For inquires of any kind, contact lab director
Off Axis Interferometric Zone Plate (IZP) - This unit has a
focal length of 25 cm @ 633nm and reconstructs with a collimated
wave introduced 20 degrees off axis. The focused spot will appear
20 degrees off axis also for a total diffraction angle of 40
degrees. It was made @ 488 nm but has few aberrations because it
was contact copied from a master that was made at 633 nm. The
master was made in a silver grain film that was cleared and
processed like dichromated gelatin (DCG) to reduce scatter at the
copy wavelength. The copy is in 8 microns of DCG sandwiched
between two pieces of thin glass.
Planer Gratings, Low Spatial Frequency - These units are made
by interfering two collimated waves at small angles. The small
angle low spatial frequency samples, (approx 100 l/mm) diffract
with many orders present over a few degrees. They are similar to
sinusoidal surface phase gratings in power spectrum and exhibit
only a small Bragg selectivity. The power distribution is a
function of the phase modulation which is in turn dependent on
the available index modulation. As the spatial frequency goes
above 500 l/mm the Bragg selectivity becomes strong and a single
order dominates. These gratings are made in DCG in the range of
12 to 20 microns and each one is an original or first generation
grating exposed at 488nm.
Planar Gratings, High Spatial Frequency- A spatial frequency
is considered high when the grating spacing is about equal to the
wavelength being used. In the visible region this is around 2000
lines/mm. Higher orders are either not possible or are very weak
in this range and diffraction efficiency is dependant on
polarization as well as modulation, thickness, wavelength and
angle. Volume phase gratings can also suppress higher orders even
at low spatial frequencies if the thickness is many times the
grating spacing. If it is thick in this sense it is said to have
a high Q. The sample in this kit would be considered medium thick
at 5 to 8 microns and of moderately high frequency at 2234 l/mm.
Blazed Binary Optic Array - This is a set of six small blazed
zone plates. Two of them are negative with focal lengths of 25 cm
and two are positive with the same focal length. The other two
are positive with focal lengths of about 75 cm. These were
computer generated using a custom program written in POSTSCRIPT
language which we call ZONE. The program writes a geometric zone
plate pattern and fills the region between zones with up to 20
shades of grey which are printed as variations in dot density at
300 or 600 dots per inch.
The output on paper was photoreduced in a common 35 mm NIKON camera using KODAK 5052 TMX negative print film. The next step was to expose a 3 micron layer of photo resist with a mercury arc lamp through the negative master which produced the desired positive blazed phase pattern. The resist master was then replicated in epoxy and the embossed copies in this kit were made by chemically softening a piece of cellulose acetate and pressing it against the epoxy master to cast a positive impression. The originals were 8 inches in diameter but were reduced about 30 times in the camera. The 25 cm focal length was generated by plotting 45 zones with 10 shades of grey and the long focal length came from a print of 15 zones with 20 shades of grey. The surface roughness is from contamination on the photo resist and will unfortunately scatter some of the input light and some moire artifacts are visible indicating that we should print the originals at a higher resolution than 300 dpi.
The dispersion is low due to the small number of zones copied so
white light may be used with these optics. Blazed zone plates
exhibit good first order efficiency when the blaze depth produces
a full wavelength of phase shift. These samples are close to
correct and have very weak second orders at shorter focal lengths
as well as fairly low minus first order. Outputs are easily
observed on a white card by imaging a clear light bulb at a
distance greater than 2 meters.
Powered Holographic Reflector - These optics are produced by
interfering a plane wave on one side of the film with a spherical
wave from the other side. They are convex mirrors on one side and
concave on the other. The micro structure resembles a layered
reflective zone plate, the layers give it wavelength selectivity
in the same fashion as a multilayer dielectric laser mirror and
the zones give it angular dispersion. If there are many uniform
layers or planes then a narrow spectral band is reflected and
dispersion is only observed as an artifact in the transmitted
light.
The unit found in this kit is one of fairly short focal length
and is easy to use in white light to observe off axis
aberrations. It is not very narrow band and will show both
longitudinal and lateral dispersion. The DCG is about 8 microns
thick and has been processed to have a chirp in the spacing of
the planes as well as a gradient in the index of modulation. The
processing makes it behave as if it were thinner than it is.
