Patent Application
20100103428
This application claims the benefit under 35 U.S.C. §119(a) of Korean Patent Application No. 10-2008-106515, filed on Oct. 29, 2008, the disclosure of which is incorporated herein in its entirety by reference.
1. Field
The following description relates to a configuration of a signal light generating apparatus, and more particularly, to a configuration of a signal light generating apparatus including an erbium-doped optical fiber.
2. Description of the Related Art
An optical fiber gyroscope generally includes a Sagnac loop formed of a coiled optical fiber, a light source, and a signal processing unit. Light emitted from the light source is incident to the optical fiber Sagnac loop, and a rotation rate is measured based on a phase difference between clockwise-rotating light and counter-clockwise rotating light, that is, the Sagnac phase difference.
To measure an accurate rotation speed from the Sagnac phase difference obtained by the optical fiber gyroscope, highly stabilized scale factors are required. From among parameters that determine the scale factors, an area surrounded by a coil is relatively stable against external perturbation. In addition, a mean wavelength of light emitted from the light source needs to be stable for more stable scale factors. Thus, the gyro light source of the optical gyroscope should have a notably stable mean wavelength in order to achieve high measurement accuracy.
A semiconductor light source utilizing a single-pass backward (SPB) arrangement which is generally used as a gyro light source has a mean wavelength variation of several hundreds ppm/° C. and thus is significantly sensitive to temperature changes. On the other hand, a light source formed of an erbium-doped filter (EDF) has much lower mean wavelength variation of several tens ppm/® C. with respect to temperature changes, when compared to the semiconductor light source.
As such, an erbium-doped signal light generating apparatus has an improved stability with respect to temperature changes, in comparison to a semiconductor light source. However, suppression of temperature dependence to greater amounts is required in order to enhance the measurement accuracy of a fiber gyroscope.
Accordingly, in one aspect, there is provided an erbium-doped signal light generating apparatus which stabilizes a mean wavelength.
According to an aspect, there is provided A signal light generating apparatus including an optical fiber which is a gain medium, a light source to emit pump light, a stabilizing unit to compensate for changes of a mean wavelength of the signal light with respect to temperature change in the optical fiber and to thereby stabilize the mean wavelength of the signal light, and an optical coupler to transmit the pump light from the light source to the optical fiber and to output signal light returning from the optical fiber and signal light returning from the optical fiber via the stabilizing unit by which the signal light is stabilized.
The stabilizing unit may compensate for the changes of the mean wavelength of the signal light by introducing a change of a mean wavelength with respect to temperature changing with a length of the optical fiber to the changes with respect to temperature. Also, the optical fiber may have a thermal coefficient which is a positive (+) value and the stabilizing unit may have a thermal coefficient which is a negative (−) value, wherein the thermal coefficient indicates a correlation between change of the mean wavelength of the signal light with respect to temperature.
The stabilizing unit may be a high-birefringence optical fiber, and specifically, the high-birefringence optical fiber may be a polarization-maintaining optical fiber. In addition, the optical fiber may be an optical fiber doped with a rare earth element, and specifically, the optical fiber may be an erbium-doped fiber.
The stabilizing unit may be provided between the optical coupler and the optical fiber.
Other features will become apparent to those skilled in the art from the following detailed description, which, taken in conjunction with the attached drawings, discloses exemplary embodiments of the invention.
Elements, features, and structures are denoted by the same reference numerals throughout the drawings and the detailed description, and the size and proportions of some elements may be exaggerated in the drawings for clarity and convenience.
The following detailed description is provided to assist the reader in gaining a comprehensive understanding of the methods, apparatuses and/or systems described herein. Various changes, modifications, and equivalents of the systems, apparatuses and/or methods described herein will suggest themselves those of ordinary skill in the art. Descriptions of well-known functions and structures are omitted to enhance clarity and conciseness.
The light source 100 is a pump light source that emits a pump light. For example, the pump light source may be a pump laser diode. The light source 100 has lower pumping efficiency in pump wavelength bands other than a pump wavelength band of 960 to 1000 nm (briefly, 0.98 μm band) and a pump wavelength band of 1440 to 1550 nm (briefly, 1.48 μm) due to an excited state absorption (ESA) phenomenon. Thus, a pump wavelength band of a signal light provided from the optical fiber to the light source 100 may be 0.98 μm band or 1.48 μm, and have a corresponding mean wavelength λ.
