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Analyzing photonic crystal fiber dispersion, bend loss, and coupling efficiency with MODE Solutions

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In this example, we analyze a commerically-available photonic crystal fiber design. The goals of the current example are six-fold: we measure the propagation loss, far field profile, dispersion, efficiency of coupling (and sensitivity to misalignment) to the photonic crystal fiber mode with a Gaussian beam and we examine the total loss experienced in a 90 degree bend with the aim of determining the maximum radius of curvature that can be used without the loss exceeding a threshold of 1 dB.


Step 1: Construct the photonic crystal fiber model with easy-to-use CAD editor

schematic of photonic crystal fiber within layout editor The layout editor shows all of the simulation objects. Objects can be moved and resized with simple mouse movements.
  • orange box shows the extent of the computation volume and the PML boundaries
  • take advantage of photonic crystal fiber symmetry to reduce computation time
  • use the array function to quickly create the triangular lattice
  • make use of a Sellmeier material to account for material dispersion in real, industrial glasses

Step 2: Calculate the near-field modal profile of the photonic crystal fiber and the propagation loss

near field mode profile of photonic crystal fiber Integrated analysis routines facilitate data analysis and visualization. Choose from drop-down menus which monitor you wish to analyze, and the field component of interest.
  • search over refractive index range to locate fundamental mode of interest
  • each mode found is expressed in terms of field profile, propagation loss, and effective index
  • the calculated mode for the ideal structure has a loss of 7.1X10-8dB/km

Step 3: Determine the far-field radiation profile of the photonic crystal fiber

far field projection of mode, linear scale Built-in far-field projection routines enable you to project mode profiles onto a flat screen or onto a hemispherical surface, and integrate the profile over a specified angular cone or plane.
  • large mode area photonic crystal fiber results in a very-low divergence angle beam in the far field
far field projection of mode, logarthmic scale
  • intricate spatial detail of the far field mode profile can be observed by plotting the field on a logarithmic scale

Step 4: Calculate the dispersion of fundamental photonic crystal fiber mode

dispersion of photonic crystal fiber over c-band Use built-in analysis routines to render complicated analysis simple. Perform a frequency sweep and choose from a pull-down whether you wish to analyze the propagation loss, effective index, group index, group delay, group velocity or dispersion as a function of wavelength or frequency.
  • a sweep versus frequency shows the total dispersion is about 20 ps/nm/km
  • re-performing the calculation using a constant material index reduces the dispersion to about 1.2 ps/nm/km, illustrating that the majority of the dispersion arises from material dispersion

Step 5: Determine the coupling efficiency of a Gaussian beam to the fundamental mode

coupling efficiency of Gaussian beam to photonic crystal fiber Extensive overlap analysis routines allow the end user to calculate the overlap integral and coupling efficiency between the mode of interest and a Gaussian beam, another waveguide mode, or data imported from another application such as ASAP 2005.
  • using a 10 micron beam waist radius Gaussian aligned to the center of the fiber, a 88.1% coupling efficiency results
  • the overlap analysis window shows the Gaussian beam has a modal area of 314 micron2 while the large-area photonic crystal fiber has a modal area of 581 micron2
  • estimating the alignment sensitivity is as simple as putting in an offset (say, 5 microns in the x direction) which reduces the coupling efficiency to 73.5%

Step 6: Automate simulation and analysis - measure total bend loss as a function of fiber radius of curvature

plot of total (propagation+bend) loss as a function of radius of curvature The built-in scripting environment can be used to perform parameter sweeps, customize analysis, or automate both simulation and analysis to optimize device performance.
  • ten automated simulations are performed as a function of the bend radius of curvature
  • the total bend loss (i.e. propagation loss + bend loss) is plotted on a logarthimic scale as a function of radius of curvature
  • calculate response shows that the total loss in the 90 degree bend increases very rapidly when the radius of curvature approaches tens of centimeters



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