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A 5MGy γ -dose tolerant ΔΣ Time-to-Digital Converter with 5.6ps resolution for LIDAR application. tin. tin2. Ying Cao ( yicao@sckcen.be ) , Paul Leroux ( paul.leroux@khk.be ), Wouter De Cock ( wdcock@sckcen.be ), Michiel Steyaert ( michiel.steyaert@esat.kuleuven.be ). tin3.

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A 5MGy γ-dose tolerant ΔΣ Time-to-Digital Converter with 5.6ps resolution for LIDAR application

tin

tin2

Ying Cao ( yicao@sckcen.be) , Paul Leroux (paul.leroux@khk.be), Wouter De Cock (wdcock@sckcen.be), MichielSteyaert (michiel.steyaert@esat.kuleuven.be)

tin3

  • Irradiation

    • Gamma-dose radiation

    • Low dose rate experiment: 1.2kGy/hexposure time: 130h

    • High dose rate experiment: 30kGy/hexposure time: 165h

  • Setup

  • On-line test

e1

e2

Abstract

Image source: SCK∙CEN

Time-to-Digital converters (TDCs) are highly demanded in digital PLLs, ADCs, and time-of-flight measurement units, which are widely used for nuclear instrumentation. Demonstrating applications can be found in the ATLAS detector at the Large Hadron Collider (LHC), or in an accelerator driven system like MYRRHA (as shown in the left picture): in the spallation target the position of the liquid lead-bismuth free surface has to be monitored by a light detection and ranging system (LIDAR), which consists of two receiver frontend channels and a TDC. This work presents a radiation tolerant multi-stage delta-sigma TDC. It adopts the noise-shaping technique, andachieves a time resolution of 5.6ps, when the oversampling ratio (OSR) is 250. A radiation assessment up to 5MGy proves its robustness.

18kHz

-3dBFS

SNDR:

60.3dB

OSR=25

After 100kHz LPF

Details of the design

22kHz

Distance=C · Time/2

-40dBFS

SNDR:

28dB

The 1-1-1 MASH ΔΣ TDC has three stages. Each stage works as a relaxation oscillator, but controlled by the input time signal. The time can be measured by counting the periods of the oscillation clock during the time signal’s active phase. By preserving the phase of the oscillation clock between measurements, first-order noise-shaping is obtained. Third-order noise-shaping can be achieved by cascading all three stages.

After 100kHz LPF

OSR=250

Structure of the LIDAR

1mm distance resolution requires a time resolution of 6.7ps.

Output spectrum and waveform

0.13µm CMOS

0.41x0.27mm2

The frequency of the

oscillation clock can be expressed as 1/(2·RC), which is depending only on passive components. Thus, the TDC exhibits inherent PVT tolerance. Additionally, other hardened-by-design techniques have also been implemented to improve the system’s radiation tolerance, such as constant-gm biasing circuit, guard ring, etc. …

Captured time signals for each stage

core

Architecture of the MASH TDC

Die photo and time signals of the TDC

Radiation assessment

Pre-rad

Post-rad

A radiation tolerant third-order ΔΣ TDC is implemented in 0.13μm CMOS. It consumes only 1.7mW power and achieves an ENOB of 11b.Even after an extremely high radiation dose of 3.4MGy, the ENOB drops only 1 bit and, for an OSR of 250, a 10.5ps time resolution is still achieved.

Conclusion


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