Conformal Holographic Reflector - These devices have no
dispersion but can be made to have bandwidths of from 8 to 200 nm
by choosing the appropriate thickness and process. They are in
every way nearly identical to multilayer dielectric coatings. As
the angle of incidence goes off normal the reflected wave goes
toward the blue.
The unit in this kit is a medium bandwidth reflector made in an 8
micron layer of DCG by the "air gate" method. It was held in
laser light by hand in such a way that some of the light passing
through would reflect back on itself at an angle and produce
planes conformal to the film surface. The unstable hand holding
is sufficient to spoil the spatial coherence of the laser
resulting in a stable interference pattern only in a small volume
near the film surface. This effectively suppresses the formation
of diffracting structures that would otherwise result from
multiple surface reflections. These devices are sometimes called
notch filters.
High Gain Holographic Diffusing Screen - These are
projection screens that have precisely defined energy windows.
The projected image is only visible and bright when it is
originating from the correct angle and is of the correct
wavelength. Even then it can only be seen when the eyes are
positioned in the energy box or output pupil of the system.
Otherwise it is a slightly hazy piece of clear glass. These units
are made by projecting a diffuser through an aperture onto the
film from one side and then introducing an appropriate reference
wave on the other side. The reference wave for this sample was
converging to a point about half a meter away. At arms length it
should produce a bright eye box when illuminated with a white
light diverging from a point just out from the right shoulder.
This is an effective screen for stacking visual inputs since it
is nearly invisible when not illuminated correctly. It also
concentrates the projected light in a small area making possible
the use of lower power projection sources. The sample in this kit
is made in 8 microns of DCG at 488nm and processed to reflect
green light.
Holographic Scanner, 'One Shot'- This is a small 8 facet
deflector intended for use in a hand held Bar Code Scanner. At
633 nm it accepts an input beam 5 degrees off normal and
diffracts at 30 degrees off axis where it focuses at 4 different
ranges between 200 and 400 mm from the deflector. It is unique in
that it can be copied at 488 nm with a single on axis exposure.
The master was made one facet at a time at 633 nm in Agfa film
and converted to a clean gelatin hologram. Copies are made in DCG
of about 5 micron thickness. The thin film and low spatial
frequency results in low angular and polarization sensitivity
over the scanned angle but also causes losses to a negative
order. It can be glued to the end of a stick or mounted on a
motor to demonstrate how a section of a zone plate can deflect
light.
Optical Interconnect HOE, -Any optical device that connects a
source of photons with one or more detectors is an optical
interconnect. In electronic circuits, clock pulses are sometimes
made to modulate a diode laser which in turn broadcasts the pulse
through free space to other parts of the device or circuit. The
optical interconnect included in this kit is of appropriate
dimensions to connect circuit boards or components on a board
with each other. It is of a general design, made up of individual
gratings or zone plates arranged side by side or "spatially
multiplexed". It could connect a clock laser with 40 detectors,
however it was originally designed to address angularly
multiplexed pages in a photorefractive Holographic memory.
Again this HOE has been fabricated from 10 microns of gelatin, in a sandwich of two pieces of glass. The method of construction was simple step and repeat, the machinery used to change angles between exposures is made from precision rotary tables and a single mode fiber optic system. The fiber is easily positioned any where in space to serve as a point source and it carries blue-green light from an Argon laser which is necessary to generate fringes in the gelatin. Plane Gratings have been formed in the sample but plane or powered reflectors are also possible to form with the same hardware. The gelatin is thick enough to allow volume multiplexing of each individual cell. As many as 25 individual overlapping exposures have been made in this film with only a small change in angle between exposures.
This HOE can act like a faceted lens that has been cut in half and glued back together to yield two focused spots. The forty facets will cause an incoming plane wave to divide into two sets of 20 little plane waves that cross at two common planes about 38mm from the HOE surface. Encoding of information and images can be done with this type of HOE where the encoded information only appears on a specifically designed plane at a certain distance and with a certain color of light. Certain kinds of matrix operations can be made with combinations of these Hoes combined with spatial light modulators. Variable or reconfigurable interconnects may be made with the same components.