High internal quality factor (~ 10<sup>6</sup>) superconducting coplanar waveguide resonators from MBE-grown titanium nitride films on c-plane sapphire
ORAL
Abstract
Coplanar waveguide microwave resonators with frequencies between 2 and 8 GHz, fabricated from titanium nitride (TiN) films showed high internal quality factors (Qi ~ 106) at the low power limit irrespective of the deposition methods, substrates, and resonator design [1-6]. This higher limit for the internal quality factor may be improved by understanding the material defects better. We deposited a 50 nm TiN on a 2-inch c-plane sapphire at 600oC growth temperature using plasma-assisted molecular beam epitaxy and an electron beam source for Ti. Using atomic force microscopy, we identified the 3-dimensional growth mode of TiN with 0.6 nm root mean square surface roughness. X-ray diffraction studies indicated a single crystal (1 1 1) surface orientation with 20 arcsecs of full width at half maximum of the rocking curves, one of the smallest reported values for TiN [6]. A superconducting transition temperature of 5.1 K and residual resistivity ratio of 2.1 were measured. Resonators were fabricated using a Cl-based etch. Using the 3-6-3 geometry for resonators standardized by NIST [7], we obtained a Qi ~ 106 in the single-photon limit. Scanning transmission electron microscope (STEM) images of the film showed columnar growth above a critical thickness of around 8 nm. Surprisingly, we found a screw dislocation in an otherwise defect-free sapphire substrate just 1 nm below the TiN/sapphire interface. This dislocation propagates into the TiN film. An etch-related damage was also found just below the TiN sidewall in sapphire. These defects, along with other defects, could be responsible for the higher limit of Qi. Further investigation of these defects and an effort to reduce them are under progress.
[1] Vissers et al., Appl. Phys. Lett. 97, 232509 (2010)
[2] S Ohya et al., Supercond. Sci. Technol. 27, 015009 (2014)
[3] Calusine et al., Appl. Phys. Lett. 112, 062601 (2018)
[4] Melville et al., Appl. Phys. Lett. 117, 124004 (2020)
[5] Richardson et al., J. Appl. Phys. 127, 235302 (2020)
[6] Gao et al., Phys. Rev. Materials 6, 036202 (2022)
[7] Kopas et al., arXiv:2204.07202 (2022)
[1] Vissers et al., Appl. Phys. Lett. 97, 232509 (2010)
[2] S Ohya et al., Supercond. Sci. Technol. 27, 015009 (2014)
[3] Calusine et al., Appl. Phys. Lett. 112, 062601 (2018)
[4] Melville et al., Appl. Phys. Lett. 117, 124004 (2020)
[5] Richardson et al., J. Appl. Phys. 127, 235302 (2020)
[6] Gao et al., Phys. Rev. Materials 6, 036202 (2022)
[7] Kopas et al., arXiv:2204.07202 (2022)
*This work was supported by the AFOSR/LPS program Materials for Quantum Computation (MQC) as part of the EpiQ team under award number FA9550-23-1-0688 monitored by Dr. Ali Sayir of AFOSR and Dr. Erin Cleveland of LPS
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Presenters
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Anand Ithepalli
- Cornell University