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P.F.Timmer Nikhef Amsterdam Electronics- Technology Very low power, High Voltage base for a Photo Multiplier Tube for the KM3NeT deep sea neutrino telescope. TWEPP, Aachen, 20-9-2010 1 P.F.Timmer* E.Heine H.Z.Peek *author NIKHEF, Amsterdam, the Netherlands

Very low power, High Voltage base for a Photo Multiplier

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Page 1: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

Very low power, High Voltage base for a Photo Multiplier Tube for the KM3NeT deep sea

neutrino telescope.

TWEPP, Aachen, 20-9-2010 1

P.F.Timmer*

E.Heine

H.Z.Peek*author

NIKHEF, Amsterdam, the Netherlands

Page 2: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

Outline

2

•Design requirements for the high voltage circuit board.

•System overview.

•HV generation.

•Diagram.

•Where will these high voltage circuit boards being used.

•Measurement results.

•Prototype of the high voltage circuit board.

•Summary

TWEPP, Aachen, 20-9-2010

Page 3: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

Multi PMT Optical Module system for detection of neutrinos

3

Location: Seabed of the Mediterranean Sea.

Embracing: several cubic kilometers of

seawater, max. 5000 meter depth.

Number of optical modules: 12000

Number of PMT’s: 372000

TWEPP, Aachen, 20-9-2010

Page 4: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

What is KM3NeT

4

•KM3NeT is an acronym for cubic kilometre size (KM3) Neutrino Telescope and

will host a neutrino telescope in the form of a water Cherenkov detector with a

volume of at least one cubic kilometre.

•KM3NeT will search for neutrinos from distant astrophysical sources like

gamma ray bursts, or colliding stars.

•An array of thousands of optical sensors will detect the faint light in the deep

sea from charged particles originating from collisions of the neutrinos and the

Earth.

•For the detection of this faint light (photons), Photon Multiplier Tubes will be

used. 31 PMT’s will be housed in a single Optical Module. A total of 300

detection units arranged in a string with 20 optical modules will be deployed.

TWEPP, Aachen, 20-9-2010

Page 5: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

Detecting photons caused by neutrinos.

5

•Photons caused by neutrinos are masked by background photons.

•Background photons come from decay of potassium 40 in the water,

the glass of the sphere and the glass of the PMT itself.

•These photons are detected by the PMT’s as single photons.

•Bioluminescence is also a source of photons.

•PMT’s will have a their own dark count (caused by thermal electrons)

•Consequently, all PMT’s generate random signals.

•Selecting the signals caused by neutrinos in the huge dataflow will be a defiant

job.

TWEPP, Aachen, 20-9-2010

Page 6: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

Vitrovex sphere 17 inch

Optical Module

6

12 PMT’s in the upper half of the optical module

19 PMT’s in the lower half of the optical module

TWEPP, Aachen, 20-9-2010

Page 7: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

Design requirements for thehigh voltage circuit

7

Every PMT must give the same output signal as it is hit by a single photon.

The gain of a PMT depends on the level of the supplied high voltage.

The HV for each PMT needs to be individually adjustable.

Consequently each PMT gets its own HV circuit board.

Limited space in the OM available.

Only in the centre of the sphere is room for the electronics.

Consequently limited board space.

Heat dissipation must be kept to a minimum.

No active cooling in the sphere available. The produced heat has to be

transferred through the glass to the seawater

Consequently low dissipation.

Good design rules imply also low ripple and low RFI generation.

Be aware, if the circuitry dissipates e.g. 0.5 W more,180 kW extra has to be

transported over 100 km from shore to the detector.

TWEPP, Aachen, 20-9-2010

Page 8: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

PMT global specifications

8

The detector will be designed for a lifetime of 15 years.

The lifetime of a PMT depends on the maximum amount of charge the anode can

supply.

Because of this property a low gain PMT has been chosen.

A low gain PMT means a dedicated pre amplifier.

Cathode characteristics

Radiant blue sensitivity at 470 nm > 130 mA/W

QE at 470 nm > 20%

Non homogeneity of cathode response target +/- 10%, +/- 20% acceptable

Characteristics with voltage divider

Maximum supply voltage 1400 V

Maximum Gain 5 *106

External electro static coating to the cathode

Anode characteristics

Dark count < 500Hz at 15 °C, > 0.3 pe threshold

Pulse rise time < 3 ns

Duration at half height 5 ns FWHM at single photon

Transit time spread < 2 ns sigma

Peak to valley ration 3, typical 2

TWEPP, Aachen, 20-9-2010

Page 9: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

Electrical/Optical Diagram of the Optical Module

9

switch

pre-ampcomp

thdac

decoder

photons

3V3

spherelogic

switchswitch

3V3

400V

tim.,sc

conversions

n

n+1

osc.1feedback

hvdac

HV

i2c

12+19

PMT-base

cpld

Connection

board

sphere-

logic

i2c

ID

additional

electronics.

