WO2023204305A1

WO2023204305A1 - Polarization direction discriminator, dual output laser, and polarization direction discrimination method

Info

Publication number: WO2023204305A1
Application number: PCT/JP2023/015918
Authority: WO
Inventors: ジイヨンセット; 康太宇山; 真司山下
Original assignee: 国立大学法人東京大学
Priority date: 2022-04-21
Filing date: 2023-04-21
Publication date: 2023-10-26
Also published as: JP2023160233A

Abstract

The purpose of the present invention is to provide a polarization direction discriminator that exhibits asymmetric transparency in accordance with the polarization direction of propagated light. This polarization direction discriminator 10 comprises: a first Faraday rotator 11 that is between a first port PO1 provided to one end of the discriminator and a second port PO2 provided to the other end, and is disposed on the first port PO1 side; a second Faraday rotator 12 that is between the first port PO1 and the second port PO2, and is disposed on the second port PO2 side; and a polarization selection device 15 that includes a polarizing plate 14 as an optical element disposed between the first Faraday rotator 11 and the second Faraday rotator 12, and that limits the passage of one among first intermediate polarized light P12, P23 and second intermediate polarized light P22, P13 incident on the polarizing plate 14.

Description

Polarization direction discriminator, dual output laser, and polarization direction discrimination method

The present invention relates to a polarization direction discriminator having reversible transparency depending on the polarization direction and propagation direction, a dual output laser using the same, and a polarization direction discrimination method.

As an optical device related to a polarization direction discriminator, there is an isolator that allows only light propagating in one direction to pass through. As this type of isolator, for example, there is an isolator having a structure in which a pair of polarizers set in orthogonal polarization directions are arranged outside a Faraday rotator that rotates the polarization direction by 45 degrees. Note that in order to maintain the polarization direction, a 1/2 wavelength plate may be placed between the Faraday rotator and one polarizer.

Since the isolator as described above transmits light from one direction and blocks light from the other direction, it becomes impossible to utilize light from the other direction.

As a mode-locked laser that generates high-intensity short pulses, one that forms a dual asynchronous pulse, that is, a dual frequency comb, whose components are two orthogonal polarized lights is known (for example, see Non-Patent Documents 1 and 2). ).

However, in Non-Patent Document 1, a general isolator is incorporated in the fiber resonator ring, and it is not easy to stably and efficiently extract the dual frequency comb.

The present invention has been made in view of the above-mentioned background art, and an object of the present invention is to provide a polarization direction discriminator that exhibits asymmetric transparency depending on the polarization direction of propagating light.

An object of the present invention is to provide a dual output laser that can efficiently extract a dual frequency comb using a polarization direction discriminator as described above.

In order to achieve the above object, the polarization direction discriminator according to the present invention is a polarization dependent device, between a first port provided at one end and a second port provided at the other end, A first Faraday rotator disposed on the first port side, a second Faraday rotator disposed on the second port side between the first port and the second port, the first Faraday rotator and the second Faraday rotator. and a polarization selection device including an optical element disposed between the rotator and the polarization selection device for restricting passage of one of the first intermediate polarized light and the second intermediate polarized light incident on the optical element.

In order to achieve the above object, the dual output laser according to the present invention includes a polarization-maintaining ring-shaped resonator, an optical gain section disposed in the resonator, and a light beam that propagates into the resonator in the first round direction. a first light supply section that supplies the first polarized light so as to propagate in the second rotation direction to the resonator, a second light supply section that supplies the second polarized light so as to propagate in the second circulation direction, and the above-mentioned polarization direction discriminator. .

In order to achieve the above object, a polarization direction discrimination method according to the present invention is a polarization direction discrimination method in which first polarized light and second polarized light are transmitted through a pair of Faraday rotators and a polarization selection device, and the polarization direction is passing the second polarized light while allowing the first polarized light to pass, and restricting the passing of the first polarized light while allowing the second polarized light incident from the other side to pass.

1A and 1B are conceptual plan views illustrating the polarization direction discriminator of the first embodiment. 2A and 2B are conceptual perspective views illustrating the polarization direction discriminator of the first embodiment. 3A and 3B are conceptual plan views illustrating the polarization direction discriminator of the second embodiment. FIG. 4 is a conceptual diagram illustrating a mode-locked laser according to the third embodiment. FIG. 5 is a diagram illustrating a polarization direction discriminator incorporated in the mode-locked laser shown in FIG. 4. FIG. 6 is a chart showing the optical spectrum of the output of the mode-locked laser shown in FIG. FIG. 7 is a chart showing an output pulse train.

