Damir F. Yagudin’s research while affiliated with Lomonosov Moscow State University and other places

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Publications (8)


Schematic representation of PL enhancement in InAs QDs embedded into the GaAs quadrumer.
Optical characterization of the quadrumer. (a) Experimental setup for dark-field spectroscopy measurements of quadrumers with embedded QDs. L1:4 are lenses, O is the objective lens, F1:2 are optical fibers, C is collimator, BS is the beam splitter, FM is the flipper mirror, FD is the field aperture. (b) Experimental scattering cross-section spectra of isolated oligomers of nanopillars with diameters of 220 nm (yellow) and 260 nm (red). Inset shows scanning electron microscope image of the sample of Mie-resonant quadrumers coupled with QDs; spacings between nanopillars are s=100±5 nm; diameters are d=250±5 nm; heights are h=400±5 nm.
Microphotoluminescence of QDs coupled to GaAs quadrumers for linearly polarized pump beams. (a) Experimental setup for microphotoluminescence measurements at cryogenic temperature of 8 K. L1:3 are lenses, O is the objective lens, M is the mirror, BS is the beam splitter, DM is the dichroic mirror, PH is the pinhole coupled to the mirror, F is the set of low pass and long pass filters. (b) The red area is the μ-PL spectrum of InAs QDs embedded into the GaAs film, obtained from the 2.5 μm spot on the sample pumped by laser radiation with 404 nm wavelength. The black curve with a set of emission lines is the representative spectrum of InAs QDs located in the GaAs nanopillars forming isolated quadrumer. (c) Experimental photoluminescence intensity normalized to the maximum value for resonant, d≈220 nm (yellow), and non-resonant, d≈260 nm (red), samples measured for different pump wavelengths and fixed PL wavelength (λPL) for each sample (λPL=950 nm and λPL=920 nm). (d) The dependence of the isolated quadrumer PL intensity on the diameter of nanopillars normalized to its maximum value.
Numerical results of QDs μ-PL for various pump polarizations. Numerically obtained PL enhancement for linear (a) and azimuthal (b) polarizations of the pump radiation for GaAs nanopillars coupled with InAs QDs on the GaAs substrate. MD is the magnetic dipole Mie-type mode, OMD—collective out-of-plane magnetic dipole mode.
Quantum Dot Photoluminescence Enhancement in GaAs Nanopillar Oligomers Driven by Collective Magnetic Modes
  • Article
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January 2023

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78 Reads

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6 Citations

Maria K. Kroychuk

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Damir F. Yagudin

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Single photon sources based on semiconductor quantum dots are one of the most prospective elements for optical quantum computing and cryptography. Such systems are often based on Bragg resonators, which provide several ways to control the emission of quantum dots. However, the fabrication of periodic structures with many thin layers is difficult. On the other hand, the coupling of single-photon sources with resonant nanoclusters made of high-index dielectric materials is known as a promising way for emission control. Our experiments and calculations show that the excitation of magnetic Mie-type resonance by linearly polarized light in a GaAs nanopillar oligomer with embedded InAs quantum dots leads to quantum emitters absorption efficiency enhancement. Moreover, the nanoresonator at the wavelength of magnetic dipole resonance also acts as a nanoantenna for a generated signal, allowing control over its radiation spatial profile. We experimentally demonstrated an order of magnitude emission enhancement and numerically reached forty times gain in comparison with unstructured film. These findings highlight the potential of quantum dots coupling with Mie-resonant oligomers collective modes for nanoscale single-photon sources development.

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Enhanced Nonlinear Light Generation in Oligomers of Silicon Nanoparticles under Vector Beam Illumination

April 2020

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57 Reads

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46 Citations

Nano Letters

All-dielectric nanoparticle oligomers have recently emerged as promising candidates for nonlinear optical applications. Their highly resonant collective modes, however, are difficult to access by linearly polarized beams due to symmetry restraints. In this paper we propose a new way to increase the efficiency of nonlinear processes in all- dielectric oligomers by tightly focused azimuthally polarized cylindrical vector beam illumination. We demonstrate two orders enhancement of the third-harmonic gener- ation signal, governed by a collective optical mode represented by coherently excited out-of-plane magnetic dipoles. Crucially, the collective mode is characterized by strong electromagnetic field localization in the bulk of the nonlinear material. For comparison, we measure third-harmonic generation in the same oligomer pumped with linearly and radially polarized fundamental beams, which both show significantly lower harmonic output. We also provide numerical analysis to describe and characterize the observed effect. Our findings open new route to enhance and modulate the third-harmonic gen- eration efficiency of Mie-resonant isolated nanostructures by tailoring the polarization of the pump beam.


