#Fs13 mods serial

Middle panel: The energy dispersion of the polariton modes versus in-plane wave vector, i.e.

A laser beam with incidence angle Оё and frequency П‰ can excite a microcavity mode with in-plane wave vector k в€Ґ = ( П‰ / c ) sin п»ї Оё, while the near-field (far-field) secondary emission from the cavity provides information on the real-space ( k-space) photon density. The cavity photon mode is strongly coupled to the excitonic transition in the QW. The wave vector in the z direction perpendicular to the cavity plane is quantized, while the in-plane motion is free. In particular, several mechanisms to obtain efficient photon blockade are presented, together with their application to the generation of novel quantum phases.ДЇigure 1Upper panel: Sketch of a planar semiconductor microcavity delimited by two Bragg mirrors and embedding a quantum well (QW). The conclusive part of the article is devoted to a review of the future perspectives in the direction of strongly correlated photon gases and of artificial gauge fields for photons. While the review is mostly focused on a specific class of semiconductor systems that have been extensively studied in recent years (planar semiconductor microcavities in the strong light-matter coupling regime having cavity polaritons as elementary excitations), the very concept of quantum fluids of light applies to a broad spectrum of systems, ranging from bulk nonlinear crystals, to atomic clouds embedded in optical fibers and cavities, to photonic crystal cavities, to superconducting quantum circuits based on Josephson junctions. A rich variety of recently observed photon hydrodynamical effects is presented, from the superfluid flow around a defect at low speeds, to the appearance of a Mach-Cherenkov cone in a supersonic flow, to the hydrodynamic formation of topological excitations such as quantized vortices and dark solitons at the surface of large impenetrable obstacles. In the presence of effective photon-photon interactions induced by the optical nonlinearity of the medium, a many-photon system can behave collectively as a quantum fluid with a number of novel features stemming from its intrinsically nonequilibrium nature. The second replicates were performed with an inverted SILAC labeling strategy.This article reviews recent theoretical and experimental advances in the fundamental understanding and active control of quantum fluids of light in nonlinear optical systems. Only one data point had a P <0.05 this is colored red in the scatter plot. We used a moderated t-test ( P < 0.05) to detect any statistically significant up- or downregulated sites among 2,131 K(GG) sites ( c) and 193 K(Ac)-sites ( d). log 2 SILAC ratios of replicates 1 and 2 are visualized as scatter plots and associated histograms. SILAC heavy (H)- and light (L)-labeled HeLa peptides (2.5 mg) were subjected to either one or two rounds of differential PTM enrichment (as indicated). ( c,d) SILAC ratio comparisons of doubly versus singly K(GG)-enriched ( c) or K(Ac)-enriched ( d) samples. error bars were calculated for three process replicates. Each identified modification-site value is that of the last PTM enriched in the sample. Label-free, tryptic HeLa peptides (2.5 mg) were either singly or doubly enriched for the indicated PTM enrichments. ( a,b) Comparison of the number of identified K(GG) ( a) and K(Ac) ( b) sites.

#Fs13 mods serial

Comparison of nonserial to serial enrichments for K(GG) and K(Ac) enrichments.