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Related Concept Videos

Lossless Lines01:23

Lossless Lines

In electrical engineering, a lossless transmission line is characterized by a purely imaginary propagation constant and a resistive characteristic impedance. The ABCD parameters, which describe the relationship between the input and output voltages and currents, indicate an equivalent π circuit with an imaginary series impedance and a shunt admittance. This results in a transmission line that, when the product of the phase constant (beta) and the length of the line is less than pi, exhibits...
Traveling Waves: Lossless Lines01:27

Traveling Waves: Lossless Lines

The provided content explores the behavior of traveling waves on single-phase lossless transmission lines. It begins with a single-phase two-wire lossless transmission line of length Δx, characterized by a loop inductance LH/m and a line-to-line capacitance C F/m. These parameters result in a series inductance LΔx and a shunt capacitance CΔx.
Propagation of Waves01:07

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When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
Boundary Conditions: Lossless Lines01:21

Boundary Conditions: Lossless Lines

Consider a single-phase, two-wire, lossless transmission line terminated by an impedance at the receiving end and a source with Thevenin voltage and impedance at the sending end. The line, with length, has a surge impedance and wave velocity determined by the line's inductance and capacitance.
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Major Losses in Pipes01:28

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When a fluid flows through a pipe, it experiences energy losses due to frictional resistance along the pipe walls, known as major losses. These energy losses result in a pressure drop, which varies based on the flow conditions — whether laminar or turbulent — and the specific physical properties of the fluid and pipe.
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Lossy Lines and Overvoltages

Transmission-line series resistance and shunt conductance cause three primary effects: attenuation, distortion, and power losses.
Attenuation
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Fabrication And Characterization Of Photonic Crystal Slow Light Waveguides And Cavities
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Simple method to characterize nonlinear refraction and loss in optical waveguides.

Jeremiah J Wathen1, Vincent R Pagán, Thomas E Murphy

  • 1Laboratory for Physical Sciences, College Park, Maryland 20740, USA. wathenjj@lps.umd.edu

Optics Letters
|November 21, 2012
PubMed
Summary

This study introduces a new method to measure the third-order nonlinearity in optical waveguides. The technique accurately determines the ratio of imaginary to real parts without needing precise optical loss or pulse shape data.

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Area of Science:

  • Nonlinear Optics
  • Materials Science
  • Optical Engineering

Background:

  • Third-order nonlinearity is crucial for all-optical signal processing.
  • Accurate characterization of nonlinear optical properties in waveguides is essential for device design.
  • Existing methods often require precise knowledge of experimental parameters, limiting their applicability.

Purpose of the Study:

  • To develop a robust and accurate method for measuring the ratio of the imaginary to real parts of third-order nonlinearity.
  • To provide a technique that is independent of coupling efficiencies, propagation loss, and pulse shape.
  • To characterize the nonlinear optical properties of various semiconductor waveguides.

Main Methods:

  • A novel measurement technique is presented.
  • The method relies on analyzing the nonlinear response of optical waveguides.
  • It bypasses the need for detailed knowledge of system parameters like coupling efficiency and optical loss.

Main Results:

  • The technique accurately measures the ratio of the imaginary and real parts of third-order nonlinearity.
  • The method was successfully applied to silicon, GaAs, and AlGaAs waveguides.
  • Characterization revealed variations in nonlinearity based on alloy concentration in AlGaAs.

Conclusions:

  • The developed method offers a reliable way to quantify third-order nonlinearity in optical waveguides.
  • This technique simplifies the characterization process, making it more accessible.
  • The findings contribute to the understanding and design of nonlinear optical devices using various semiconductor materials.