S S Harilal
Articles written in Pramana – Journal of Physics
Volume 42 Issue 3 March 1994 pp 231-237
P R Sasikumar S S Harilal V P N Nampoori C P G Vallabhan
High resolution optogalvanic spectrum of the (11, 7) band in the first positive system of nitrogen molecule has been recorded from 17179 to 17376 cm−1. Assignment of 432 rotational lines belonging to the 27 branches of this band has been carried out.
Volume 43 Issue 5 November 1994 pp 401-406
Achamma Kurian C V Bindhu S S Harilal Riju C Issac V P N Nampoori C P G Vallabhan
A simple method based on laser beam deflection to study the variation of diffusion coefficient with concentration in a solution is presented. When a properly fanned out laser beam is passed through a rectangular cell filled with solution having concentration gradient, the emergent beam traces out a curved pattern on a screen. By taking measurements on the pattern at different concentrations, the variation of diffusion coefficient with concentration can be determined.
Volume 44 Issue 3 March 1995 pp 225-229
Anomalous variation of thermal lens signal with concentration from rhodamine B in methanol solution
C V Bindhu S S Harilal Riju C Issac Geetha K Varier V P N Nampoori C P G Vallabhan
Thermal lens signals in solutions of rhodamine B laser dye in methanol are measured using the dual beam pump-probe technique. The nature of variations of signal strength with concentration is found to be different for 514 and 488 nm Ar+ laser excitations. However, both the pump wavelengths produce an oscillatory type variation of thermal lens signal amplitude with the concentration of the dye solution. Probable reasons for this peculiar behaviour (which is absent in the case of fluorescent intensity) are mentioned.
Volume 44 Issue 3 March 1995 pp 231-235
Pulsed photoacoustic technique to study nonlinear processes in liquids: Results in toluene
C V Bindhu S S Harilal Riju C Issac Geetha K Varier V P N Nampoori C P G Vallabhan
Pulsed photoacoustic measurements have been carried out in toluene at 532 nm wavelength using a Q-switched frequency doubled Nd:YAG laser. The variation of photoacoustic signal amplitude with incident laser power indicates that at lower laser powers one photon absorption takes place at this wavelength while a clear two photon absorption occurs in this liquid at higher laser powers. The studies made here demonstrate that pulsed photoacoustic technique is simple and effective for the investigation of multiphoton processes in liquids.
Volume 46 Issue 2 February 1996 pp 145-151
Spatial and time resolved analysis of CN bands in the laser induced plasma from graphite
S S Harilal Riju C Issac C V Bindhu Geetha K Varier V P N Nampoori C P G Vallabhan
Analysis of the emission bands of the CN molecules in the plasma generated from a graphite target irradiated with 1.06 µm radiation pulses from a Q-switched Nd:YAG laser has been done. Depending on the position of the sampled volume of the plasma plume, the intensity distribution in the emission spectra is found to change drastically. The vibrational temperature and population distribution in the different vibrational levels have been studied as function of distance from the target for different time delays with respect to the incidence of the laser pulse. The translational temperature calculated from time of flight is found to be higher than the observed vibrational temperature for CN molecules and the reason for this is explained.
Volume 49 Issue 3 September 1997 pp 317-322
Fine structure in the time of flight distribution of C2 in laser produced plasma from graphite
S S Harilal Riju C Issac C V Bindhu V P N Nampoori C P G Vallabhan
Time resolved optical emission spectroscopy is employed to study the expansion dynamics of C2 species in a graphite plasma produced during the Nd : YAG ablation. At low laser fluences a single peak distribution with low kinetic energy is observed. At higher fluences a twin peak distribution is found. It has been noted that these double peak time of flight distribution splits into a triple peak structure at distances ≥17mm from the target surface. The reason for the occurrence of multiple peak is due to different formation mechanisms of C2 species.
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