Hydrogenated Amorphous Silicon Carbide: A Low-Loss Deposited Dielectric for Microwave to Submillimeter-Wave Superconducting Circuits
B.T. Buijtendorp, S. Vollebregt, K. Karatsu, D.J. Thoen, V. Murugesan, K. Kouwenhoven, S. Hähnle, J.J.A. Baselmans, A. Endo
DOI 10.1103/PhysRevApplied.18.064003 · Physical Review Applied
Active bibliographic source — not scientific approval
Bibliographic access preserves source history; it does not approve extracted materials or validate reported claims. Review warnings on each occurrence separately.
Abstract
Low-loss deposited dielectrics will benefit superconducting devices such as integrated superconducting spectrometers, superconducting qubits, and kinetic inductance parametric amplifiers. Compared with planar structures, multilayer structures such as microstrips are more compact and eliminate radiation loss at high frequencies. Multilayer structures are most easily fabricated with deposited dielectrics, which typically exhibit higher dielectric loss than crystalline dielectrics. We measure the subkelvin and low-power microwave and millimeter-submillimeter-wave dielectric loss of hydrogenated amorphous silicon carbide (a-SiC:H), using superconducting chips with Nb-Ti-N/a-SiC:H/Nb-Ti-N microstrip resonators. We deposit the a-SiC:H by plasma-enhanced chemical vapor deposition at a substrate temperature of 400∘C. The a-SiC:H has a millimeter-submillimeter loss tangent ranging from 0.9×10−4 at 270 GHz to 1.5×10−4 at 385 GHz. The microwave loss tangent is 3.1×10−5. These are the lowest low-power subkelvin loss tangents that have been reported for microstrip resonators at millimeter-submillimeter and microwave frequencies. The a-SiC:H films are free of blisters and have low stress: −20 MPa compressive at 200-nm thickness to 60 MPa tensile at 1000-nm thickness.
Source-reported materials — not catalogue approval
| Formula | Reported Tc (K) | Pressure (GPa) | Type |
|---|---|---|---|
| NbTiN Archive — visibility unverified Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula. | — | Pressure not reported | unknown |
Similar papers
Strongly Disordered TiN and NbTiN s-Wave Superconductors Probed by Microwave Electrodynamics
similarity 0.92E. F. C. Driessen et al.
Source status unknown — claims are unverified
Erasing odd-parity states in semiconductor quantum dots coupled to superconductors
similarity 0.91Z. Su et al.
Source status unknown — claims are unverified
Reversible Tuning of Superconductivity in Ion-Gated NbN Ultrathin Films by Self-Encapsulation with a High-κ Dielectric Layer
similarity 0.90Erik Piatti et al.
Source status unknown — claims are unverified
Magnetic-field-resilient high-impedance high-kinetic-inductance superconducting resonators
similarity 0.90C. Roy et al.
Source status unknown — claims are unverified
Infrared vortex-state electrodynamics in type-II superconducting thin films
similarity 0.90Xiaoxiang Xi et al.
Source status unknown — claims are unverified
Compact and Tunable Forward Coupler Based on High-Impedance Superconducting Nanowires
similarity 0.90Marco Colangelo et al.
Source status unknown — claims are unverified