21–25 Sept 2009
Institut des Cordeliers 15, rue de l'Ecole de Médecine (Métro Odéon) Paris, France
Europe/Paris timezone
<strong>The deadline for paper submission has been extended to 23 October 2009</strong>

Total dose effects on a deep-submicron SOI technology for Monolithic Pixel Sensor development

24 Sept 2009, 16:15
2h 15m
Institut des Cordeliers 15, rue de l'Ecole de Médecine (Métro Odéon) Paris, France

Institut des Cordeliers 15, rue de l'Ecole de Médecine (Métro Odéon) Paris, France

Poster Radiation tolerant components and systems POSTERS SESSION

Speaker

Mrs Serena Mattiazzo (Dipartim. di Fisica Galileo Galilei-Universita degli Studi di Pa)

Description

A monolithic pixel detector in deep-submicron Silicon On Insulator (SOI) technology has been developed and characterized. This summary presents the first assessments of the effect of ionizing radiation as regards the total dose damage on single transistors in the technology used for the development of the first prototype chip. This work shows the decisive effect of the substrate bias condition during irradiation on the radiation induced damage on the electronics.

Summary

SOI technology allows the fabrication of CMOS integrated circuits on a thin Silicon layer, electrically isolated from the rest of the silicon wafer by means of a thick oxide layer. The isolation of the electronics from a high-resistivity substrate, used as sensitive volume, allows the production of monolithic pixel sensors for particle tracking and imaging. Vias etched through the oxide contact the substrate from the electronics layer, so that pixel implants can be created and a reverse bias can be applied.
A prototype chip, named LDRD-SOI-1, has been obtained in 2007 in a 0.15µm Fully Depleted (FD) SOI technology. In the chip, some single transistor test structures are implemented, including both I/O and core transistors (n-type and p-type).
The thick buried oxide (200nm) is expected to be sensitive to ionizing doses, which lead to positive charge trapping and consequently to an increase of the top-gate leakage current. This effect is even larger for the kind of structures we are studying. In fact, when a depletion voltage is applied to the detector, a strong electrical field is present inside the BOX. When exposed to ionizing radiation, electron-hole pairs are created inside the thick oxide. Due to the presence of the electrical field, these charges are immediately separated and do not recombine. This greatly increases the amount positive charge which is trapped throughout the BOX. The total dose damage is hence expected to be strongly dependent on the substrate voltage.
The test structures were characterized as regards their tolerance to total dose effects, by measuring the Ids-Vgs curves of each transistor before and after irradiation with X-ray photons. The irradiations were performed with the transistors in the worst-case bias conditions. A first chip was irradiated with a dose of 15krad (SiO2), in one single step. The substrate bias was Vsub = 40V, to maximize the number of electron-hole pairs escaping recombination. A second chip was irradiated up to a dose of 54krad(SiO2) with the same transistors bias conditions, but applying a Vsub = 10V (a typical operative value for the substrate bias of the pixel detector).
On the same dose given to the transistor, the two bias voltages induce two different damages: while the irradiation with Vsub =10V increments the leakage current less than one order of magnitude, the same dose given with Vsub =40V during irradiation induces an increase of the leakage current of a factor 104. The positive charge trapped inside the buried oxide in the first irradiation (Vsub = 40V) is sufficient to invert the back-channel interface, which forms a conducting path between the source and the drain and leads to a huge increase of the leakage current (the transistor is “ON” state even without any voltage applied to the gate).
Further investigation on the substrate bias conditions are planned for a 0.20µm FD SOI technology of the same producer, which was used for the development of the second prototype chip (LDRD-SOI-2). Also the effects of different dose rates will be addressed to.

Primary author

Mrs Serena Mattiazzo (Dipartim. di Fisica Galileo Galilei-Universita degli Studi di Pa)

Co-authors

Mr Dario Bisello (Università degli Studi di Padova, Dipartimento di Fisica and 4. Istituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 Padova, Italy) Mr Devis Contarato (Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA) Mr Devis Pantano (Università degli Studi di Padova, Dipartimento di Fisica and Istituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 Padova, Italy) Mr Jeffery Wyss (DiMSAT, Università degli Studi di Cassino, Cassino, Italy and Istituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 Padova, Italy) Mr Marco Battaglia (Department of Physics, University of California and 2. Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA) Mr Mario Tessaro (Istituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 Padova, Italy) Mr Nicola Pozzobon (3. Università degli Studi di Padova, Dipartimento di Fisica and Istituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 Padova, Italy) Mr Peter Denes (Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA) Mr Piero Giubilato (Lawrence Berkeley National Laboratory, Berkeley, CA 94720, USA, Università degli Studi di Padova, Dipartimento di Fisica and Istituto Nazionale di Fisica Nucleare, Sezione di Padova, I-35131 Padova, Italy)

Presentation materials