JP2010028016A - Optical amplifying device - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide an optical amplifying device which is excellent in the cooling efficiency of an optical fiber for amplification, and is capable of miniaturization. <P>SOLUTION: The optical amplifying device 10 includes a heat pipe 11 forming a shape curved into an approximate circle, an optical fiber 12 for amplification wound concentrically forming the shape almost equal to the curved shape of the heat pipe 11 and arranged so as to contact the heat pipe 11, a heat radiating portion 13 provided in one end portion 11a of the heat pipe 11. <P>COPYRIGHT: (C)2010,JPO&INPIT

Description

  The present invention relates to an optical amplifying device used in an optical transmission device and an optical fiber laser device, and more particularly to an optical amplifying device having a function capable of efficiently cooling a heated optical fiber for amplification. .

In recent years, a technique for directly amplifying an optical signal using an optical fiber has been actively used in an optical transmission device, an optical fiber laser device, and the like.
This optical amplifying device inputs an optical signal and a pump light for amplification into an optical fiber for amplification (such as a double clad fiber) doped with erbium (Er) or ytterbium (Yb) to amplify an optical signal. It is a device that can directly amplify an optical signal.

  However, in the optical amplifying device, there is a problem that a part of the pump light that is not used for amplification in the amplification optical fiber becomes heat when the optical signal is amplified, and the temperature of the amplification optical fiber is increased. When the temperature of the amplification optical fiber becomes high, the resin coating covering the periphery of the amplification optical fiber deteriorates and affects the optical amplification effect. Therefore, a technique for cooling the amplification optical fiber is required.

  An optical fiber for amplification used for optical amplification includes a double-clad fiber including a core doped with a rare earth element, a first cladding covering the periphery of the core, and a second cladding covering the periphery of the first cladding. It is. In this double clad fiber, signal light propagates in the core, and pump light propagates in the first clad. Since this double clad fiber has an outer diameter larger than that of a normal communication optical fiber (outer diameter 125 μm), when the double clad fiber is wound concentrically and stored in a container or the like, the curvature of the fiber is reduced. If too much, the fiber may be broken by bending stress. Therefore, when the double clad fiber is wound and stored, it is necessary to increase its curvature. Further, since the transmission loss of the amplification optical fiber increases as the curvature of the amplification optical fiber decreases, the double clad fiber cannot be wound with the curvature reduced.

Therefore, the double clad fiber is usually wound and stored so that the diameter is 100 mm or more. This solves the problem of an increase in transmission loss of the amplification optical fiber, but still does not solve the problem of deterioration of the resin coating due to heat generation of the amplification optical fiber itself. Therefore, conventionally, there has been proposed an optical amplifying device in which the amplification optical fiber is housed and fixed in a groove provided in the heat sink, and the amplification optical fiber is cooled using the heat sink, thereby preventing the resin coating from being deteriorated. (For example, refer to Patent Document 1).
JP 2006-114769 A

Even in the cooling structure of the amplification optical fiber using the heat sink, the double clad fiber is wound and stored so that the diameter becomes 100 mm or more, so the size of the heat sink needs to be 100 mm square or more. Further, in order to uniformly cool the entire heat sink, it is necessary to use a cooling fan having an outer diameter of 100 mm or more. Therefore, in order to accommodate the heat sink and the cooling fan, a large space is required inside the optical amplifying device, and there is a problem that the entire device becomes large.
In the future, high-power optical fiber laser devices and optical amplification transmission devices will be required. In this case, the power of the pump light input to the amplification optical fiber increases, and the amplification optical fiber Since the amount of heat generation also increases, a technique for cooling the amplification optical fiber becomes more and more important.

  The present invention has been made in view of the above circumstances, and an object of the present invention is to provide an optical amplifying device that is excellent in cooling efficiency of an amplifying optical fiber and that can be miniaturized.

  An optical amplifier according to the present invention includes a heat pipe having a substantially circular shape, a concentric shape that is substantially the same as the curved shape of the heat pipe, and disposed so as to be in contact with the heat pipe And an amplifying optical fiber, and a heat radiating portion provided at one end of the heat pipe.

