Conventional lamp-based imaging projection technology is unable to simultaneously satisfy the demands from consumer-electronics manufacturers for projectors that are small, low in cost, con- sume little power, and offer a robust implementation, all while providing high-quality images. A number of LED- or laser-based microprojector technologies are now being developed to address these issues. Here, one manufacturer details its approach – a unique holographic laser projection technology that offers advantages over imaging and scanned-beam display technologies. from Light Blue Optics (LBS)
2. rial in existence that can independently and which is noise-free, as illustrated in Fig. 2.
continuously modulate both amplitude Auv Uniquely, the key to this holographic laser-
and phase ϕuv where huv = Auvexpjϕuv. Even projection technology lies not in the optical
if such a material became available, the result design but in the algorithms used to calculate
contains amplitude components that would the phase hologram huv from the desired
absorb incident light and reduce system effi- image Fxy. LBO has developed and patented
ciency. A much better approach is to restrict proprietary algorithms for the purposes of
the hologram huv to a set of phase-only values calculating N sets of holograms per video
ϕuv such that huv = expjϕuv. As a result, when frame, both efficiently and in real time, as first
the hologram patterns are displayed on a demonstrated in 2004.4 Crucially, such algo-
phase-modulating microdisplay and subse- rithms can be efficiently implemented in a
quently illuminated, no light is blocked. custom silicon chip.
LBO’s system uses a custom-manufactured A practical realization of a holographic
ferroelectric-liquid-crystal–on–silicon laser projector is rather simple and is shown in
(LCoS) microdisplay from Displaytech, Inc., the schematic of Fig. 3. A desired image is
to display the hologram patterns, which converted into sets of holograms by LBO’s
requires that the hologram phase ϕuv is quan- proprietary algorithms and displayed on a
tized to a set of binary values. This proce- phase-modulating microdisplay that is time-
dure inevitably introduces quantization noise sequentially illuminated by red, green, and
into the resultant image Fxy, which must be blue laser light, respectively. The subsequent
mitigated in order to maintain high image diffraction pattern passes through a lens pair
Fig. 1: The relationship between hologram
quality. Thus, the microdisplay is used to L1 and L2, which is chosen to provide an ultra-
huv and image Fxy present at the back focal
display N independent holograms per video wide projection angle in excess of 100°. As a
plane of a lens of focal length f, when illumi-
frame within a temporal bandwidth of the eye result of the phase-modulating microdisplay,
nated by coherent monochromatic light of
of 40 msec, each of which produces a sub- the incident light is steered into the desired
wavelength λ .
frame Fxy exhibiting statistically independent image pixels – without blocking – and, due to
quantization noise.3 If the intensity of the ith Fourier optics, the image remains in focus at
reasonable first guess might be to calculate displayed image is I = Fxy 2, then the time- all distances from the lens L2.
the inverse Fourier transform of the image Fxy averaged percept over N sub-frames is
to obtain the desired result. However, the Advantages of Holographic Laser Projection
1 N ( 2
result of this calculation would be fully com- Vxy = ∑ Fxyi )
N i =1
(2) Low Speckle Contrast: One of the huge
plex, and there is no liquid-crystal (LC) mate- advantages of LBO’s technology is the ability
Hologram Subframe Frame
1 N ( 2
huv = exp jϕuv Fxy = F [huv] Vxy = ∑ Fxyi )
N i =1
Fig. 2: The relationship between hologram huv, sub-frame Fxy, and frame Vxy in LBO’s holographic projection technology.
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3. holographic projection
methods 11-13 have been demonstrated to remove A demonstration of the efficacy of LBO’s
speckle, but each require that the operation is combined speckle reduction techniques is
performed multiple times per laser dwell period. shown in Fig. 4; note that laser speckle is
This is straightforward in LBO’s system substantially reduced in the projected image,
because the laser modulation frequency is low without significant loss of focal depth or
and all pixels are formed simultaneously. In resolution.
addition, the intermediate image plane formed High Brightness and Efficiency: It has
between L1 and L2 in Fig. 3 makes it simple to previously been shown15 that, due to the
embed a speckle-reduction mechanism in the phase-modulating approach to image forma-
projector optics. The high laser modulation tion, a holographic display can project signifi-
frequency and lack of an image plane make cantly brighter images than imaging and
time-varying speckle reduction techniques dif- scanned-beam systems when displaying video
ficult to implement in a scanned-beam system, and photo content. In addition, because the
as experts in the field have noted.14 These image pixels are formed using an expanded
restrictions dictate that speckle in a scanned- beam which has an extremely wide projection
beam projector can only be acceptably sup- angle, it is possible to make a holographic
pressed by using potentially costly custom laser projection system much brighter than a
diffusing screens, thereby limiting the utility scanned-beam display for the equivalent laser
of such systems in CE applications. safety classification.
Fig. 3: A schematic diagram of LBO’s pro-
jection technology.
to substantially reduce laser speckle, a phe-
nomenon that makes the image “sparkle” due
to scattering of coherent light from an opti-
cally rough projection surface and subsequent
interference at the retina. The ability to
reduce speckle is important because, not only
do users find the artifact very unpleasant, it
also severely impacts the perceived image
quality and effective resolution.
Although there have been several demon- (a) (b)
strations of speckle reduction in the literature,5-10
thus far only LBO has demonstrated the possi-
bility for speckle reduction within the projec-
tion optics of a miniature laser projector.
