Elsevier

Solid-State Electronics

Volume 79, January 2013, Pages 65-74
Solid-State Electronics

2 MeV electron irradiation effects on the electrical characteristics of metal–oxide–silicon capacitors with atomic layer deposited Al2O3, HfO2 and nanolaminated dielectrics

https://doi.org/10.1016/j.sse.2012.06.011Get rights and content

Abstract

The effects of 2 MeV electron irradiation on the electrical characteristics of atomic layer deposited (ALD) high permittivity (high-k) layers of Al2O3, HfO2 and a nanolaminate of them are evaluated. Metal–oxide–semiconductor capacitors with a nominal dielectric physical thickness of 10 nm were fabricated on different p-type and n-type silicon substrates. The capacitance–voltage (CV) and current–voltage (IV) characteristics of the different structures are analyzed as a function of electron irradiation. A progressive negative shift of the CV characteristics is observed with increasing electron irradiation, indicating the generation of effective positive charges. Similar generation rates for effective trapped charges and interface states are obtained for all the different high-k dielectric layers studied. The hysteresis of the CV curves after irradiation increases in the case of Al2O3 samples, for HfO2 decreases while the irradiation has little impact on the hysteresis of the nanolaminate stack. A progressive increase of the leakage current with electron irradiation dose is observed for all the studied dielectrics. The analysis of the current–voltage characteristics measured at different temperatures point to Poole–Frenkel as the dominant conduction mechanism. Under the studied conditions, no impact of electron irradiation fluence on dielectric breakdown voltage has been appreciated.

Highlights

► 2 MeV electron irradiation on ALD Al2O3, HfO2 and nanolaminate Si MOS capacitors. ► Similar charge trapping and interface states generation for the three high-k dielectrics. ► Increase of leakage current with electron irradiation fluence. ► Poole–Frenkel emission as the dominant conduction mechanism. ► No apparent impact of electron irradiation fluence on dielectric breakdown voltage.

Introduction

A number of high permittivity (high-k) dielectrics have been investigated as candidates to replace the SiO2 as gate dielectric in complementary metal–oxide–semiconductor (CMOS) technologies, being Al2O3 and HfO2 among the most studied ones [1], [2], [3], [4]. Apart from CMOS technologies, high-k dielectrics are also of strong interest for a wide range of micro/nanoelectronics applications, including, dynamic random access memories (DRAM) [5], emerging nanodevices [6], [7], organic light emitting diodes [8], as a surface passivation layer on high-efficiency crystalline silicon solar cells [9], and for a variety of microelectromechanical systems [10]. For all these applications, atomic layer deposition (ALD) has shown great potential to meet the requirements concerning dielectric properties, large area uniformity, conformality and accurate thickness control. Moreover, taking advantage of ALD unique properties, some works have also studied the possibility to deposit alternate layers of different high-k materials (nanolaminates). This can be useful to tailor the dielectric properties of the stack, reduce leakage currents in the presence of possible crystallization processes or improve the interface in contact with the semiconductor [11], [12], [13].

The integration of new materials and processes requires the study of different aspects for technology assessment. In recent years, a lot of work has been devoted to physical and electrical characterization, as well as to reliability issues, of alternative high-k dielectrics [14], [15], [16]. However, much less is known about their behaviour in radiation-harsh environments. The study of ionizing radiation effects on high-k dielectrics is of special interest for space applications [17], but also for high energy physics experiments and even to gain insight into possible effects of some advanced micro/nanofabrication processes like e-beam or X-rays lithography.

Since the early days of microelectronics, radiation-induced effects on conventional SiO2 dielectrics for CMOS technologies have been investigated [18], [19]. Total ionizing dose (TID) damage, with charge trapping in the gate dielectric and interface states generation at the silicon interface, have been the main radiation-induced degradation mechanisms for a wide range of SiO2 layer thickness [20]. A trap assisted tunnelling phenomenon, the radiation-induced leakage current (RILC), was observed for SiO2 layers with thickness in the range of about 3–8 nm [21], [22]. Fortunately, the continuous miniaturization process has led to radiation-harder SiO2 layers, with reduced charge trapping and flat band voltage shifts [23], and with thickness below the trapped-hole tunnelling limit (around 3 nm) [20].

The introduction of high-k dielectrics brings some uncertainty in terms of their radiation hardness. Moreover, due to the dependence of TID damage on the physical dielectric thickness, the radiation response could be an issue for such thicker high-k dielectric layers used in place of SiO2 [24]. Although some works have already been published on radiation effects on a few high-k dielectrics, these have been mostly limited to irradiations with heavy ions or X-rays, and only separated studies addressing either capacitance–voltage or current–voltage characterization have been generally considered [24], [25], [26], [27], [28], [29].

In this work, the effects of different doses of 2 MeV electron irradiation on the electrical characteristics of ALD-deposited layers of Al2O3, HfO2 and a nanolaminate of them are evaluated. Metal–oxide–semiconductor (MOS) structures with a nominal high-k dielectric physical thickness of 10 nm were fabricated on p-type and n-type silicon substrates. The capacitance–voltage and current–voltage characteristics of the different structures are analyzed as a function of electron irradiation dose paying special attention to the study of the effective trapped charges, generation of interface states, presence of hysteresis and electrical conduction through the layers.

Section snippets

Atomic layer deposition and fabrication of MOS capacitors

Three high-k dielectric layers, Al2O3, HfO2 and a nanolaminate of them, are studied in the present work. The layers were deposited by ALD in a Cambridge NanoTech Savannah 200 system, by using trimethylaluminium (TMA), tetrakis (Dimethylamido)-hafnium (TDMAH) and H2O as precursors, and N2 as carrier and purge gas. In the case of Al2O3, the ALD process was done at 200 °C with 95 cycles, for HfO2, a 100 cycles deposition process was carried out at 225 °C and in the case of the nanolaminate, a 5-layer

Capacitance–voltage characteristics

Fig. 1 shows an example of typical CV characteristics measured from inversion to accumulation (lines) and accumulation to inversion (symbols) for Al2O3 capacitors on 1 Ω cm p-type silicon substrate. The different curves correspond to non-irradiated and 2 MeV electron-irradiated devices at different fluences. Although only CV plots for a single dielectric and substrate are given in Fig. 1, the results are qualitatively similar for all the different conditions studied, where a progressive negative

Conclusions

The effects of 2 MeV electron irradiation on the capacitance–voltage (CV) and current–voltage (IV) characteristics of metal-oxide-silicon capacitors with three different atomic layer deposited (ALD) high-k dielectrics (Al2O3, HfO2 and a nanolaminate of them) have been evaluated. Similar radiation-induced generation rates for positive trapped charges and interface states have been obtained for all the studied high-k dielectric layers. While a radiation-induced increase of the CV curves

Acknowledgements

This work has been partially funded by the Spanish Ministry of Science and Innovation through Project TEC2008-06698-C02 and by Inter-University Laboratory for the Joint Use of the JAERI irradiation facilities in Japan.

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