Visible laser

From the Heisenberg uncertainty principle as stated in Equation (1.16) estimate, in cm and Hz, the wavenumber and frequency spread of pulsed radiation with a pulse length of 30 fs, typical of a very short pulse from a visible laser, and of 6 ps, typical of pulsed radiofrequency radiation used in a pulsed Fourier transform NMR experiment. 

One method of mode locking a visible laser is by placing an acoustic modulator in the cavity and driving it at a frequency of c/2d. 

GaAs/AlGalnP visible lasers, orange LEDs HgCdTe detectors... 

A dilute I2/CCI4 solution was pumped by a 520 nm visible laser pulse, promoting the iodine molecule from its ground electronic state X to the excited states A,A, B, and ti (Fig. 4). The laser-excited I2 dissociates rapidly into an unstable intermediate (I2). The latter decomposes, and the two iodine atoms recombine either geminately (a) or nongeminately (b) ... 

Vj = 1 <— v" = 1 transition will be at a different energy than the Vj = 0 <— v" = 0. We use this fact to measure the vibrational spectrum of V (OCO) in a depletion experiment (Fig. 12a). A visible laser is set to the Vj = 0 Vj = 0 transition at 15,801 cm producing fragment ions. A tunable IR laser fires before the visible laser. Absorption of IR photons removes population from the ground state, which is observed as a decrease in the fragment ion signal. This technique is a variation of ion-dip spectroscopy, in which ions produced by 1 + 1 REMPI are monitored as an IR laser is tuned. Ion-dip spectroscopy has been used by several groups to study vibrations of neutral clusters and biomolecules [157-162]. 

Figure 12. Vibrational action spectra of V (OCO) in the OCO antisymmetric stretch region, (a) Spectrum obtained by monitoring depletion in the photofragment produced by irradiation at the vibronic origin at 15,801 cm The IR absorption near 2391.5 cm removes molecules from V[" = 0, leading to an 8% reduction in the fragment yield, (b) Spectrum obtained by monitoring enhancement in the VO+ photofragment signal as the IR laser is tuned, with the visible laser fixed at 15,777 cm (the Vj = 1 v" = 1 transition). The simulated spectrum gives a more precise value of the OCO antisymmetric stretch vibration in V" (OCO) of 2392.0 cm .

Second-order NLO processes, including SFG, are strictly forbidden in media with inversion symmetry under the electric dipole approximation and are allowed only at the interface between these media where the inversion symmetry is necessarily broken. In the IR-Visible SFG measurement, a visible laser beam (covis) and a tunable infrared laser beam (cOir) are overlapped at an interface and the SFG signal is measured by scanning cOir while keeping cOvis constant. The SFG intensity (Isfg) is enhanced when coir becomes equal to the vibration levels of the molecules at the interface. Thus, one can obtain surface-specific vibrational spectra at an interface... 

Visible lasers are typically used for sample excitation, although near-IR lasers can be used when visible excitation sources cause sample fluorescence, obscuring the Raman scatter. 

As an alternative to planar waveguiding structures we report here the fabrication of crystal cored fibres in which it is possible to maintain uniform guide dimensions over long lengths. These fibres with organic crystal core material having large second order non-linearity could be used for miniaturization of visible laser sources and realization of parametric amplifiers for optical communications. 

Fig. 3.5. Experimental apparatus for time-resolved THz transmission spectroscopy. The sample is excited with a visible laser pulse delivered by delay line 3. A singlecycle THz electric-field transient probes the polarization response of the sample after time delay tv scanned by delay line 1. The transmitted THz amplitude is monitored via ultrabroadband electro-optic sampling in a THz receiver as a function of time T scanned by delay line 2. From [13]...

The subsequent development of laser diode sources at low cost, and improved electronic detection, coupled with new probe fabrication techniques have now opened up this field to higher-temperature measurement. This has resulted in an alexandrite fluorescence lifetime based fiber optic thermometer system,(38) with a visible laser diode as the excitation source which has achieved a measurement repeatability of l°C over the region from room temperature to 700°C, using the lifetime measurement technique. 

The existence of a strong absorption band, at low energy region that corresponds to the 4Az — 47 transition, allows the use of a great variety of diode light sources, especially the powerful visible laser diodes recently developed, as discussed. This is... 

Z. Y. Zhang, K. T. V. Grattan, and A. W. Palmer, Thermal characteristics of alexandrite fluorescence decay at high temperatures, induced by a visible laser diode emission, J. Appl. Phys. 73(1), 3493-3498 (1993). 

M. A. Gondal, A. Hameed, and A. Suwaiyan, Photo-catalytic conversion of methane into methanol using visible laser, Appl. Catal. A 243(1), 165-174 (2003). 

In the case of the sulphur triimide S(NBu-f)3, the dispersive Raman technique applying a double monochromator and a CCD camera was employed to obtain the information from polarized measurements (solution studies) and also to obtain high-resolution spectra by low-temperature measurements. In the case of the main group metal complex, only FT-Raman studies with long-wavenumber excitation were successful, since visible-light excitation caused strong fluorescence. The FT-Raman spectra of the tetraimidosulphate residue were similar to those obtained from excitation with visible laser lines. 

Room temperature ILs have been the object of several Raman spectroscopy studies but often ILs emit intensive broad fluorescence. In our own experiments, the use of visible laser light (green 514.5 nm or red 784 nm) resulted in strong fluorescence [29,46]. Similar observations have been reported for many IL sysfems. Our experimental spectra needed to be obtained by use of a 1064 nm near-IR exciting source (Nd-YAC laser at 100 mW of power). The scattered light was filtered and collected in a Bruker... 

Multifunctional oxime ester photoiniators, (II), were prepared by Kunimoto et al. (2), which were activated in the 150- to 600-nm range using ultraviolet (UV) and visible lasers and were used in imaging applications. 

As with terbium, a great deal of study has been made upon this ion in hopes of using it in a visible laser. Experiments along this line appear to have been very successful, and reports have been made on oscillation in crystals (757), glasses, and liquids (138). 

Ultraviolet lasers such as the He-Cd laser used in 3D Systems SLA 1 and SLA 250 have a number of drawbacks. The power available is somewhat limited and the lifetime of the laser tube tends to be uneconomical. Since high power, stable visible lasers are available and convenient, targeting stereolithographic systems to them is an obvious goal. 

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