17–21 Sept 2012
Oxford University, UK
Europe/Zurich timezone

Field Programmable Gate Array Based Data Digitisation with Commercial Elements

18 Sept 2012, 16:05
25m
Lindemann Lecture Theatre (Oxford University, UK)

Lindemann Lecture Theatre

Oxford University, UK

<font face="Verdana" size="2"><b>Clarendon Laboratory</b> Parks Road OX1 3PU, Oxford, United Kingdom
Oral B2

Speaker

Dr Michael Traxler (GSI Helmholtz Centre for Heavy Ion Research)

Description

One of the most important aspects of particle identification experiments is the digitisation of time, amplitude and charge data from detectors. These conversions are done mostly with Application Specific ICs (ASICs). However, the recent developments in Field Programmable Gate Array (FPGA) technology allow us to use commercial electronic components for the required Front-End Electronics (FEE) and do the digitisation in the FPGA. It is possible to do Time-of-Flight (ToF), Time-over-Threshold (ToT), amplitude and charge measurements with converters implemented in FPGA. We call this principle come & kiss: Use COMplex COMmercial Elements & Keep It Small and Simple.

Summary

Particle identification in nuclear physics experiments requires the digitisation of analogue data generated by the detectors, such as time, amplitude and charge information. Up to now digitisation of data is done mainly by Application Specific Integrated Circuits (ASICs), which requires a long time and a lot of resources for development. With the recent developments in the Field Programmable Gate Array (FPGA) technology, it is now possible to use FPGAs for data digitisation by using complex commercial electronic components for the necessary Front-End Electronics (FEE). We call this concept come & kiss: COMplex COMmercial Elements & Keep It Small and Simple.
To gain the time information (e.g., Time-of-Flight (ToF) or Time-over-Threshold (ToT)) of a signal generated by the necessary detectors, it is pre-amplified using available cell phone amplifiers to a certain level. The amplified signal is digitised in an FPGA differential input buffer used as a discriminator. By this configuration the time information of the particle is encoded in the rising and falling edges of a digital pulse. ToF measurements can be carried out by measuring the rising edges of 2 signals, whereas the ToT measurements can be done by measuring the pulse width of the discriminated signal. For precise time measurements a Time-to-Digital Converter (TDC) is implemented in the FPGA with high time resolution (<15 ps RMS).
For amplitude measurements an Analogue-to-Digital Converter (ADC) can be implemented in a FPGA by means of a TDC. The signal to be measured is applied to a differential input buffer of an FPGA with a reference voltage generated by a linear sawtooth generator on the second input. The differential buffer behaves as a comparator and generates a digital signal at the crossing of the reference sawtooth signal and the analogue signal. From the shape of the reference signal and the switching time measured by the TDC the amplitude of the input signal can be calculated.
Charge measurements are done in a similar fashion. The charge of the signal above the threshold is encoded in the width of a digital pulse via a constant current discharge of the integrated signal. The width of the pulse is proportional to the charge of the analogue signal. Using a TDC the width of the pulse is measured and the charge value is calculated.
The FPGA based data digitisation has advantages over the traditional ASIC solutions as well as disadvantages. The components used for a come & kiss system, basic cell phone amplifiers and FPGAs, are cheap and are always easily available removing the risks of mature devices. This method doesn't require as much amount of time, resource and cost as an ASIC design and has the advantage of being easily adaptable to different requirements. Of course, creating a solution by using commercial components is not as small as a special ASIC solution.
For all described digitisation methods test boards were developed and the results and limits are presented.

Author

Mr Cahit Ugur (Helmholtz-Institut Mainz)

Co-authors

Dr Marek Palka (Jagiellonian University) Dr Michael Traxler (GSI Helmholtz Centre for Heavy Ion Research) Dr Wolfgang Koenig (GSI Helmholtz Centre for Heavy Ion Research)

Presentation materials