  An optical amplifying device of the present invention includes a heat pipe having a spiral shape, an amplification optical fiber disposed along the spiral shape of the heat pipe and in contact with the heat pipe, and the heat pipe And a heat dissipating part provided at one end.

It is preferable that the light output end portion of the amplification optical fiber is disposed on the heat radiating portion side of the heat pipe.
It is preferable that the light input end of the amplification optical fiber is disposed below the light output end of the amplification optical fiber in the direction of gravity.

It is preferable that a groove-like recess extending along the axial direction is provided on the surface of the heat pipe, and the amplification optical fiber is accommodated in the recess.
It is preferable that a plurality of heat pipes are disposed so as to surround the amplification optical fiber.
It is preferable that a hollow portion is provided at the center along the axial direction of the heat pipe, and the amplification optical fiber is inserted into the hollow portion.

  An optical amplifier according to the present invention includes a heat pipe having a substantially circular shape, a concentric shape that is substantially the same as the curved shape of the heat pipe, and disposed so as to be in contact with the heat pipe Since the amplification optical fiber and the heat radiating portion provided at one end of the heat pipe are provided, the heat of the amplification optical fiber generated by inputting the amplification pump light is input to the heat pipe. Since the optical fiber for amplification can be efficiently cooled by being absorbed, a decrease in the optical amplification effect due to deterioration of the resin coating of the optical fiber for amplification can be prevented. In addition, the heat pipe can be cooled by cooling the heat dissipating part provided at one end of the heat pipe, so that a large cooling fan is not required and the energy required for cooling can be reduced as compared with the conventional system. Miniaturization can be achieved. Furthermore, since it is only necessary to cool only the heat pipe having a substantially circular shape, the space in the center of the circle can be used for mounting other components, and this space can be used effectively.

  An optical amplifying device of the present invention includes a heat pipe having a spiral shape, an amplification optical fiber disposed along the spiral shape of the heat pipe and in contact with the heat pipe, and the heat pipe And a heat dissipating part provided at one end, so that heat of the amplification optical fiber generated by inputting the pump light for amplification is absorbed by the heat pipe over its entire length, so that it is more efficient In addition, since the amplification optical fiber can be cooled, it is possible to prevent a decrease in the optical amplification effect due to deterioration of the resin coating of the amplification optical fiber. In addition, the heat pipe can be cooled by cooling the heat dissipating part provided at one end of the heat pipe, so that a large cooling fan is not required and the energy required for cooling can be reduced as compared with the conventional system. Miniaturization can be achieved. Furthermore, since only the spiral heat pipe needs to be cooled, the space in the center of the spiral can be used for mounting other components, and this space can be used effectively.

The best mode of the optical amplifying device of the present invention will be described.
This embodiment is specifically described for better understanding of the gist of the invention, and does not limit the present invention unless otherwise specified.

(1) First Embodiment FIG. 1 is a schematic configuration diagram showing a first embodiment of the optical amplifying device of the present invention.
The optical amplifying device 10 of this embodiment includes a heat pipe 11, an amplification optical fiber 12 provided so as to be in contact with the heat pipe 11, and a heat radiating part 13 provided at one end 11 a of the heat pipe 11. The cooling fan 14 is arranged roughly so as to face the heat radiating part 13.

The heat pipe 11 includes a curved portion that is curved in a substantially circular shape, and a straight straight pipe portion that follows the curved portion, and the circular diameter is about 100 mm.
The amplification optical fiber 12 has a shape substantially equal to the curved shape of the heat pipe 11 and is wound concentrically. That is, the amplification optical fiber 12 is concentrically wound so that the diameter thereof is about 100 mm.

  In addition, the arrangement where the amplification optical fiber 12 is in contact with the heat pipe 11 means that the wound amplification optical fiber 12 is in contact with the surface of the heat pipe 11. Say. In other words, the amplifying optical fibers 12 wound and bundled are arranged so as to be in contact with the surface of the heat pipe 11.

