Dark solitons in mode-locked lasers Mark J. Ablowitz , Theodoros P. Horikis
... underlies the mode-locking mechanism: its effect is to mode-lock to a black soliton of the pure NLS equation with the appropriate background, Eq. (3). On the other hand, mode-locking to grey solitons, namely moving dark pulses with a phase-jump less than π at their (non-zero) intensity minima, are n ...
... underlies the mode-locking mechanism: its effect is to mode-lock to a black soliton of the pure NLS equation with the appropriate background, Eq. (3). On the other hand, mode-locking to grey solitons, namely moving dark pulses with a phase-jump less than π at their (non-zero) intensity minima, are n ...
“Pixel” team
... We are now willing to install a new instrument combining improved versatility, multiple beam alignment capability and stability. This instrument is based on two objectives instead of three in the previous versions. The change in design from three to two objectives necessitates the simultaneous coupl ...
... We are now willing to install a new instrument combining improved versatility, multiple beam alignment capability and stability. This instrument is based on two objectives instead of three in the previous versions. The change in design from three to two objectives necessitates the simultaneous coupl ...
EP23850853
... A transimpedence amplifier amplifies the photo detector signals to 1V signals which are further amplified by an amplifier card in the RLG to a 5V p-p signal. The sin/cos signals have a frequency range spanning from 10Hz to 1MHz. ...
... A transimpedence amplifier amplifies the photo detector signals to 1V signals which are further amplified by an amplifier card in the RLG to a 5V p-p signal. The sin/cos signals have a frequency range spanning from 10Hz to 1MHz. ...
Generation and Application of Bessel Beams in Electron Microscopy
... Here, we report a detailed study of the first off-axis Fresnel phase hologram to generate electron Bessel beams [5], and examine: 1) the conditions under which Bessel beams can be generated and applied to microscopy and imaging; 2) techniques by which key beam and hologram parameters, including topo ...
... Here, we report a detailed study of the first off-axis Fresnel phase hologram to generate electron Bessel beams [5], and examine: 1) the conditions under which Bessel beams can be generated and applied to microscopy and imaging; 2) techniques by which key beam and hologram parameters, including topo ...
Soliton pairs in a fiber laser: from anomalous to normal average
... 50-cm long open-air section containing wave plates and polarizing cubes. Due to nonlinear polarization evolution that takes place along with propagation in the fibers, the transmission through the polarizer P1 is intensity dependent, and an appropriate adjustment of the preceding wave plates trigger ...
... 50-cm long open-air section containing wave plates and polarizing cubes. Due to nonlinear polarization evolution that takes place along with propagation in the fibers, the transmission through the polarizer P1 is intensity dependent, and an appropriate adjustment of the preceding wave plates trigger ...
Landau Quantization of Neutral Particles in an External Field
... Where n is an integer number. With this condition, we obtain discrete values for the energy, given by ...
... Where n is an integer number. With this condition, we obtain discrete values for the energy, given by ...
Rapid fabrication of 3D terahertz split ring resonator arrays by novel
... In order to advance lithographic capabilities for future applications, innovative strategies must be available in a scalable and cost-effective set of techniques. This is especially the case when approaching the fabrication of complex 3D architectures not amenable to conventional layerby-layer proce ...
... In order to advance lithographic capabilities for future applications, innovative strategies must be available in a scalable and cost-effective set of techniques. This is especially the case when approaching the fabrication of complex 3D architectures not amenable to conventional layerby-layer proce ...
Optical Fibers and Waveguides
... that decay exponentially into the external medium. The propagating waves in this case, because they are guided along by the slab, but are not totally confined within it, are often called surface waves. This distinguishes them from the types of wave that propagate inside, and are totally confined by, ...
... that decay exponentially into the external medium. The propagating waves in this case, because they are guided along by the slab, but are not totally confined within it, are often called surface waves. This distinguishes them from the types of wave that propagate inside, and are totally confined by, ...
Heuristic Green`s function of the time dependent
... solution it can be foreseen to overcome the limits of the DE and to immediately obtain a twofold improvement: (i) the error determined by approximations of the theory would be drastically reduced, therefore modelling by simulations would be more accurate; (ii) measurements carried out in conditions ...
... solution it can be foreseen to overcome the limits of the DE and to immediately obtain a twofold improvement: (i) the error determined by approximations of the theory would be drastically reduced, therefore modelling by simulations would be more accurate; (ii) measurements carried out in conditions ...
Nomarski differential interference-contrast microscopy
... cemented surface of th is prism. (For greater clarity, one of the prism segments is dotted) . If the center plane of the Wollaston prism lies in the iamp-side focal plane of the condenser, the two beams will travel along parallel path s, slightly separated laterally in relati on to each other, after ...
... cemented surface of th is prism. (For greater clarity, one of the prism segments is dotted) . If the center plane of the Wollaston prism lies in the iamp-side focal plane of the condenser, the two beams will travel along parallel path s, slightly separated laterally in relati on to each other, after ...
Time-resolved detection of propagating Lamb waves in thin
... modes are visible. All observed frequencies are plotted in Fig. 4 with respect to their grating period including the first three harmonics. Because it is not possible to distinguish, which mode belongs to which wavevector, we did not assign any mode to an individual wavevector. As for the 100 nm gra ...
... modes are visible. All observed frequencies are plotted in Fig. 4 with respect to their grating period including the first three harmonics. Because it is not possible to distinguish, which mode belongs to which wavevector, we did not assign any mode to an individual wavevector. As for the 100 nm gra ...