JP5367446B2 - Optical amplification device and optical transmission system - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To improve analog characteristics while suppressing the generation of residual excitation light. <P>SOLUTION: An optical amplification device includes: an input unit (an input port 11) for input of an optical signal; a laser beam source (a laser diode 20) generating a laser beam; an optical fiber (an amplifying optical fiber 12) amplifying the optical signal by induced emission based on the laser beam generated from the laser beam source and for output of the amplified signal; an output unit (an output port 24) for output of the optical signal having been amplified by the optical fiber; and a passive optical component (an optical isolator 16 or the like) arranged between the optical fiber and the output unit. The laser beam source and/or the passive optical component are thermally coupled with the optical fiber via a medium having thermal conductivity. <P>COPYRIGHT: (C)2011,JPO&amp;INPIT

Description

  The present invention relates to an optical amplifying apparatus and an optical transmission system that are applied to the field of optical communication and the like.

  In recent years, an optical fiber communication network called FTTx (Fiber To The x) for a user's home has penetrated the society. In such an optical fiber communication network, an optical amplifying apparatus is used for the purpose of compensating for transmission loss of a transmission line and compensating for distribution loss in a distributor for distributing an optical signal to a plurality of subscribers.

  As such an optical amplifying device, for example, by inputting an optical signal such as a video signal into an optical fiber in which erbium is added to the core as an optical amplifying substance, and by inputting excitation light from an excitation light source, A fiber type optical amplifying device (EDFA: Erbium Doped Fiber Amplifier) that amplifies an optical signal is known. In recent years, ytterbium which can be applied as a pumping light source with a high-power laser having a watt-class output as an absorption band has been added to the core. In addition, in order to increase the intensity of pumping light that can be coupled in the core part, the optical signal is propagated in the single mode in the core part, and the pump light from the high-mode multimode laser light source is propagated in the multi-mode in the cladding part surrounding the core part. A double clad type optical fiber is also used (see Patent Document 1).

JP 2008-53294 A

  By the way, in the amplification of the video in the optical amplifying apparatus using the optical fiber described above, there are noise and signal distortion generated in the optical amplifying apparatus as factors that degrade the image quality. There is a noise figure (NF) as one of the indices representing the noise of the optical amplifier. If the NF is large, the noise of the optical amplifying device is superimposed on the video signal, so that snow-like noise appears on the reception screen. Indexes representing signal distortion include CSO (Composite Second Order Distortion) and CTB (Composite Triple Beat Distortion), and these distortions have a great influence on image quality.

  In order to reduce such image quality deterioration factors in analog transmission, it is desirable to shorten the length of the optical fiber. However, when the length of the optical fiber is shortened, residual pumping light that remains without being used for stimulated emission is generated. FIG. 10 is a diagram showing the relationship between the length of the optical fiber and the intensity of the residual pumping light when pumped with pumping light having a center wavelength of 933 nm. As shown in this figure, the intensity of the residual excitation light tends to increase as the length of the optical fiber becomes shorter. When such residual pumping light is generated, there is a problem that the heat and energy resulting from the residual pumping light may adversely affect the optical fiber and the like.

  Therefore, the problem to be solved by the present invention is to provide an optical amplifying device capable of improving analog characteristics while suppressing the generation of residual pumping light.

In order to solve the above problems, the present invention provides an optical amplifying apparatus for amplifying an optical signal, comprising: an input unit for inputting the optical signal; an uncooled multimode semiconductor laser element; and an excitation for generating multimode laser light outputs the use laser light source, an optical fiber of a double clad type for amplifying and outputting the optical signal by stimulated emission based on the laser light from the excitation laser light source, the optical signal amplified by the optical fiber has an output unit, and a passive optical component disposed between said optical fiber and said output section, the fiber-optic and the excitation laser light source is thermally coupled via the thermally conductive medium It is, especially by the thus generated heat the fiber-optic, allowed to warm to the excitation laser light source, varying the oscillation wavelength of the excitation laser light source To.
According to such a configuration, it is possible to improve analog characteristics while suppressing the generation of residual excitation light.

In another invention, in addition to the above-described invention, the fiber-optic to the thus generated heat is transferred to the excitation laser light source, the excitation laser light source occurs when it reaches the thermal steady state The wavelength band of the laser beam to be set is set so as to substantially match the wavelength band where the absorption rate of the optical fiber is high.
According to such a configuration, it is possible to improve analog characteristics and improve conversion efficiency while suppressing residual excitation light.

In another invention, in addition to the above-described invention, the thermally conductive medium is a heat sink for radiating heat the fiber-optic occurs by placing the excitation laser light source to the heat sink It is characterized by thermal bonding.
According to such a configuration, by using a heat sink having high thermal conductivity as the thermal conductive medium, both can be reliably thermally coupled without increasing the number of components.