Further, the light output end 12a of the amplification optical fiber 12 is disposed on the one end 11a side of the heat pipe 11 provided with the heat radiating portion 13, while the light input end 12b of the amplification optical fiber 12 is provided. The heat pipe 11 is disposed on the other end 11b side.
In the optical amplifying device 10, the temperature of the light input end 12b of the amplification optical fiber 12 becomes the highest, and the temperature gradually decreases toward the light output end 12a. Such a decrease in temperature is that the amplification pump light input from the optical input end of the amplification optical fiber 12 is attenuated by transmission loss while propagating through the amplification optical fiber 12. caused by. In addition, the heat pipe is used in a place where there is a temperature distribution in the longitudinal direction due to its principle. In other words, a heat pipe will not function unless there is a temperature difference between its one end and the other end. Therefore, the light output end portion 12a of the amplification optical fiber 12 is disposed on the one end portion 11a side of the heat pipe 11 provided with the heat radiating portion 13, while the light input end portion 12b of the amplification optical fiber 12 is disposed. It arrange | positions at the other end part 11b side of the heat pipe 11, operates the heat pipe 11 efficiently, and cools the optical fiber 12 for amplification.

The heat pipe 11 is a well-known one, and is roughly configured by a container made of a metal tube, a wick having a capillary action, and a working fluid made of a condensable liquid such as water sealed in the container. ing.
In this example, in the heat pipe 11, one end 11a provided with the heat dissipating part 13 is a cooling part, and the other end 11b is a heating part.

  In the heat pipe 11, when the heat of the amplification optical fiber 12 is transmitted to the working fluid on the heating unit side, the working fluid evaporates, and the vapor of the working fluid flows to the low-temperature / low-pressure cooling unit. This vapor dissipates heat and condenses. Here, the latent heat of vaporization is transferred, and the condensed working fluid is returned to the heating unit by the capillary action of the wick in the container. By repeating the delivery of heat by the working fluid, heat is transmitted from the heating part of the heat pipe 11 to the cooling part, and accordingly, the amplification optical fiber 12 is cooled.

  The amplification optical fiber 12 includes a double clad fiber including a core doped with a rare earth element, a first clad covering the periphery of the core, and a second clad covering the periphery of the first clad. .

Although it does not specifically limit as the thermal radiation part 13, In order to raise the cooling efficiency of the heat pipe 11, a thing with the large surface area is preferable, for example, the several rectangular-shaped thermal radiation fin was arrange | positioned at predetermined intervals. The thing of composition is mentioned.
Moreover, as a material of the heat radiating part 13, a metal such as aluminum is used.

  Although it does not specifically limit as the cooling fan 14, The magnitude | size is determined according to the magnitude | size of the thermal radiation part 13, and the flow of the air which the cooling fan 14 generate | occur | produces hits the thermal radiation part 13 whole.

Further, in the optical amplifying device 10, it is preferable that the amplifying optical fiber 12 is disposed so as to be in contact with the heat pipe 11 through a resin having high thermal conductivity.
In order to maintain the state where the amplification optical fiber 12 is disposed so as to be in contact with the heat pipe 11, it is preferable to fix the amplification optical fiber 12 to the surface of the heat pipe 11 with a resin such as an adhesive. In order to increase the cooling efficiency of the amplification optical fiber 12 by the heat pipe 11, it is preferable to use a resin having high thermal conductivity.

Moreover, it is preferable that the amplification optical fiber 12 is disposed so as to be in contact with the heat pipe 11 through a resin having a low Young's modulus.
Since the thermal expansion coefficients of the heat pipe 11 and the amplification optical fiber 12 are different, when the amplification optical fiber 12 is fixed to the surface of the heat pipe 11 using a hard resin having a high Young's modulus, the thermal expansion of the heat pipe 11 is achieved. As a result, the amplification optical fiber 12 may be pulled and broken. Therefore, in order to prevent the amplification optical fiber 12 from being broken, it is preferable to use a soft resin having a low Young's modulus.
Examples of such a resin having a high thermal conductivity and a low Young's modulus include rubber-modified epoxy resins and silicone resins filled with a large amount of metal powder such as aluminum powder.

