Elsevier

Physica B: Condensed Matter

Volumes 374–375, 31 March 2006, Pages 379-382
Physica B: Condensed Matter

Oxide muonics: A new compendium

https://doi.org/10.1016/j.physb.2005.11.106Get rights and content

Abstract

A new survey of muonium states brings the total of binary non-magnetic oxides studied to 30, with normal muonium—the interstitially trapped atomic state—found in 15 of these. The number of shallow-donor states of the type known in ZnO now also totals 15, but there are hints of several others. Tantalizingly, the shallow-donor and deep-atomic states are found to coexist in several of the candidate high-permittivity dielectrics. Highly anisotropic states, resembling anomalous muonium in semiconductors and including examples of muonium trapped at oxygen vacancies, complete a spectrum of hyperfine parameters covering five powers of ten. Effective ionization temperatures range from 10 K for shallow to over 1000 K for deep states, with corresponding activation energies between several meV and several eV. The oxide band gap emerges as a parameter controlling the systematics of the deep-to-shallow transition for muonium and, by inference, monatomic hydrogen.

Introduction

Since the earliest spectroscopic studies of muonium in quartz, and in a relatively small number of other wide-gap non-magnetic oxides, the use of muonium as a model for hydrogen has taken on a new importance. This follows μSR confirmation that hydrogen forms a shallow-donor state in ZnO; that is, its electron wave function does not retain atomic character but delocalizes into conduction-band states. The question arises as to whether hydrogen can similarly act as an n-type dopant and induce electronic conductivity in other oxides. A particular concern is that it might do so in those high-permittivity materials such as HfO2 and ZrO2 that are destined to replace SiO2 as nano-scale gate dielectrics. We have therefore undertaken a new survey of muonium states in a wide selection of oxides, both semiconducting and dielectric. We use the term muonics to describe the use of muonium data as a model for the electronic structure and electrical activity of hydrogen in the dilute monatomic limit. Comparable ESR data for H in oxides is sparse, but fortunately include the trapped atoms in SiO2 and Li2O, as well as the donor in ZnO, thereby validating the muonics principle both for deep and shallow states.

Section snippets

Normal muonium

Much studied in quartz and ice, the interstitially trapped atom known as normal muonium was also known to early μSR studies in Al2O3, BeO, CaO and MgO [1], [2], [3], [4], [5], [6]. Using the longitudinal-field method of hyperfine decoupling or repolarization (as in the first studies of Al2O3 [1]), we have also detected normal muonium in polycrystalline samples of Bi2O3, Cu2O, HfO2, La2O3, Li2O, Sb2O3, SrO, Y2O3, ZrO2 and YSZ.1

Shallow-donor muonium

In the early studies, it was puzzling why muonium did not seem to be formed in all other wide-gap oxides. It may be that shallow-donor states of the type now known in ZnO [11], [12] were overlooked: the weak binding energy and very low hyperfine constants require a careful search for broadening or splitting of the Larmor precession spectrum at cryogenic temperatures. Thus TiO2 was originally thought to show only a diamagnetic muon state [4] and the significance of a low-T broadening of its

Anomalous muonium

The oxides also show several examples of highly anisotropic muonium states with hyperfine parameters reminiscent of anomalous muonium (Mu*) in tetrahedral semiconductors. Muonium in HgO shows a contact term of 15 MHz and a dipolar term of 5 MHz, giving rise to a striking level-crossing resonance at 55 mT [18]; motional effects described in an accompanying paper suggest a muon site not at the bond-centre but antibonding to oxygen [19]. The parameters imply a reasonably compact electronic orbital,

Band gap correlation, systematics and implications for doping

The shallow-donor muonium states all dissociate below about 100 K (in BaO and rutile-TiO2 as low as 10 K), with effective ionization energies varying from several meV to several tens of meV. The anomalous muonia show varying degrees of thermal stability and probably act as deep donors, dissociating below room temperature in HgO (125–225 K, 0.15–0.3 eV) but above room temperature for the vacancy-complex in GeO2 (500–700 K, 0.9 eV). Normal muonium disappears only well above room temperature, with a

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