In another invention, in addition to the above-described invention, for detecting the temperature of the excitation laser light source, the excitation laser light source and thermally coupled temperature detecting means, temperature detection by the temperature detecting means Based on the result, a temperature for adjusting the temperature of the system including the excitation laser light source so that the wavelength band of the laser light generated by the excitation laser light source substantially coincides with the wavelength band where the absorption rate of the optical fiber is high comprising an adjusting means, wherein the temperature adjusting means includes a cooling unit that cools the heat sink which is heated to the fiber-optic to control the power of the excitation laser light source thus by generated heat , and controlling the oscillation wavelength of the excitation laser light source by the cooling portion.
According to such a configuration, since the temperature of the excitation laser light source can be kept constant at all times, for example, residual excitation light can be reliably suppressed without being affected by the environmental temperature or the like.
According to another aspect of the invention, in addition to the above-described invention, the optical fiber is characterized in that Yb and Er are co-added to the core.

In addition to the above invention, another invention is characterized in that the power of the residual pumping light output from the optical fiber is set to 500 mW or less.
According to this configuration, it is possible to prevent the residual excitation light from adversely affecting the optical fiber or the like.

The optical transmission system of the present invention includes an optical transmission device that transmits an optical signal, the optical amplification device, and an optical reception device that receives the optical signal amplified by the optical amplification device. And
According to this configuration, it is possible to improve the communication quality of the transmission system, reduce power consumption, and save expenses necessary for maintaining the system.

  According to the optical amplification device and the optical transmission system of the present invention, it is possible to improve analog characteristics while suppressing the generation of residual pumping light.

It is a block diagram which shows the structural example of the optical amplifier of this invention. It is a figure which shows the cross-section of the amplification optical fiber shown in FIG. 1, and the refractive index of each site | part. It is a figure which shows the outline of the wavelength characteristic of the excitation light which a laser diode generate | occur | produces. It is a figure which shows an example of the relationship between the amplification optical fiber arrange | positioned at a heat sink, and a laser diode. It is a figure which shows the relationship between the ground state absorption and excitation state gain of an amplification optical fiber, and a wavelength. It is a figure which shows the relationship between the amplification optical fiber length in this embodiment and a prior art example, and residual excitation light. It is a figure which shows the structural example of the optical transmission system using the optical amplifier of this embodiment. It is a figure which shows another example of the relationship between the amplification optical fiber arrange | positioned at a heat sink, and a laser diode. It is a figure which shows another example of the relationship between the amplification optical fiber arrange | positioned at a heat sink, and a laser diode. It is a figure which shows the relationship between the amplification optical fiber length in a prior art example, and residual excitation light.

Next, an embodiment of the present invention will be described.
(A) Configuration of Embodiment FIG. 1 is a diagram illustrating a configuration example of an optical amplification device according to an embodiment of the present invention. As shown in this figure, the optical amplifying device 10 includes an input port 11, an amplifying optical fiber 12, optical couplers 13 and 14, optical isolators 15 and 16, an excitation light mixer 17, photodiodes 18 and 19, a laser diode 20, A control circuit 21, a thermistor 22, a cooling means 23, and an output port 24 are provided.

  The input port 11 is configured by, for example, an optical connector. In the input port 11, for example, light having a wavelength of 1550 nm obtained by modulating laser light by an AM-VSB (Amplitude Modulation-Vestigial Side-Band) signal composed of a 40-carrier sine wave having a frequency range of 91.25 to 343.25 MHz. A signal is input. An amplification optical fiber (EYDF: Erbium Ytterbium Doped Fiber) 12 amplifies an optical signal by stimulated emission by excitation light generated by a laser diode 20.

  FIG. 2 is a diagram showing a cross-sectional structure of the amplification optical fiber 12 and its refractive index. As shown in FIG. 2, the amplification optical fiber 12 is a double-clad optical fiber having a core portion 12a, a first cladding portion 12b, and a second cladding portion 12c. Further, as shown in the lower part of FIG. 2, the refractive index of each part is highest in the core part 12a, followed by the first clad part 12b and the second clad part 12c in this order. 12a is propagated in a single mode, and excitation light from the laser diode 20 is propagated in a multimode through the core portion 12a and the first cladding portion 12b. The core portion 12a is made of, for example, quartz glass, and erbium (Er) and ytterbium (Yb) are added together. The first cladding portion 12b is made of, for example, quartz glass. The second cladding part 12c is made of, for example, resin or quartz glass. The amplification optical fiber 12 is attached to a heat sink 30 (see FIG. 4) as will be described later, and a laser diode 20 is thermally coupled to the heat sink 30 (hereinafter simply referred to as “thermal coupling”). Yes. Note that FIG. 2 shows an example in which the first cladding portion 12b has a circular cross-sectional shape, but the shape is not limited to a circle, and may be, for example, a rectangle, a triangle, or a star shape. .

