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1.
An accurate theoretical analysis is presented describing optical amplification in Er-diffused Ti:LiNbO3 channel waveguides. It follows as far as possible the theory already developed for Er-doped fibers. As optical pumping around λp≈1.48 μm is considered, a quasi-two-level model for the Er3+ ions is used with wavelength-dependent cross sections. The optical gain in the 1.53 μm<λ<1.64-μm wavelength range is evaluated. The characteristic parameters, as Er concentration profile, cross sections, pump, and signal mode distributions and waveguide (scattering) losses are taken from experiments. Examples of numerically calculated pump-, small-signal-gain-, and ASE-evolutions are presented. The model has been tested by comparing computed and experimentally observed gain characteristics for Xˆ- and Yˆ-cut LiNbO3; an almost quantitative agreement has been obtained  相似文献   
2.
The first integrated optical amplifying acoustically tunable wavelength filter in Er-doped LiNbO3 is reported. At the signal wavelength of λs=1531 nm a maximum gain of 4.8 dB has been obtained with a coupled pump power of 160 mW (λp =1484 nm). Lossless signal transmittance has been achieved with a pump power as low as 13.5 mW for λs>1561 nm  相似文献   
3.
Water extraction of semi-retted flax (Linum usitatissimum L.) fiber bundles yielded a mixture of pectic oligosaccharides and two acidic rhamnogalacturonide tetrasaccharides that were separated by size-exclusion chromatography. One- and two-dimensional nuclear magnetic resonance studies and fast atom bombardment-mass spectrometry experiments indicated that the two tetrasaccharides have a common primary structure, i.e. alpha-D-delta GalpA(1-->2)-alpha-L- Rhap(1-->4)-alpha-D-GalpA-(1-->2)-L-alpha,beta-Rhap, with a rhamnopyranose as terminal reducing end, and a 4-deoxy-beta-L-threo-hex-4-enopyranosiduronic acid at the nonreducing end. However, the two tetrasaccharides differ by an acetyl group located at the O-3 position of the internal galacturonic acid residue. These two tetrasaccharides induce the activation of D-glycohydrolases of Rubus fructicosus L. cells or protoplasts within minutes.  相似文献   
4.
An analysis of relaxation oscillations (λs~1.5 μm) in locally Er-doped optically pumped (λp~1.48 μm) waveguide lasers is reported. The theoretical model is based on time dependent rate equations for a quasi-two-level-system and on the equation of continuity for a gain medium. For the first time a numerically reliable simulation of the elementary properties of the laser oscillations was possible: the build-up time and decay of the relaxation oscillations, the time-dependent repetition period, the steady state signal output power and the evolution of the pump power versus time. Mathematically the problem can be characterized as a large boundary value problem, which can approximately be replaced by a stiff initial value problem of ordinary differential equations. In this report, pump- and signal evolution versus time are presented for planar Er-diffused Ti:LiNbO3 waveguide lasers. The numerically obtained results show a good quantitatively agreement with experimental investigations  相似文献   
5.
Single-pass and double-pass Er-diffused Z- and X-cut Ti:LiNbO3 waveguide amplifiers, optically pumped at λ p≈1484 nm, have been investigated. With a 48 mm long Z-cut amplifier device, Er-diffusion doped at 1100°C, 6.7 dB (coupled pump power Pp,c=170 mW) and 14.7 dB (Pp,c=90 mW) net small-signal gain have been achieved with a single-pass and a double-pass configuration, respectively, at the signal wavelength λs=1531 nm. A Z-cut sample doped at 1135°C showed a considerably improved behavior. 11.3 dB single-pass net small-signal gain has been obtained (Pp,c=170 mW; sample length 5.7 cm). Theoretical calculations predict gain figures up to 20 dB in single-pass and 40 dB in double-pass Er:Ti:LiNbO3 amplifiers with increased (realistic) lengths of 10 cm  相似文献   
6.
The development of a Fabry-Perot-type Ti,Er:LiNbO3 waveguide laser of optimized CW output power up to 63 mW (λs =1561 nm) at a pump power level of 210 mW (λp=1480 nm) and a slope efficiency of up to 37% is reported. The theoretical model for the waveguide laser is presented and applied to determine the optimum resonator configuration using waveguide parameters obtained from a detailed characterization of the laser sample. With pulsed pumping, waveguide laser pulses of up to 6.2 W peak power were observed. Apart from residual relaxation oscillations, the laser emission proved to be shot-noise limited  相似文献   
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