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The sound wave generated by the elds E2 and E3 scatters the pump beam 1 into the conjugate beam 4 The beating of the elds 1 and 4 ampli es the sound wave and leads to an increasing intensity of the conjugate beam This is equivalent to an increasing re ectivity of the SBS mirror A distinct attenuation of E2 takes place This enables the switching from BEFWM to SBS in the description of the PCM Then, only the elds E1 and E4 are of signi cant importance in the resonator The scattering of the weaker pump E2 into the signal beam E3 is also possible, but this process has only a low ef ciency as pointed out in Refs 23 and 60 Figure 3.

blocking solution, which blocks any nonspeci c antibody binding sites. This is followed by washing with an antibody solution (e.g. rabbit IgG). Antibodies bind to epitopes on proteins. Bound antibodies are visualized by washing with a second antibody speci c for the class of antibodies to

19 shows how the ignition of the SBS mirror and consequently the Q-switch operation of the SBS-laser oscillator can be achieved best by choosing a resonant-start resonator length that is a multiple of the particular Brillouin length If the start resonator length is too far from this resonant length, the laser operates in spiking only In those cases the beat frequencies of the start resonator modes are spectrally too far away from nB to stimulate the sound wave in the SBS mirror For the measurements of Fig 319 the length of the start resonator in an Nd:YALO SBSlaser oscillator was varied The pulse energy, its standard deviation, the longitudinal mode frequencies, and their beat frequencies were measured While varying the start resonator length, it was assured that the start resonator remained stable.

Figure 10.17. Protein arrays. There are two general types of protein arrays. (a) Analytical array for detection of antigens in serum. Multiple antibodies are attached at spots on array. These can bind speci c uorescently labelled antigens in biological uid (e.g. serum). In this example antigens a and d are detected. (b) Functional protein arrays are based on bioactivity of proteins such as receptor-ligand, enzyme-substrate recognition

Also, an almost constant fundamental mode volume in the laser rod was used by setting the second telescope length appropriately (see Fig 320) The suspension of the Q switch at the resonator lengths Lstart % 4LB (SBS cell in the middle of the start resonator) can be explained by two counterpropagating sound waves in the SBS cell [8, 61] which are the result of a BEFWM without an effective re ectivity [62] Working with liquid SBS materials, this resonance behavior of the start resonator length does not have to be that distinct and can even vanish For the same start resonator length the ratio of the Brillouin line width and spectral width of the longitudinal modes in the start resonator will be bigger.

Figure 15-11: Setting up the Target2Frames Action to have one link change the contents of two frames at once

An ef cient generation of the sound wave becomes possibly independent of the start resonator length Lstart if the Brillouin gain line overlaps with the beat frequency of the longitudinal modes which is closest to the Brillouin frequency: k Dnstart(Lstart) % nB 36 LONGITUDINAL MODES OF THE LINEAR SBS LASER.

major advantage of this con guration is that the phase conjugate re ectivity may be larger than unity if the signal intensity is small enough This principle can be used in self-starting oscillators [30, 31] The use of a phase conjugate mirror by degenerate four-wave mixing as the end mirror of a laser cavity has been studied theoretically [32] and experimentally [33], but this architecture needs an additional laser source to provide two pump beams, which is not favorable to applications In self-pumped phase conjugation, this drawback is bypassed at the expense of a re ectivity limited to unity Self-pumped phase conjugation has been widely studied since the early 1980s In 1982, a self-pumped phase conjugator using BaTiO3 was proposed [1].