  The optical coupler 13 branches a part of the optical signal input from the input port 11 and inputs it to the photodiode 18, and inputs the rest to the optical isolator 15. The photodiode (PD) 18 converts the optical signal branched by the optical coupler 13 into a corresponding electric signal, and supplies it to the control circuit 21. The control circuit 21 converts the electrical signal supplied from the photodiode 18 into an analog signal or a corresponding digital signal, and detects the light intensity of the input signal.

  The optical isolator 15 has a function of transmitting light from the optical coupler 13 and blocking light returning from the excitation light mixer 17 and the amplification optical fiber 12. The laser diode (LD) 20 is configured by, for example, a multimode semiconductor laser element that generates laser light as excitation light having a wavelength in the 900 nm band. FIG. 3 is a diagram showing an outline of the wavelength characteristics of the laser beam generated by the laser diode 20. As shown in this figure, the laser beam generated by the laser diode 20 has a characteristic having a predetermined spread around the center wavelength λc. This example is an example, and other characteristics may be used. The laser diode 20 is an uncooled semiconductor laser element that does not have a Peltier element as a cooling element.

  The excitation light mixer 17 inputs the excitation light generated by the laser diode 20 to the amplification optical fiber 12 and propagates it in the core portion 12a and the first cladding portion 12b in multimode. In addition, the excitation light mixer 17 inputs the optical signal output from the optical isolator 15 to the amplification optical fiber 12 and propagates it in the core portion 12a in a single mode.

  The optical isolator 16 has a function of transmitting light from the amplification optical fiber 12 and blocking light returning from the optical coupler 14. The optical coupler 14 branches a part of the optical signal output from the optical isolator 16, inputs it to the photodiode 19, and outputs the rest from the output port 24. The output port 24 is constituted by, for example, an optical connector and outputs an amplified optical signal to the outside. The photodiode (PD) 19 converts the optical signal branched by the optical coupler 14 into a corresponding electrical signal, and supplies it to the control circuit 21. The control circuit 21 converts the electrical signal supplied from the photodiode 19 into an analog signal or a corresponding digital signal, and detects the light intensity of the output signal.

  The control circuit 21 includes, for example, a CPU (Central Processing Unit), a ROM (Read Only Memory), a RAM (Random Access Memory), an A / D (Analog to Digital) conversion circuit, and a D / A (Digital to Analog) conversion. In accordance with a program stored in the ROM, the CPU executes arithmetic processing using the RAM as a work area, and drives the laser diode 20 based on signals supplied from the photodiodes 18 and 19. By controlling the above, ALC (Automatic Output Power Level Control) or constant gain control AGC (Automatic Gain Control) is executed so that the intensity of the optical signal output from the optical amplifying apparatus 10 becomes constant. Further, based on the temperature of the laser diode 20 detected by the thermistor 22, the cooling means 23 is driven and controlled so that the temperature of the laser diode 20 becomes a desired temperature. The control circuit 21 may be configured by a DSP (Digital Signal Processor) or the like, for example.

  The thermistor (TH) 22 is thermally coupled to the laser diode 20, detects the temperature of the laser diode 20, and supplies it to the control circuit 21. The cooling means (FAN) 23 is composed of, for example, a small motor and a fan for blowing air. The cooling unit (FAN) 23 is driven according to the control of the control circuit 21 and blows air to the heat sink 30, so that the laser diode 20 is brought to a desired temperature. Control to be. The control of the cooling means 23 may be, for example, simply turning on / off according to the temperature level, or controlling the number of rotations according to the temperature level.

  FIG. 4 is a diagram illustrating a configuration example of the heat sink 30. The heat sink 30 is formed of a metal plate having good thermal conductivity such as aluminum or copper. On one surface of the metal plate (the surface on the near side in FIG. 4), a linear groove portion 31 in which one linear portion of the amplification optical fiber 12 wound in a coil shape is accommodated, and the other linear portion is accommodated. The linear groove part 32 and the circular groove part 33 in which the wound circular part is accommodated are formed. Since the radius inside the coiled portion of the amplification optical fiber 12 and the radius of the inner side surface of the circular groove 33 are substantially the same, the amplification optical fiber 12 is accommodated in the circular groove 33 of the heat sink 30. Then, the inner side of the wound portion of the amplification optical fiber 12 and the inner side surface of the circular groove portion 33 come into contact with each other, and thermal coupling is achieved between them. In order to increase the thermal conductivity, the width of the straight groove portions 31 and 32 and the circular groove portion 33 is set to be substantially the same as the thickness of the amplification optical fiber 12 so that both side surfaces of the groove portion are in contact with both sides of the amplification optical fiber 12. Also good. Further, for example, thermal conductivity may be further increased by interposing thermal conductive silicon or the like between them.

