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Antonis Papanestis 1 Laser Alignment Laser Alignment Monitoring Monitoring System (LAMS) for the System (LAMS) for the RICH RICH Andrew Macgregor 1 , Paul Soler 1,2 , Gabriel Vidal-Sitjes 3 Antonis Papanestis 2 1 University of Glasgow 2 STFC, Rutherford Appleton Laboratory 3 Imperial College, London 2nd LHC Detector Alignment Workshop

1 Antonis Papanestis Laser Alignment Monitoring System (LAMS) for the RICH Laser Alignment Monitoring System (LAMS) for the RICH Andrew Macgregor 1, Paul

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3 Antonis Papanestis Laser alignment monitoring system  Requires 0.1 mrad resolution as seed for final software alignment  Monitors changes in selected mirror segments  Laser with optical fibre coupling system delivers light to 16 fibres.  Each fibre has a focusing unit at its end and is focused onto a mirror segment (4 spherical and 4 flat per side).  A beam splitter provides a reference beam for each fibre  All laser signals monitored by CCDs on roof of RICH2. Mirror Focuser Beam Splitter Spherical Mirror CCDs HPD Plane Flat Mirror Common Mounting Plate  Mirror alignment system for RICH2:

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Page 1: 1 Antonis Papanestis Laser Alignment Monitoring System (LAMS) for the RICH Laser Alignment Monitoring System (LAMS) for the RICH Andrew Macgregor 1, Paul

Antonis Papanestis 1

Laser Alignment Monitoring Laser Alignment Monitoring System (LAMS) for the RICH System (LAMS) for the RICH

Andrew Macgregor1, Paul Soler1,2, Gabriel Vidal-Sitjes3 Antonis Papanestis2

1University of Glasgow2STFC, Rutherford Appleton Laboratory

3Imperial College, London

2nd LHC Detector Alignment Workshop

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Antonis Papanestis 2

ContentsContents

1. Laser Alignment Mirror monitoring System (LAMS) for RICH2

2. LAMS for RICH1 3. Analysis software and resolution4. Conclusions

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Laser alignment monitoring systemLaser alignment monitoring system

Requires 0.1 mrad resolution as seed for final software alignment

Monitors changes in selected mirror segments

Laser with optical fibre coupling system delivers light to 16 fibres.

Each fibre has a focusing unit at its end and is focused onto a mirror segment (4 spherical and 4 flat per side).

A beam splitter provides a reference beam for each fibre

All laser signals monitored by CCDs on roof of RICH2.

MirrorFocuser

Beam Splitter

Spherical Mirror

CCDs

HPD Plane

Flat Mirror

Common Mounting Plate

Mirror alignment system for RICH2:

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Laser and fibre couplersLaser and fibre couplers Laser system:

Multi-mode connector can connect to 16 fibres All components commercially available

Multi-mode fibre connector

Fibre connector

Focusing Unit

100m Radiation-Hard 532nm Fibre

532nm CW 50mW Laser

Fibre-fibre connector

~10 m focal length

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Prototype systemPrototype system

Beam spot at 10 m

Prototype setup

Y2-1025 532nm mirror

Laser

Focusing Unit

Pulnix CCD Camera

Optical Bread-board

Diameter of beam Vs. Distance

0500

100015002000250030003500400045005000

5 6 7 8 9 10 11

Distance (m)

Dia

met

er (u

m)

3.5 mm

Focal length at 10 m gives optimal size at ~8m

CCD: 752(H) x 582(V) pixels withdimensions: 8.6m(H) x 8.3m(V)

Used single mode fibre (2 m core); Multi-mode fibre (200 m core) also tested.

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Test of mirror supportTest of mirror support Adjustment mirror support

and measurement mirror movement:

LT

R TR Hysteresis

Hysteresis

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Simulation of laser systemSimulation of laser system Implemented within Gauss (GEANT4) “Particle gun” to fire visible photons onto mirror segments Software implementation done in 2003-04. Recording plane (sensitive volume) on top of RICH2 to simulate

CCD. Observe movement of beam spot onto recording plane Linear transformation between tilt (x,y) vs movement of spot

on CCD (x,y) :x = A x + B yy = C x + D yCan recover tilts by inverting transformation after observing spotmovement.

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Component location processComponent location process

Flat Mirror

HPD Plane

Spherical Mirror

Particle gun(G4OpticalPhotons)

CCD

Flat Mirror

Spherical Mirror

Focusing Unit

CCD

Local Z axis

Global Z axis

Focusing unit and CCD are placed along the Local Z axis of the mirror segment (perpendicular to the centre of the segment).