Further, it is preferable that the amplification optical fiber 12 is disposed so as to be in contact with the heat pipe 11 through a resin having a refractive index lower than that of the resin coating covering the periphery thereof.
In the double clad fiber, the pump light for amplification is also propagated near the inside of the resin coating covering the periphery of the optical fiber. Therefore, if a resin having a refractive index higher than that of the resin coating is used, the pump light for amplification is used. Leaks out of the optical fiber and cannot be used for amplification. Therefore, in order to prevent the amplification pump light from leaking from the amplification optical fiber 12, it is preferable to use a resin having a lower refractive index than the resin coating covering the periphery of the amplification optical fiber 12.

Furthermore, the surface of the heat pipe 11 preferably has a hue that absorbs light in the same wavelength region as the amplification pump light propagating through the amplification optical fiber 12.
As described above, when the amplification optical fiber 12 is disposed so as to be in contact with the heat pipe 11 through a resin having a lower refractive index than the resin coating covering the periphery thereof, impurities and minute amounts of the amplification optical fiber 12 may be reduced. Due to the bending, a part of the amplification pump light input to the amplification optical fiber 12 leaks out of the amplification optical fiber 12. The pump light for amplification hits other parts in the amplifying apparatus 10 and changes into heat, and there is a risk of raising the temperature of the part and causing the part to break down. That is, the heat generation of the amplification optical fiber 12 is caused by the heat generation of the amplification optical fiber 12 itself and the light leaked from the amplification optical fiber 12 being absorbed by other parts and converted into heat. Therefore, in order to cause the heat pipe 11 to absorb the light leaked from the amplification optical fiber 12 and suppress heat generation in other components, the amplification pump that propagates the surface of the heat pipe 11 through the amplification optical fiber 12. A hue that absorbs light in the same wavelength region as that of light (usually infrared rays) is preferable.

  According to the optical amplifying device 10 of this embodiment, a heat pipe 11 having a substantially circular shape, a concentric shape that is substantially the same as the curved shape of the heat pipe 11, and a heat pipe 11 is provided with an amplifying optical fiber 12 disposed so as to be in contact with 11 and a heat radiating portion 13 provided at one end portion 11a of the heat pipe 11, and is generated by inputting amplification pump light. Since the heat of the amplification optical fiber 12 is absorbed by the heat pipe 11 and the amplification optical fiber 12 can be efficiently cooled, the optical amplification effect is reduced due to deterioration of the resin coating of the amplification optical fiber 12. Can be prevented. In addition, since the heat pipe 11 only needs to cool the heat dissipating part 13 provided at one end 11a thereof, a large cooling fan becomes unnecessary, and the energy required for cooling can be reduced as compared with the conventional case. In addition, the apparatus can be reduced in size. Furthermore, since only the heat pipe 11 needs to be cooled, the space in the center of the circle can be used for mounting other components, and this space can be used effectively.

(2) Second Embodiment FIG. 2 is a schematic configuration diagram showing a second embodiment of the optical amplifying device of the present invention.
The optical amplifying device 20 of this embodiment includes a heat pipe 21, an amplification optical fiber 22 provided so as to be in contact with the heat pipe 21, and a heat radiating part 23 provided at one end 21 a of the heat pipe 21. The cooling fan 24 is arranged roughly so as to face the heat radiating portion 23.

In the optical amplifying device 20, the heat pipe 21 has a spiral shape, and the diameter of the spiral circle is about 100 mm.
The amplification optical fiber 22 is disposed along the spiral shape of the heat pipe 21 so as to be in contact with the heat pipe 21. That is, the amplification optical fiber 22 is wound concentrically on the surface of the heat pipe 21 so that the diameter thereof is about 100 mm.

  The amplification optical fiber 22 is arranged so as to contact the heat pipe 21. In other words, the amplification optical fibers 22 are arranged along the spiral shape of the heat pipe 21 without overlapping each other, It says that it is arranged in contact with the surface of the heat pipe 21.

Further, the light output end 22a of the amplification optical fiber 22 is disposed on the one end 21a side of the heat pipe 21 provided with the heat radiating portion 23, while the light input end 22b of the amplification optical fiber 22 is provided. The heat pipe 21 is disposed on the other end 21b side.
Also in this optical amplifying device 20, the light output end 22 a of the amplification optical fiber 22 is arranged on one end 21 a side of the heat pipe 21 provided with the heat radiating portion 23, while the amplification optical fiber 22 The optical input end 22b is disposed on the other end 21b side of the heat pipe 21, and the heat pipe 21 is efficiently operated to cool the amplification optical fiber 22.
In this example, in the heat pipe 21, one end 21a provided with the heat dissipating part 23 is a cooling part, and the other end 21b is a heating part.