  In addition, the laser diode 20 is disposed substantially at the center of the top of the convex portion surrounded by the circular groove portion 33. In addition, in order to improve thermal conductivity, heat conductive silicon or the like may be interposed between them as in the case described above. Although not shown in FIG. 4, the thermistor 22 shown in FIG. 1 is thermally coupled to the laser diode 20 so that the temperature of the laser diode 20 can be detected. Similarly, although not shown in FIG. 4, the cooling means 23 shown in FIG. 1 is disposed at a position where the laser diode 20 can be cooled, for example. In addition, you may make it provide the cooling means 23 not in the front side (front side of FIG. 4) of the heat sink 30, but in the back side (back side of FIG. 4). Alternatively, a plurality of fins (Fin) may be provided on the back side of the heat sink 30 and the fins may be cooled by the cooling means 23.

(B) Operation of Embodiment In the following, after describing the outline of the operation of the present embodiment, the detailed operation will be described. In this embodiment, a double clad amplification optical fiber 12 in which erbium and ytterbium are co-doped is used. FIG. 5 is a diagram illustrating changes in the ground-state absorption and excited-state gain of the amplification optical fiber 12 depending on the wavelength. The curve indicating the ground state absorption has a flat band B around 910 to 960 nm and a peak around 975 nm. Incidentally, in the uncooled multimode laser diode 20, the wavelength of the generated laser light shifts to the longer wavelength side as the temperature rises. For example, when the temperature rises by 75 ° C., it shifts to the 22.5 nm long wavelength side. Therefore, in general, the center wavelength λc of the pumping light generated by the laser diode 20 is within a flat band B shown in FIG. It is common to be designed to fit.

  On the other hand, in the present application, the amplification optical fiber 12 that generates heat during operation and the laser diode 20 are thermally coupled by a heat sink 30 that is a thermally conductive medium, and the heat generated by the amplification optical fiber 12 is positively absorbed. The temperature of the laser diode 20 is increased by using it. When the thermal diode is in a steady state (when the heat generated from the amplification optical fiber 12 and the heat radiated from the heat sink 30 are balanced and the temperature of the laser diode 20 becomes constant), the laser diode 20 Is set so that the center wavelength λc of the pumping light generated by the laser beam substantially coincides with the peak wavelength λa of the ground state absorption of the amplification optical fiber 12 (975 nm in the example of FIG. 5). By setting in this way, the absorptance of pumping light can be increased as compared with the case of using a flat band B as in the prior art. Even when the length is set short, the intensity of the residual excitation light can be reduced. In addition, the conversion efficiency can be improved by using the amplification optical fiber 12 in a band having a high absorption rate. In addition, even if the temperature fluctuates and the wavelength of the excitation light generated by the laser diode 20 fluctuates, as long as the absorptance is within a range higher than the band B, compared to the conventional case, The residual excitation light can be reduced and the conversion efficiency can be increased.

  FIG. 6 is a diagram showing the relationship between the residual pumping light and the length of the amplification optical fiber 12 in the conventional example and this embodiment. The points shown in the upper ellipse in this figure indicate the relationship between the residual pumping light and the fiber length in the conventional example. Moreover, the point shown in the ellipse on the lower side of the figure shows the relationship between the residual pumping light and the fiber length in the present embodiment. From these comparisons, in the case of the present application, even if the length of the amplification optical fiber 12 is shortened, the residual pumping light does not increase as in the conventional case.

  Thus, in the present application, the laser diode 20 and the amplification optical fiber 12 are thermally coupled via the heat sink 30 and the center of the excitation light generated from the laser diode 20 when they reach a thermal steady state. Since the wavelength λc is set so as to substantially match the peak wavelength λa of the ground state absorption of the amplification optical fiber 12, an increase in residual pumping light can be suppressed while improving the analog characteristics. Further, the conversion efficiency can be improved by using the peak position of the absorption characteristic of the amplification optical fiber 12.

  Further, since an uncooled type can be used as the laser diode 20, the power consumed by the Peltier element (power about twice that required to drive the laser diode 20) becomes unnecessary, and the optical amplification device 10 power consumption can be reduced to 1/3 or less. Moreover, the size of the entire apparatus can be reduced by omitting the Peltier element radiator. Furthermore, a high gain can be easily obtained by using the double clad amplification optical fiber 12 in which erbium and ytterbium are co-doped.

  Next, the detailed operation of the present embodiment will be described.

  In the present embodiment, for example, a case where an optical signal having a wavelength of 1550 nm obtained by modulating a laser beam with an AM-VSB signal composed of a sine wave of 40 carriers having a frequency in the range of 91.25 to 343.25 MHz is exemplified. explain. When an optical signal is input from the input port 11, the optical coupler 13 branches a part and inputs it to the photodiode 18. Specifically, when the optical coupler 13 is a 20 dB coupler (when the branching ratio is 1/100), 1/100 of the optical signal is input to the photodiode 18 and the rest is input to the optical isolator 15. The

  The photodiode 18 converts the input optical signal into an electric signal and supplies it to the control circuit 21. The control circuit 21 converts the input electric signal into an analog signal or a corresponding digital signal, and then the intensity of the optical signal input from the input port 11 according to the obtained data and the branching ratio of the optical coupler 13. Is calculated.

