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Michael A. Tarkhov

Publications and source records attributed to Michael A. Tarkhov.

3 recordsLinked to original sources

Low-confinement silicon nitride waveguides manufactured via direct glass bonding

Reducing the fabrication cost of photonic integrated circuits while maintaining low optical losses and technological simplicity is essential for their wider implementation. In conventional manufacturing methods, the dielectric cladding thickness around waveguides is usually limited to $\sim20$~$μ$m, which complicates suppression of radiative losses and parasitic scattering in low-confinement geometries. In this paper, we propose and experimentally demonstrate an alternative technology for forming low-confinement waveguides in Borofloat~33 glass by thermal fusion bonding of two glass wafers. The waveguide pattern is formed by etching trenches with depths on the order of tens of nanometers into the glass, filling them with silicon nitride, removing the excess layer, and bonding the planarized glass surfaces, thereby forming a thick, symmetric dielectric cladding. As a proof of concept, we fabricated straight waveguides with a core height of 50~nm and widths from 1.3 to 3.5~$μ$m. With butt coupling to standard SMF-28 single-mode fiber at 1550~nm, we obtained chip transmissions up to 60\%, corresponding to input/output coupling losses of $\sim1$~dB per facet and consistent with numerical estimates. Fabry--Perot analysis of high-resolution spectra measured with AR-coated lensed fibers gave effective propagation losses down to $0.62\pm0.36$ dB/cm, depending on waveguide width and polarization. The proposed approach provides a simple and scalable route to low-confinement glass-encapsulated photonic circuits with passive butt coupling, promising for long delay lines, external-cavity laser feedback circuits, and ring-resonator sensors.

physics.optics↗

Silicon nitride on-chip C-band spontaneous emission generation based on lanthanide doped microparticles

The integration of active light-emitting elements into planar photonic circuits on a silicon nitride platform remains challenging due to material incompatibilities and high-temperature processing. Proposed hybrid method embeds monodisperse luminescent particles into lithographically defined wells above a 200 nm-thick silicon nitride taper coupler. A fabrication process involving wells etching, particle deposition, and planarization enables precise integration while maintaining waveguide integrity. When pumped at 950 nm with a diode laser, the device emits broadband radiation in the 1500-1600 nm range, covering the optical telecommunication C-band. Numerical simulations yield an average coupling efficiency of 0.25% into the fundamental waveguide mode, suggesting significant potential for further device optimization. The approach provides a scalable route for integrating broadband telecommunications emitters on a silicon nitride platform.

physics.optics↗

Superconducting single-photon detector integrated in DBR with optical microconnector for MM or SM fiber

This paper presents the development of a superconducting nanowire single-photon detector (SNSPD) integrated into a distributed Bragg reflector (DBR) with a design center wavelength of 830 nm and a width of 200 nm. This SNSPD is made of a superconducting niobium nitride (NbN) thin film that is produced using plasma-enhanced atomic layer deposition (PEALD). The DBR is made of 15 alternating layers of silicon nitride and silicon oxide that are produced through plasma-enhanced chemical vapor deposition (PECVD). The reflection efficiency of the mirror is 90% at a wavelength of 830 nm. For sufficient optical coupling, an optical micro-connector optimized for multimode or single-mode optical fibers with a diameter of 128 μm was formed using two-photon polymerization techniques. The niobium nitride film was deposited onto the DBR surface in-situ in two separate reactors connected by a vacuum transfer. The in-situ technique of deposition of a superconducting niobium nitride film and a distributed Bragg reflector has allowed achieving a detection efficiency of 90% at a wavelength of 830 nm and a dark count rate of 10 s-1 at a temperature of 2.5 K. Additionally, the detector jitter was 50 ps.

cond-mat.supr-con↗