Figure 1. a) Electric field profile in the vicinity of magnetic dipolar resonance is shown, white arrows indicate polarization direction of pump beam. b) Optical scattering spectrum for quadrumer excited by a linearly polarized plane wave. Inset shows an example of geometric parameters for resonant nanoparticles, their height is fixed at 200 nm.
Collective magnetic modes excitation in GaAs nanoclusters by azimuthally polarized vector beams

March 2020

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66 Reads

Journal of Physics Conference Series

We investigate optical response of oligomers of dielectric nanodisks made of GaAs – anisotropic material with bulk quadratic nonlinearity. By using numerical approach, we analyse linear response of nanoparticle clusters in the vicinity of the magnetic dipole resonance for two types of incident radiation: linearly polarized plane wave and azimuthally polarized vector beams. Achieved results may be used to design highly efficient nonlinear optical nanoantennas with controllable radiation characteristics.


Nonlinear Light Generation Driven by Collective Magnetic Modes in Oligomers of Silicon Nanoparticles Excited by Vector Beams

January 2020

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14 Reads

We demonstrated two orders of magnitude enhancement of the third-harmonic intensity for isolated nanoclusters of silicon nanoparticles illuminated by normally incident azimuthally polarized cylindrical vector beams at the wavelength of oligomer’s out-of-plane magnetic mode.


Nonlinear Anisotropy: Tailored Nonlinear Anisotropy in Mie‐Resonant Dielectric Oligomers (Advanced Optical Materials 20/2019)

October 2019

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42 Reads

In article number 1900447, Andrey A. Fedyanin, Maria K. Kroychuk and co‐workers introduce a new concept of tailoring nonlinear properties of all‐dielectric nanoscale structures in accordance with the oligomers' point‐group symmetries while their linear scattering remains isotropic. This concept provides a viable path towards artificial anisotropic nonlinear systems, expanding the scope of their applications in nanophotonics.


a) Schematic representation of the THG microscopy of isolated oligomers. TH intensity in transmission is measured as a function of the sample azimuthal rotation angle. b–d) Scanning electron microscope images of the nanoparticles under study. A monomer—an isolated silicon nanodisk (b); a trimer—three silicon nanodisks located at the vertices of an equilateral triangle (c); a quadrumer—four silicon nanodisks arranged in a square pattern (d).
a) Schematic of the TH nonlinear microscopy setup (N‐lin) and linear microscopy setup (Lin) based on an ytterbium solid‐state femtosecond laser: GT are Glan‐Taylor polarizers, BS is a beam splitter, FM is a mirror on a flipper mount, O are objective lenses mounted on micrometer stages, FH is a fiber holder, M is a metallic mirror, CH is an optical chopper, GP is a glass plate, C is a camera, S is the sample on a three‐coordinate micrometer stage that allows azimuthal sample rotation, L are optical lenses, LED is a diode lamp, F is a set of BG39 filters, PMT is a photomultiplier assembly connected to a lock‐in amplifier, n‐F is a set of neutral density filters; the dashed red line illustrates the reference channel with an amorphous silicon film as a source of the reference TH output. b) Experimental transmittance spectra of the isolated trimer and quadrumer with various diameters (285 and 270 nm, respectively). c) Experimental (blue) and numerical (red) transmittance spectra of the isolated trimer with d = 285 nm and s = 50 nm. The inset to the right shows the electric field distribution inside one of the nanodisks at the central wavelength of the laser (λ = 1050 nm), which corresponds to the MD resonance of the single disk in the oligomer.
Experimental results. a) Transmittance of the trimer (s = 50 nm, d = 285 nm, red dots) and quadrumer (s = 70 nm, d = 270 nm, black dots) as a function of the polarization azimuthal angle for a fixed wavelength of λ = 1050 nm. b–d) TH microscopy of the isolated oligomers—TH intensity from the samples as a function of the azimuthal angle: monomer (b), trimer (c), and quadrumer (d). Solid black curves indicate sine approximations of the experimental results.
Numerical results. a) Scattering cross‐section spectrum for the resonant oligomers of silicon nanodisks: trimer (blue) and quadrumer (red) at normal incidence. The dashed vertical gray line marks the laser wavelength position. b) TH power depending on the in‐plane rotation angle of the pump polarization at fixed fundamental wavelength 1050 nm. The power is calculated over the full solid angle and independently normalized by the average power levels for each oligomer. c,d) Simulated near‐field distributions at the fundamental and third‐harmonic frequencies corresponding to the angles of minimum and maximum THG: c) [0, π/6] for trimer, and d) [0, π/4] for quadrumer. The false‐color maps represent the absolute value of the electric field strength. The arrows indicate the electric field orientation in the incident wave.
Tailored Nonlinear Anisotropy in Mie‐Resonant Dielectric Oligomers

