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Figure 7.6. Outline design of a centrifuge. Samples contained in sample tubes (only four are shown for clarity) are placed in a rotor which is xed on a spindle. Centrifugation takes place in the rotor chamber (dashed lines) which is often armoured, refrigerated and evacuated.

that even wider pulses having the same characteristic leading-edge rise time associated with the short pulse can also produce a Stokes pulses with poor phase delity Noise modes ampli ed early in the SBS extraction by the high pump beam irradiance reached at focus can dominate the SBS extraction from the incoming pump for the duration of the pulse The competition by these modes would be expected to diminish after many tB in the case of a very long input pulse For the case of slow rise times, the irradiance shielding of the focal volume that results from pump extraction by the PC mode initiated early in the pump pulse also decreases the possibility of delity degradation by other nonlinear mechanisms such as optical breakdown, Raman conversion, and self-focusing Previous investigators have noted this pulse shape dependence of competition by other nonlinear processes [22].

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If you don t see the toolbar when you close the Customize User Interface dialog box, rightclick in any empty toolbar area (off all toolbars) and choose AS29-01 Special to display the toolbar.

It is of signi cance that the laser ampli er system used to generate the laser pulses reported in Ref 20 incorporated an SBS mirror in the ampli er chain [23] since the threshold turn-on characteristics of such a mirror combined with gain saturation in the ampli ers would be expected to generate an input pulse with a steep leading edge We believe that this explains the delity uctuations observed in that report, even when using TiCl4 with tB*2 ns It is important to note that these results do not completely resolve experimental and theoretical inconsistencies concerning the dependence of SBS phase conjugation delity on input energy They demonstrate, however, that the laser pulse shape is also very signi cant and should be given careful consideration in designing SBS phase conjugate mirrors.

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Figure 10.7. Blue native gel electrophoresis. (a) Mixtures of protein complexes are rst separated under nondenaturing conditions. (b) A track excised from the rst dimension is overlaid with agarose under denaturing conditions and electrophoresed through a second gel, separating protein components of each complex. Four complexes (1 4) are shown

The measurements suggest that for optimal wavefront reversal using an SBS focused oscillator cell and high input powers, the rise time of the incoming pulse should be comparable to or longer than the acoustic decay time in the medium This can be accomplished by a combination of pulseshape tailoring and the judicious selection of the SBS medium, and this criterion has been incorporated into our high-energy laser designs..

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Figure 4.11. Generation of ions during ESI. Charged droplets are generated in a ne spray. When exposed to warm, drying N2 gas, they undergo evaporation of matrix. Charge density increases as a result of decreasing droplet size, leading to an unstable droplet which explodes in a Coulombic explosion. Thus ions are liberated into the gas phase where they are accessible to MS analysis.

To interface the HIS, RIS, and PACS, some common guidelines are necessary. 1. Each system (HIS, RIS, PACS) remains unchanged in its con guration, data, and functions. 2. Each system is extended in both hardware and software for allowing communications with other systems.

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