Liquid crystal on silicon

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Liquid crystal on silicon (LCoS or LCOS) is a "micro-display" technology developed initially for projection televisions but now used also in Wavelength Selective Switches, structured illumination and Near-eye displays. It is a reflective technology similar to DLP projectors; however, it uses a liquid crystal layer on top of a silicon backplane instead of individual mirrors. By way of comparison, some LCD projectors use transmissive LCD, allowing light to pass through the liquid crystal.

A sketch of a Liquid Crystal on Silicon (LCoS) Cell is shown in Figure 1 (to be uploaded). The CMOS chip controls the voltage on plates buried just below the chip surface, each controlling one pixel. For example, chip with XGA resolution will have 1024x768 plates, each with an independently addressable voltage. This conceptual drawing of a Liquid Crystal on Silicon cell with the vertical dimension exaggerated to reveal the different layers. Typical cells are about 1-3 centimeters square and about 2 mm thick, pixel pitch as small as 2.79μm.[1] A common voltage for all the pixels is supplied by a transparent conductive layer made of indium tin oxide on the cover glass.

Displays[edit]

History[edit]

Figure 2 Conceptual diagram of an LCoS projector.

General Electric first demonstrated a low-resolution LCoS display in the late 1970s.[citation needed] Starting in the late 1990s a number of companies attempted to develop products for both near-eye and projection applications.

At the 2004 CES, Intel announced plans for the large scale production of inexpensive LCoS chips for use in flat panel displays. These plans were cancelled in October 2004. Sony has made it to market (December 2005) with the Sony-VPL-VW100 or "Ruby" projector, using SXRD, 3 LCoS chips each with a native resolution of 1920×1080, with a stated contrast ratio of 15,000:1 using a dynamic iris.[citation needed]

Whilst LCoS technology was initially touted as a technology to enable large-screen, high-definition, rear-projection televisions with very high picture quality at relatively low cost, the development of large-screen LCD and plasma flat panel displays obsoleted rear projection televisions. As of October 2013, LCoS-based rear-projection televisions are no longer produced.

Commercial implementations of LCoS technology include Sony's SXRD (Silicon X-tal Reflective Display) and JVC's D-ILA (Digital Direct Drive Image Light Amplifier). Every company which produces and markets LCoS rear-projection televisions uses three-panel LCoS technology,[citation needed]. Sony and JVC both produce and market front-projection displays that use three LCoS panels. Canon too, with XEED projectors.

Developers and manufacturers who have left the LCoS imaging market include: Intel, Philips, MicroDisplay Corporation (the only company to successfully bring to market a single-panel LCoS television[2] ), S-Vision, Colorado Microdisplay, Himax, Spatialight, Syntax-Brillian.

Display system architectures[edit]

There are two broad categories of LCoS displays: three-panel and single-panel. In three-panel designs, there is one display chip per color, and the images are combined optically. In single-panel designs, one display chip shows the red, green, and blue components in succession with the observer's eyes relied upon to combine the color stream. As each color is presented, a color wheel (or an RGB LED array) illuminates the display with only red, green or blue light. If the frequency of the color fields is lower than about 540 Hz[citation needed], an effect called color breakup is seen, where false colors are briefly perceived when either the image or the observer's eye is in motion. While less expensive; single-panel projectors require higher-speed display elements to process all three colors during a single frame time, and the need to avoid color breakup makes further demands on the speed of the display technology.

Three-panel designs[edit]

Compared to three chip DLP devices, where the light is separated into three components and then combined back, light is additionally polarized in LCoS devices. As a result, four beam splitters are needed (compared to two beam splitters for three chip DLP).

One-panel designs[edit]

Both Toshiba's and Intel's single-panel LCOS display program were discontinued in 2004 before any units reached final-stage prototype.[3] There were single-panel LCoS displays in production: One by Philips and one by Microdisplay Corporation. Forth Dimension Displays offers a Ferroelectric LCoS display technology (known as Time Domain Imaging) available in QXGA, SXGA and WXGA resolutions which is used for fringe projection in superresolution microscopy, automated optical inspection and high resolution near-eye applications such as Training & Simulation. Micron's FLCoS technology is another single panel RGB solution used in pico-projectors, and near-eye display applications.

