Richard C. Hollins
Defence Evaluation and Research Agency
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Featured researches published by Richard C. Hollins.
Applied Physics Letters | 1997
Stewart N. R. Swatton; Kevin Roy Welford; Richard C. Hollins; J. Roy Sambles
We report a novel time resolved double pump–probe experimental technique that may be used to characterize the excited-state parameters of organic dyes. We show that by monitoring the time evolution of the transmittance of a dye after excitation with two pump pulses, the excited singlet and triplet absorption cross sections, the lifetime of the excited singlet state, and the triplet quantum yield may all be measured. This technique has been demonstrated for silicon 2,3-naphthalocyanine bis(trihexylsiloxide).
Journal of Laser Applications | 2000
Joseph A. Zuclich; Peter R. Edsall; David J. Lund; Bruce E. Stuck; Richard C. Hollins; Stephen Till; Peter A. Smith; Leon N. McLin; Paul K. Kennedy
The dependence of retinal damage threshold on laser spot size was examined for two pulse width regimes; nanosecond-duration Q-switched pulses from a doubled Nd:Yttrium–aluminum–garnet laser and microsecond-duration pulses from a flashlamp-pumped dye laser. Threshold determinations were conducted for nominal retinal image sizes ranging from 1.5 to 100 mrad of visual field, corresponding to image diameters of ∼22 μm to 1.4 mm on the primate retina. In addition, base line collimated-beam damage thresholds were determined for comparison to the extended source data. Together, this set of retinal damage thresholds reveals the functional dependence of threshold on spot size. The threshold dose was found to vary with the area of the image for larger image sizes. This experimentally determined trend was shown to agree with the predictions of thermal model calculations of laser-induced retinal damage for spot sizes ≳150 μm. The results are compared to previously published extended source damage thresholds and to th...
High-power lasers and applications | 1998
Richard C. Hollins
Nonlinear materials offer a wavelength-agile means of protecting sensors against damage by pulsed lasers. The paper reviews the study and development of nonlinear protection materials within DERA. Materials under study include nonlinear absorbers, scatterers, and refractors, and a powerful suite of diagnostic techniques has permitted fundamental study of the underlying nonlinear processes.
Journal of Laser Applications | 2008
Joseph A. Zuclich; P. E. Edsall; David J. Lund; Bruce E. Stuck; Stephen Till; Richard C. Hollins; Paul K. Kennedy; Leon N. McLin
In earlier studies, we examined the dependence of the laser induced retinal damage threshold on retinal image size for extended-source ocular exposures. We reported the spot-size dependence of the retinal threshold (based on ophthalmic observations at 24 h postexposure) for two pulsewidth regimes: nanosecond-duration (Q-switched) pulses from a doubled Nd:yttrium–aluminum–garnet laser and microsecond-duration pulses from a flashlamp-pumped dye laser at 590 nm. In either case, the retinal threshold was shown to vary with the area (i.e., diameter squared) for image diameters >5 mrad. More recently, we have collected additional data for the intermediate spot-size range (1.5–10 mrad) and have compared both the absolute values and the spot-size trend of retinal thresholds determined via ophthalmoscopic observation at 1 h postexposure to the analogous threshold data collected with observations at 24 h postexposure. These additional data and analyses reinforce our earlier conclusions regarding the threshold vs. s...
MRS Proceedings | 1994
Kevin Welford; Stewart Swatton; S. Hughes; S. J. Till; G. Spruce; Richard C. Hollins; B. S. Wherrett
The non-linear optical properties of chloro-aluminium phthalocyanine and 1,3,3,1′,3′,3′- hexamethylindotricarbocyanine have been studied as model systems using z-scan and time resolved experimental techniques. Excited state lifetimes and absorption cross sections have been measured as well as the spectral response of the induced absorption. Excited state lifetimes are critical in determining the performance of a reverse saturable absorber. Even though a first excited state absorption cross section may be large compared with the ground state absorption cross section the lifetimes and transition probabilities of higher lying states can lead to constraints upon how effective organic dyes are as optical limiting materials. Both novel saturation of the induced absorption at high laser fluences and intermolecular quantum beats in 1,3,3, 1′,3′,3′-hexamethylindotricarbocyanine are demonstrated experimentally and accounted for theoretically. Quantum chemical calculations have been developed to propose a probable inter-molecular mechanism for the observed quantum beats.