LVDSapd

2

break

out

box

375V

Vertical

Electric

Optical Cable

TWEPP, Aachen, 20-9-2010

Page 10: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

HV generation 1

10

Uhv

k d1 d2 d9 d10 a

~

Resistor Base

Cockroft Walton base

+: Low power dissipation then RB

- : Fixed voltage ratio

- ‘High’ power dissipation

- Temperature Sensitive output voltage

- Bigger volume then CW base

- DC current 10 times anode current

no DC current

TWEPP, Aachen, 20-9-2010

Uhv

ad10d9d2d1k

k

Cb

Cp

Page 11: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

HV generation 2

11

control

3V3

S

Fly back principle

IpIs

Us Ip

Is

Us

e=-LdI/dt

E=½LI2

E=½CV2

Ixt=CxV

D1

D2C1

C2

U control

TWEPP, Aachen, 20-9-2010

Page 12: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

PMT proposed form factor

12

<1

05

dimensions in mm

cathode voltage -800 - -1400 V

Voltage dividing ratio

(between Cathode and Anode Photonis XP53B20)

K DA G D1 D2 D3 D4 D5 D6 D7 D8 D9 D10 A

0.15 1 1.5 2 1 1 1 1 1 1 1 1 1

(total: 13.65)

PCB = 38 mmØ

TWEPP, Aachen, 20-9-2010

Page 13: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

Component choices,

-Transformer core

-Diode switching characteristics

-Control IC

-ASIC, low dissipation, less space

Diagram

13

k

a

d10

d9

d8

da

g

d1

d2

3V3

ADP1111

L2

L3L1a

L1b

DAC

OPAMP

+-

DAC, OPAMP and 1.3V in

ASIC

On/Off, controlled by ASIC

1.3V

On/Off

I

U1

U2

I2C

Pre Amp

Comparator

LVDS Driver

TWEPP, Aachen, 20-9-2010

Page 14: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

HV versus frequency and Isupply

14

0

1

2

3

4

5

6

7

8

9

800 900 1000 1100 1200

Ukathode (V)

rep

.ra

te (

kH

z)

0

0.2

0.4

0.6

0.8

1

1.2

1.4

1.6

1.8

Isu

pp

ly (

mA

)

rep.rate kHz

Isupply mA

Power and frequency

2 - 9 kHz at 800 - 1200 V

0.6 - 1.4 mA3v3 at 800 - 1200 V (0.66mW-4.6mW)

TWEPP, Aachen, 20-9-2010

Page 15: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

EMC

15

RF shielded

boxprobe analyzeranalyzer

10dB/div

MHz/div

5V/div

20mV/div

5µs/div

event

RFI -20 dB @ 150 kHz-10 MHz

TWEPP, Aachen, 20-9-2010

Page 16: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

PMT and HV circuit

16TWEPP, Aachen, 20-9-2010

Page 17: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

<1

05

dimensions in mm

Form factor mostly dictated by PMT

17

PCB space

TWEPP, Aachen, 20-9-2010

Page 18: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

PMT base

18

Analogue part

Identifier

Digital part

Vripple 706 mV1056 8.5 < T(°C) < 22.1

Vripple 0.07% 8.5 < T(°C) < 22.1

Vripple < 150 mV/dynode

Voltage stabilization 0.95% on 38% input variation

Supply voltage 2V5 < 3V3 < 4V0

Power .6 - 1.4 mA3v3 at 800 - 1400 V < 4.5 mW

dV/dt < 75 mV/µs, RFI -20 dB @ 150 kHz-10 MHz

cathode voltage -800 - -1400 V

Voltage divider (between D1 – D10 and A for Photonis XP53B20)

K DA G D1 D2 D3 D4 D5 D6 D7 D8 D9 D10 A

0.15 1 1.5 2 1 1 1 1 1 1 1 1 1

(total: 13.65)

PCB = 38 mmØ

Time resolution 2 ns

Two-hit time separation 25 ns

Threshold DAC 8 bits

HV DAC 8 bits

PROM (ID) 20 bits

Communication I2C

Supply voltage 3V0 < 3V3 < 3V6

Power consumption 20 mW

Technology 350 nm CMOS

Silicon area 1.6 mm x 1.8 mm

TWEPP, Aachen, 20-9-2010

Presentation given by Deepak Gajanana

A Front End ASIC for the read out of the PMT

in the KM3NeT Detector

Page 19: Very low power, High Voltage base for a Photo Multiplier

P.F.Timmer

Nikhef

Amsterdam

Electronics-

Technology

Summary

19

HV circuit, designed for a 10 dynodes PMT after the requirements

Adjustable HVcathode voltage -800 - -1400 V

Small footprintPCB = 38 mmØ

Low powerVinput 3.3V

0.6 - 1.4 mA3v3 at 800 - 1200 V < 4.5 mW

(commercial available 50 mW)

Low ripple706 mV1056 8.5 < T(°C) < 22.1

0.07% 8.5 < T(°C) < 22.1

Vripple < 150 mV/dynode

Low RFIRFI -20 dB @ 150 kHz-10 MHz

AmplifierWith a prototype of the dedicated amplifier 80 fC was successfully detected. (PMT gain 0.5*106)

No influence of the switching cycle of the HV converter was seen.

TWEPP, Aachen, 20-9-2010