Polarized light enters the device from the top,
passes through the cover glass, transparent electrode and liquid crystal layer,
is reflected off the aluminum pixel electrodes, and returns on the same path.
Drive signals travel through
Reflective Analog SLMs
All of our liquid crystal on silicon (LCoS) backplanes incorporate analog data
addressing with high refresh rates to provide the lowest phase ripple SLMs
available. Users can select standard or high speed liquid crystal for optimal
performance. Liquid cooling systems are available to remove heat via the back of
the SLM chip in order to maximize optical power handling capabilities:
Small 512 x 512 � Entry Level � Educational � Economical
Our legacy SLM is now available as our E-Series
model. It is ideally suited for labs with a limited budget or researchers who do
not require the high speed features of our premium SLMs, yet still demand high
performance. This entry-level SLM is affordably priced without sacrificing
quality.
Specification:
Resolution |
512 x 512 |
Fill Factor |
83.4 - 100% |
Array Size |
7.68 x 7.68 mm |
Diffraction
Efficiency* |
61 - 99% |
Pixel Pitch |
15 x 15 �m |
Controller |
PCIe 8-bit, PCIe
16-bit, DVI 16-bit |
Wavelength (nm) |
Wavefront distortion |
Liquid crystal response time
[standard / high efficiency]
(ms) |
AR coatings [Ravg<1%] (nm) |
|
|
Model E512/PDM512 |
Model HSP512/HSPDM512 |
Model ODP512/ODPDM512 |
|
405 |
λ/5 |
25 / 33.3 |
N/A |
3 / 4 |
400 - 850 |
532 |
λ/7 |
33.3 / 45 |
7 / 10 |
3.5 / 4.5 |
400 - 850 |
635 |
λ/8 |
33.3 / 45 |
12 / 16.7 |
4 / 5 |
400 - 850 |
785 |
λ/10 |
55.5 / 80 |
17.2 / 22.2 |
4.5 / 5.5 |
600 - 1300 |
1064 |
λ/10 |
66.7 / 100 |
10 / 16.7 |
5 / 6 |
600 - 1300 |
1550 |
λ/12 |
100 / 130 |
20 / 28.5 |
6 / 7 |
850 - 1650 |
*Silicon
backplane, performance varies as a function of wavelength.
Large 512 x 512 � Analog Spatial Light Modulator
This high voltage, large pixel SLM is optimized for
high power applications requiring faster response times. The analog, high fill
factor, high refresh rate backplane provides better optical efficiency and high
temporal stability. Large pixels reduce pixel-to-pixel crosstalk.
Specification
Resolution |
512 x 512 |
Fill Factor |
96% |
Array Size |
12.8 x 12.8 mm |
Diffraction
Efficiency* |
2% |
Pixel Pitch |
25 x 25 �m |
Controller |
PCIe 8-bit, PCIe
16-bit, DVI 16-bit |
Wavelength (nm) |
Wavefront distortion |
Liquid crystal response time
[standard / high efficiency]
(ms) |
AR coatings [Ravg<1%] (nm) |
|
|
Model P512L/PDM512L |
Model HSP512L/HSPDM512L |
|
405 |
λ/5 |
3.0 / 4.5 |
N/A |
400 - 850 |
532 |
λ/5 |
4.0 / 6.0 |
1.2 / 2.0 |
400 - 850 |
635 |
λ/6 |
4.5 / 7.0 |
1.7 / 3.0 |
400 - 850 |
785 |
λ/7 |
7.5 / 12.0 |
2.5 / 4.0 |
600 - 1300 |
1064 |
λ/10 |
10.0 / 15.0 |
3.3 / 5.0 |
600 - 1300 |
1550 |
λ/12 |
15.0 / 25.0 |
4.2 / 6.5 |
850 - 1650 |
1920 x 1152 � Analog Spatial Light Modulator
This SLM offers large format, high fill factor (high
optical efficiency), high-speed (as fast as 1.4 ms), low phase ripple (.2 � 3%),
high optical power handling (up to 15 GW/cm2 peak power density), and high
refresh rate. This analog, high voltage backplane produces very stable phase
patterns, coupled with fast liquid crystal response times.
Specification
Resolution |
1920 x 1152 |
Fill Factor |
95.7% |
Array Size |
17.6 x 10.7 mm |
Diffraction
Efficiency* |
88% |
Pixel Pitch |
9.2 x 9.2 �m |
Controller |
PCIe 8/12-bit,
HDMI 8/12-bit |
Wavelength (nm) |
Wavefront distortion |
Liquid crystal response time
[standard / high speed] (ms) |
AR coatings [Ravg<1%] (nm) |
|
|
Model P1920 |
Model HSP1920 |
|
405 |
λ/3 |
6 |
N/A |
400 - 850 |
532 |
λ/5 |
9 |
1.4 |
400 - 850 |
635 |
λ/6 |
12 |
1.8 |
400 - 850 |
785 |
λ/7 |
19 |
2.5 |
600 - 1300 |
1064 |
λ/10 |
25 |
3.3 |
600 - 1300 |
1550 |
λ/12 |
33 |
5.0 |
850 - 1650 |
1 x 12,288 � Linear series Spatial Light Modulator
The only high resolution linear array on a silicon
backplane available on the market. The high refresh rate analog backplane
provides excellent temporal stability. Our production process results in 100%
fill factor, giving high optical efficiency.
