Abstract

Films of the all‐important compound hafnia (HfO2) can be prepared in an orthorhombic ferroelectric (FE) state that is ideal for applications, e.g., in memories or negative‐capacitance field‐effect transistors. The origin of this FE state remains a mystery, though, as none of the proposed mechanisms for its stabilization—from surface and size effects to formation kinetics—is fully convincing. Interestingly, it is known that doping HfO2 with various cations favors the occurrence of the FE polymorph; however, existing first‐principles works suggest that doping by itself is not sufficient to stabilize the polar phase over the usual nonpolar monoclinic ground state. Herein, first‐principles methods are used to re‐examine this question. Two representative isovalent substitutional dopants, Si and Zr, are considered, and their preferred arrangement within the HfO2 lattice is studied. The results reveal that small atoms like Si can adopt very stable configurations (forming layers within specific crystallographic planes) in the FE orthorhombic phase of HfO2 but comparatively less so in the nonpolar monoclinic one. Further, it is found that, at low concentrations, such a dopant ordering yields a FE ground state, the usual paraelectric phase becoming a higher‐energy metastable polymorph. The implications of the findings are discussed.

Highlights

  • It is found that, at low concentrations, such a dopant ordering yields a FE ground state, the usual paraelectric phase becoming a higher-energy metastable polymorph

  • The results reveal that small atoms like Si can adopt very tropic phase boundary like many perovskite stable configurations in the FE orthorhombic phase of HfO2 but comparatively less so in the nonpolar monoclinic one

  • Ever since it was shown that HfO2 films can be prepared in a ferroelectric (FE) phase,[1,2] much effort has focused on elucidatstabilize the FE polymorph over the PE ground state of the compound.[17,18,19,20,21,22]

Read more

Summary

Introduction

It is found that, at low concentrations, such a dopant ordering yields a FE ground state, the usual paraelectric phase becoming a higher-energy metastable polymorph.

Results
Conclusion

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.