28 September 2015 to 2 October 2015
Lisbon
Europe/Zurich timezone

Front end Optimization for the Monolithic Active Pixel Sensor of the ALICE Inner Tracking System Upgrade

30 Sep 2015, 09:50
25m
Grande Anfiteatro (Lisbon)

Grande Anfiteatro

Lisbon

IST (Instituto Superior Técnico ) Alameda Campus Av. Rovisco Pais, 1 1049-001 Lisboa Portugal
Oral ASICs ASICs

Speaker

Daehyeok Kim (Yonsei University (KR))

Description

ALICE plans to replace its Inner Tracking System in 2018 with a new 10 m2 tracker constructed entirely with monolithic active pixel sensors. The TowerJazz 180 nm CMOS imaging Sensor process has been selected to produce the sensor as it offers a deep pwell allowing full CMOS in-pixel circuitry and different starting materials. First full-scale prototypes have been fabricated and tested. Radiation tolerance has also been verified. In this paper the development of the charge sensitive front end and in particular its optimization for uniformity of charge threshold and time response will be presented.

Summary

A monolithic active pixel sensor for the upgrade of the ALICE Inner Tracking System [1] is being developed in the TowerJazz 180 nm CMOS imaging Sensor process [2] wich offers a deep pwell allowing full CMOS in-pixel circuitry and different starting materials.
To limit material budget, power consumption should not exceed 100 mW/cm2. The collected charge over input capacitance (Q/C) ratio determines analog power consumption. Varying sensor geometry and applying reverse bias yields an input capacitance of around 2.5 fF [3] and a Q/C for an 18 μm epitaxial layer of about 80 mV distributed over a few pixels in a cluster. This allowed the implementation of a ~40nW open-loop binary charge sensitive front end with minimum charge threshold below 100 electrons. A front end peaking time of a few μs allows it to function as a memory: a strobe or trigger with this latency can be applied to latch hit information. A first large-scale prototype fully satisfies ALICE requirements [4]. Measurements revealed an ENC of only a few electrons, but a threshold spread of 18 electrons RMS much larger than simulations predicted. Better channel-to-channel uniformity of charge threshold and time response, intimately related, would further improve operating margins. An in-depth optimization of the front end was carried out: 8 different sectors of 65536 pixels each are equipped with a different version of the pixel gradually introducing various changes to the front end and sensor expected to improve uniformity. These include resizing certain transistors, modification of the circuit including the part to clip large signals, and the introduction of local protection diodes for gates of bias transistors as this was observed to improve matching in other projects [5] even if antenna rules were respected without them.
This third full-scale ALPIDE prototype is being submitted for fabrication now. It is also the first one to include a 1.2 Gb/s data transmission unit. With the 40nW front end, analog power consumption on the full chip is about 5 mW/cm2. Total power consumption is expected to be about 40 mW/cm2, dominated by digital circuitry and the data transmission unit. Further power optimization is planned as part of the R&D towards a production-ready prototype at the end of this year. The paper will present relevant measurement results on the present prototypes, the front-end design optimization, and hopefully first measurement results on the new full-scale prototype.
References
[1] L. Musa et al., CERN-LHCC-2012-013. LHCC-P-005, CERN, Geneva (2012). http://cds.cern.ch/record/1431539?ln=en
[2] S. Senyukov et al.,
http://dx.doi.org/10.1016/j.nima.2013.03.017
[3] J. Van Hoorne et al., https://indico.cern.ch/event/192695/session/7/contribution/284
[4] Y. Ping et al., JINST 10 C03030, http://dx.doi.org/10.1088/1748-0221/10/03/C03030
[5] R. Ballabriga,
https://indico.cern.ch/event/228972/session/16/contribution/224

Primary authors

Daehyeok Kim (Yonsei University (KR)) Walter Snoeys (CERN)

Co-authors

Alberto Collu (Universita e INFN (IT)) Alessandra Lattuca (Universita e INFN Torino (IT)) Andrei Dorokhov (IPHC) Antoine Junique (CERN) Carlo Puggioni (Universita e INFN (IT)) Cesar Augusto Marin Tobon (Autonomous University of Puebla (MX)) Chaosong Gao (Central China Normal University CCNU (CN)) Costanza Cavicchioli (Acad. of Sciences of the Czech Rep. (CZ)) Davide Marras (Universita e INFN (IT)) Deepak Gajanana (NIKHEF) Felix Reidt (Ruprecht-Karls-Universitaet Heidelberg (DE)) Gianluca Aglieri Rinella (CERN) Gianluca Usai (Universita e INFN (IT)) Gianni Mazza (Universita e INFN Torino (IT)) Hartmut Hillemanns (CERN) Herve Mugnier (Unknown) Jacobus Willem Van Hoorne (Vienna University of Technology (AT)) Jerome Rousset Luciano Musa (CERN) Magnus Mager (CERN) Markus Keil (CERN) Monika Kofarago (Nikhef National institute for subatomic physics (NL)) Narong Chanlek (Suranaree University of Technology (TH)) Paolo Martinengo (CERN) Petra Riedler (CERN) Ping Yang (Central China Normal University CCNU (CN)) Sabyasachi Siddhanta (Universita e INFN (IT)) Thanh Hung PHAM (CNRS) Thanushan Kugathasan (CERN) Youngil Kwon (Yonsei University (KR))

Presentation Materials