Specification
Resolution |
1 x 12,288 |
Fill Factor |
100% |
Array Size |
19.66 x 19.66 mm |
Diffraction
Efficiency* |
99% |
Pixel Pitch |
1.6 �m x 19.66 mm |
Controller |
PCIe 16-bit |
Wavelength (nm) |
Liquid crystal response time
(ms) |
AR coatings [Ravg<1%] (nm) |
|
Model P1920 |
|
405 |
N/A |
N/A |
532 |
4.5 |
400 - 850 |
635 |
5 |
400 - 850 |
785 |
8.5 |
600 - 1300 |
1064 |
15 |
600 - 1300 |
1550 |
30 |
850 - 1650 |
Transmissive Spatial Light Modulator
Our transmissive hexagonal array SLMs are designed
for adaptive optics applications. The two dimensional array of Liquid Crystal
Variable Retarders acts as a real time programmable phase mask for wavefront
correction of a linear polarized source.
Unwanted aberration effects are removed by introducing the opposite phase shift
through the Hex SLM. The most common applications involve high-resolution
imaging where viewing through an aberrant medium is unavoidable. Examples
include astronomical imaging with ground-based telescopes and medical imaging
through body fluids. High-energy laser users also benefit from active phase
compensation for beam profile correction.
Optical
head specifications |
Retarder
material |
Nematic liquid crystal |
Substrate material |
Optically quality synthetic
fused silica |
Center
wavelength |
450-1800nm (specify) |
Modulation range |
Phase
(min) amplitude |
1λ optical path difference
0-100% |
Retardance uniformity |
<2%rms variation over clear
aperture |
Transmitted wavefront distortion |
≤ λ/4 (P-V @ 633)
[≤ λ/10 (RMS @ 633)] |
Surface
quality |
40-20 scratch-dig |
Beam
deviation |
< 2 arc min |
Transmittance |
> 90% (without polarizers) |
Reflectance (per surface) |
≤ 0.5% at nominal incidence |
Dimension |
7.00 x 2.96 x 0.74 in |
Recommended safe operating limit |
500W/cm�, CW
300mJ/cm�, 10ns, 532nm |
Temperature range |
10 - 45 �C |
Controller specifications |
Output voltage |
2kHz ac square wave digitally
adjustable
0-10 Vrms |
Voltage resolution |
2.44mV (12 bit) |
Computer interface |
USB |
Power requirements |
100 � 240VAC @ 47-63Hz, 1A |
Dimensions |
9.50 x 6.25 x 1.50 in |
Weight |
2 lbs. |
Note that the D31258 in
included with the purchase of the SLM system |
SLM Optics Kit
Spend your time on important research rather than
designing an optical system for your SLM. The SLM Optics Kit provides you with a
set of optics and cage-mount components enabling the user to start research with
the SLM system immediately. The kit includes a Half-Wave Retarder, a pair of
Linear Polarizers, lenses, and all necessary mount hardware, including a custom
adapter plate to quickly align the SLM system to the optics in an off-axis
configuration. Optional items are also available including a laser, beam
expander optics, and a camera. This approach provides optimum efficiency with
minimal design effort.
Optics Kit includes:
1-Photon SLM
Microscopy Kit
The
1-Photon SLM Microscopy Kit is a scan-less SLM-based epi-fluorescence upright
microscope that enables three dimensional calcium imaging and/or photoactivation
of neurons in brain slices. The microscope can be used to excite and monitor
activity of neuronal ensembles, enabling studies of neuronal circuit activity
both in vitro and in vivo. Add-on to existing microscope or use as stand-alone
microscope.
KEY
FEATURES
-
Scan-less SLM-based
-
Fully
functional programmable excitation system
-
Brightfield and/or Epifluorescence microscope
-
3D
calcium imaging capability
-
Point
and click software to define excitation patterns
Optical
Tweezers Cube
Our Cube
provides researchers with a portable, stand-alone, optical tweezers system just
one cubic foot in size. This compact instrument allows a user to optically trap
and thus physically manipulate hundreds of microscopic objects in three
dimensions (3D) using computer control to set and move each optical trap
independently.
Optical trapping can be used to manipulate objects ranging in size from 10�s of
nanometers to 10�s of microns and objects with a variety of material
characteristics. Trapping examples include cellular organisms, dielectric
spheres, metallic spheres, metallic nanoshells, carbon nanotubes, air bubbles,
and even water droplets in air.
One application of the CUBE includes biological research. This tool enables
measurements of cell properties and controlled studies of how cells interact
with foreign objects. Another application example is trapping metallic objects
and carbon nanotubes for engineering materials with unique thermal and
electrical properties.
KEY
FEATURES
-
Complete optical trapping system
-
3D
particle manipulation using holographic beam control
-
100�s
of traps (demonstrated 400)
-
High
temporal trap stability
-
Spatially uniform trapping across 200x200 micron field of view
SPM |