July 2019

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154 Reads

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23 Citations

The field of Mie‐resonant nanophotonics has attracted a lot of attention recently due to many promising applications in linear and nonlinear metaoptics. Optically induced magnetic resonances define novel characteristics of isolated high‐index dielectric nanoparticles and their oligomers. Here, the orientation‐dependent nonlinear frequency generation from dielectric oligomers with different symmetries, being all characterized by isotropic linear response, is demonstrated. The rotational dependence of the third‐harmonic signal emitted by the nanoparticle oligomers in accord with their point‐group symmetry (e.g., C3 or C4) is observed experimentally, while their linear scattering remains isotropic. The experimental data are in a good agreement with numerical simulations and the symmetry analysis of the nonlinear susceptibility tensor. The results open a new avenue for tailoring nonlinear properties of nanoscale structures.


Citations (3)


... However, plasmonic structures also introduce additional losses, which can degrade the quantum efficiency and indistinguishability of the emitted photons. An alternative approach is to use high-refractive-index (HRI) dielectric nanostructures, which can support Mie resonances and exhibit low ohmic losses in the visible range compared to plasmonic structures [21,22]. These resonances can also lead to strong field enhancements and large Purcell factors, while maintaining high quantum efficiencies. ...

Reference:

An Evaluation of Moderate-Refractive-Index Nanoantennas for Enhancing the Photoluminescence Signal of Quantum Dots
Quantum Dot Photoluminescence Enhancement in GaAs Nanopillar Oligomers Driven by Collective Magnetic Modes

... Also, tightly focused light beams from high numerical aperture (NA) objective converge energy of input light in focus area, resulting in stronger near-field confinement for TH enhancement. As demonstrated by Maria K. Kroychuk et al., the collective mode is excited by tightly focused APB illumination, resulting in two-order enhancement in the TH signal in all-dielectric oligomers [24]. The anapole mode excited by a tightly focused radially polarized beam (tf-RPB) can provide strong field confinement in isotropic nanosphere, but has not yet been utilized to enhance TH signals. ...

Enhanced Nonlinear Light Generation in Oligomers of Silicon Nanoparticles under Vector Beam Illumination
  • Citing Article
  • April 2020

Nano Letters

... fact that the nth-order harmonic generation is proportional to the electric energy over the volume of a nanostructure unit cell. Therefore, the all-dielectric metasurfaces with low losses and various high-quality-factor Mie resonances have received growing attention for boosting nonlinear frequency conversion efficiency at the subwavelength scale [19][20][21][22]. Importantly, flexible designs of all-dielectric metasurfaces enable control of the amplitude, phase, and spin of harmonic signals and thus catalyze numerous nonlinear optical applications, including wavefront shaping, image encoding, and nonlinear holography [23][24][25][26]. ...

Tailored Nonlinear Anisotropy in Mie‐Resonant Dielectric Oligomers