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Observing Transfer Functions

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Holograms need to be aligned in XYZ, two axis of tilt and ... hologram. Detector. A white light input is broken into its spectral components and spread across ... – PowerPoint PPT presentation

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Title: Observing Transfer Functions


1
Observing Transfer Functions
  • For Multimode Spectrometers

2
What is a Transfer Function
  • This is an expression for the final output of a
    system that depends on the spatial and spectral
    characteristics of the input.
  • H is of course the function that we are looking
    for.

3
Ideal situations
  • The ideal filter for a multi-mode spectrometer is
    independent of the Input position and takes an
    averaging of the spectral distribution of the
    input plane.
  • Random photonic crystals could possibly achieve
    this ideal situation.
  • Volume holograms will always be dependent on the
    input position and form of the source.

4
Measurement Setups
5
Measurement Setups
6
Measurement Setups
7
Point Mapped Spectral Response of Photonic
Crystals
  • This setup is not yet built due to the fact that
    any serious measurement will require the computer
    controlled actuators that are on the way. It
    simply consists of a broad band white light
    illumination incident on a photonic crystal and a
    spectrometer behind the filter measuring its
    response.

8
Point Mapped Spectral Response of Photonic
Crystals
9
Difficulties with Setups
  • Holograms need to be aligned in XYZ, two axis of
    tilt and in an axis of rotation. If you have any
    of these angles misaligned you diffracted beam
    will go off in odd directions and be difficult to
    map on a detector.

10
Output of Holographic Filters
  • 2D Holograph filters give a liner shift in
    wavelength acting as a dispersive element.
  • 3D Holographic filters have the standard response
    coupled with a brag matching condition. This
    condition although it can contribute to a greater
    spectral diversity makes it much more difficult
    to understand the transfer function of the
    material

11
Basic Holographic response
A white light input is broken into its spectral
components and spread across a large spatial
area. If the input component has infinite spatial
extent and infinite angular variation the output
will wash out and become white light.
Source
hologram
Detector
12
Examples of position dependent Response (Brag
Matching)
Note100.04in, tests done with a white
light Point source
13
Notes on Masked Input
  • With the holographic systems we are building a
    mask that will interact with the calculated
    transfer function of a hologram. This transfer
    function will be a liner shift function with a
    brag matched condition. The final inversion of
    the data to make a spectrometer will be a known
    calculation and will not involve a calibration

14
Response of Photonic Crystals
  • Response of photonic Crystals is not dependent on
    the position of the Input function and is best
    expressed as a display of spectral variances.

15
Basic Photonic Crystal Response
  • Randomly arranged photonic domains allow
    different wavelengths of light to pass or even to
    be stopped all together making for a diverse
    output

16
Simplicity Of a Photonic crystal Spectrometer
The final goal of a photonic crystal spectrometer
is to mount it directly to the focal plane of a
camera and take the near field image of its
spectral response. We hope to get more variance
and a better understanding of the filter
properties of photonic crystals by looking at its
near field response. Also finer resolution with
new equipment (monochromatic and cameras)
will enable us to use the transfer properties to
complete A spectrometer.
17
Future Work
  • To complete permanent testing stations, with
    automated scanning of the inputs and outputs.
    This will enable a very detailed mapping of the
    point response of holograms, the point mapped
    spectral response of photonic crystals and the
    impulse response of both filtering mediums.
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