2. Spectral Stray Light
... ranges”, it is not suited for the channels in the vicinity of the originating channel. These are characterised by a different method described in sec. 2.2. 2.2 Using a monochromator The measurements to quantify the stray light in the neighbourhood of the originating channel were performed using a mo ...
... ranges”, it is not suited for the channels in the vicinity of the originating channel. These are characterised by a different method described in sec. 2.2. 2.2 Using a monochromator The measurements to quantify the stray light in the neighbourhood of the originating channel were performed using a mo ...
Observation of Cooper minimum in Krypton using high harmonic
... both angular momentum components is shown. The = 2 partial wave component goes through zero near 83 eV, resulting in a gradual phase shift between 80 and 100 eV. The total dipole moment has a small minimum around 85 eV. We now turn to the high harmonic spectrum of argon, shown in figure 3. The Coo ...
... both angular momentum components is shown. The = 2 partial wave component goes through zero near 83 eV, resulting in a gradual phase shift between 80 and 100 eV. The total dipole moment has a small minimum around 85 eV. We now turn to the high harmonic spectrum of argon, shown in figure 3. The Coo ...
LAB - 1 AMPLITUDE MODULATION AND DEMODULATION
... varied in accordance with a modulating signal. The base band signal is referred to as the modulating signal and the output of the modulation process is called as the modulation signal. Amplitude modulation is defined as the process in which is the amplitude of the carrier wave is varied about a mean ...
... varied in accordance with a modulating signal. The base band signal is referred to as the modulating signal and the output of the modulation process is called as the modulation signal. Amplitude modulation is defined as the process in which is the amplitude of the carrier wave is varied about a mean ...
Third-harmonic Rayleigh scattering: theory and experiment
... than a beam-waist radius, a confocal parameter, and a coherence length, scales as the fourth power of particle radius. This fourth-power dependence puts this nonlinear optical technique in an advantageous position compared with the other scattering methods to detect nanoscopic objects. (ii) For part ...
... than a beam-waist radius, a confocal parameter, and a coherence length, scales as the fourth power of particle radius. This fourth-power dependence puts this nonlinear optical technique in an advantageous position compared with the other scattering methods to detect nanoscopic objects. (ii) For part ...
Nonlinear Optical Methods to Study Condensed Phase
... plotted in Figure 9. The echo signals themselves in Figure 9 are very nearly symmetric (fits to a Gaussian function are shown) meaning that it would be very difficult to extract dynamical information from fits to the echo decay. However the signals, for small values of T , do not peak at 0 . The ...
... plotted in Figure 9. The echo signals themselves in Figure 9 are very nearly symmetric (fits to a Gaussian function are shown) meaning that it would be very difficult to extract dynamical information from fits to the echo decay. However the signals, for small values of T , do not peak at 0 . The ...