Biomedical optics | 2004
Paul K. Kennedy; Joseph A. Zuclich; David J. Lund; Peter R. Edsall; Stephen Till; Bruce E. Stuck; Richard C. Hollins
The dependence of retinal damage thresholds on laser spot size, for annular retinal beam profiles, was measured in vivo for 3 μs, 590 nm pulses from a flashlamp-pumped dye laser. Minimum Visible Lesion (MVL)ED50 thresholds in rhesus were measured for annular retinal beam profiles covering 5, 10, and 20 mrad of visual field; which correspond to outer beam diameters of roughly 70, 160, and 300 μm, respectively, on the primate retina. Annular beam profiles at the retinal plane were achieved using a telescopic imaging system, with the focal properties of the eye represented as an equivalent thin lens, and all annular beam profiles had a 37% central obscuration. As a check on experimental data, theoretical MVL-ED50 thresholds for annular beam exposures were calculated using the Thompson-Gerstman granular model of laser-induced thermal damage to the retina. Threshold calculations were performed for the three experimental beam diameters and for an intermediate case with an outer beam diameter of 230 μm. Results indicate that the threshold vs. spot size trends, for annular beams, are similar to the trends for top hat beams determined in a previous study; i.e., the threshold dose varies with the retinal image area for larger image sizes. The model correctly predicts the threshold vs. spot size trends seen in the biological data, for both annular and top hat retinal beam profiles.
BiOS '99 International Biomedical Optics Symposium | 1999
Joseph A. Zuclich; David J. Lund; Peter R. Edsall; Richard C. Hollins; Peter Alan Smith; Bruce E. Stuck; Leon N. McLin
The dependence of retinal damage threshold on laser spot size was examined for two pulsewidth regimes; nanosecond- duration Q-switched pulses from a doubled Nd:YAG laser and microsecond-duration pulses from a flashlamp-pumped dye laser. Threshold determinations were conducted for nominal retinal image sizes ranging from 1.5 mrad to 100 mrad of visual field, corresponding to image diameters of approximately 22 μm to 1.4 mm on the primate retina. In addition, baseline collimated-beam damage thresholds were determined for comparison to the extended source data. Together, this set of retinal damage thresholds reveals the functional dependence of threshold on spot size. The threshold dose was found to vary with the area of the image for larger image sizes. The results are compared to previously published extended source damage thresholds and to the ANSI Z136.1 laser safety standard maximum permissible exposure levels for diffuse reflections.
Laser-Induced Damage in Optical Materials: 1999 | 2000
Joseph A. Zuclich; David J. Lund; Peter R. Edsall; Richard C. Hollins; Peter Alan Smith; Bruce E. Stuck; Leon N. McLin; Paul K. Kennedy; Stephen Till
The dependence of retinal damage threshold on laser spot size was examined for two pulsewidth regimes; nanosecond- duration Q-switched pluses from a doubled Nd:YAG laser and microsecond-duration pulses from a flashlamp-pumped dye laser. Threshold determination were conducted for nominal retinal image sizes ranging form 1.5 mrad to 100 mrad of visual field, corresponding to image diameters of approximately 22 micrometers to 1.4 mm on the primate retina. Together, this set of retinal damage threshold reveals the functional dependence of threshold on spot size. The threshold dose was found to vary with the area of the image for larger image sizes. The experimental results were compared to the predictions of the Thompson-Gerstman granular model of laser-induced retinal damage. The experimental and theoretical trends of threshold variation with retinal spot size were essentially the same, with both data sets showing threshold dose proportional to image area for spot sizes >= 150 micrometers . The absolute values predicted by the model, however, were significantly higher than experimental values, possibly because of uncertainty in various biological input parameters, such as the melanosome absorption coefficient and the number of melanosomes per RPE cell.
Laser-Induced Damage in Optical Materials: 1999 | 2000
Richard C. Hollins; Stephen Till
Although most laser injuries involve a beam which is tightly focused on the retina, some laser or laser-derived sources are inherently non-focusable and produce a large image. These sources include nonlinear optical limiters, which might be used to protect the eye against injury. Nonlinear refraction, scattering, and other processes in these devices degrade the focusability of the beam. The resultant retinal image is complex in shape, contain both focusable and non- focusable components. This paper will review the influence of these processes in different types of limiter and will examine the issues which affect retinal damage threshold for these and other large-image sources. Recent experimental data will be discussed in the light of physical models.
MRS Proceedings | 1999
Richard C. Hollins; Kenneth J. McEwan; Stephen Till; D J Lund; J A Zuclich