Optical waveguides – With optical coupler – Particular coupling function
Reexamination Certificate
2001-01-19
2003-10-07
Healy, Brian (Department: 2874)
Optical waveguides
With optical coupler
Particular coupling function
C385S027000, C385S007000, C385S029000, C385S039000, C385S031000, C385S042000, C385S037000, C385S140000
Reexamination Certificate
active
06631224
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates generally to an acousto-optic wavelength tunable bandpass filter, and more particularly to an acousto-optic wavelength tunable bandpass filter that includes a core mode blocker.
2. Description of Related Art
In modern telecommunication systems, many operations with digital signals are performed on an optical layer. For example, digital signals are optically amplified, multiplexed and demultiplexed. In long fiber transmission lines, the amplification function is performed by Erbium Doped Fiber Amplifiers (EDFA's). The amplifier is able to compensate for power loss related to signal absorption, but it is unable to correct the signal distortion caused by linear dispersion, 4-wave mixing, polarization distortion and other propagation effects, and to get rid of noise accumulation along the transmission line. For these reasons, after the cascade of multiple amplifiers the optical signal has to be regenerated every few hundred kilometers. In practice, the regeneration is performed with electronic repeaters using optical-to-electronic conversion. However to decrease system cost and improve its reliability it is desirable to develop a system and a method of regeneration, or signal refreshing, without optical to electronic conversion. An optical repeater that amplifies and reshapes an input pulse without converting the pulse into the electrical domain is disclosed, for example, in the U.S. Pat. No. 4,971,417, Radiation-Hardened Optical Repeater”. The repeater comprises an optical gain device and an optical thresholding material producing the output signal when the intensity of the signal exceeds a threshold. The optical thresholding material such as polydiacetylene thereby performs a pulse shaping function. The nonlinear parameters of polydiacetylene are still under investigation, and its ability to function in an optically thresholding device has to be confirmed.
Another function vital to the telecommunication systems currently performed electronically is signal switching. The switching function is next to be performed on the optical level, especially in the Wavelength Division Multiplexing (WDM) systems. There are two types of optical switches currently under consideration. First, there are wavelength insensitive fiber-to-fiber switches. These switches (mechanical, thermo and electro-optical etc.) are dedicated to redirect the traffic from one optical fiber to another, and will be primarily used for network restoration and reconfiguration. For these purposes, the switching time of about 1 msec (typical for most of these switches) is adequate; however the existing switches do not satisfy the requirements for low cost, reliability and low insertion loss. Second, there are wavelength sensitive switches for WDM systems. In dense WDM systems having a small channel separation, the optical switching is seen as a wavelength sensitive procedure. A small fraction of the traffic carried by specific wavelength should be dropped and added at the intermediate communication node, with the rest of the traffic redirected to different fibers without optical to electronic conversion. This functionality promises significant cost saving in the future networks. Existing wavelength sensitive optical switches are usually bulky, power-consuming and introduce significant loss related to fiber-to-chip mode conversion. Mechanical switches interrupt the traffic stream during the switching time. Acousto-optic tunable filters, made in bulk optic or integrated optic forms, (AOTFs) where the WDM channels are split off by coherent interaction of the acoustic and optical fields though fast, less than about 1 microsecond, are polarization and temperature dependent. Furthermore, the best AOTF consumes several watts of RF power, has spectral resolution about 3 nm between the adjacent channels (which is not adequate for current WDM requirements), and introduces over 5 dB loss because of fiber-to-chip mode conversions.
Another wavelength-sensitive optical switch may be implemented with a tunable Fabry Perot filter (TFPF). When the filter is aligned to a specific wavelength, it is transparent to the incoming optical power. Though the filter mirrors are almost 100% reflective no power is reflected back from the filter. With the wavelength changed or the filter detuned (for example, by tilting the back mirror), the filter becomes almost totally reflective. With the optical circulator in front of the filter, the reflected power may be redirected from the incident port. The most advanced TFPF with mirrors built into the fiber and PZT alignment actuators have only 0.8 dB loss. The disadvantage of these filters is a need for active feedback and a reference element for frequency stability.
A VOA is in opto-mechanical device capable of producing a desired reduction in the strength of a signal transmitted through a optical fiber. Ideally, the VOA should produce a continuously variable signal attenuation while introducing a normal or suitable insertion loss and exhibiting a desired optical return loss. If the VOA causes excessive reflectance back toward the transmitter, its purpose will be defeated.
Although fixed band-rejection filters are readily available using Bragg or long-period gratings impressed into the core of an optical fiber there are no simple, adjustable all-fiber bandpass filters. Such filters would vary the amplitude of signals within a fixed wavelength range. Although a variable transmission bandpass filter of sorts can be made by varying the center wavelength of a Bragg or long-period grating, as one channel is attenuated another channel is unavoidably strengthened.
Accordingly, there is a need for a bandpass filter that changes its amplitude transmission over a fixed wavelength spectrum. There is a further need for a bandpass filter with variable transmission over a fixed wavelength range, and which blocks all other wavelengths.
SUMMARY OF THE INVENTION
Accordingly, an object of the present invention is to provide an acousto-optic wavelength tunable bandpass filter.
Another object of the present invention is to provide an acousto-optic wavelength tunable bandpass filter that is widely tunable.
Still another object of the present invention is to provide a bandpass filter that has an adjustable transmission.
A further object of the present invention is to provide a bandpass filter with variable transmission over a fixed wavelength range, and which blocks all other wavelengths
These and other objects of the present invention are achieved in an optic apparatus that includes an optical fiber with a cladding surrounding a core and a core-mode blocker included in at least a portion of an interactive region of the optical fiber. A mode coupler is coupled to the optical fiber and couples a first mode to a different spatial mode in a forward direction of the optical fiber.
In another embodiment of the present invention, an optic apparatus includes an optical fiber with a cladding surrounding a core and a core-mode blocker included in at least a portion of an interactive region of the optical fiber. A mode coupler is coupled to optical fiber and couples a first mode to a different spatial mode in a forward direction of the optical fiber. A Faraday mirror coupled to the optical fiber.
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J.N. Blake, B.Y. Kim, H.E. Engan, and H.J. Shaw, “Analysis of intermodal coupling in a two-mode fiber with periodic microbends”, Op
Hwang In-Kag
Kim Byoung Yoon
Lee Myoung Soo
Sorin Wayne V.
Blakely , Sokoloff, Taylor & Zafman LLP
Healy Brian
Novera Optics, Inc.
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