The optical signal that has passed through the optical isolator 15 is guided to the excitation light mixer 17. The excitation light mixer 17 inputs the optical signal that has passed through the optical isolator 15 to the core portion 12a of the amplification optical fiber 12, and propagates the inside of the core portion 12a in a single mode. On the other hand, the pumping light generated by the laser diode 20 is input by the pumping light mixer 17 to the core portion 12a and the first cladding portion 12b of the amplification optical fiber 12, and the inside of the core portion 12a and the first cladding portion 12b is multiplexed. Propagated in mode. The excitation light is absorbed by ytterbium ions (Yb ³⁺ ) in the core portion 12 a while propagating through the amplification optical fiber 12, and the ytterbium ions indirectly excite erbium ions (Er ³⁺ ). The optical signal propagated through the core portion 12a is amplified by stimulated emission from the excited erbium ions.

  The amplification optical fiber 12 generates heat during the amplification operation. For example, when the amplification optical fiber 12 having a length of 8 m is excited by the laser diode 20 having an output of 8 W, the ambient temperature rises to nearly 60 ° C. In this embodiment, since the amplification optical fiber 12 is attached to the heat sink 30 shown in FIG. 4, the heat generated by the amplification optical fiber 12 is transmitted to the heat sink 30 as a thermally conductive medium. The laser diode 20 is disposed at the center of the heat sink 30, and the laser diode 20 is thermally coupled to the heat sink 30, so that the temperature of the laser diode 20 is increased by the heat transmitted from the amplification optical fiber 12. To do. Further, the heat transmitted through the heat sink 30 is radiated to the surroundings by heat radiation. The thermistor 22 is thermally coupled to the laser diode 20 to detect the element temperature. The temperature of the laser diode 20 detected in this way is supplied to the control circuit 21. The control circuit 21 determines whether or not the temperature of the laser diode 20 is equal to a preset and stored temperature Tc (for example, 50 ° C. (a temperature at which λc and λa substantially coincide)). If the detected temperature is high, the cooling means 23 is driven, otherwise the cooling means 23 is not driven. By such control, the temperature of the laser diode 20 is controlled to become the temperature Tc. Therefore, when the system including the cooling unit 23 reaches a thermal steady state, the element temperature of the laser diode 20 is the temperature. Equal to Tc.

  When the temperature of the laser diode 20 rises, the wavelength of the excitation light generated by the laser diode 20 shifts to the long wavelength side. Here, the center wavelength λc of the pumping light generated when the temperature of the laser diode 20 becomes equal to Tc (see FIG. 3), and the peak wavelength λa of the ground state absorption of the amplification optical fiber 12 (see FIG. 5). Are set to approximately match. As a result, the excitation light generated from the laser diode 20 is absorbed by the amplification optical fiber 12 at a high rate and used for amplification of the optical signal. For this reason, even if the length of the amplification optical fiber 12 is set short for the purpose of improving the analog characteristics, the intensity of the residual excitation light can be reduced. FIG. 6 is a diagram showing the relationship between the length of the amplification optical fiber 12 and the intensity of the residual excitation light, as described above. The points surrounded by the upper ellipse in FIG. 6 indicate the relationship between the length of the conventional amplification optical fiber 12 and the intensity of the residual pumping light. As the length of the amplification optical fiber 12 becomes shorter, the residual pumping The light intensity has increased significantly. On the other hand, the points enclosed by the lower ellipse in FIG. 6 indicate the relationship between the length of the amplification optical fiber 12 and the intensity of the residual pumping light in this embodiment, and the length of the amplification optical fiber 12 becomes shorter. Even so, the intensity of the residual excitation light is only slightly increased. The power of the residual pumping light output from the amplification optical fiber 12 is desirably set to 500 mW or less in consideration of the strength of the optical passive component. In addition, 500 mW is a value generally used as a high power proof stress value of the optical passive component. By setting the residual pumping light to 500 mW or less, the optical passive component is prevented from being damaged and has a long life. It becomes possible to plan.

  The optical signal amplified by the amplification optical fiber 12 is input to the optical coupler 14 via the optical isolator 16. The optical coupler 14 branches a part of the input optical signal and inputs it to the photodiode 19. Specifically, when the optical coupler 14 is a 20 dB coupler (when the branching ratio is 1/100), 1/100 of the optical signal is input to the photodiode 19 and the rest is output from the output port 24. The

  The photodiode 19 converts the input optical signal into an electric signal and supplies it to the control circuit 21. The control circuit 21 converts the input electrical signal into an analog signal or a corresponding digital signal, and then calculates the intensity of the amplified optical signal according to the obtained data and the branching ratio of the optical coupler 14. . Then, the control circuit 21 obtains the gain of the optical amplifying device 10 based on the intensity of the input light and the intensity of the output light calculated by the processing described above. Then, based on the obtained gain, constant gain control (AGC), which is control for making the gain constant, is executed. Alternatively, only output light intensity is detected, and output constant control (ALC: Automatic Output Power Level Control) is performed to keep the output intensity constant. In addition, control may be performed based on constant excitation current control (ACC: Automatic Current Control) or constant excitation power control (APC: Automatic Pump Power Control).

