untitledTransparent color pixels using plastic MEMS technology for
electronic papers
Y. Taii1,2a), A. Higo1,2, H. Fujita1, and H. Toshiyoshi1,2
1 Institute of Industrial Science, the University of Tokyo
4–6–1 Komaba, Meguro-ku, Tokyo 153–8505, Japan 2 Kanagawa Academy
of Science and Technology
3–2–1 Sakado, Takatsu-ku, Kawasaki-shi, Kanagawa 213–0012,
Japan
a)
[email protected]
Abstract: We present a new type of image display device that could
be used as, for instance, over-sized rewritable color posters by
using a simple MEMS fabrication technique. The mechanism of making
colors is based upon the optical interference of the Fabry-Perot
interferome- ter. A thin PEN (polyethylene naphthalate) film with
metal half-mirror was laminated over a glass substrate with an
optical cavity, and the electrostatic deformation of the film
controlled the color of the trans- mitting light. Color pixels of
three primary colors (red, green and blue) were successfully
demonstrated with driving voltage ranging from 80 to 120Vdc.
Keywords: flexible display, electronic paper, Fabry-Perot interfer-
ometer, PEN, plastic MEMS Classification: Micro- or
nano-electromechanical systems
References
[1] B. Comiskey, J. D. Albert, H. Yoshizawa, and J. Jacobson, “An
elec- trophoretic ink for all-printed reflective electronic
displays,” Nature, vol. 394, pp. 253–255, 1998.
[2] A. Yoshida, S. Fujimura, T. Miyake, T. Yoshizawa, H. Ochi, A.
Sugimoto, H. Kubota, T. Miyadera, S. Ishizuka, M. Tsuchida, and H.
Nakada, “3- inch Full-color OLED Display using a Plastic
Substrate,” Society for In- formation Display (SID) Symp. Dig.
Tech. Papers, pp. 856–859, 2003.
[3] M. S. Wu, G. S. Li, W. Yuen, and C. J. Chang-Hasnain, “Widely
tunable 1.5 µm micromechanical optical filter using AlOx/AlGaAs
DBR,” Elec- tron. Lett., vol. 33, pp. 1702–1704, 1997.
[4] C. K. Madsen, J. A. Walker, J. E. Ford, K. W. Goossen, T. N.
Nielsen, and G. Lenz, “A tunable dispersion compensating MEMS
all-pass filter,” IEEE Photon. Technol. Lett., vol. 12, pp.
651–653, 2000.
[5] M. Miles, E. Larson, C. Chui, M. Kothari, B. Gally, and J.
Batey, “Dig- ital PaperTM for Reflective Displays,” SID Symp. Dig.
Tech. Papers, pp. 115–117, 2002.
c© IEICE 2006 DOI: 10.1587/elex.3.97 Received February 10, 2006
Accepted February 21, 2006 Published March 25, 2006
97
IEICE Electronics Express, Vol.3, No.6, 97–101
[6] T. Oguchi, M. Hayase, and T. Hatsuzawa, “Driving Performance
Im- provement of the Interferometric Display Device (IDD),”
IEEE/LEOS Int. Conf. Optical MEMS and Their Applications, pp.
107–108, 2001.
[7] W. A. MacDonald, “Engineered films for display technologies,”
J. Mater. Chem., vol. 14, pp. 4–10, 2004.
[8] OPTAS-FILM http://www.cybernet.co.jp/optical/optas-film/ [9]
JIS Z8701, “Colour specification — The CIE 1931 standard
colorimetric
system and the CIE 1964 supplementary standard colorimetric
system,” 1952.
1 Introduction
Pulp papers have advantages compared with electronic displays in
terms of, for instance, thin thickness, light mass, and
portability. Clear visibility of pa- per is the most significant
attraction to viewers, who tend to read materials on printed papers
rather than on computer displays of poorer image reso- lution and
contrast. However, a problem is that the consumption of papers does
not show a sign of reduction in this information technology age,
and it is still giving strong impact to the forestry resources. For
this reason, electronic papers are expected to have the performance
equivalent or superior to those of the conventional papers before
replacing the vast amount of pulp papers.
Various kinds of electronic papers or thin image displays have been
de- veloped to meet the wide range of application requirements; for
instance, the electronic ink display based on encapsulated
electrophoresis developed by E-Ink Corporation delivers superior
wide view angle and low power con- sumption [1]. Organic
electroluminescence is suitable for making flexible full color
displays for motion pictures [2].
Besides crucial requirements such as clear visibility, mechanical
flexibility, and low power-consumption, electronic papers need to
meet the demands for low-cost productivity and the scalability to
large display area. In this report, we present a Fabry-Perot
interferometer type of image display element that could be used for
over-sized rewritable color posters, by using a simple MEMS (Micro
Electro Mechanical Systems) fabrication technique.
MEMS versions of the Fabry-Perot interferometers are commonly used
for wavelength tunable lasers [3] and optical modulators [4].
Fabry-Perot interferometers have also been employed in a MEMS
display of reflection type [5, 6], in which solid structures are
used for micromechanically movable parts and that the structures
are developed by delicate photolithography steps. In contrast to
this, our approach aims at the mechanical flexibility in future by
using a thin plastic film for the deformable Fabry-Perot membrane
and also at the scalability to larger display area.
