Searcharxiv⌕ Search

arXiv · 2609.39555

Judd-Ofelt analysis of holmium-doped alumino-silicate optical glass prepared by MCVD combined with nanoparticle doping

Abstract

We present a detailed Judd--Ofelt (JO) analysis of Ho$^{3+}$-doped alumino-silicate optical fiber preforms in a wide range of compositions and prepared by both the standard solution doping method as well as the more advanced nanoparticle doping. The absorption spectra were measured, the absorption cross sections were calculated for each observed transition, and the Judd--Ofelt analysis was conducted. The preforms exhibited the values of JO parameters of $Ω_2 = (7.2--10.6) \times 10^{-20}\,\mathrm{cm}^2$, depending on the Al$_2$O$_3$ content, and $Ω_4$ and $Ω_6$ around $2.5$ and $1.2 \times 10^{-20}\,\mathrm{cm}^2$, respectively. The radiative transition parameters, such as transition probabilities, branching ratios, and radiative lifetimes, were calculated. The radiative lifetime of the ${}^5I_7 \rightarrow {}^5I_8$ transition, in the $16.1--17.2\,\mathrm{ms}$ range, combined with a measured value in the $0.9--1.9\,\mathrm{ms}$ range, was used to calculate the quantum efficiency, which was in the $5--11\,\%$ range. The preforms prepared by nanoparticle doping containing high Al$_2$O$_3$ contents above $8\,\mathrm{mol.}\,\%$ exhibited superior values of measured lifetime (above $1.5\,\mathrm{ms}$) and quantum efficiency (above $8\,\%$) compared to the standard solution-doped samples. To the best of our knowledge, this work is the first comprehensive report on the JO analysis of Ho$^{3+}$-doped alumino-silicate glass. The calculated parameters may be used in various calculations, simulations, and modelling of holmium-doped fiber lasers and other devices.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Petr Varak, Michal Kamradek, Pavla Nekvindova, Jan Hrabovsky, Pavel Peterka. 2026-09-30. Judd-Ofelt analysis of holmium-doped alumino-silicate optical glass prepared by MCVD combined with nanoparticle doping. https://arxiv.org/abs/2609.39555

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Long-Term $10^{-18}$-Level Flexible Stability Transfer with a Hybrid-Locked Kerr Microcomb

Optical atomic clocks are moving toward deployable systems, with commercial instruments entering the $10^{-17}$ fractional-frequency-instability regime. Transferring this performance to accessible microwave and radio-frequency signals requires compact optical frequency combs that preserve long-term stability during frequency division. Integrated Kerr microcombs have opened a new era in chip-scale precision metrology, enabling optical-frequency division and low-noise microwave generation. Yet, whether they can robustly preserve the stability required by state-of-the-art optical lattice and single-ion clocks over hour-long timescales remains an open question. Here we demonstrate that a hybrid passive-active stabilization of a Kerr microcomb, combining injection-locking of one tooth with active stabilization of a second, freely selected tooth through pump-frequency actuation, can indeed satisfy the metrological requirements at the highest level. The separated control channels effectively orthogonalize stabilization of the two microcomb frequency degrees of freedom while leaving the pump frequency unconstrained. A continuous five-hour measurement, without drift removal, yields a residual relative instability of $1.4\times10^{-16}$ at 1 s and $2\times10^{-18}$ at 4000 s on an out-of-loop tooth. We further show that the residual instability remains unchanged as the injection power is varied over 14 dB, demonstrating robust operation across a broad locking range. These results bring integrated microcomb stabilization into the residual-noise regime required to preserve the long-term performance of emerging optical lattice and single-ion clock systems.

physics.optics↗

Momentum-space non-Hermitian skin effect in an exciton-polariton system

Localization of a macroscopic number of eigenstates on a real-space boundary, known as the non-Hermitian skin effect, is one of the striking topological features emerging from non-Hermiticity. Realizing this effect typically requires periodic (lattice) systems with asymmetry of intersite coupling, which is not readily available in many physical platforms. Instead, it is meticulously engineered, e.g., in photonics, which results in complex structures requiring precise fabrication steps. Here, we propose a simpler mechanism: introducing an asymmetric, purely imaginary potential in a topologically trivial system induces momentum-space localization akin to the skin effect. We experimentally demonstrate this localization using exciton polaritons, hybrid light-matter quasi-particles in a simple engineered `round box' trap, pumped by a laser pump offset from the trap center. The effect disappears if the pump is concentric with the trap. The localization persists and becomes stronger at higher densities of polaritons, when a non-equilibrium Bose-Einstein condensate is formed and the system becomes nonlinear. Our approach offers a new route to realizing skin effects in continuous, non-periodic systems and exploring the interplay of non-Hermiticity, topology, and nonlinearity in macroscopic quantum states.

physics.optics↗

Highly-efficient perturbative Raman shifting by engineering the nonlinear temporal response

Raman scattering underlies a broad range of spectroscopic and light-generation techniques, yet its conventional description, based on the Raman gain spectrum, accurately describes only long-pulse, steady-state dynamics. We employ a time-domain theoretical approach to account for spectrotemporal aspects of continuous frequency-shifting, which are not addressed by prior theories. In particular, molecules with strong Raman responses do not produce an efficient soliton self-frequency shift in gas-filled hollow-core fibers. The time-domain analysis exposes temporal and spectral distortions from the Raman response that impact frequency-shifting detrimentally, and identifies how these distortions can be suppressed by reducing the Raman interaction to a perturbation on the electronic response. Experiments that employ gas mixtures with tunable Raman fractions of the nonlinear response demonstrate up to a four-fold increase in quantum efficiency (from 20 to 80%) compared to the pure molecular gas, and unity-efficiency Raman shifting will be possible. The time-domain framework uncovers phenomena that are inaccessible through the frequency-domain treatment of Raman scattering, and it applies to Raman interactions in solids, liquids, and gases across Raman temporal regimes.

physics.optics↗