The optical coupler 110 may be a wavelength division multiplexing (WDM) coupler. The optical fiber 130 is doped with a rare earth element. For example, the optical fiber 130 may be implemented as an erbium-doped fiber (EDF). The erbium-doped optical fiber has an optical gain in 1.55 μm wavelength band which is the lowest loss band of the optical fiber 130 due to a transition of energy levels between 4I13/2 and 4I15/2 of an ion Er3+, which is an element of the rare-earth group.
In one example, a pump light emitted from the light source 100 is incident to the optical fiber 130 through the optical coupler 110. Spontaneous emission light is generated in the optical fiber 130, amplified while traveling along the optical fiber, and is emitted as amplified spontaneous emission (ASE) from each end of the optical fiber 130.
In practice, an absorption/emission cross-section of the optical fiber 130 and a mean wavelength of signal light change with temperature. Configuration and operation requirements of a signal light source may affect the characteristics of change of a mean wavelength with temperature.
The stabilizing unit 120 compensates for change of a mean wavelength with temperature in the optical fiber 130. The stabilizing unit 120 is implemented between the optical coupler 110 and the light fiber 130 as shown in
If the optical fiber 130 has a positive (+) thermal coefficient, the stabilizing unit 120 may be implemented to have a negative (−) thermal coefficient, wherein thermal coefficient indicates a correlation of change of a mean wavelength of the signal light with respect to temperature. Accordingly, the change of a mean wavelength generated in the optical fiber 130 can be compensated for by the stabilizing unit 120.
The stabilizing unit 120 may be implemented as a nonlinear high-birefringence optical fiber. The nonlinear high-birefringence optical fiber can be configured in various forms. Also, a birefringence value of the nonlinear high-birefringence optical fiber will vary dependant on the configuration. In the nonlinear high-birefringence optical fiber, birefringence decreases with the increase of temperature. Therefore, as the temperature increases, a mean wavelength of inner signal light is shifted toward shorter wavelengths, so that the change of a mean wavelength with respect to temperature results in a negative (−) value. In particular, a PANDA type optical fiber has the greatest thermal coefficient. A general polarization-maintaining fiber which is a nonlinear high-birefringence optical fiber may include two or more different materials having different temperature expansion coefficients. Hence, a traveling wave experiences a change of polarization when the temperature changes, and therefore the light source is significantly affected by temperature change.
As shown in
Since light source for navigation ultimately aims for a stability of 1 ppm, the change of a mean wavelength with respect to temperature is required to be more stabilized. As shown in
For example, the stabilizing unit 120 formed as a nonlinear high-birefringence optical fiber may be appropriately provided to a leading end of the optical fiber 130 which has a positive (+) thermal coefficient. Accordingly, it is possible for the stabilizing unit 120 to compensate for the signal light, i.e. ASE, from the optical fiber 130, of which a mean wavelength lengthens as temperature increases, by using the characteristic that a mean wavelength of the signal light shortens as temperature increases in the stabilizing unit 120. In other words, temperature dependence of the signal light can be cancelled out between the optical fiber 130 and the stabilizing unit 120, and thus a mean wavelength of the signal light can be stabilized with respect to temperature change. Therefore, even when the temperature changes, a mean wavelength of signal light in the signal light generating apparatus can be stable.
Also, a signal light generating apparatus may be mounted in a rotation sensing apparatus. Since the signal light generating apparatus for measuring a rotation rate can lower the amount of change of a mean wavelength with respect to temperature and lower a pump power required of a pump light source, temperature dependence can be reduced, and as the stability of the mean wavelength with respect to temperature change is increased, accuracy of rotation rate measurement can be enhanced.
A number of exemplary embodiments have been described above. Nevertheless, it will be understood that various modifications may be made. For example, suitable results may be achieved if the described techniques are performed in a different order and/or if components in a described system, architecture, device, or circuit are combined in a different manner and/or replaced or supplemented by other components or their equivalents. Accordingly, other implementations are within the scope of the following claims.
| Number | Date | Country | Kind |
|---|---|---|---|
| 10-2008-0106515 | Oct 2008 | KR | national |
