Title: Observing Transfer Functions
1Observing Transfer Functions
- For Multimode Spectrometers
2What 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.
3Ideal 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.
4Measurement Setups
5Measurement Setups
6Measurement Setups
7Point 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.
8Point Mapped Spectral Response of Photonic
Crystals
9Difficulties 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.
10Output 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
11Basic 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
12Examples of position dependent Response (Brag
Matching)
Note100.04in, tests done with a white
light Point source
13Notes 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
14Response 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.
15Basic 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
16Simplicity 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.
17Future 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.