There is, I think, something ethereal about i —the square root of minus one. I remember first hearing about it at school. It seemed an odd beast at that time—an intruder hovering on the edge of reality.

Usually familiarity dulls this sense of the bizarre, but in the case of i it was the reverse: over the years the sense of its surreal nature intensified. It seemed that it was impossible to write mathematics that described the real world in …

I and i

Bose-Einstein condensation (BEC) has been observed in a dilute gas of sodium atoms. A Bose-Einstein condensate consists of a macroscopic population of the ground state of the system, and is a coherent state of matter. In an ideal gas, this phase transition is purely quantum-statistical. The study of BEC in weakly interacting systems which can be controlled and observed with precision holds the promise of revealing new macroscopic quantum phenomena that can be understood from first principles.

Bose-Einstein condensation in a gas of sodium atoms

A topical review of numerical and experimental studies of supercontinuum generation in photonic crystal fiber is presented over the full range of experimentally reported parameters, from the femtosecond to the continuous-wave regime. Results from numerical simulations are used to discuss the temporal and spectral characteristics of the supercontinuum, and to interpret the physics of the underlying spectral broadening processes. Particular attention is given to the case of supercontinuum generation seeded by femtosecond pulses in the anomalous group velocity dispersion regime of photonic crystal fiber, where the processes of soliton fission, stimulated Raman scattering, and dispersive wave generation are reviewed in detail. The corresponding intensity and phase stability properties of the supercontinuum spectra generated under different conditions are also discussed.

Supercontinuum generation, photonic crystal fiber

Thirty years ago, Coullet et al. proposed that a special optical field exists in laser cavities bearing some analogy with the superfluid vortex. Since then, optical vortices have been widely studied, inspired by the hydrodynamics sharing similar mathematics. Akin to a fluid vortex with a central flow singularity, an optical vortex beam has a phase singularity with a certain topological charge, giving rise to a hollow intensity distribution. Such a beam with helical phase fronts and orbital angular momentum reveals a subtle connection between macroscopic physical optics and microscopic quantum optics. These amazing properties provide a new understanding of a wide range of optical and physical phenomena, including twisting photons, spin-orbital interactions, Bose-Einstein condensates, etc., while the associated technologies for manipulating optical vortices have become increasingly tunable and flexible. Hitherto, owing to these salient properties and optical manipulation technologies, tunable vortex beams have engendered tremendous advanced applications such as optical tweezers, high-order quantum entanglement, and nonlinear optics. This article reviews the recent progress in tunable vortex technologies along with their advanced applications.

/pdf/optical-vortices-30-years-on-oam-manipulation-from-2yknluuuga.pdf

Optical vortices 30 years on: OAM manipulation from topological charge to multiple singularities

On blockchain and its integration with IoT. Challenges and opportunities

Erratum to: Several Articles in JETP Letters

A composite resonant material consisting of amplifying and absorbing two-level quantum dots in a semiconductor host with conductive loss compresses a femtosecond pulse down to one-two optical cycles forming stable solitons.

Compression of femtosecond pulses into dissipative few-cycle optical solitons in coherent nonlinear resonant media

Superradiance of an Extended Resonant Medium Excited by Half-Cycle Attosecond Pulses

Unipolar and quasi-unipolar half-cycle pulses having nonzero electric pulse area are a limit of pulse shortening in a given spectral range. In spite of the fact that existence of such pulses was considered by Jackson (1962), V.L. Ginzburg (1960-s), Bullough and Ahmad (1971) as well as Bessonov (1981), the possibility of their existence and propagation in space remained questionable for many years. Only within the past decades both the possibility of unipolar pulse existence and their propagation dynamics were shown and analyzed in detail theoretically and experimentally. So far such pulses became a subject of active research due to their potential in the ultra-fast optics and study of new regimes of light-matter interactions with subcycle resolution. Here, we show the possibility of the effective ultrafast control of the level populations in quantum well nanostructures by the half-cycle unipolar attosecond light pulses in comparison to the single-cycle ones. It is shown that the population dynamics can be determined by the electric pulse area divided to its characteristic"scale"determined by the quantum well width. The selective excitation of quantum states and the feasibility of the population inversion by the subcycle unipolar pulses is demonstrated.

pdf/excitation-and-control-of-quantum-well-nanostructures-by-3om1f6hb.pdf

Excitation and control of quantum well nanostructures by unipolar half-cycle attosecond pulses

It is shown analytically that, in a trap filled by a Bose-Einstein condensate of atoms with a negative S-scattering length, there exists an instability caused by the nonlocal interaction of atoms. For this effect to be efficiently discovered experimentally, it is necessary to considerably decrease the absolute value of the scattering length using the Feshbach effect.

New type of instability of a Bose-Einstein condensate in a trap due to the onlocal interaction of atoms

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