Further, in the optical amplifying device 20, it is preferable that the light input end 22 b of the amplification optical fiber 22 is disposed below the light output end 22 a of the amplification optical fiber 22 in the gravity direction.
In the heat pipe 21 (particularly, the one having no wick inside), the high temperature portion (the other end portion 21b) is arranged below the gravity direction (arrow direction in FIG. 2), and the temperature is low. The heat conduction effect becomes higher when the portion (one end portion 21a) is arranged on the upper side with respect to the direction of gravity. This is because when the working fluid in the heat pipe 21 is cooled and liquefied by the cooling unit (one end 21a), the working fluid easily returns to the heating unit (the other end 21b) due to its weight. is there. Accordingly, the optical input end 22b of the amplification optical fiber 22 is disposed below the light output end 22a of the amplification optical fiber 22 in the direction of gravity, thereby efficiently cooling the amplification optical fiber 22. be able to.

  As the heat pipe 21, the amplification optical fiber 22, the heat radiating unit 23, and the cooling fan 24, the same ones as in the previous embodiment are used.

Moreover, in the optical amplifying apparatus 20, it is preferable that the amplification optical fiber 22 is disposed so as to be in contact with the heat pipe 21 through a resin having high thermal conductivity.
Further, it is preferable that the amplification optical fiber 22 is disposed so as to be in contact with the heat pipe 21 through a resin having a low Young's modulus.

Further, it is preferable that the amplification optical fiber 22 is disposed so as to be in contact with the heat pipe 21 through a resin having a refractive index lower than that of the resin coating covering the periphery thereof.
Furthermore, the surface of the heat pipe 21 preferably has a hue that absorbs light in the same wavelength range as the amplification pump light propagating through the amplification optical fiber 22.

Further, as shown in FIG. 3, a groove-like recess 21c extending along the axial direction (longitudinal direction) is provided on the surface of the heat pipe 21, and the amplification optical fiber 22 is accommodated in the recess 21c. Good.
The heat pipe 21 has a cylindrical shape, and it is difficult to fix the heat pipe 21 with the amplification optical fiber 22 along the surface. Therefore, the recess 21c is provided on the surface of the heat pipe 21 along the axial direction thereof, and the amplification optical fiber 22 is accommodated in the recess 21c, so that the amplification optical fiber 22 is aligned with the surface of the heat pipe 21. It can be easily fixed in a wet state. As a result, the cooling efficiency of the amplification optical fiber 22 is improved.
The configuration in which the groove-like recess extending along the axial direction is provided on the surface of the heat pipe and the amplification optical fiber is accommodated in the recess is also applied to the first embodiment described above. I can do this.

Moreover, as shown in FIG. 4, the heat pipe 21 with a large outer diameter may be produced, and the amplification optical fiber 22 may be spirally wound around the outer peripheral surface (side surface) 21d. In this case, the outer diameter of the heat pipe 21 is preferably a size that does not increase the transmission loss of the wound optical fiber 22 for amplification, and is more preferably about 100 mm.
In this way, the amplification optical fiber 22 can be easily fixed along the surface of the heat pipe 21, the cooling efficiency of the amplification optical fiber 22 can be improved, and the amplification light can be improved. The length of the heat pipe 21 can be shortened with respect to the fiber 22.

Further, as shown in FIG. 5A, three heat pipes 21 may be arranged so as to surround one amplification optical fiber 22, or as shown in FIG. Four heat pipes 21 may be arranged so as to surround the two amplification optical fibers 22.
As shown in FIG. 2, when one amplification optical fiber 22 is arranged along one heat pipe 21, heat is only applied to the portion in contact with the amplification optical fiber 22 in the heat pipe 21. Is not transmitted, the heat absorption effect is low. Therefore, by arranging a plurality of heat pipes 21 so as to surround one amplification optical fiber 22, it is possible to enhance the heat absorption effect of the heat pipe 21 and improve the cooling efficiency of the amplification optical fiber 22. it can.

