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Different TDCs - The TEMPO TDC - A first version @ 180nm - The final chip @ 90nm (3)Why a time measure

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(1)

Tens Picosenconds Digital ASIC Time To Digital Converter for

Phisics Experiments stefano russo

LPNHE, Electronics group 9/03/2012

(2)

Outline

- Why a time measure?

- Different TDCs

- The TEMPO TDC

- A first version @ 180nm

- The final chip @ 90nm

(3)

Why a time measure?

Time To Digital Converters (TDC) are widely used in many different fields

Physics experiments

Time Of Flight

Positron Emission Tomography (PET)

Laser applications

Applied Electronics

All digital frequency synthesis

GFSK transceivers (frequency

modulators)

On chip test structures

(4)

All Digital TDC

Many different schemes to implement a TDC (both analogic and digital)

Digital Scheme

More performances on Avaliable Technologies

Easy to port design in different tech

Performances scale almost linearly with tech

(5)

How to design a TDC

To have a good resolution on a wide dynamic range a synchronous counter and asynchronous

fine interpolator are realized

Course measure (sync)

fine measure (async)

(6)

The fine measure

There are many different schemes to design the fine interpolator

Vernier Based

The time interval is compared to a fixed time

scale (like a caliper)

Direct Measure

The time interval in measured in terms of a

fixed quantity (like a meter)

(7)

Vernier Based design examples

Resolution is |τ2-τ1|

τ2 ≠ τ1

TLtH ≠ THtL

(8)

Direct Measure design

Resolution = tinv

(9)

Which inverter?

In a direct measure scheme the inverter design is the key element to achieve a good resolution

CMOS inverter (static)

The inverter delay optimization is a tradeoff between:

- MOS dimensions

- parasitic C

- rise fall time

(10)

Which inverter?

NORA inverter (dynamic)

The inverter needs a precharge signal

(PRE) to be activated.

The output is valid after the signal EVAL

N type Inverter P type Inverter

OUTPUT N PRE N

INPUT N

EVAL N

OUTPUT P INPUT P

PRE P EVAL P

(11)

NORA Logic pros & cons

PRO

- speed (Eval parasites are not on the signal path)

- TH2L ≠ TL2H

CONs

- Many signals

- TH2L ≠ TL2H N type Inverter

OUTPUT N PRE N

INPUT N

EVAL N

P type Inverter

OUTPUT P INPUT P

PRE P EVAL P

(12)

NORA vs. CMOS

To evaluate the performances a comparative simulations was performed @ 180nm

0 0.5 1 1.5

0 1 2

ns

StartCMOSNORA

0 0.5 1 1.5

0 1 2

ns

0 0.5 1 1.5

0 1 2

ns 1.17 ns

0.77 ns

3rd inverter 37th inverter

NORA is Faster 34%

than CMOS

(13)

The TEMPO scheme

Inverters in the fine interpolator are

designed using NORA logic

D Q D Q

D Q

Start

Stop

synchronous counter Start

Stop

N P P

High resolution

Reduced dead time

Low power

(14)

The TEMPO scheme

(15)

A first chip @ 180nm (UMC)

To validate our scheme a first version was realized

TDC1 TDC2

Full custom design for delay lines

TDC1 measure the time between START

& Stop

TDC2 measure a clock period

(calibration)

(16)

A first chip @ 180nm Experimental Results

Resolution = 41 ps on 18 μs range

11 11.5 12 12.5 13

0 20 40 60

measured time (ns)

fine interpolator output

(17)

A first chip @ 180nm Experimental Results

Max Differential Non Linearity

0.35 LSB

0 10 20 30 40 50 60

-0.3 -0.2 -0.1 0 0.1 0.2 0.3 0.4

fine interpolator output

DNL(LSB)

0 10 20 30 40 50 60

-0.6 -0.4 -0.2 0 0.2 0.4 0.6 0.8

fine interpolator output

INL(LSB)

Max Integral Non Linearity

0.75 LSB

(18)

A first chip @ 180nm Experimental Results

Single shot precision histograms

117 118 119 120 121 122 123

0 200 400 600 800 1000 1200 1400 1600 1800 2000

result of the measure

number of hits 5ns

41 hits

237 238 239 240 241 242 243

0 200 400 600 800 1000 1200 1400 1600 1800 2000

result of the measure

number of hits

10ns

168 hits

467 468 469 470 471 472 473

0 500 1000 1500 2000 2500

result of the measure

number of hits 20ns

929 930 931 932 933 934 935

0 200 400 600 800 1000 1200 1400 1600 1800

result of the measure

number of hits 40ns

a) b)

c) d)

(19)

A first chip @ 180nm Experimental Results

Single shot precision temperature dependence

0 10ns 20ns 30ns 40ns 50ns 60ns 70ns

0 500 1000 1500

measured time

taps

(20)

NORA vs. CMOS @ 90nm

NORA is Faster 29%

than CMOS

(21)

The TEMPO Differential scheme

The delay element compute two differential outputs.

The output is stabilized by the latch and acquired by a Strong Arm FF

(22)

A second chip @ 90nm (UMC)

In the second chip the differential scheme was implemented

Full custom design for delay lines

TDC1 measure the time between START

& Stop

TDC2 measure a clock period

(calibration)

Measured resolution 25 ps over 10.6 μs

(23)

A second chip @ 90nm Experimental Results

Max Differential Non Linearity

0.35 LSB

Max Integral Non Linearity

0.65 LSB

(24)

Experimental Results Summary

Technology Resolution Range Area Power INL DNL

180nm 41ps 18μs 0.09mm 25mW 0.77LSB 0.35LSB

90nm 25ps 10.6μs 0.1mm 19mW 0.65LSB 0.35LSB

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