Effect of Stimulated Radial Scattering Accompanied by Excitation of Converging Acoustic Waves in Optical Media Pumped by High-Power Nanosecond Pulses with Broad Spectrum

Author(s):  
N. E. Bykovskii
2021 ◽  
Vol 129 (7) ◽  
pp. 876
Author(s):  
Н.Е. Быковский

The mechanism of stimulated radial scattering and the specific damages caused by it in the surface layers of optical media, which are most clearly manifested in media with a low threshold of the bree transition phases, are considered. These fractures are the result of plastic deformation of the surface under the action of converging acoustic waves generated by radial scattering. It is shown that stimulated radial scattering can be responsible for laser destruction of interference mirrors, and a mechanism for its excitation in thin layers is proposed.


2017 ◽  
Vol 60 (3) ◽  
pp. 356-361 ◽  
Author(s):  
V. V. Kladukhin ◽  
S. V. Kladukhin ◽  
A. A. Novoselov ◽  
S. P. Khramtsov
Keyword(s):  

2000 ◽  
Vol 10 (03) ◽  
pp. 735-792 ◽  
Author(s):  
IVAN D. AVRAMOV

Since the first successful surface transverse wave (STW) resonator was demonstrated by Bagwell and Bray in 1987, STW resonant devices on temperature stable cut orientations of piezoelectric quartz have enjoyed a spectacular development. The tremendous interest in these devices is based on the fact that, compared to the widely used surface acoustic waves (SAW), the STW acoustic mode features some unique properties which makes it very attractive for low-noise microwave oscillator applications in the 1.0 to 3.0 GHz frequency range in which SAW based or dielectric resonator oscillators (DRO) fail to provide satisfactory performance. These STW properties include: high propagation velocity, material Q-values exceeding three times those of SAW and bulk acoustic waves (BAW) on quartz, low propagation loss, unprecedented 1/f device phase noise, extremely high power handling ability, as well as low aging and low vibration sensitivity. This paper reviews the fundamentals of STW propagation in resonant geometries on rotated Y-cuts of quartz and highlights important design aspects necessary for achieving desired STW resonator performance. Different designs of high- and low-Q, low-loss resonant devices and coupled resonator filters (CRF) in the 1.0 to 2.5 GHz range are characterized and discussed. Design details and data on state-of-the-art STW based fixed frequency and voltage controlled oscillators (VCO) with low phase noise and high power efficiency are presented. Finally, several applications of STW devices in GHz range data transmitters, receivers and sensors are described and discussed.


Author(s):  
John S. Viator ◽  
Steven L. Jacques ◽  
Guillermo Aguilar

Successful treatment of port wine stain (PWS) birthmarks in human skin utilizes cryogen spray cooling (CSC) in conjunction with laser treatment. CSC pre-cools the epidermis to protect it from subsequent laser irradiation which raises the temperature of both the epidermis and the deeper PWS. As the epidermal temperature is depressed by cryogen, damage to the skin surface is minimized while the PWS reaches temperatures sufficient to permanently damage the lesion. In order to optimize cooling and laser heating dosages and to properly guide laser therapy, the spatial relationship of epidermal melanin and PWS must be known. Photoacoustic depth profiling of human skin uses low energy, nanosecond pulses of laser light to induce acoustic waves in optically absorbing media, such as blood and melanin. We used a 532 nm Nd:YAG laser to measure total epidermal melanin content in human skin, comparing the results with visible reflectance spectroscopy. Furthermore, we performed numerical simulations of photoacoustic generation in skin, showing that a hemisperical acoustic sensor array could be used to reconstruct the rete pattern of epidermal melanin in the basal layer. Finally, we built a hemispherical probe for use in future experiments for imaging of human skin.


2007 ◽  
Vol 52 (7) ◽  
pp. 756-764 ◽  
Author(s):  
A. M. Efremov ◽  
V. I. Koshelev ◽  
B. M. Koval’chuk ◽  
V. V. Plisko ◽  
K. N. Sukhushin
Keyword(s):  

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