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Mirrors monitored in RICH2Mirrors monitored in RICH2

01

5 4

3 2

9 8

7 6

10

17 16

15 14 13 12

11

25 24

23 22 21 20

19 18

27 26

282931 30

34 33 3235

3639 3738

43 42 41 40

4447 46 45

4851 50 49

5255 54 53

Positive x Negative x

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Flat mirrors monitored in RICH2 Flat mirrors monitored in RICH2

0 1 32

4 5 76

8 9 1110

12 13 1514

16 17 1918

20 21 2322

24 25 2726

28 29 31 30

32 33 3534

36 37 3937

Looking towards the interaction point

Positive xNegative x

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x (mm)

z (mm)

Positions of optical elementsPositions of optical elementsFocusing units (bottom)x (mm)

z (mm)

CCDs (top)

Plates installed FebruaryCCDs 11-14 July

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Mount holdersMount holders Mount holders (focusing

units at bottom): Mount holders (CCD at top):

Side view

Front view

Top view

Side view

Front view

Top view

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Position optical elementsPosition optical elements

10000

10200

10400

10600

10800

11000

11200

11400

-3000-2000-10000100020003000

10000

10200

10400

10600

10800

11000

11200

11400

-3000-2500-2000-1500-1000-500050010001500200025003000

Focusingunits:

CCDs:

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Lumenera (Ontario, Canada) Le175M monochrome camera: 1280x1024 CMOS sensor (1/2”, 7.7mm x 6.1mm) 1.3 M pixels, 6 m square pixels at 25 frames/s Ethernet connection Power: 9-24 V (< 4W) 300 g

Dose at y= +- 3000 m: < 6x10-14 Gy/collision x1.6x1014 collisions/yr = 10 Gy/yr = 1 kRad/yr (http://lhcb-elec.web.cern.ch/lhcb-elec/html/radiation_hardness.htm) Standard CMOS should be able to withstand this radiation.

SensorsSensors

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LAMS for RICH1LAMS for RICH1 System for RICH1 should be similar to RICH2, except in

horizontal plane rather than vertical plane Required accuracy 0.3 mrad Monitor 4 spherical mirrors (R=2700mm): 4 fibres + 4 CCDs, same laser as RICH2

CCD

Fibre &focalizer

splitter

Spherical mirrors

CCDs

fibre tips

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LAMS for RICH1LAMS for RICH1

CCD

Fibres

LAMS included inmechanical designs

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LAMS for RICH1LAMS for RICH1 Issue: radiation dose for CCD sensors in RICH1 x=700-800mm, y=+-275mm Dose: 10-12 Gy/collision x 1.6x1014 collisons/yr = 160 Gy/yr= 16 kRad/yr!! (http://lhcb-elec.web.cern.ch/lhcb-elec/html/radiation_hardness.htm) Off-the-shelf CMOS sensors rated to 1-2 kRad, so Lumenera

sensors not suitable. Thermo Sceintific CID8712D1M Radiation Hard Solid State Camera.

Dose up to 1 MegaRad. Separate sensor and readout electronics.

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RICH1 LAMS schematic diagramRICH1 LAMS schematic diagram

Front endElectronics(Balcony)

Video to ethernetserver Switch Readout PC

30 m

120 m

Special cable

Video coax

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Analysis softwareAnalysis software Analysis software needs to recover centre position of reference

and reflected beam with optimum accuracy and robustness. Beam not a perfect Gaussian so fitting method is not appropriate

for a variety of differently shaped beams Adopt a different approach using techniques borrowed from

image processing. Have a multi stage approach:

1. Smoothing filter2. Edge enhancement3. Sobel mask edge detection4. Hough transform accumulator to determine centre of beam5. Anomaly cut for spurious centre elimination6. Centre spot location mask7. Weighted average for centre determination.

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Analysis softwareAnalysis software1. Smoothing filter

Removes striations in image (dark and light diagonal bands) probably due to CCD aliasing effects.

Filter works by averaging blocks of 5x5 pixelsscanned over whole CCD:

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Analysis softwareAnalysis software2. Edge enhancement: cuts at > 60% and <80% of maximum

3. Sobel mask edge detection: 2D spatial gradient method using two spatial masks Finds magnitude: G=sqrt(Gx2+Gy2) and angle: =arc tan(Gy/Gx)

Gx Gy

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Analysis softwareAnalysis software3. Sobel mask edge detection (cont.)

4. Hough transform accumulator From Sobel edge, sum of image values along Sobel gradient angle. Central accumulator gives maximum at centre image

Gradient: ¦G¦

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Analysis softwareAnalysis software3. Sobel mask edge detection (cont.)

4. Hough transform accumulator From Sobel edge, sum of image values along Sobel gradient angle. Central accumulator gives maximum at centre image

Gradient: ¦G¦

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Analysis softwareAnalysis software4. Hough transform accumulator (cont.)

Can find centre outside detector:

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Analysis softwareAnalysis software5. Anomaly cut for spurious centre elimination:

Apply 70% cut on Hough accumulator Spurious maxima removal by selecting masks of increasing size (regions of interest)

6. Centre spot location mask:Finds region of interest around centre:

7. Weighted average for centroid determination.

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Analysis softwareAnalysis softwareFinal centroid finding result: robust algorithm that does not depend

on shape of beam

x

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Analysis softwareAnalysis softwareCan track difference between two beam spots, even if spots move:Accuracy of monitoring less than 0.01 mrads.

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ConclusionsConclusions Main design:

o Basic idea of laser alignment monitoring system well developedo System consists of 532 nm laser coupled to 16 optic fibres

attached to focusing units on bottom of RICH2. Readout to be carried out with CCDs on top of RICH2

o GEANT4 simulations have shown optimal positions for focusing units and CCDs 16 mirror segments in RICH2

o For RICH1, concept is the same except that CCD and focusing units on horizontal plane on either side of RICH1. Mechanical design includes shelves for LAMS.

Sensors:o Lumenera Le175 CMOS sensor 1280x1024 with ethernet readout

for Rich2o CID8712D1M Radiation Hard Solid State Camera for Rich1.

Multi stage image analysis software.