Pico Projectors, Near-eye and Head Mounted Displays[edit]

Whilst initially developed for large-screen projectors, LCoS displays have found a consumer niche in the area of pico-projectors, where their small size and low power consumption are well-matched to the constraints of such devices.

LCoS devices are also used in Near-Eye applications such as electronic viewfinders for digital cameras, film cameras, and Head Mounted Displays (HMDs). These devices are made using ferroelectric liquid crystals (so the technology is named FLCoS) which are inherently faster than other types of liquid crystals.[4] Google's initial foray into wearable computing, Google glass,[5] also uses a near-eye LCoS display based on an LCoS chip from Himax Technologies.[6]

See also[edit]

Wavelength Selective Switches[edit]

LCoS is particularly attractive as a switching mechanism in a Wavelength Selective Switch (WSS). LCoS-based WSS were initially developed by Australian company Engana,[7] now part of Finisar.[8] The LCoS can be employed to control the phase of light at each pixel to produce beam-steering[9] where the large number of pixels allow a near continuous addressing capability. Typically, a large number of phase steps are used to create a highly efficient, low-insertion loss switch shown schematically in Figure 3(to be uploaded). This simple optical design incorporates polarisation diversity, control of mode size and a 4-f wavelength optical imaging in the dispersive axis of the LCoS providing integrated switching and optical power control.

In operation, the light passes from a fibre array through the polarisation imaging optics which separates physically and aligns orthogonal polarisation states to be in the high efficiency s-polarisation state of the diffraction grating. The input light from a chosen fibre of the array is reflected from the imaging mirror and then angularly dispersed by the grating which is at near Littrow incidence, reflecting the light back to the imaging optics which directs each channel to a different portion of the LCoS. The path for each wavelength is then retraced upon reflection from the LCoS, with the beam-steering image applied on the LCOS directing the light to a particular port of the fibre array. As the wavelength channels are separated on the LCoS the switching of each wavelength is independent of all others and can be switched without interfering with the light on other channels. There are many different algorithms that can be implemented to achieve a given coupling between ports including less efficient “images” for attenuation or power splitting.

WSS based on MEMS[10] and/or Liquid Crystal[11] technologies allocate a single switching element (pixel) to each channel which means the bandwidth and centre frequency of each channel are fixed at the time of manufacture and cannot be changed in service. In addition, many designs of first-generation WSS (particularly those based on MEMs technology) show pronounced dips in the transmission spectrum between each channel due to the limited spectral ‘fill factor’ inherent in these designs. This prevents the simple concatenation of adjacent channels to create a single broader channel.

LCoS-based WSS, however, permit dynamic control of channel centre frequency and bandwidth through on-the-fly modification of the pixel arrays via embedded software. The degree of control of channel parameters can be very fine-grained, with independent control of the centre frequency and either upper- or lower-band-edge of a channel with better than 1 GHz resolution possible as shown in Figure 4 (to be uploaded). This is advantageous from a manufacturability perspective, with different channel plans being able to be created from a single platform and even different operating bands (such as C and L) being able to use an identical switch matrix. Additionally, it is possible to take advantage of this ability to reconfigure channels while the device is operating. Products have been introduced allowing switching between 50 GHz channels and 100 GHz channels, or a mix of channels, without introducing any errors or “hits” to the existing traffic. More recently, this has been extended to support the whole concept of Flexible or Elastic networks under ITU G.654.2 through products such as Finisar's Flexgrid™ WSS.

For more detailed information on the applications of LCoS in optical communications and, in particular, Wavelength Selective Switches, see chapter 16 in Optical Fiber Telecommunications VIA, edited by Kaminov, Li and Wilner, Academic Press ISBN 978-0-12-396958-3.

Other LCoS Applications[edit]

Optical Pulse Shaping[edit]

The ability of an LCoS-based WSS to independently control both the amplitude and phase of the transmitted signal leads to the more general ability to manipulate the amplitude and/or phase of an optical pulse through a process known as Fourier-domain pulse shaping.[12] This process, which requires full characterisation of the input pulse in both the time and spectral domains, is shown schematically in Figure 5 (to be uploaded).