Furthermore, as shown in FIG. 6, a hollow portion 21d may be provided in the center along the axial direction (longitudinal direction) of the heat pipe 21, and the amplification optical fiber 22 may be inserted into the hollow portion 21d.
In this way, the amplification optical fiber 22 can be easily fixed in the hollow portion 21d of the heat pipe 21 and the cooling efficiency of the amplification optical fiber 22 can be improved.

  According to the optical amplifying apparatus 20 of this embodiment, the heat pipe 21 having a spiral shape and the optical fiber for amplification arranged along the spiral shape of the heat pipe 21 and in contact with the heat pipe 21 are arranged. 22 and the heat radiating portion 23 provided at one end 21a of the heat pipe 21, the heat of the amplification optical fiber 22 generated by inputting the amplification pump light is reduced to the entire length. Since the amplifying optical fiber 22 can be cooled more efficiently than the optical amplifying apparatus 10 of the first embodiment by being absorbed by the heat pipe 21, the light due to deterioration of the resin coating of the amplifying optical fiber 22 A decrease in amplification effect can be prevented. In addition, since the heat pipe 21 only needs to cool the heat dissipating part 23 provided at one end 21a thereof, a large cooling fan becomes unnecessary, and the energy required for cooling can be reduced as compared with the conventional case. In addition, the apparatus can be reduced in size. Furthermore, since only the heat pipe 21 needs to be cooled, the space at the center of the spiral shape of the heat pipe 21 can be used for mounting other components, and this space can be used effectively.

  Hereinafter, the present invention will be described more specifically with experimental examples, but the present invention is not limited to the following experimental examples.

"Experiment 1"
A double clad fiber having a length of 1 m was concentrically wound with a diameter of 100 mm.
Next, 50 W of amplification pump light was input to the wound double clad fiber, and the temperature of the double clad fiber at this time was measured.
The double clad fiber in this state was fixed to a heat sink having a thickness of 40 mm × length of 120 mm × width of 120 mm via a heat conductive resin.
Next, this heat sink was cooled by a cooling fan having a thickness of 32 mm and an outer diameter of 120 mm at an air volume of 2.5 m ³ / min, and the temperature of the double clad fiber at this time was measured and found to be about 80 ° C.
In addition, when the temperature of the double clad fiber was measured by a thermoviewer, the temperature of the double clad fiber near the light output end at the lowest temperature was about 50 ° C., and the double clad fiber near the light input end at the highest temperature Was about 80 ° C., and the temperature difference between the light output end and the light input end was about 30 ° C.

"Experimental example 2"
A heat pipe having a thickness of 6 mm and a length of 500 mm processed into a circle having a diameter of 100 mm was prepared.
Next, four aluminum plates having a thickness of 1 mm × length of 60 mm × width of 60 mm were attached to one end of the heat pipe at intervals of 5 mm as heat radiating fins.
Next, a double clad fiber having a length of 1 m was wound concentrically with a diameter of 100 mm.
Next, the wound double clad fiber was fixed to the surface of the heat pipe via a heat conductive resin.
Next, 50 W of amplification pump light was input to the double-clad fiber, and the temperature of the double-clad fiber at this time was measured.
Next, the heat dissipating fin of the heat pipe was cooled by a cooling fan having a thickness of 32 mm and an outer diameter of 60 mm at an air volume of 1.2 m ³ / min, and the temperature of the double clad fiber at this time was measured. there were.
In addition, when the temperature of the double clad fiber was measured by a thermoviewer, the temperature of the double clad fiber near the light output end at the lowest temperature was about 50 ° C., and the double clad fiber near the light input end at the highest temperature Was about 60 ° C., and the temperature difference between the light output end and the light input end was about 10 ° C.

