Performance of Laser Distance Sensors Ralph M uller February, 13 th - - PowerPoint PPT Presentation

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Performance of Laser Distance Sensors Ralph M uller February, 13 th - - PowerPoint PPT Presentation

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook Performance of Laser Distance Sensors Ralph M uller February, 13 th 2015 IMPRS PPSMC LS Schaile Ludwig-Maximilians-Universit at-M unchen February, 13 th 2015


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SLIDE 1

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Performance of Laser Distance Sensors

Ralph M¨ uller February, 13th 2015 IMPRS PPSMC LS Schaile Ludwig-Maximilians-Universit¨ at-M¨ unchen

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SLIDE 2

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Table of Contents

1

Motivation for ATLAS NSW Upgrade

2

Micromegas and sTGC Detectors for the NSW Upgrade

3

Principle of Topology Measurements

4

Performance of the Panasonic HLG-112-S-J

5

Performance of the microEpsilon ILD2300-20

6

Summary and Outlook

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SLIDE 3

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Atlas Detector

Atlas Detector 2018: New Small Wheel

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SLIDE 4

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Trigger Isue

Level 1 Trigger Rate

1 all L1 MU11 Triggers

(10 GeV muons)

2 reconstructed tracks with

PT > 3 GeV

3 reconstructed tracks with

PT > 10 GeV homogeneous distribution 90% false triggers in endcap region (|η| > 1) Extrapolated rate of L1 MU20: 60 kHz for design luminosity L = 1034 Close to bandwidth limit: 100 kHz

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SLIDE 5

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Reasons for High Trigger Rate

1/4 of ATLAS detector Sofar only Big Wheel included in L1 trigger including angular information After reconstruction a currently good µ-trigger in Big Wheel can be: A Track pointing to IP Correct muon track B No hit in Small Wheel e.g. proton faking muon C Track not pointing to Interaction Point e.g. background event

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SLIDE 6

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Reasons for High Trigger Rate

1/4 of ATLAS detector Idea False triggers can be sorted out by including the Small Wheel in the Level 1 trigger. ⇒ Upgrade of the Small Wheel, ∆θ ≤ 1 mrad

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SLIDE 7

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

New Small Wheel Assembly

Sectors of NSW disklike structure:

eight large sectors eight small sectors

Each sector subdivided into two detector units Detector unit: two quadruplets

  • f MM and sTGC each

trigger: eight layers of sTGC precision: eight layers of Micromegas SM2 to be built at LMU

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SLIDE 8

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Working Principle of Micromegas Detectors

Sketch of a MM Detector electronic single strip readout measure charge center σ < 50 µm need of a precise readout plane

pitch planarity drift gap amplification gap

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SLIDE 9

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Achieved Resolution

Resolution of Micromegas (Bortfeld, 2014)

(50 × 50 cm2 MM, 120 GeV Pions, H6-Beamline CERN, perpendicular beam)

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SLIDE 10

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

MM Construction as quadruplets

Sketch of a MM Quadruplet 1 quadruplet = 5 sandwhich panels Panel size ≈ 2 m2 (SM2) Planarity requirement 80 µm

  • ver 2 m2

About 160 surfaces to measure Measurment duration / panel: Tactile: ≈ 8 h Laser: ≈ 1 h

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SLIDE 11

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Sectors of the New Small Wheel

Small and large sector Red and Blue: sTGC’s: small strip Thin Gap Chambers for trigger Orange and green: Micromegas: micromesh gaseous structure for precision coordinate Structure of a single sector:

  • ne module sTGC
  • ne module Micromegas
  • ne module Micromegas
  • ne module sTGC

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SLIDE 12

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Sectors of the New Small Wheel

Small and large sector SM2: three readout boards per readout plane 1024 strips each 0.45mm pitch alignment requirement: 20 µm/2 m = 10−5

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SLIDE 13

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Glueing Process

Steps of the glueing process Two step glueing process Need precision needed during glueing Need to monitor the glueing process using the stiffback

