178 research outputs found
Ladder of Eckhaus instabilities and parametric conversion in chi(2) microresonators
Low loss microresonators have revolutionised nonlinear and quantum optics
over the past decade. In particular, microresonators with the second order,
chi(2), nonlinearity have the advantages of broad spectral tunability and low
power frequency conversion. Recent observations have highlighted that the
parametric frequency conversion in chi(2) microresonators is accompanied by
stepwise changes in the signal and idler frequencies. Therefore, a better
understanding of the mechanisms and development of the theory underpinning this
behaviour is timely. Here, we report that the stepwise frequency conversion
originates from the discrete sequence of the so-called Eckhaus instabilities.
After discovering these instabilities in fluid dynamics in the 1960s, they have
become a broadly spread interdisciplinary concept. Now, we demonstrate that the
Eckhaus mechanism also underpins the ladder-like structure of the frequency
tuning curves in chi(2) microresonators.Comment: 10 pages, 5 figure
Soliton metacrystals: topology and chirality
Designing metamaterials with the required band structure, topology and
chirality using nano-fabrication technology revolutionises modern science and
impacts daily life. The approach of this work is, however, different. We take a
periodic sequence, i.e., metacrystal, of the dissipative optical solitons
rotating in a single ring microresonator and demonstrate its properties as of
the electromagnetic metamaterial acting in the radio to terahertz frequency
range. The metacrystal unit cell consists of the bound pair of solitons, and
the distance between them is used as a control parameter. We are reporting the
soliton metacrystal band structure and its topological properties. The latter
is confirmed by the existence of the steps experienced by the crystal
phonons' geometrical (Zak) phase. Furthermore, we found the phononic edge
states in the metacrystals with defects made by removing several solitons.
Optical frequency combs corresponding to the soliton metacrystals reveal the
spectral butterfly pattern serving as a signature of the spatio-temporal
chirality and bearing a resemblance to the butterfly wings illustrating natural
occurrences of chirality.Comment: 11 pages with an interesting Methods section. Title of the published
version has been changed to "Topological soliton metacrystals
Walk-off induced dissipative breathers and dissipative breather gas in microresonators
Dissipative solitons in optical microcavities have attracted significant
attention in recent years due to their direct association with the generation
of optical frequency combs. Here, we address the problem of dissipative soliton
breathers in a microresonator with second-order nonlinearity, operating at the
exact phase-matching for efficient second-harmonic generation. We elucidate the
vital role played by the group velocity difference between the first and second
harmonic pulses for the breather existence. We report the dissipative breather
gas phenomenon, when multiple breathers propagate randomly in the resonator and
collide nearly elastically. Finally, when the breather gas reaches an
out-of-equilibrium statistical stationarity, we show how the velocity locking
between first and second harmonic is still preserved, naming such phenomena
turbulence locking.Comment: 10 pages, 10 figure
Universal threshold and Arnold tongues in Kerr ring microresonators
We report that an instability boundary of a single-mode state in Kerr ring
microresonators with ultrahigh quality factors breaks the parameter space span
by the pump laser power and frequency into a sequence of narrow in frequency
and broad in power resonance domains - Arnold tongues. Arnold resonances are
located between the Lugiato-Lefever (lower) and universal (higher) thresholds.
Pump power estimates corresponding to the universal threshold are elaborated in
details. RF-spectra generated within the tongues reveal a transition between
the repetition-rate locked and unlocked regimes of the side-band generation.Comment: 6 page
Application of mixed formulations of quasi-reversibility to solve ill-posed problems for heat and wave equations: the 1d case
International audienceIn this paper we address some ill-posed problems involving the heat or the wave equation in one dimension, in particular the backward heat equation and the heat/wave equation with lateral Cauchy data. The main objective is to introduce some variational mixed formulations of quasi-reversibility which enable us to solve these ill-posed problems by using some classical La-grange finite elements. The inverse obstacle problems with initial condition and lateral Cauchy data for heat/wave equation are also considered, by using an elementary level set method combined with the quasi-reversibility method. Some numerical experiments are presented to illustrate the feasibility for our strategy in all those situations. 1. Introduction. The method of quasi-reversibility has now a quite long history since the pioneering book of Latt es and Lions in 1967 [1]. The original idea of these authors was, starting from an ill-posed problem which satisfies the uniqueness property, to introduce a perturbation of such problem involving a small positive parameter ε. This perturbation has essentially two effects. Firstly the perturbation transforms the initial ill-posed problem into a well-posed one for any ε, secondly the solution to such problem converges to the solution (if it exists) to the initial ill-posed problem when ε tends to 0. Generally, the ill-posedness in the initial problem is due to unsuitable boundary conditions. As typical examples of linear ill-posed problems one may think of the backward heat equation, that is the initial condition is replaced by a final condition, or the heat or wave equations with lateral Cauchy data, that is the usual Dirichlet or Neumann boundary condition on the boundary of the domain is replaced by a pair of Dirichlet and Neumann boundary conditions on the same subpart of the boundary, no data being prescribed on the complementary part of the boundary
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