"Experiment 3"
A heat pipe having a length of 1 m was processed so as to form a spiral shape. At this time, the diameter of the spiral circle was 100 mm.
Next, an aluminum plate having a size of 60 mm in length and 60 mm in width was attached as a heat radiating fin to one end of the heat pipe.
Next, a double clad fiber having a length of 1 m was arranged along the spiral shape of the heat pipe and in contact with the surface of the heat pipe.
Next, 50 W of amplification pump light was input to the double clad fiber, and the temperature of the double clad fiber at this time was measured.
Next, the heat dissipating fins of the heat pipe were cooled by a cooling fan having an outer diameter of 60 mm, and the temperature of the double clad fiber at this time was measured and found to be about 60 ° C.
In addition, when the temperature of the double clad fiber was measured by a thermoviewer, the temperature of the double clad fiber near the light output end at the lowest temperature was about 50 ° C., and the double clad fiber near the light input end at the highest temperature Was about 60 ° C., and the temperature difference between the light output end and the light input end was about 10 ° C.

Based on the above results, the double clad fiber was placed in contact with the heat pipe, and the cooling fin provided at one end of the heat pipe was cooled with a cooling fan, thereby cooling the double clad fiber using a heat sink. It was also found that the double clad fiber can be cooled efficiently.
When the heat sink is used in Experimental Example 1, the heat sink volume 576 cm ³ (120 mm × 120 mm × 40 mm) and the cooling fan volume about 361 cm ³ (3.14 × 60 mm × 60 mm × 32 mm) are combined. Approximately 937 cm ³ of space was required.
On the other hand, when a heat pipe is used in Experimental Example 2, the volume of the heat pipe is about 14 cm ³ (3.14 × 3 mm × 3 mm × 500 mm), and the space for four aluminum plates is about 68 cm ³ (60 mm × 60 mm × 19 mm) and a cooling fan volume of about 90 cm ³ (3.14 × 30 mm × 30 mm × 32 mm) required a space of about 172 cm ³ .
Therefore, in Experimental Example 2, the space required for cooling the double clad fiber can be set to 1/5 or less of Experimental Example 1.

It is a schematic block diagram which shows 1st embodiment of the optical amplifier of this invention. It is a schematic block diagram which shows 2nd embodiment of the optical amplifier of this invention. It is a schematic sectional drawing which shows an example of the structure which fixes the optical fiber for amplification to a heat pipe in 2nd embodiment of the optical amplifier of this invention. FIG. 6 is a schematic perspective view showing another example of a structure for fixing an amplification optical fiber to a heat pipe in the second embodiment of the optical amplification device of the present invention. It is a schematic sectional drawing which shows the example which has arrange | positioned the several heat pipe so that one optical fiber for amplification may be enclosed in 2nd embodiment of the optical amplifier of this invention. In 2nd embodiment of the optical amplification apparatus of this invention, it is a schematic sectional drawing which shows the example which penetrated the optical fiber for amplification in the hollow part provided along the axial direction of the heat pipe.

Explanation of symbols

DESCRIPTION OF SYMBOLS 10,20 ... Optical amplifier, 11,21 ... Heat pipe, 12, 22 ... Amplifying optical fiber, 13, 23 ... Radiating part, 14, 24 ... Cooling fan.

Claims (7)

  A heat pipe having a substantially circular shape, an amplification optical fiber wound in a concentric manner in a shape substantially equal to the curved shape of the heat pipe, and disposed so as to contact the heat pipe; An optical amplifying apparatus comprising: a heat dissipating part provided at one end of the heat pipe.   A heat pipe having a spiral shape, an amplification optical fiber disposed along the spiral shape of the heat pipe and in contact with the heat pipe, and a heat radiating portion provided at one end of the heat pipe And an optical amplifying device.   3. The optical amplifying device according to claim 1, wherein an optical output end portion of the amplification optical fiber is disposed on a heat radiating portion side of the heat pipe.   4. The optical amplifying device according to claim 2, wherein the optical input end of the amplification optical fiber is disposed below the optical output end of the amplification optical fiber in the direction of gravity.   5. The groove according to claim 1, wherein a groove-like recess extending along the axial direction is provided on the surface of the heat pipe, and the amplification optical fiber is accommodated in the recess. The optical amplifying device described.   5. The optical amplifying device according to claim 2, wherein a plurality of heat pipes are disposed so as to surround the optical fiber for amplification. The axial direction of the said heat pipe is provided with the hollow part in the center, The said optical fiber for amplification was penetrated in this hollow part, The any one of Claim 2 thru | or 4 characterized by the above-mentioned. Optical amplification device.

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