  As described above, according to the embodiment of the present invention, the laser diode 20 and the amplification optical fiber 12 are thermally coupled by the heat sink 30 as the heat conductive medium, and the heat generated by the amplification optical fiber 12 is converted into the laser. The central wavelength λc of the pumping light that is transmitted to the diode 20 and is generated by the laser diode 20 when reaching a thermal steady state substantially matches the peak wavelength λa of the pumping light absorption rate of the amplification optical fiber 12. Therefore, even if the length of the amplification optical fiber 12 is shortened for the purpose of improving the analog characteristics, it is possible to prevent the intensity of the residual pumping light from increasing.

  In the present embodiment, the amplification optical fiber 12 and the laser diode 20 are thermally coupled via the heat sink 30. Since the heat sink 30 is generally made of a metal such as aluminum having high thermal conductivity, the heat generated by the amplification optical fiber 12 can be quickly transferred to the laser diode 20 and the temperature can be controlled without delay. it can.

  Further, in the present embodiment, the thermistor 22 is thermally coupled to the laser diode 20 and the cooling means 23 is controlled based on the temperature detected by the thermistor 22, so that the laser diode 20 always has a constant temperature. Can be. By such control, the intensity of the residual excitation light can be controlled to be constant at a low level without being affected by the environmental temperature or the like. Moreover, the conversion efficiency of the amplification optical fiber 12 can be maintained at a high level.

  In this embodiment, since the uncooled type is used as the laser diode 20, the power consumed by the Peltier element is not required, so that the power consumption of the optical amplifying device 10 can be reduced to about 1/3. At the same time, the size of the entire apparatus can be reduced by omitting the radiator of the Peltier element. In the present embodiment, the cooling means 23 is used. However, since the power consumption of the cooling means 23 is smaller than that of the Peltier element, even when the cooling means 23 is operated frequently (or continuously). Even if it exists, power consumption can be reduced compared with a Peltier device.

  Further, in this embodiment, as shown in FIG. 4, the amplification optical fiber 12 is wound so that the side of the amplification optical fiber 12 to which the excitation light is input is disposed in front. The amplification optical fiber 12 has a distribution in which the temperature on the side where the excitation light is input is high and the temperature decreases as the distance from the input end increases. Therefore, the heat of the amplification optical fiber 12 can be efficiently transferred to the laser diode 20 by disposing the high temperature side of the amplification optical fiber 12 on the side close to the laser diode 20.

  FIG. 7 is a schematic configuration diagram for explaining an example when the optical amplifying apparatus of this embodiment is applied to the optical transmission system 50. In the example of this figure, the optical transmission system 50 includes an optical transmission device 60, a transmission-side optical transmission path 70, the optical amplification device 10 of the present embodiment, a reception-side optical transmission path 80, and an optical signal reception device 90. ing. In this example, the optical signal transmitted from the optical transmission device 60 is propagated through the transmission side optical transmission path 70 and reaches the optical amplification device 10. In the optical amplifying device 10, as described above, after the optical signal is amplified, the optical signal is propagated through the receiving side optical transmission line 80 and reaches the optical signal receiving device 90, where the signal is demodulated. Since the optical amplifying apparatus 10 of the present embodiment has good analog characteristics and low power consumption, the optical transmission system 50 using such an optical amplifying apparatus 10 improves the communication quality of the entire system. , Reduce power consumption and save the cost of maintaining the system.

(C) Modified embodiment

  In the above embodiment, the heat sink 30 as shown in FIG. 4 is used. However, for example, a configuration as shown in FIG. In the example of FIG. 8, the heat sink 130 is formed of a thermally conductive metal plate such as aluminum or copper. A straight groove 131 in which one end of the amplification optical fiber 12 is embedded is formed on one surface of the metal plate, and the straight portion on the side where the excitation light of the amplification optical fiber 12 is input into the straight groove 131. Embedded. The amplification optical fiber 12 extending upward from the straight groove 131 is rotated from the inside to the outside so as to draw a spiral, the radius gradually increases, and the other end is in the same direction as the straight groove 131. It extends toward the outside of the heat sink 130. In addition, since the linear part into which the excitation light of the amplification optical fiber 12 is input is embedded in the linear groove 131 and the surface thereof is substantially the same height as the surface of the heat sink 130, the spiral part is Arrangement is possible without bending to avoid the straight part. The amplification optical fiber 12 is attached to the heat sink 130 by, for example, an adhesive. In the vicinity of the center of the spiral portion of the amplification optical fiber 12, the laser diode 20 is disposed, for example, via thermally conductive silicon for increasing the thermal conductivity so as to be thermally coupled to the heat sink 130. . As in the case described above, the thermistor 22 shown in FIG. 1 is thermally coupled to the laser diode 20 so that the temperature of the laser diode 20 can be detected. Moreover, the cooling means 23 shown in FIG. 1 is arrange | positioned in the position which can be cooled with respect to the laser diode 20, for example. The heat sink 130 may be provided not on the front side but on the back side, or a plurality of fins may be provided on the back side of the heat sink 130 and the fins may be cooled by the cooling means 23.