2 Design of MEMS Transparent Color Pixels
Figure 1 shows the layered structure of the developed MEMS
transparent color pixels. A bitmap array of the miniature
Fabry-Perot interferometer
c© IEICE 2006 DOI: 10.1587/elex.3.97 Received February 10, 2006
Accepted February 21, 2006 Published March 25, 2006
98
IEICE Electronics Express, Vol.3, No.6, 97–101
constitutes the color images illuminated by a transmitting white
backlight. A thin PEN (polyethylene naphthalate) [7] film with an
aluminum semi- transparent mirror is placed on the glass substrate
with an air-gap in be- tween. The aluminum layers work as optical
reflectors and as electrodes for electrostatic operation of the PEN
membrane. The air gap spacer is simply made by a photoresist layer
of 600 nm thick.
For fabrication, an aluminum reflector/electrode and a
color-developing silicon dioxide layer (310 nm thick) were first
deposited on a glass substrate by vacuum evaporation and
sputtering, respectively. The aluminum layer was only 12 nm thick
for acceptable optical transparency. In the next step, photoresist
patterns of square openings (600 um x 600 um in area, 600 nm in
depth) were defined by the photolithography for the air cavity. On
a 16- um-thick PEN film, another metal reflector of 12-nm-thick
aluminum was deposited. The PEN film was finally laminated onto the
glass substrate.
Fig. 1. Layered structure of the transparent color pixels. An
electrostatically deformable plastic membrane with an aluminum
mirror is used in the form of the Fabry-Perot interferometer for
color development.
3 Operation of Color Development
Figure 2 illustrates the OFF and ON states of the device in
operation along with the transmission spectrum obtained by the
numerical simulation using OPTAS-FILM [8]. The pictures in Figure 2
show the top view color images taken with the optical microscope
with a color CCD camera. When no voltage was applied and the PEN
membrane stayed at the flat rest position, the transmitting light
looked dark gray to the eyes as shown in Figure 2 (a). When the
voltage was applied between two aluminum layers, on the other hand,
the upper film was electrostatically attracted to the bottom
substrate to squeeze the air gap, resulting in the change of the
color. The transmitted light interferes only in the silicon dioxide
layer, and it made green color as shown in Figure 2 (b). The
attached movie shows the ON/OFF operation
c© IEICE 2006 DOI: 10.1587/elex.3.97 Received February 10, 2006
Accepted February 21, 2006 Published March 25, 2006
99
IEICE Electronics Express, Vol.3, No.6, 97–101
of an 800-um-size pixel under the voltage of 100 Vp-p of 0.2Hz
sinusoidal wave. At operating voltage of 90V to the 600-um-size
pixel, the membrane was brought into contact to make a color with
the effective area of 62% with respect to the total pixel area. By
increasing the applied voltage to 118 volts, the colored area
increased to 68%. Aperture at the given voltage (118V) was found to
depend upon the pixel size; the 200-um-size pixel exhibited maximum
20% aperture, while the 800-um-size pixel made 78%.
Fig. 2. Schematic illustration of the OFF and ON state of the
deformable membrane. (a) Gray color with a suspended membrane with
no bias, and (b) green color in electrostatic pull-in at 90 Vdc. A
movie file attached.
We designed the thickness of the silicon dioxide to be 310 nm for
the green pixels, and the pixels of other colors were designed by
changing the silicon dioxide thickness; 240 nm for a blue pixel and
370 nm for a red pixel. Figure 3 shows the three primary colors on
the CIE chart [9] that shows the purity and the gamut of the color
compared with the standard cathode ray tube (CRT) display. The
color was measured by the display tester (Yokogawa Electric. Corp.,
3298F). The CIE color coordinates were determined to be (x, y) =
(0.31, 0.38) for the pixels under zero voltage, (0.31, 0.56) for
the green pixel in operation, (0.36, 0.23) for the red, (0.19,
0.21) for the blue. The backlight was a light bulb of continuous
white spectrum of (0.34, 0.37).
The developed green pixel was found to have the purity and the
gamut equivalent to those of CRT. On the other hand, the red and
blue pixels were found to be still poor in color purity. Optical
analysis using the optical spectrum analyzer discovered that the
red pixel had two transmission peaks in the visible wavelength
range (a red peak at 670 nm and a blue peak at 450 nm), which is
believed to be the cause of the degraded color purity. More vivid
red and blue colors are currently under development by
re-designing
c© IEICE 2006 DOI: 10.1587/elex.3.97 Received February 10, 2006
Accepted February 21, 2006 Published March 25, 2006
100
IEICE Electronics Express, Vol.3, No.6, 97–101
the layered structure of color-making silicon dioxide. The pixel at
the OFF state did not show deep black but gray, as shown in Figure
2 (a), because of the white back light of continuous spectrum. Real
black color could be made by using a back light of narrow peaks at
red, green, and blue wavelengths such that none of them could pass
the transmission channels at the pixel’s OFF state.
Fig. 3. Measured color gamut in the CIE chart for the obtained
green, red, and blue pixels. The col- ors are designed by the
silicon dioxide thicknesses: 310 nm for green, 370 nm for red, and
240 nm for blue.
4 Conclusion
We have developed a new type of transparent display pixels based
upon the MEMS Fabry-Perot interferometer mechanism using an
electrostatically deformable plastic film. Three primary colors
were successfully demonstrated by pre-defining the thicknesses of
the color-making layer of silicon dioxide. The solid glass
substrate could be potentially replaced with the flexible plastic
film to make a totally flexible electronic paper.
Acknowledgments
The authors thank Teijin DuPont Films Japan Limited for providing
us with the PEN films used in this work. This study has been
performed in the Op- tomechatronics Project (April 2005 – March
2008) with Kanagawa Academy of Science and Technology (KAST).
c© IEICE 2006 DOI: 10.1587/elex.3.97 Received February 10, 2006
Accepted February 21, 2006 Published March 25, 2006
101