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nm pulse from ampli ed and frequency-doubled output from an SBS compressor was shifted to 629 nm by the rst SRS stage and then converted to an 780-nm pulse by the second SRS compressor stage When the Ti:sapphire was pumped by a 40-mJ pulse at 532 nm, single-pass ampli cation factors of between 10 and 15 were observed with resultant 2- to 3-mJ/picosecond pulse outputs 77 APPLICATION OF SBS PULSE COMPRESSION TO DIODE-PUMPED SOLID-STATE LASERS WITH HIGH PULSE REPETITION RATE For Brillouin optical compression in laser systems running at relatively high pulse repetition rates, competing and detrimental effects such as SRS and optical breakdown in nonlinear liquids degrade output performances and can obstruct reliable operation of the system This is on account of the surplus energy and resultant convective ows in the nonlinear media that both of these effects cause.

The previous XML Schema-based configuration example simply references a fully qualified class and method name that contains a @AspectJ annotation to define the pointcuts. This is a very simply way to reuse @AspectJ annotations which can be far more powerful than the XML Schema-based style alone. Although a method that handles security was used above, please note that private methods cannot be advised in this manner. Now that you have an understanding of how to define pointcuts using the @AspectJ style, let s move on and take a look at how advice is defined.

On the left side of the Table Style dialog box is a list of styles. From the List drop-down box, you can choose to display all styles or only styles that are in use in your drawing. To make a table style current, choose the style that you want and click Set Current.

Optical breakdown of SBS-active liquids is usually associated with microparticles in the focal waist area At low pulse repetition rates these occasional breakdowns do not signi cantly affect the SBS phase conjugation/pulse compression processes The probability of breakdown occurrence, however, not only is a function of microparticle concentration in the liquid per se, but also increases nonlinearly with pulse repetition rate Increasing the pulse repetition rate with its attendant increase in optical breakdown leads to heat accumulation in the focal region and hence increased convective ow As a result, more particles per unit time are drawn through the focal region by the convective ow including microparticles from the inner wall of the SBS cell and the frequency of optical breakdown increases In addition, this effect gives rise to the increase of the SBS threshold and subsequent phase conjugation degradation.

that it makes up to thousands of proteins amenable to examination in a single experiment and that separated proteins are made available for further analysis by procedures such as N-terminal microsequencing, MS or immunoblotting. However, it should be borne in mind that some categories of proteins are often under-represented in 2-D SDS PAGE separations including membrane, low abundance and extreme pI proteins. Except for the simplest organism, it is therefore not yet possible to separate whole proteomes in a single experiment. For this reason, we frequently concentrate instead on subproteomes. These can be selected in various ways including structural (e.g. organelles) and functional (e.g. af nity-puri ed, glycoproteins, phosphoproteins etc.). Proteomics has harnessed and developed a wide range of selection or detection methodologies.

SRS may also be detrimental for SBS compressor operation at high pulse repetition rates The adverse in uence of SRS on reliable optical pulse compression is associated with additional energy absorption in nonlinear medium due to Stokes losses in the process of Raman conversion of laser radiation Because a Raman frequency shift of 300 500 cm21 is observed for most of liquids used as SBS media, even a few percent of laser energy converted into Raman scattering, generates heat, and therefore contributes to convective ows in the medium Usually these effects can be observed under action of 2- to 3-ns pulses if the average laser power reaches approximately 10 W Convective ows lead to SBS quality degradation as well as to increasing probability of optical breakdown, as noted above In pulse compression geometry, the interaction length should be equal to or longer than half of pump pulse length.