As an example, an LCoS-based Programmable Optical Processor(POP) has been used to broaden a mode-locked laser output into a 20 nm supercontinuum source whilst a second such device was used to compress the output to 400 fs, transform-limited pulses.[13] Passive mode-locking of fiber lasers has been demonstrated at high repetition rates, but inclusion of an LCoS-based POP allowed the phase content of the spectrum to be changed to flip the pulse train of a passively mode-locked laser from bright to dark pulses.[14] A similar approach uses spectral shaping of optical frequency combs to create multiple pulse trains. For example, a 10 GHz optical frequency comb was shaped by the POP to generate dark parabolic pulses and Gaussian pulses, at 1540 nm and 1560 nm, respectively.[15]

Modal Switching in Space Division Multiplexed Optical Communications Systems[edit]

One of the interesting applications of LCoS is the ability to transform between modes of few-moded optical fibers[16] which have been proposed as the basis of higher capacity transmission systems in the future. Similarly LCoS has been used to steer light into selected cores of multicore fiber transmission systems, again as a type of Space Division Multiplexing.

Tunable Lasers[edit]

LCoS has been used as a filtering technique, and hence a tuning mechanism, for both semiconductor diode and fibre lasers.[17]

References[edit]

  1. ^ Compound Photonics. "Products Compound Photonics". Retrieved 2014-10-13. 
  2. ^ Chin, Spencer. "MicroDisplay LCoS panel comes in under an inch". EE Times. 
  3. ^ Hachman, Mark. "Update: Intel Cancels LCOS Chip Plans". 415.992.5910. Extreme Tech. Retrieved June 17, 2011. 
  4. ^ N.Collings et al, "The Applications and Technology of Phase-Only Liquid Crystal on Silicon Devices", IEEE Journal of Display Technology, Vol 7, Iss 3, pp.112-119
  5. ^ http://www.google.com/glass/start/
  6. ^ http://www.kguttag.com/2013/03/11/google-glass-is-using-field-sequential-color-fsc-lcos-likely-himax/
  7. ^ G. Baxter et al., “Highly Programmable Wavelength Selective Switch Based on Liquid Crystal on Silicon Switching Elements,” in Optical Fiber Communication Conference, 2006 and the 2006 National Fiber Optic Engineers Conference. OFC 2006
  8. ^ http://www.finisar.com/products/wss-roadms
  9. ^ K. M. Johnson, D. J. McKnight, and I. Underwood, “Smart spatial light modulators using liquid crystals on silicon”, IEEE J. Quant. Electron., 29, 699 (1993)
  10. ^ D. M. Marom et al. “Wavelength-selective 1x4 switch for 128 WDM channels at 50 GHz spacing,” in Proc. Optical Fiber Communications (OFC 2002), Anaheim, CA, Postdeadline Paper FB7, pp. FB7-1–FB7-3
  11. ^ J. Kondis, et al. “Liquid crystals in bulk optics-based DWDM optical switches and spectral equalizers,” in Proc. LEOS 2001, Piscataway, NJ, 2001, pp. 292–293.
  12. ^ A.M. Weiner, “Femtosecond pulse shaping using spatial light modulators”, Rev. Sci. Instrum. 71, 1929–1960 (2000).
  13. ^ A. M. Clarke, D. G. Williams, M. A. F. Roelens, M. R. E. Lamont, and B. J. Eggleton, “Parabolic pulse shaping for enhanced continuum generation using an LCoS-based wavelength selective switch,” in 14th OptoElectronics and Communications Conference (OECC) 2009.
  14. ^ Jochen B. Schroeder et al., “Dark and Bright Pulse Passive Mode-locked Laser with In-cavity Pulse-shaper,” Optics Express 18, no. 22 (October 25, 2010): pp.22715–22721.
  15. ^ T. T Ng et al., “Complete Temporal Optical Fourier Transformations Using Dark Parabolic Pulses,” in 35th European Conference on Optical Communication, 2009.
  16. ^ M. Salsi et al., “Mode-Division Multiplexing of 2 x 100 Gb/s Channels Using an LCOS-Based Spatial Modulator,” Journal of Lightwave Technology, 30, no. 4 (February 2012): pp.618 –623.
  17. ^ Feng Xiao, Kamal Alameh, and TongTak Lee, “Opto-VLSI-based Tunable Single-mode Fiber Laser,” Optics Express 17, no. 21 (October 12, 2009): 18676–18680.

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