[First embodiment]
Hereinafter, a first embodiment of a polarization direction discriminator according to the present invention will be described with reference to FIGS. 1A, 2A, etc. In FIG. 1 and the like, X, Y, and Z indicate the overall coordinate system, and x and y indicate the local coordinate system of the point of interest. In particular, X and Y correspond to two directions perpendicular to the direction of incidence of light, and Z corresponds to the direction of incidence of light. x and y give coordinates at a point on the optical axis AX, and correspond to two directions perpendicular to the optical axis AX, and z corresponds to a direction parallel to the optical axis AX.

1A shows a case where the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the left side, and FIG. 1B shows the case where the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the right side. A case is shown in which two polarized lights P2 are incident. The upper region AR1 in FIGS. 1A and 1B is described as a state in which the polarization state or polarization direction at each position passing through the polarization direction discriminator 10 is viewed from the left side of the paper along the optical axis AX.

2A shows a case where the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the left side, and FIG. 2B shows the case where the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the right side. A case is shown in which two polarized lights P2 are incident.

The polarization direction discriminator 10 shown in FIGS. 1A, 1B, etc. is a non-reciprocal optical element, more specifically a polarization-dependent non-reciprocal discriminator. Polarization direction discriminator 10 can also be referred to as a polarization dependent device. The polarization direction discriminator 10 includes a first Faraday rotator 11, a polarizing plate 14, and a second Faraday rotator between a first port PO1 on the left side, that is, on the -Z side, and a second port PO2 on the right side, that is, on the +Z side. 12. The first Faraday rotator 11 is arranged on the first port PO1 side, and the second Faraday rotator 12 is arranged on the second port PO2 side. The polarizing plate 14 is an optical element disposed between the first Faraday rotator 11 and the second Faraday rotator 12, and functions alone as the polarization selection device 15.

In the illustrated example, the first port PO1 is not an independent member, but the end surface 11a of the first Faraday rotator 11 also serves as the function. The first port PO1 may be a diaphragm disposed adjacent to the end surface 11a of the first Faraday rotator 11. Furthermore, a lens may be added to the first port PO1 to adjust the condensing state of light.

The second port PO2 is not an independent member, but the end surface 12a of the second Faraday rotator 12 also serves this function. The second port PO2 may be a diaphragm disposed adjacent to the end surface 12a of the second Faraday rotator 12. Further, a lens may be added to the second port PO2 to adjust the condensing state of light.

The first Faraday rotator 11 includes a block-shaped ferromagnetic crystal 11i and a magnet 11j that forms a magnetic field B1 in the ferromagnetic crystal 11i. The magnetic field B1 formed in the ferromagnetic crystal 11i is directed in the -Z direction. The ferromagnetic crystal 11i has a pair of

flat end faces

11a and 11b, and when linearly polarized light passes through the ferromagnetic crystal 11i, the polarization direction of the linearly polarized light changes regardless of the angle of the polarization direction at the time of incidence. Rotate 45°. Specifically, when the first polarized light P1 and the second polarized light P2 enter from the left end surface 11a and pass through the ferromagnetic crystal 11i, the polarization directions are rotated by 45° counterclockwise when viewed from the -Z side. Although not shown, even if the first polarized light P1 and the second polarized light P2 pass through the ferromagnetic crystal 11i from opposite directions, the polarized light directions are rotated by 45° counterclockwise when viewed from the -Z side.

The second Faraday rotator 12 includes a block-shaped ferromagnetic crystal 12i and a magnet 12j that forms a magnetic field B2 in the ferromagnetic crystal 12i. The magnetic field B2 formed in the ferromagnetic crystal 12i is directed in the +Z direction. The ferromagnetic crystal 12i has a pair of

flat end faces

12a and 12b, and when linearly polarized light passes through the ferromagnetic crystal 12i, the polarization direction of the linearly polarized light changes regardless of the angle of the polarization direction at the time of incidence. Rotate 45°. Specifically, when the first polarized light P1 and the second polarized light P2 enter from the right end surface 12a and pass through the ferromagnetic crystal 12i, the polarization directions are rotated by 45° clockwise when viewed from the -Z side. Although not shown, even if the first polarized light P1 and the second polarized light P2 pass through the ferromagnetic crystal 12i from opposite directions, the polarized light directions are rotated by 45° clockwise when viewed from the -Z side.

