Optical: systems and elements – Optical amplifier – Optical fiber
Reexamination Certificate
1999-12-27
2002-07-16
Tarcza, Thomas H. (Department: 3662)
Optical: systems and elements
Optical amplifier
Optical fiber
C359S337100, C359S337400
Reexamination Certificate
active
06421172
ABSTRACT:
FIELD OF THE INVENTION
The present invention relates generally to long band optical amplifiers. More particularly, the invention relates to a long band optical amplifier employing a rare earth doped fiber and an improved dual pumping technique.
BACKGROUND OF THE INVENTION
Optical amplifiers increase the amplitude of an optical wave through a process known as stimulated emission in which a photon, supplied as the input signal, excites electrons to a higher energy level within an optical material, which then undergo a transition to a lower energy level. In the process, the material emits a coherent photon with the same frequency, direction and polarization as the initial photon. These two photons can, in turn, serve to stimulate the emission of two additional photons coherently, and so forth. The result is coherent light amplification. Stimulated emission occurs when the photon energy is nearly equal to the atomic transition energy difference. For this reason, the process produces amplification in one or more bands of frequencies determined by the atomic line width.
While there are a number of different optical amplifier configurations in use today, the optical fiber amplifiers are quite popular, particularly for optical communications applications. The optical fiber amplifier typically includes an optical material such as glass, combined with a rare earth dopant such as such as Erbium and configured as an optical waveguide. Rare-earth-doped silica fibers are popular today in part because they offer the advantages of single-mode guided wave optics. Optical fiber amplifiers made of such fibers can be made to operate over a broad range of wavelengths, dictated by the atomic properties of the host and rare earth dopant. For example, Erbium doped fiber amplifiers (EDFAs) operate at two signal bands of the fiber transmission window. These signal bands are a conventional-band (C-band) with wavelength range from approximately 1528 nm to approximately 1565 nm and a long band (L-band) with wavelength range from approximately 1568 nm up to approximately 1610 nm.
In a typical optical amplifier fabricated using Erbium doped silica fiber, electrons are excited (pumped) from the ground state (
4
I
15/2
) to the metastable state (I
13/2
) by either a pump at 980 nm wavelength or 1480 nm wavelength. In the case of 980 nm pump, the electrons are first pumped to the excited state (
4
I
11/2
) and then non-radiactively decay into the metastable state (
4
I
13/2
) (See FIG.
11
). In the case of 1480 nm pump the electrons are directly pumped into
4
I
13/2
state. The amplification occurs when the electrons in I
13/2
state decay into the ground state by stimulated emission. After the electrons decay to the ground energy level
4
I
15/2
, they can be re-pumped to the excited energy level
4
I
11/2
where they can take part in further stimulated emission processes.
Erbium doped fiber amplifiers (EDFAs) are typically made out of multiple stages of coiled Er-doped fibers. An example of such Erbium doped fiber amplifier is shown in FIG.
2
. The most critical parameters on the performance of EDFAs are noise figure (NF) and gain G. The noise figure, NF, measured in dBs is defined as
10
times Log
10
of the ratio of the signal (S) to noise (N) ratio at the input of the amplifier to that at the output of the amplifier. That is, NF=
10
×Log
10
(S/N) in/ (SIN) out. The gain, G, is defined as the ratio of signal output power to signal input power. In multistage amplifiers the noise figure NF is largely determined by the gain G in the front end of the amplifier. Thus, the higher the gain G of the first coil of the EDFA, the lower NF. Another measure of EDFA performance is the power efficiency, which is defined as the ratio between the numbers of photons amplified to the numbers of photons extracted from the pump. Since the performance of the communication system is determined by the noise performance of the amplifiers in the system, signal power of the amplifiers, and fiber transmission properties, optical communication systems require that the EDFAs have the lowest possible noise figure (NF), and provide the highest possible gain, (G).
FIG. 3
illustrates the absorption spectrum of the Erbium doped fiber (EDF). This figure shows that a strong absorption peak is present in the 980 nm-pumping band. Because of the strong absorption at the 980 nm wavelength, some long-band EDFAs use a 980 nm pump in conjunction with a first EDF coil. The use of the 980 nm wavelength pump introduces high inversion at the front end of the optical amplifier, thus resulting in a low noise figure (See FIG.
2
). The 980 nm pump provides less efficient power conversion relative to 1480 nm pump and is relatively difficult to build. Therefore, a to 980 nm pump is expensive. However, it appears to be a common belief that the use of a less efficient, more expensive 980 nm pump (as the first pump in the L-band amplifier) is needed in order to provide low noise and thus, high signal to noise ratio so that a cleaner signal is provided to the second EDF coil for further amplification.
In order to extract maximum power, the second stage pump (i.e., the pump that is coupled to the second EDF coil) is typically a more efficient, less expensive to manufacture, 1480 nm wavelength pump (see FIG.
2
). It is known that this second pump will improve the efficiency of the multiple stage EDF amplifier without introducing too much noise into the system.
It is desirable to provide low noise L-band optical amplifiers that are also more efficient than prior art long band optical amplifiers.
SUMMARY OF THE INVENTION
According to one aspect of the present invention an optical amplifier comprises: a first gain medium having an optical host that contains a rare earth dopant and a first pump that supplies optical energy at a first wavelength into this first gain medium. The first pump operates at a pump wavelength that has a lower inversion saturation than the highest wavelength of absorption of the first gain medium. The optical amplifier further comprises a second gain medium operatively coupled to the first gain medium and a second pump that supplies optical energy into the second gain medium.
According to another aspect of the invention, the optical amplifier comprises an optical waveguide having an optical host that contains a rare earth dopant. The host and dopant define a ground energy state. The amplifier further includes a first pump optically coupled to the waveguide. This first pump supplies optical energy into the waveguide at a first wavelength. The first pump establishes a metastable energy state above the ground energy state. An input, coupled to the optical waveguide, introduces an optical signal to be amplified, where amplification is produced by stimulated emission of photons from the metastable energy state. This establishes a termination energy state below the first metastable energy state and above the ground energy state. The optical amplifier further comprises a second pump optically coupled to a second waveguide. The second pump supplies optical energy to the second waveguide at a wavelength that is the same as the wavelength of the first pump. The second pump repopulates the first metastable energy state by depopulating the termination energy state.
Embodiments of the present invention can provide an optical amplifier and a pumping technique that overcomes the difficulties associated with prior art L-band optical amplifiers. It is an advantage of this optical amplifier that it has low noise and high pumping efficiency.
For a more complete understanding of the invention, its objects and advantages, refer to the following specification and to the accompanying drawings. Additional features and advantages of the invention are set forth in the detailed description, which follows.
It should be understood that both the foregoing general description and the following detailed description are merely exemplary of the invention, and are intended to provide an overview or framework for understanding the nature and character of the i
Flood Felton A.
Liu Yongqian
Smart Richard G.
Corning Incorporated
Hughes Deandra M.
Short Svetlana
Tarcza Thomas H.
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