  FIG. 9 shows yet another embodiment of the heat sink. In the example of FIG. 8, only a part of the amplified optical fiber 12 is embedded in the heat sink 130, but in FIG. 9, the entire amplified optical fiber 12 is embedded in the heat sink 230. That is, in this example, the heat sink 230 includes a linear groove portion 231 in which one linear portion of the amplification optical fiber 12 is accommodated, a linear groove portion 232 in which the other linear portion is accommodated, and a spirally wound portion. And a spiral groove portion 233 in which is accommodated. Note that the linear groove portion 231 in which one end portion of the amplification optical fiber 12 is embedded has a groove depth deeper than the other portion by the thickness of the fiber. In this manner, the structure embedded in the heat sink 230 can increase the contact area between the amplification optical fiber 12 and the heat sink, thereby increasing the thermal conductivity. Although not shown in FIG. 9, after embedding the amplification optical fiber 12, the surface of the heat sink 230 is sealed with a resin sheet or the like having an opening corresponding to the laser diode 20, for example, It is possible to prevent the amplification optical fiber 12 from being damaged. Further, by using a resin having thermal conductivity, the thermal coupling between the amplification optical fiber 12 and the heat sink 230 can be further enhanced.

  In the examples of FIGS. 8 and 9, the temperature of the amplification optical fiber 12 is increased because the side to which the excitation light of the amplification optical fiber 12 is input is spirally wound. By disposing the portion in the vicinity of the laser diode 20, heat can be efficiently transferred to the laser diode 20.

  In the above embodiment, the amplification optical fiber 12 and the laser diode 20 are thermally coupled. However, other than this, a passive optical component (for example, an optical fiber) positioned on the output side of the amplification optical fiber 12 is used. The isolator 16 or the optical coupler 14) and the laser diode 20 may be thermally coupled. This is because the passive optical component located on the output side also generates heat. As described above, as a thermal coupling method, as described above, thermal coupling may be performed via a heat sink, or the laser diode 20 and the passive optical component may be directly thermal coupled. Further, a passive optical component is disposed in the vicinity of the laser diode 20 of the heat sinks 30, 130, and 230 shown in FIGS. 4, 8, and 9 so as to utilize heat from both the amplification optical fiber 12 and the passive optical component. May be. In the case of the amplification optical fiber 12, the absorptance fluctuates in accordance with the shift of the wavelength output from the laser diode 20 and the heat generation amount changes. However, the heat generation amount of the passive optical component located on the output side is Since it is stable with respect to the shift of the wavelength, stable reduction control of the residual pumping light becomes possible by thermally coupling the passive optical component and the laser diode 20.

  Further, in the above embodiment, the thermistor 22 and the cooling means 23 are provided and the temperature control is performed based on these, but for example, the temperature of the laser diode 20 is set to a desired value without performing the temperature control. If the temperature can be maintained, these need not be provided.

  In the above embodiment, a heat sink is used as the heat conductive medium. However, a medium other than the heat sink may be used as the heat conductive medium. Specifically, for example, a metal housing in which the optical amplifying device 10 is accommodated may be used as the heat conductive medium. Moreover, as a heat conductive medium, it is not limited to a metal, For example, you may make it use air as a heat conductive medium. That is, the laser diode 20 may be simply disposed in the vicinity of the amplification optical fiber 12 or the passive optical component. In addition to this, examples of the heat conduction medium include liquids such as water and organic solvents, resins, and the like. It goes without saying that these can be used.

  In the above embodiment, the pump light input side of the amplification optical fiber 12 is arranged near the laser diode 20. However, when the temperature of the laser diode 20 is equal to or higher than the desired temperature. The pump light input side may be arranged at a position far from the laser diode 20. Also, the mounting position of the laser diode 20 is not limited to the positions shown in FIGS. 4, 8, and 9. For example, the laser diode 20 may be mounted at any one of the four corners of the heat sink or attached to the back side surface of the heat sink. Also good.