The polarizing plate 14 is an absorption type polarizer, and limits the light passing through the polarizing plate 14 to linearly polarized light in a specific polarization direction. The polarizing plate 14 is a polarizing film obtained by stretching a polymeric material containing an iodine compound or a dye in a specific direction, for example, and adhered to a parallel plate substrate. The polarization axis of the polarizing plate 14 is set between the -x direction and the +y direction, and forms an angle of 45° with respect to both the -x direction and the +y direction. The polarization axis of the polarizing plate 14 is inclined by 45 degrees with respect to the polarization direction of the first polarized light P1 and the second polarized light P2 that are input to the first Faraday rotator 11 and the second Faraday rotator 12. The polarizing plate 14 is not limited to an absorption type, and can be replaced with a polarizing beam splitter incorporating a dielectric multilayer film, for example. In this case, unnecessary light is branched out of the optical path.

Although the explanation has been omitted above, an anti-reflection film can be formed on the end faces 11a and 11b of the first Faraday rotator 11, and an anti-reflection film can be formed on the end faces 12a and 12b of the other second Faraday rotator 12. A film can be formed. Further, an antireflection film can also be formed on the surface of the polarizing plate 14.

The operation of the polarization direction discriminator 10 will be described with reference to FIGS. 2A and 2B. In FIGS. 2A and 2B, the sine waveform E1 drawn in the first Faraday rotator 11 or before and after the first Faraday rotator 11 indicates the oscillation of the electric field of the first polarized light P1 and the polarized light derived from this, and the sine waveform E2 , which shows the oscillation of the electric field of the second polarized light P2 and the polarized light derived therefrom.

In the case of FIG. 2A, the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the left side. Here, the first polarized light P1 is linearly polarized light having a plane of polarization parallel to the Y direction, that is, the y direction, and the second polarized light P2 is linear polarized light having a plane of polarization parallel to the X direction, that is, the x direction. The polarization direction of the first polarized light P1 and the polarization direction of the second polarized light P2 are orthogonal to each other. When the first polarized light P1 and the second polarized light P2 pass through the first Faraday rotator 11, the planes of polarization are rotated counterclockwise by 45 degrees. In other words, the first polarized light P1 has a polarization plane in a −45° inclined direction, which is rotated by 45° counterclockwise with respect to the +y direction. This state is called first intermediate polarized light P12. On the other hand, the second polarized light P2 has a polarization plane in a +45° inclined direction, which is rotated 45° clockwise with respect to the +y direction. This state is called second intermediate polarized light P22. The first intermediate polarized light P12 originating from the first polarized light P1 and the second intermediate polarized light P22 originating from the second polarized light P2 enter the polarizing plate 14. The polarization direction of the first intermediate polarized light P12 derived from the first polarized light P1 coincides with the polarization axis of the polarizing plate 14, and passes through the polarizing plate 14 with low loss. On the other hand, the polarization direction of the second intermediate polarized light P22 originating from the second polarized light P2 is perpendicular to the polarization axis of the polarizing plate 14, and is absorbed and blocked by the polarizing plate 14. The polarizing plate 14 has a role of relatively suppressing passage of the second intermediate polarized light P22, which is one of the first intermediate polarized light P12 and the second intermediate polarized light P22. After passing through the polarizing plate 14, the first intermediate polarized light P12 enters the second Faraday rotator 12 from the end surface 12b side. When the first intermediate polarized light P12 passes through the second Faraday rotator 12, the plane of polarization is rotated by 45° clockwise. As a result, the first Faraday rotator 11 and the second Faraday rotator rotate the polarization direction by 45° in opposite directions. In other words, the first intermediate polarized light P12 changes from a state where the direction is tilted at -45° to a state where it has a polarization plane parallel to the +y direction, and is returned to the original state of the first polarized light P1. As a result, the first polarized light P1 passes through the polarization direction discriminator 10 in one direction, that is, the +Z direction, while maintaining its polarization state. The second polarized light P2 cannot pass through the polarization direction discriminator 10 and is blocked.

