/
ECAL electronics ECAL electronics

ECAL electronics - PowerPoint Presentation

jane-oiler
jane-oiler . @jane-oiler
Follow
368 views
Uploaded On 2015-12-11

ECAL electronics - PPT Presentation

Guido Haefeli Lausanne PEBS meeting 10Jan 2011 1 Overview SPIROCA in testbeam 92010 Jean Baptiste Why change from SPIROCA to VATA64 VATA64 measurements Plans for the electronics ID: 221639

large gain vata64 high gain large high vata64 spiroca range card measurement signal power adc dynamic chip channels baseline tps time ecal

Share:

Link:

Embed:

Download Presentation from below link

Download Presentation The PPT/PDF document "ECAL electronics" is the property of its rightful owner. Permission is granted to download and print the materials on this web site for personal, non-commercial use only, and to display it on your personal computer provided you do not modify the materials and that you retain all copyright notices contained in the materials. By downloading content from our website, you accept the terms of this agreement.


Presentation Transcript

Slide1

ECAL electronics

Guido Haefeli, Lausanne PEBS meeting 10.Jan. 2011

1Slide2

OverviewSPIROCA in

testbeam 9.2010(Jean-Baptiste)

Why change from SPIROCA to VATA64?VATA64 measurementsPlans for the electronics

for testbeam in 2011 2Slide3

Output dependence on the rate

A SiPM is illuminated with stable light pulses produced by a LED

(Light pulses are monitored with a PMT)

3Slide4

Baseline shift (fluctuation)

Pedestal spectra

4

Without common mode correction

After common mode correctionSlide5

SpirocA card problem causing oscillation

The shaping time settings (175ns) make the chip to oscillate, maybe also other settings have a negative effect on the stability. The settings were crosschecked with the Aachen electronics and are correct. Same chip module as on Aachen board used.

no hint where the problem is.

5Slide6

SpirocA

With the use of the high and low gain output on the two sides, 4 measurements for each event are taken.Why are high and low gain measurement required? Noise in high gain mode is too large for small signal measurement!

Difficult to calibrate Large baseline fluctuation for large signal. In the ECAL for large energy showers, order of 9 channels receive large signal, this

gives large baseline fluctuations.Difficult to remove this on the flight!Output dependent on the injection frequencyNo or very limited single photon detection possible with the ECAL detector, would be nice for calibration.

6Slide7

VATA64Very low noise, with one gain the range of 0..100pC can be covered. (see slide on dynamic range)

Therefore only two measurements need to be calibrated! Noise below one photon. Resolution restricted by the 12-bit ADC.No baseline fluctuation for large signals can be observed. Injection of 8 channels with large signal leaves

rms of neighbours unchanged.Single photon detection possible in high gain mode, this is useful for calibration.

Power consumption, some power saved by less drivers (only one gain output) and only half the number of cards. Reduction to current ECAL budget possible.7Slide8

Power consumption measurement

SPIROCA Pch=13mW,

Pcard=428mW, PECAL=51W (120 cards) (

A large fraction not used by the SPIROC but by the other components.High and low gain readout consumes power also in the ADC board (doubles the number of channels).

VATA64

P

ch

=23mW,

P

card

=1.5W, P

ECAL

=75W (50 cards)

Power saving options (shutting down fast shaper has to be implemented first)

Remove additional amp for debugging, power measured on the total card (~10mW/CH for the VA chip only)8Slide9

Dynamic range

Required dynamic range for the ECAL is

0..2000 photons. The number of effective pixels is below 2000, the detectable range should include some margin.

With the nominal gain (0.26Me/PE) this converts in a dynamic range

of

0..

83pC.

Since the

VATA64

offers a dynamic range of

0..50pC

a external current divider must be placed to reduce the signal by a factor 2.

The external

current divider

has only a very small or no impact on the noise and the dynamic range can be extended to

0…100pC

. This will be implemented on the next version electronics.9Slide10

Linearity in lowest gain 0..47pC, (before attenuation)

10Slide11

Baseline change with 8 pulsed channels

11

Rms

=0.75 ADC

Neighbouring channelSlide12

Measurement with high gain and low gain

12

High gain

8 ADC/PE

Low gain

4 ADC/PESlide13

Measurement with high gain and low gain

13

High gain

8 ADC/PE

Measurement with

detector as used by the

t

racker (50umx50um)Slide14

Shaping time settings 50ns to 300ns

Tp

=50ns

Tps

=200ns

Tp

=100ns

Tps

=250ns

Tp

=150ns

Tps

=300ns

Tp

=300ns

Tps

=450ns

Fastest setting is

50ns which corresponds

to a

peaking time

of the slow shaper

Tps

=200ns

Time of maximum measured after the arrival of the input signal (green in the plots)

14Slide15

Testbeam 9.2011

Use VATA64 v2, the chips are available now. The v2 was tested in the lab.Use intermediate PCB for connection of the SiPMs

with the PCB.Separate electronics card with the possibility to read 3x21 channels on the 64 channel readout chip.Card to card connection with small stacking height connectors. Has the advantage that different chips can be used to read the detectors without removing the connections to the

SiPMs.15Slide16

Testbeam 9.2011

Should we also provide a new version of the SPIROC readout? Card could

be plugged instead of the VATA64.

16Slide17

ConclusionWe still need to find the shaping time bug on the

SpirocA cardWe need to decide if we produce a new version SpirocA

card for the next testbeamThe VATA64 chip has clearly advantages over the

SpirocA so we want to use it in the next testbeam17