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It is capable of finding the bound, leaky, and complex modes for optical fibers and waveguides including photonic crystal fibers (PCF), dielectric fibers and waveguides.
In a homogeneous and isotropic solid, elastic waves can propagate through three different polarization modes, two transverse modes and one longitudinal mode, in contrast to only two transverse modes (TE and TM modes) for optical waves.
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We summarize how OAM enables efficient mode multiplexing for optical communications, with emphasis on the design of OAM fibers.
We present a second kind integral equation (SKIE) formulation for calculating the electromagnetic modes of optical waveguides, where the unknowns are only on material interfaces.
This paper establishes what we call Position-Referenced Microscopy (PRM) as a mature technique for live cell culture monitoring by using various modes of optical microscopy.
Our discovery extends applicability of the Dirac mode in designing for optical devices.
A correspondence between available notations for optical modes of graphene in the different points of the Brillouin zone are provided.
A multi-channel waveguide-mode sensor was used for optical measurement.
We present a 1300 nm Fourier domain mode locked (FDML) laser for optical coherence tomography (OCT) that combines both, a high 1.6 MHz wavelength sweep rate and an ultra-long instantaneous coherence length for rapid volumetric deep field imaging.
The factor group analysis predicts that there should be 105 optical modes for Pca21 structure of Bi2WO6 distributed among 26A1 + 27A2 + 26B1 + 26B2 irreducible representations.
Since the other optical modes for intra-cavity cooling in the high-finesse IR cavity are derived via EOMs and AOMs from the fundamental laser mode (see Section 7.2.3), they also follow any changes of the cavity resonance frequency.
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