In the case of FIG. 2B, the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the right side. When the first polarized light P1 and the second polarized light P2 pass through the second Faraday rotator 12, the planes of polarization are rotated by 45° clockwise. That is, the first polarized light P1 has a polarization plane in a +45° inclined direction, which is rotated by 45° clockwise with respect to the +y direction. This state is called second intermediate polarized light P13. On the other hand, the second polarized light P2 has a polarization plane tilted at −45°, which is rotated by 45° counterclockwise with respect to the +y direction. This state is called first intermediate polarized light P23. The second intermediate polarized light P13 derived from the first polarized light P1 and the first intermediate polarized light P23 derived from the second polarized light P2 enter the polarizing plate 14. The polarization direction of the first intermediate polarized light P23 derived from the second polarized light P2 matches the polarization axis of the polarizing plate 14, and passes through the polarizing plate 14 with low loss. On the other hand, the polarization direction of the second intermediate polarized light P13 derived from the first polarized light P1 is perpendicular to the polarization axis of the polarizing plate 14, and is absorbed and blocked by the polarizing plate 14. The polarizing plate 14 has a role of relatively suppressing passage of the second intermediate polarized light P13, which is one of the first intermediate polarized light P23 and the second intermediate polarized light P13. After passing through the polarizing plate 14, the first intermediate polarized light P23 enters the first Faraday rotator 11 from the end surface 11b side. When the first intermediate polarized light P23 passes through the first Faraday rotator 11, the plane of polarization is rotated counterclockwise by 45 degrees. In other words, the first intermediate polarized light P23 changes from a state in which the direction is tilted at -45° with respect to the +y direction to a state in which it has a polarization plane parallel to the -x direction, and is returned to the second polarized light P2 in the original state. As a result, the second polarized light P2 passes through the polarization direction discriminator 10 in the other direction, i.e., the -Z direction, while maintaining its polarization state. The first polarized light P1 cannot pass through the polarization direction discriminator 10 and is blocked.

In FIGS. 2A and 2B, the first Faraday rotator 11 and the second Faraday rotator 12 rotate the polarization direction by 45° in opposite directions. As a result, the transmittance of the first polarized light P1 incident from the first port PO1 side and the second polarized light P2 incident from the second port PO2 side can be increased.

The polarization direction discriminator 10 of the first embodiment described above is located between the first port PO1 provided at one end and the second port PO2 provided at the other end, and is located on the first port PO1 side. a first Faraday rotator 11 disposed between the first Faraday rotator 11 and a second Faraday rotator 12 disposed between the first port PO1 and the second port PO2 and on the second port PO2 side; It includes a polarizing plate 14 as an optical element disposed between the two Faraday rotators 12, and restricts the passage of one of the first intermediate polarized light P12, P23 and the second intermediate polarized light P22, P13 incident on the polarizing plate 14. A polarization selection device 15 is provided.

In the polarization direction discriminator, the polarization selection device 15 restricts the passage of one of the second intermediate polarized lights P22 and P13 that enters the polarizing plate 14, so that the first polarized light P1 that enters from the first port PO1 side is selectively transmitted. It is now possible to selectively pass the second polarized light P2 incident from the second port PO2 side, and force the two types of polarized light P1 and P2 to propagate in opposite directions. It becomes easier to realize.

The polarization direction discrimination method in the first embodiment is a polarization direction discrimination method in which the first polarized light P1 and the second polarized light P2 are transmitted through a pair of

Faraday rotators

11 and 12 and the polarization selection device 15, and the polarized light is incident from one side. Passage of the second polarized light P2 is restricted while allowing the first polarized light P1 to pass, and passage of the first polarized light P1 is restricted while allowing the second polarized light P2 incident from the other side to pass.

[Second embodiment]
The polarization direction discriminator of the second embodiment will be described below. Note that the polarization direction discriminator of the second embodiment is a modification of the device of the first embodiment, and is the same as the first embodiment with respect to parts not particularly described.

3A shows a case where the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the left side, and FIG. 3B shows the case where the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the right side. A case is shown in which two polarized lights P2 are incident. The upper and lower regions AR1 and AR2 in FIGS. 2A and 2B describe the polarization state or polarization direction at each position passing through the polarization direction discriminator 10 as seen from the left side of the paper along the optical axis AX. It is. In this case, the plane of the paper extends parallel to an intermediate direction that is parallel to the Z axis and at an angle of 45° to the X and Y directions.