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SLIDE 14

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Glueing Process of a Prototype

Glueing the first side Glueing the second side

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SLIDE 15

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Assembly of Four Mechanicle Prototypes in Freiburg

Mechanicle Prototype in Freiburg

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SLIDE 16

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Planarity Measurment Freiburg - Tactile

CNC - Measurment Freiburg CNC coordinate measurment system Topology Measurement of all five panels Sensor of CNC Machine

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SLIDE 17

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Result of Planarity Measurment in Freiburg

Topology of a Panel Grid visible 15 µm structure included intentiully for diagnostics ⇒ Planarity OK Edge effects outside active area

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SLIDE 18

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Laser Distance Sensor Using Triangulation

Scheme of Triangulation Known constants: a, a′, δ According to the scheme one gets α = 90◦ − δ − β ≡ δ′ − β (1) tan β = x a (2) sin α a′ = sin β z (3) Using (1), (2) and (3) one

  • btains

z = x · a′ a · 1 sin δ′ − x

a cos δ′ (4)

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SLIDE 19

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Available Sensors

Panasonic HLG-112-S-J microEpsilon ILD2300-20 Results obtained with both sensors mounted on a vertical translator will be displayed in the following slides

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SLIDE 20

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Comparison between Laser Sensor and Reference Measurement

  • quad. panel
  • quad. panel (ref)

50 × 54cm2 panel Differences caused by permanent deformation Time between measurments ≈ 0.5 a Laser based topology measurement seems aplicable

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SLIDE 21

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Semitransparent Surfaces measurable using Panasonic?

Measurement of Granite Table Granite table as reference surface Four line measurements along identical line:

Granite table: contains semitransparent crystals Kapton foil: 20 µm semitrsparent Aluminum: rough surface Teflon: smooth non transparent surface

⇒ Panasonic sensor not suitable for semitransparent surfaces

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SLIDE 22

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

microEpsilon Sensor

Spot size 40 × 40 µm2 specular reflection measurment mode (for semiransparent surfaces) 40 mm working distance ±10 mm

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SLIDE 23

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Topology of Calibration Profiles

Profile 1 Profile 2 Profile 3 Machined Aluminum Profile Possibility to measure very small deviations.

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SLIDE 24

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Sag of Aluminum Profile against Granite Table

Measurement of Granite Table Residuals of Granite Table Visible bending of aluminum profile Deviation from parabolic fit ⇒ additional non planarity

granite surface imperfection in alu profile

Overall planarity: σ = 4.6 µm

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SLIDE 25

Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Summary

Upgrade project of the ATLAS muon spectrometer Construction of SM2 modules at LMU Quality controll of the MM panel surface mandatory Non tactile, laser based measurements Panasonic Sensor HLG-112-S-J:

1

8 µm Resolution

2

Able to measure nontransparent surfaces

microEpsilon ILD2300-20:

1

0.3 µm Resolution

2

Able to measure semitransparent surfaces such as PCB or granite table

3

Smaller beamspot ⇒ strips can be resolved

4

total resolution of measurment system < 10 µm

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Motivation Upgrade Topology HLG-112-S-J ILD2300-20 Summary and Outlook

Thank you

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SLIDE 27

Backup

Planarity Measurment of Stiff-Back in Freiburg

Topology of Old Stiffback (E. Pree) Stiff-back shows a sag of more than 160 µm under its own weight Explanation of deformation of panels A more rigit stiff-back is needed for NSW production

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SLIDE 28

Backup

Micromegas Strip Pattern

Topology of Strippattern Topology of Strippattern

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SLIDE 29

Backup

Topology of PCB with Cu Strips

Topology of Strippattern Strip pattern with 203 strips and 450 µm pitch Measuring the strip pitch by

1

Distance between min / max µ = 450.8 µm; σ = 74.5 µm

2

Distance between falling edges µ = 451.1 µm; σ = 52.5 µm

Zoom Strip Pitch

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