:

σ = 0.29 µrad

∆Θ

number of samples @ 0.4 Hz horizontal angle [µrad]

  • 1.5
  • 1
  • 0.5

0.5 1 1.5

σ = 0.19 µrad

∆Θ

number of samples @ 0.4 Hz vertical angle [µrad]

  • 1.5
  • 1
  • 0.5

0.5 1 1.5

slide-11
SLIDE 11
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002 8.6 17.2 25.8 34.4

time [h]

  • 80
  • 75
  • 70
  • 65
  • 60
  • 85
  • 90
  • 95
  • 100

y position [µm]

X-BPM Results

! X-BPM @ ! start of X-BPM commissioning: middle of Aug. 2002 ! data from 3 days run: 9 Aug - 12 Aug 2002 Protein Crystallography Beamline

  • 10
  • 5

5 10

number of samples @ 0.4 Hz x position [µm]

σ = 2.7 µm

x

  • 10
  • 5

5 10

number of samples @ 0.4 Hz y position [µm]

σ = 1.5 µm

y

! drift: X1.7 µm per day ! subtracting the drift

1

1

horizontal: vertical:

slide-12
SLIDE 12
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

Fast Orbit Feedback

Properties: ! ! ! ! !

!

update rate: BPM

  • nly between
  • ver point-to-point fibre optic links

(40 Mbytes/s) (1reflecting the localized structure of the inverted response matrix)

  • f magnet power supplies

(by-passing control system) global BPM data exchange < 8 µs implementing communication between beam dynamics server and individual BPM/feedback stations planned start of commissioning: Dec. 2002 (priority to multibunch feedback system) 4 kHz data exchange adjacent sectors direct control Status: Important Prerequisite: reliable BPM data 1 “intelligent” BPM software which detects faulty data and disables BPM 1already implemented for slow orbit feedback

slide-13
SLIDE 13
  • T. Schilcher

26th Advanced ICFA Beam Dynamics Workshop ,Sep. 2 - 6, 2002

Conclusion !

stabilized to in both planes with a rate of 0.4 Hz

!

to compensate path length changes

!

beam stability @ low beta insertion devices to (sub)micron level: position angle horizontal vertical

!

thermally stable machine only needs feedback when

  • moving IDs
  • changing RF frequency

!

fast feedback required in order to

  • compensate ID movements
  • suppress beam oscillations in the low

frequency band (<40 Hz) - if necessary global orbit 1 µm RF frequency control X 1.0 µm X 0.3 µrad X 0.7 µm X 0.2 µrad