  In the above embodiment, the relationship between the output control (for example, ALC) and the temperature control is not described. However, the response speed of the control is fast for the output control, while the response speed is high for the temperature control. Slower than output control. Therefore, for example, in order to control the output to be constant, control is performed based on output control in the short term, and control is performed so that the temperature of the laser diode 20 becomes a desired temperature by temperature control in the long term. Thus, the analog characteristics can be improved while reducing the intensity of the residual excitation light. Note that, by setting the temperature of the laser diode 20 to a desired temperature, not only can the intensity of the residual excitation light be reduced, but also the conversion efficiency can be increased, so it is desirable to prioritize temperature control.

  In the above embodiment, the excitation light generated by the laser diode 20 has been described as having the wavelength characteristics shown in FIG. 3. However, when the excitation light has characteristics different from this (for example, when there is no significant peak wavelength) ) May be set so that the absorptance by the amplification optical fiber 12 becomes the highest when the wavelength shifts due to temperature rise. That is, when the temperature rises, the wavelength characteristic as shown in FIG. 3 and the absorption characteristic as shown in FIG.

  In the above embodiment, the forward excitation method is employed as the excitation method. However, for example, a backward excitation method or a bidirectional excitation method may be employed. Although the backward excitation method is inferior to the forward excitation method in noise characteristics, it can increase the output. In addition, the bidirectional excitation method enables amplification that combines the characteristics of both the forward excitation method and the backward excitation method.

  Further, in the above embodiment, the optical amplifying apparatus 10 is configured with only the booster amplifier. For example, in order to improve NF as a noise figure, for example, after amplification by a preamplifier provided in the previous stage of the booster amplifier, Further amplification may be performed by a booster amplifier.

  In the above embodiment, the case where erbium and ytterbium are co-added to the core portion 12a has been described as an example. Or other substances having an amplification effect similar to that of the rare earth element may be added. In this case, although the amplification band is different from the above embodiment, the same effect as the present invention can be obtained.

10 Optical amplifier 11 Input port (input unit)
12 Amplified optical fiber (optical fiber)
12a Core part 12b First clad part 12c Second clad part 13 Optical coupler 14 Optical coupler (passive optical component)
15 Optical isolators 16 Optical isolators (passive optical components)
17 Excitation light mixer 18, 19 Photodiode 20 Laser diode (laser light source)
21 Control circuit (part of temperature adjustment means)
22 Thermistor (temperature detection means)
23 Cooling means (part of temperature adjusting means)
24 Output port (output unit)
30, 130, 230 Heat sink (thermally conductive medium)
50 Optical Transmission System 60 Optical Signal Transmitter (Optical Transmitter)
70 Transmission-side optical transmission line 80 Reception-side optical transmission line 90 Optical signal reception device (optical reception device)

Claims (7)

In an optical amplification device that amplifies an optical signal,
An input unit for inputting the optical signal;
An excitation laser light source including an uncooled multimode semiconductor laser element and emitting multimode laser light;
A double-clad optical fiber that amplifies and outputs the optical signal by stimulated emission based on the laser light from the excitation laser light source;
An output unit for outputting the optical signal amplified by the optical fiber;
A passive optical component disposed between the optical fiber and the output unit,
The fiber-optic and the excitation laser light source is thermally coupled via a heat conductive medium,
By the thus generated heat the fiber-optic, allowed to warm to the excitation laser light source, to change the oscillation wavelength of the excitation laser light source,
An optical amplification device characterized by that. The heat thus generated in the fiber-optic is transmitted to the excitation laser light source, the wavelength band of the laser light the excitation laser light source when it reaches the thermal steady state occurs, the absorption of the optical fiber It is set to approximately match the wavelength band where the rate is high,
The optical amplifying apparatus according to claim 1. Wherein the thermally conductive medium is a heat sink for radiating heat the fiber-optic occurs claim 1, characterized in that the thermally coupled by placing the excitation laser light source to the heat sink The optical amplifying device described. Said to detect the temperature of the excitation laser light source, the excitation laser light source and thermally coupled temperature detecting means,
Based on the temperature detection result of the temperature detecting means, the wavelength band of the laser light the excitation laser light source is generated, including the excitation laser light source so that the absorption rate of the optical fiber coincides high wavelength band and substantially Temperature adjusting means for adjusting the temperature of the system;
Have
It said temperature adjusting means includes a cooling unit that cools the heat sink which is heated to the fiber-optic to control the power of the excitation laser light source thus by generated heat, for the excitation by the cooling unit 4. The optical amplifying apparatus according to claim 3, wherein an oscillation wavelength of the laser light source is controlled. The optical amplifying apparatus according to claim 1, wherein Yb and Er are co-doped in the core of the optical fiber. Optical amplifying device according to any one of claims 1 to 5, the power of the residual pump light output from the optical fiber is characterized in that it is set to be less than 500 mW. An optical transmitter for transmitting an optical signal;
The optical amplification device according to any one of claims 1 to 6,
An optical receiver for receiving the optical signal amplified by the optical amplifier;
An optical transmission system comprising:

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