Optical: systems and elements – Polarization without modulation – By relatively adjustable superimposed or in series polarizers
Reexamination Certificate
2000-10-11
2002-08-27
Shafer, Ricky D. (Department: 2872)
Optical: systems and elements
Polarization without modulation
By relatively adjustable superimposed or in series polarizers
C359S490020, C359S558000, C359S566000, C359S615000, C359S629000, C359S199200, C359S199200, C359S199200, C359S199200, C356S365000, C356S925000, C385S031000, C385S033000
Reexamination Certificate
active
06441959
ABSTRACT:
FIELD OF THE INVENTION
The present invention relates to chromatic dispersion, dispersion slope, and polarization mode dispersion compensation, and more particularly to dispersion compensation accumulated in a wavelength division multiplexed optical fiber transmission line.
BACKGROUND OF THE INVENTION
Fiber optic networks are becoming increasingly popular for data transmission because of their high speed and high capacity capabilities. Wavelength division multiplexing is used in such fiber optic communication systems to transfer a relatively large amount of data at a high speed. In wavelength division multiplexing, multiple information-carrying signals, each signal comprising light of a specific restricted wavelength range, may be transmitted along the same optical fiber.
In this specification, these individual information-carrying lights are referred to as either “signals” or “channels.” The totality of multiple combined signals in a wavelength-division multiplexed optical fiber, optical line or optical system, wherein each signal is of a different wavelength range, is herein referred to as a “composite optical signal.”
One common and well-known problem in the transmission of optical signals is chromatic dispersion of the optical signal. Chromatic dispersion refers to the effect wherein the channels comprising an optical signal travel through an optic fiber at different speeds, e.g., longer wavelengths travel faster than shorter wavelengths. This is a particular problem that becomes more acute for data transmission speeds higher than 2.5 gigabytes per second. The resulting pulses of the signal will be stretched, will possibly overlap, and will cause increased difficulty for optical receivers to distinguish where one pulse begins and another ends. This effect seriously compromises the integrity of the signal. Therefore, for a fiber optic communication system to provide a high transmission capacity, the system must compensate for chromatic dispersion. The exact value of the chromatic dispersion produced in a channel of a wavelength-division multiplexed fiber optic communications system depends upon several factors, including the type of fiber and the wavelength of the channel.
For dense wavelength division multiplexer (DWDM) systems or for WDM or DWDM systems with a wide wavelength spacing between the shortest and longest wavelength channels, the common approach is to allow chromatic dispersion to accumulate within spans of fiber and to compensate for dispersion at the ends of spans through the use of in-line dispersion compensator apparatuses.
A second common and well-known problem in the transmission of optical signals is polarization mode dispersion (PMD). PMD is the phenomenon by which differently polarized components, or sub-signals, comprising an optical signal propagate with different speeds or, alternatively, propagate along differing-length optical paths. This duality of speeds or paths can also cause unacceptable broadening of the digital pulses comprising a signal that increases in severity with increasing transmission speed. The maximum acceptable PMD-induced optical path length difference is the cumulative result of all PMD effects in all the optical elements through which a signal propagates, including fiber and non-fiber optical components. Although the PMD broadening of optical fiber increases as the square root of fiber length, the PMD broadening caused by birefringent components is linearly related to the cumulative optical path difference of all such components.
The chromatic dispersion characteristics of optical fibers are not constant but depend upon wavelength, as illustrated in
FIG. 1
, which presents graphs of Group Velocity Dispersion, D, against wavelength, for typical examples of three commonly used fiber types. In
FIG. 1
, the quantity D (ps-km
−1
-nm
−1
) is defined by the relationship of Eq. 1
D
=
ⅆ
ⅆ
λ
(
1
v
g
)
=
1
L
(
ⅆ
τ
g
ⅆ
λ
)
(
1
)
in which &lgr; is the channel wavelength (nm), &ngr;
g
is the group velocity (km/ps), &tgr;
g
is the group delay time (ps), and L is the fiber length (km). If &ngr;
g
decreases with increasing wavelength (i.e., longer or “red” wavelengths travel slower than relatively shorter or “blue” wavelengths) then D is positive, otherwise D is negative. Because all three fiber types illustrated in
FIG. 1
are deployed in telecommunications systems, the requirements for dispersion compensators vary widely. Furthermore, because of the existence of non-zero dispersion slope, S, a constant level of dispersion compensation does not accurately negate the dispersion of all channels. This inaccuracy can become a significant problem for high-speed data propagation, long span distances, and/or wide distances between the shortest and longest wavelength channels.
Conventional apparatuses for dispersion compensation include dispersion compensation fiber, chirped fiber Bragg gratings coupled to optical circulators, and conventional diffraction gratings disposed as sequential pairs.
A dispersion compensation fiber, which is used in-line within a fiber communications system, has a special cross-section index profile so as to provide chromatic dispersion that is opposite to that of ordinary fiber within the system. The summation of the two opposite types of dispersion negates the chromatic dispersion of the system. However, dispersion compensation fiber is expensive to manufacture, has a relatively large optical attenuation, and must be relatively long to sufficiently compensate for chromatic dispersion.
A chirped fiber Bragg grating is a special fiber with spatially modulated refractive index that is designed so that longer (shorter) wavelength components are reflected at a farther distance along the chirped fiber Bragg grating than are the shorter (longer) wavelength components. A chirped fiber Bragg grating of this sort is generally coupled to a fiber communications system through an optical circulator. By causing certain wavelength components to travel longer distances than other wavelength components, a controlled delay is added to those components and opposite dispersion can be added to a pulse. However, a chirped fiber Bragg grating has a very narrow bandwidth for reflecting pulses, and therefore cannot provide a wavelength band sufficient to compensate for light including many wavelengths, such as a wavelength division multiplexed light. A number of chirped fiber Bragg gratings may be cascaded for wavelength multiplexed signals, but this results in an expensive system. Furthermore, fiber Bragg gratings generally do not compensate polarization mode dispersion.
A conventional diffraction grating has the property of outputting different wavelengths at different angles. By using a pair of gratings in a coupled spatial arrangement, this property can be used to compensate chromatic dispersion in a fiber communications system. In such a spatial grating pair arrangement, lights of different wavelengths are diffracted from a first grating at different angles. These lights are then input to a second grating that diffracts them a second time so as to set their pathways parallel to one another. Because the different lights travel with different angles between the two gratings, certain wavelength components are made to travel longer distances than other wavelength components. Chromatic dispersion is produced in the spatial grating pair arrangement because the wavelength components that travel the longer distances incur time delays relative to those that travel the shorter distances. This grating-produced chromatic dispersion can be made to be opposite to that of the fiber communications system, thereby compensating the chromatic dispersion within the system. However, a practical spatial grating pair arrangement cannot provide a large enough dispersion to compensate for the relatively large amount of chromatic dispersion occurring in a fiber optic communication system. More specifically, the angular dispersion produced by a diffraction grating is usually extremely small, and is typically a
Cao Simon
Lin Christopher
Ma Jiyong
Yang Jialing
Avanex Corporation
Sawyer Law Group LLP
Shafer Ricky D.
LandOfFree
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