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                    and routers will routinely process and share data at aggregate data rates of several
                    terabits per second using short-reach optical transceivers that employ optical
                    interconnects between chips on a multiprocessor board, and between boards “inside
                    the box.” The term “inside the box” generally refers to the inner portion of one of many
                    node enclosures that constitutes a supercomputer. It may also signify the enclosure that
                    defines the physical space of a stand-alone computer, such as a blade center server.
                    Optical interconnections “outside the box” will continue to use parallel, telecom-type
                    optical transceivers modified to accommodate high channel density.
                       Optoelectronic SOP provides options not available in conductive data transport:
                    (1) Since the optical signal bandwidth is independent of distance over distances of
                    several meters, extended memory may be placed in a separate box. (2) Optical links do
                    not require shielding and separation to reduce crosstalk to the extent that electrical lines
                    do. Less than 10 μm of cladding separation is sufficient at all data bandwidths. (3) Because
                    parallel optical links can be high density, potentially on a 60-μm pitch, and flexible,
                    typically capable of a 1-cm turn radius, they can, in principle, support direct processor-to-
                    processor wiring on a multiprocessor core module. (4) High-density  flexible optical
                    interconnects will diminish the dependence of high-speed signal routing through the
                    backplane.
                       Optical-digital signaling “inside the box” will eventually migrate to optical-digital
                    signaling at the chip level. This paradigm shift will probably occur when the internal
                    processor clock speed increases to ≥10 GHz and clock synchronization and processor
                    temperature becomes difficult to manage. At that time, optimal codesign will integrate
                    on- and off-chip optical signaling at bit rates that are commensurate with that of an
                    internal processor clock. In this scenario, synchronization on- and off-chip will become
                    equally demanding.  Alternatively, even if asynchronous processing is adopted, the
                    need for increasing bandwidth capacity will not diminish. One needs to be aware that,
                    in the near future, the total information transfer per year of the Internet is expected to
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                    surpass the zettabyte (10  bytes) level. It is currently at the exabyte (10  bytes) level [1].
                    To meet this jump in information density, the Ethernet electrical and optical infrastructure
                    companies are busy developing 100-Gb/s capabilities worldwide [2].

                    6.2.2 RF-Optical Communication Systems
                    Optics is an effective enabling technology in the digital domain. Not only does optics
                    transcend the limitations of copper-based signaling (bandwidth × distance), but it also
                    transcends the limitation of impedance matching in three dimensions. Impedance matching
                    limits the transmission lines in two dimensions. Any long unshielded line along the signal
                    path acts as discontinuities, and impedance matching becomes difficult. Flexible, high-
                    speed, high-density copper interconnects increase the challenge because of radiative signal
                    losses, interference, and pulse distortion [3–4]. Flexible optical interconnects are subject to
                    fewer and less severe limitations: (1) The optical leakage is independent of bit rate. This is
                    not true for bent copper lines whose radiative losses increase with frequency [3–4]. For
                    example, polymer waveguides having a relatively small index contrast of 0.03 between
                    core and cladding can support a bend radius of 1 cm with about –0.12 dB loss [5]. (2) Straight
                    or curved copper lines are notorious for picking up and generating crosstalk primarily
                    through capacitive coupling. Design rules on minimum separation and minimum shielding
                    depending on the application are necessary. On the other hand, crosstalk between two
                    adjacent waveguides occurs when the evanescent field of one overlaps the other, which
                    translates to a distance of the order of a few wavelengths of light in the medium of propagation.
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