As has been shown previously,3 several
methods can be combined in the LBO projector
in order to reduce speckle. The first results
from the method of image generation and display
used in the LBO system. Since N phase-inde-
pendent sub-frames per video frame are shown
within the eye’s integration period, then the eye
acts to add N independent speckle patterns on an
intensity basis, and the contrast of the low-
frequency components of the speckle in the field
Vxy falls as N1/2. Evidently, some speckle reduc-
tion is inherent in LBO’s multiple holograms (c) (d)
per video frame approach to image display.
Additional methods can be combined to Fig. 4: A sample image from LBO’s projector (a) without speckle removal and (b) using a com-
further reduce the speckle contrast because N bination of speckle reduction techniques. The close-ups (c) and (d) clearly show substantial
cannot be increased indefinitely. Several speckle reduction.
24 Information Display 12/08
4. 6
The same combination of laser and phase- in fact, each pixel on the microdisplay con- L. Wang, T. Tschudi, T. Halldorsson, and
modulating hologram provides a highly tributes to every pixel in the image, making P. R. Petursson, “Speckle reduction in laser
power-efficient method of projection since, the system tolerant to microdisplay defects. projection systems using diffractive optical
unlike imaging displays, no light is blocked in It is generally accepted that microdisplay- elements,” Appl. Opt. 37, 1770–1775 (1998).
7
the system. Furthermore, the phase-modulating based technologies, whether LCoS or DLP- J. I. Trisnadi, “Speckle contrast reduction in
nature of the microdisplay means that it is not based, have the capability to offer higher laser projection displays,” Technical Report
necessary to continuously illuminate the micro- image qualities than scanned-beam systems.17 (2003).
8
display; the lasers are modulated in accordance Scanned-beam systems tend to suffer from J. I. Trisnadi, “Hadamard speckle contrast
with the frame brightness, thereby only utiliz- poor image quality due to the unacceptably reduction,” Opt. Lett. 29, No. 1, 11–13
ing the power required to illuminate “on” pixels high speckle contrast ratios,18,19 scanning (2004).
in the same way as a scanned-beam system. artifacts,20 and image distortion, making the 9
A. Mooradian, S. Antikichev, B. Cantos,
Although LBO’s projection technology use of such a technology unfeasible in appli- G. Carey, M. Jansen, S. Hallstein, W. Hitchens,
carries the overhead of hologram computa- cations where high image quality is required. D. Lee, J. M. Pelaprat, R. Nabiev, G. Niven,
tion, the overall system efficiency is expected It is well known that laser sources can pro- A. Shchegrov, A. Umbrasas, and J. Watson,
to be comparable to that of scanned-beam vide images with extremely wide color gamuts, “High power extended vertical cavity surface
systems. This is principally due to the low due to their narrow spectral bandwidth; the emitting diode lasers and arrays and their
frequency at which the lasers are modulated in Helmoltz-Kohlrausch effect can also increase applications,” Micro-Optics Conference
LBO’s system; since gray scale is formed by perceived brightness due to the psychophysical (Tokyo) (2005).
10
the hologram and because the phase-modulat- effects of highly saturated primaries. RGB LED B. Dingel, S. Kawata, and S. Minami,
ing microdisplay directs a fixed proportion of systems exhibit an acceptable color space for “Speckle reduction with virtual incoherent
light onto the image, it is only necessary to CE applications, although systems that use laser illumination using a modified fiber
modulate the laser sources with respect to white LEDs have significantly reduced array,” Optik 94, 132–136 (1993).
11
average video-frame brightness. This neces- gamuts due to the strong absorption of the S. Lowenthal and D. Joyeux, “Speckle
sitates a laser modulation frequency on the microdisplay color filters at red wavelengths. removal by a slowly moving diffuser associ-
order of 1 kHz, allowing efficient digital ated with a motionless diffuser,” J. Opt. Soc.
modulation schemes to be used for each color. Conclusion Am. 61, 847–851 (1971).
12
This is significantly more efficient than the LBO’s holographic laser projection technology Y. Imai and Y. Ohtsuka, “Laser speckle
method typically employed by scanned-beam represents a revolutionary approach to the pro- reduction by ultrasonic modulation,” Opt.
projectors, where the pixel-by-pixel method jection and display of information, exploiting the Commun. 27, 18–22 (1978).
13
of image formation requires the lasers to be physical process of two-dimensional diffraction L. Wang, T. Tschudi, T. Halldorsson, and
switched at high currents and frequencies of to form video images. Such an approach simul- P. Petursson, “Speckle reduction in laser pro-
tens of MHz using complex and power- taneously provides many compelling benefits jections with ultrasonic waves,” Opt. Eng. 39,
hungry circuitry. Furthermore, limitations in compared to competing LED- and laser-based No. 6, 1659–1664 (2000).
14
green-laser switching speed also necessitate miniature projection systems, and the ability of J. W. Goodman, Speckle Phenomena in Optics:
that the laser is inefficiently analog modulated this technology to satisfy the stringent require- Theory and Applications (2008), p. 223.
15
above and below threshold to render gray scale. ments outlined by CE and automotive customers E. Buckley, A. Corbett, P. Surman, and
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Wide Color Gamut: In imaging systems, it is display technology to market in 2009. display with dynamically addressable holo-
difficult to achieve high resolutions while graphic backlight,” SID Symposium Digest 39,
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1 16
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2
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4
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