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Lars Wendel

Publications and source records attributed to Lars Wendel.

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Planar GHz Resonators on SrTiO3: Suppressed Losses at Temperatures below 1 K

The complex dielectric constant $\hatε = ε_1 + i ε_2$ of SrTiO$_3$ reaches high values $ε_1 \approx 2*10^{4}$ at cryogenic temperatures, while the dielectric losses ($ε_2$) are much stronger than for other crystalline dielectrics. SrTiO$_3$ is a common substrate for oxide thin films, like the superconducting LaAlO$_3$/SrTiO$_3$ system, but the large $ε_1$ and $ε_2$ restrict high-frequency quantum devices on SrTiO$_3$. Here we present superconducting coplanar Nb resonators on SrTiO$_3$, which we successfully operate in a distant-flip-chip geometry at frequencies that exceed 1 GHz. We find a pronounced and unexpected increase in resonator quality factor $Q$ at temperatures below 1 K, reaching up to $Q \approx 800$. We attribute this to substantial changes of the dielectric losses in SrTiO$_3$ at mK temperatures, and we also detect non-monotonous changes in the temperature-dependent $ε_1$. These findings challenge our present understanding of the dielectric properties of SrTiO$_3$ and at the same time demonstrate that cryogenic high-frequency devices on SrTiO$_3$ are more feasible than previously assumed.

cond-mat.supr-con

Microwave probing of bulk dielectrics using superconducting coplanar resonators in distant-flip-chip geometry

Dielectric measurements on insulating materials at cryogenic temperatures can be challenging, depending on the frequency and temperature ranges of interest. We present a technique to study the dielectric properties of bulk dielectrics at GHz frequencies. A superconducting coplanar Nb resonator is deposited directly on the material of interest, and this resonator is then probed in distant-flip-chip geometry with a microwave feedline on a separate chip. Evaluating several harmonics of the resonator gives access to various probing frequencies, in the present studies up to 20 GHz. We demonstrate the technique on three different materials (MgO, LaAlO3, and TiO2), at temperatures between 1.4 K and 7 K.

cond-mat.supr-con