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1 > 1. This, of course, will increase the number of guided modes and will increase their confinement at the probe-beam wavelength.
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20 Gaussian beam [i.e., the horizontal beam profile shown in Fig. 9(b) is not ideally proportional to an m = 2 Gauss-Hermite beam], its far-field diffraction pattern [Fig. 9(d)] is not an ideal three-lobe pattern but rather has some additional structure. Nevertheless, this method enables us to excite the third guided mode in a waveguide rather efficiently because most of the optical power is at the vicinity of the three central lobes that are formed by two π-phase jumps.
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