The fiber detector calculates the coupling efficiency of an incident field into a single-mode optical fiber. The coupling efficiency is defined as the "fraction of the power of the incident optical field mode that is coupled into the propagating mode of an optical system" [1]. Optiscan calculates the coupling efficiency using the overlap integral described in the important equations section. It should be noted that the coupling efficiency is always a number between 0 and 1, because it is the fraction of the incident power that is accepted by the fiber.
Select Build -> Detectors -> Fiber in the main model panel.
Click on Arrange Object and drag the fiber detector 
to the desired position.
On opening the fiber detector icon for editing, the propagating mode patterns
for X, Y, and Z polarizations are displayed.
The default fiber detector in Optiscan is square-shaped with
dimensions of (10 microns x 10 microns) and a sampled array size of (200x200).
The default X and Y polarization mode patterns are single-mode Gaussians [2] with
1/e2 radii of 1.944 microns at a wavelength of 1550 nm, corresponding to
a fiber core diameter of 5 microns. The indices of refraction for the core and cladding used in
calculating the 1/e2 radius are nco = 1.5 and ncl = 1.4.
The default mode pattern for the Z-polarization direction is zero, because the optical fields
are presumed to be completely transverse to the axis of the fiber.
The size and sampling of the fiber detector can be reconfigured by the user by
selecting the PROPERTIES menu item and clicking on GO. This
opens the DETECTOR DIMENSIONS window. This window functions
exactly like the DIMENSIONS windows for the SOURCE object, SIMPLE RESPONSIVITY
DETECTOR, and the many TARGET objects. The size, offset and sampling rates can be
easily reconfigured by the user. However, always remember to
check your sample size so that the total array size of the
detector is reasonable. For example, be careful not to
have a detector whose size is 1cm x 1cm and whose sampling is 1e-7
x 1e-7, because this would result in an array size of 100000x100000,
which is far too large for the computer. A good rule of
thumb is to set the sampling such that the array size of the
detector is between 100 x 100 and 1000 x 1000.
The propagating mode patterns of the FIBER DETECTOR may be reconfigured.
The procedure for editing a propagating mode pattern is
identical to editing the shapes of the SOURCE or TARGET objects.
The user selects one of the editing options (replace a piece, multiply a piece, or add a piece)
in the menu selection, and follows the instructions to build
the desired propagating mode pattern. The user should note that the propagating
mode pattern of the fiber is equal to 
(see Important Equations).
Unlike the SIMPLE RESPONSIVITY DETECTOR, the user may independently alter
the mode patterns of the FIBER DETECTOR in the X,Y, and Z polarization
directions.
The output data file for the detector can be changed by selecting
the PROPERTIES menu item, and clicking on GO. When the new window
appears, click on the RESULTS FILE tab in the upper section of
the window.
Note: if more than one fiber detector is used in a project, each output file
must be named differently. This is done in the last step of editing
the fiber detector propagating mode pattern. The user must uniquely specify the
filename that the propagating mode pattern is saved under.
Once the desired detector pattern is generated, the user
links the detector into the project workspace.
Running a simulation determines the amount of power transferred from the
optical system to the fiber (i.e. the coupling efficiency).
The format of the data file is a simple ASCII text file that is tab delimited. The
following is a sample of how the data looks when imported into a spreadsheet:
| 3.52113298e-001 | 3.87943171e-001 | 3.95755503e-001 | 3.84127019e-001 | 15:32:43 |
| 3.52113298e-001 | 3.87943171e-001 | 3.95755503e-001 | 3.84127019e-001 | 15:32:47 |
| 3.52113298e-001 | 3.87943171e-001 | 3.95755503e-001 | 3.84127019e-001 | 15:32:50 |
| 3.52113298e-001 | 3.87943171e-001 | 3.95755503e-001 | 3.84127019e-001 | 15:32:53 |
Coupling Efficiency
represent the optical fields incident upon the fiber.
represent the complex conjugates of the propagating optical field modes inside the fiber.
Gaussian Beamwidth of a Single-Mode Fiber (from Reference [2])
represents the 1/e2 radius of the propagating Gaussian fiber mode.
where "a" is the radius of the fiber core, and "k" is the wave-number.
where 
is the propagating wavelength in air.
There is a slight bug that occurs when changing the mode pattern of the detector. The Y axis is reversed in the viewer that is used to select the window size and position for the new pattern element. This will cause an element positioned in the upper half of the screen in the edit window to actually appear in the lower half of the screen when the mode pattern is actually updated.
[1] K. Garcia, Calculating Component Coupling Coefficients. Laser Focus World. August 2000. Retrieved June 10, 2003.
<http://www.breault.com/ftp/docs/coupling.pdf>
A copy of this article is also available here.
[2] D. Marcuse, Loss Analysis of Single-Mode Fiber Splices, The Bell System Technical Journal, Vol. 56, No. 5, May-June 1977.
A copy of this article is also available here.
