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Microstrip PSD detectors

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Microstrip PSD detectors. C. Fermon, V. Wintenberger , G. Francinet, F. Ott, Laboratoire Léon Brillouin CEA/CNRS Saclay. Outline. Present state of the art at the LLB micro-strip detectors (MS) geometry electronics performances projects, problems and improvements Projects within TECHNI - PowerPoint PPT Presentation
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1 Microstrip PSD detectors C. Fermon, V. Wintenberger , G. Francinet, F. Ott, Laboratoire Léon Brillouin CEA/CNRS Saclay
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Page 1: Microstrip PSD detectors

1

Microstrip PSD detectors

C. Fermon, V. Wintenberger, G. Francinet, F. Ott, Laboratoire Léon Brillouin CEA/CNRS Saclay

Page 2: Microstrip PSD detectors

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Outline

Present state of the art at the LLB– micro-strip detectors (MS) geometry– electronics– performances– projects, problems and improvements

Projects within TECHNI– large size (300×300mm²) detectors

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Principle: charge division

Position determination :

Qa Qb

ba

a

QQ

QPos

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Microstrip geometry

Typical voltages: Anode 1000-1200VCathode 400V

– VAC max = 1000V; avalanche gain ~ typ. 106 (105- 107)

Use of the ILL geometry; line resistance = 6 kPitch 0.5 mm or 1 mm

Size : 100×100 mm² or 200×100 mm²Possible to make 200 × 200 mm²

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Detector casing

100 × 100 detector

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Gas Maximum pressure in the casing is 10 bars

– Flat Al window, 4-5 mm thick

Typically – 1.5 bar CF4

– 2-4 bar 3He (depending on the wavelength)

Use of indium seals (Cu or Al did not work) Pumping down to 10-7 mbar + etuvage at 80°C Purification of the gas:

nitrogen trap while filling the detector (for 3He) fractional distillation for CF4

In the future, use of oxygen getter(provided by SAES)

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Preamplifiers “Home made” charge amplifier (based on OPA621)

associated with a 50 line driver. Gain: 10 mV/fC (with an input capacitance of 20 pF)

– Small detector (100x100 mm²): 20 pF– Large detector (100x200 mm²): 40 pF

Output noise 15 mV Typical avalanche gain = 106 (at VAC = 900V)

– Output signal = 1 V

Rise time 1.3 µs; Signal length = 5 µs tests of (8) integrated charge amplifiers (from Delft, van

Eijk): smaller signals because of the high input capacitance

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Anodes and Cathode signals

5 µs

5 µs5 µs

500 mV

250 mV

500 mV

Anode 1

Anode 2

Anode 1Anode 1

Cathode 1

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Signals outputs dispersion

Energy (a.u.)

Cou

nts

(a.u

.)

Cathode signal

Dispersion 8%

Discriminationlevels

Anode 1 Anode 2

Width 15-20%

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Translation scan Scan over 100 mm with a 0.5 mm slit

Position (mm)

Inte

nsity

(co

unts

)

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Detector linearity (w/o correction)

0

20

40

60

80

100

120

0 20 40 60 80 100

Real position (mm)

Me

as

ure

d p

os

itio

n (

mm

)

Page 12: Microstrip PSD detectors

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Overall characteristics

Spatial resolution:– 1.3 mm on the small detector– 2-2.5 mm on the large detectors

Background noise:– 0.2 count per minute over whole detector (because of the good

discrimination)

Maximum counting rate:– 104 n/s without deformation of the peak. – 105 n/s if one allows a 5% error on the total counting.

Efficiency : 95% (2.5 bars at 0.4 nm)

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Time and flux stability

Time stability:– Small detector has been under vacuum for under 18

months: no deterioration of the output signals (amplitude nor

energy spectrum)

High flux illumination– has sustained a flux of 3×107 n/s for over 1 month

(fluence of 2×106 n/s.cm²)

Page 14: Microstrip PSD detectors

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Detector cost (w/o manpower)

Microstrip 1.4 k€ (double side)0.7 k€ (single side)

He3 gas 1 k€ (at 4 bar)

Casing 3 k€Electronics 3 k€

Shielding - (B4C)

2 HV Power supplyTOTAL 8.4 k€

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Short term projects (year 2000)

Use of the detectors (200×100) for the reflectivity spectrometer PRISM.(and later for EROS)

Building of a banana shaped set of 12 detectors for 7C2 (liquid and amorphous materials on the hot source)

Validation of the long term stability while in operation(but in a limited flux environment however)

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Problems and improvements

Large spread of performances between the MS plates:– gain varying by a factor of ten between plates– no explanation yet

Building of a standard interface (hardware and software) with the LLB electronics (Daffodil) => swappable devices

Improvement in the signal conversion: integration or averaging.

Band pass filters Use of FPGA components for processing and linearisation

(to replace the use of EPROMs.)

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Project within TECHNI Project: use of multidetectors for

Very Small Angle Neutron Scattering Large size (300×300 mm²) detectors set at a

distance of 8-10 m :– angular opening of 0.03 rad = 1.7°– angular resolution of 2×10-4 rad (= 0.02°)

(q = 5×10-5 nm-1 objects sizes of 1 µm)

Solutions– assembly of smaller detectors (200×100 mm²)– use of GEM and resistive plate

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Assembly of detectors

Set of 4 detectors (6 wires per plate)– spacing of 8 mm between the plates grids

300 mm

300

mm

Page 19: Microstrip PSD detectors

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GEM scheme

Gain 103

Two grids (total gain 106) associated with a resistive plate

Gain 103

Resistive plate

Top view

ne-


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