The polarization direction discriminator 10 has a birefringent element 14a instead of the polarizing plate 14 as an optical element between the first Faraday rotator 11 and the second Faraday rotator 12. The polarization direction discriminator 10 includes a first diaphragm 14b located outside the first Faraday rotator 11 and a second diaphragm 14c located outside the second Faraday rotator 12. Here, "inner" with respect to the first Faraday rotator 11 and the second Faraday rotator 12 means between the

Faraday rotators

11 and 12. The birefringent element 14a functions as a polarization selection device 115 in combination with the first aperture 14b and the second aperture 14c.

The birefringent element 14a is a birefringent prism whose optical axis 14p extends in a direction parallel to the plane of the paper and inclined at a predetermined angle with respect to the optical axis AX. The S-polarized light (polarization direction component perpendicular to the paper) that is perpendicularly incident on the first surface 14g of the birefringent element 14a from the left side of the paper propagates as an ordinary ray, traveling straight in the direction perpendicular to the first surface 14g, and becomes complex. P-polarized light (polarization direction component parallel to the paper) that is perpendicularly incident on the first surface 14g of the refractive element 14a from the left side of the paper is deflected from the optical axis AX in a direction oblique to the first surface 14g as an extraordinary ray. propagate. The S-polarized light that is perpendicularly incident on the second surface 14h of the birefringent element 14a from the right side of the paper propagates as an ordinary ray in a direction perpendicular to the first surface 14h, and is transmitted to the second surface 14h of the birefringent element 14a. The P-polarized light incident perpendicularly from the right side of the page propagates as an extraordinary ray in a direction oblique to the second surface 14h, deviating from the optical axis AX.

The first diaphragm 14b has an aperture 14o, and passes the first polarized light P1 and the second polarized light P2 that are incident from the left side of the paper along the optical axis AX and its vicinity. The second diaphragm 14c has an aperture 14o, and passes the first polarized light P1 and the second polarized light P2 that are incident from the right side of the paper along the optical axis AX and its vicinity.

In the case of FIG. 3A, the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the left side. Here, the first polarized light P1 is linearly polarized light having a plane of polarization parallel to the Y direction, that is, the y direction, and the second polarized light P2 is linear polarized light having a plane of polarization parallel to the X direction, that is, the x direction. The polarization direction of the first polarized light P1 and the polarization direction of the second polarized light P2 are orthogonal to each other. The first polarized light P1 and the second polarized light P2 that have passed through the aperture 14o of the first diaphragm 14b pass through the first Faraday rotator 11, so that their polarization directions are rotated counterclockwise by 45 degrees. In other words, the first polarized light P1 becomes the first intermediate polarized light P12, which is rotated 45° counterclockwise and has a polarization direction in a −45° inclined direction. On the other hand, when the second polarized light P2 passes through the first Faraday rotator 11, the polarization direction is rotated counterclockwise by 45 degrees. In other words, the second polarized light P2 becomes the second intermediate polarized light P22 having a polarization direction in a +45° tilt direction which is rotated by 45° counterclockwise. The first intermediate polarized light P12 originating from the first polarized light P1 and the first intermediate polarized light P22 originating from the second polarized light P2 enter the birefringent element 14a. The polarization direction of the first intermediate polarized light P12 originating from the first polarized light P1 is perpendicular to the plane of the paper, and travels straight through the birefringent element 14a. On the other hand, the polarization direction of the second intermediate polarized light P22 derived from the second polarized light P2 is parallel to the paper surface and deviates from the optical axis AX. The first intermediate polarized light P12 emitted from the birefringent element 14a goes straight along the optical axis AX and enters the second Faraday rotator 12, and the second intermediate polarized light P22 emitted from the birefringent element 14a is a light It is refracted in a direction parallel to the axis AX and enters the second Faraday rotator 12. When the first intermediate polarized light P12 passes through the second Faraday rotator 12, the plane of polarization is rotated by 45° clockwise. As a result, the first Faraday rotator 11 and the second Faraday rotator rotate the polarization direction by 45° in opposite directions. That is, the first intermediate polarized light P12 has a polarization plane parallel to the +y direction from the -45° tilt direction with the +y direction as a reference, and is returned to the original first polarized light P1. As a result, the first polarized light P1 passes through the polarization direction discriminator 10 in one direction, that is, the +Z direction, while maintaining its polarization state. The second intermediate polarized light P22 is returned to the second polarized light P2, but enters outside the aperture 14o of the second aperture 14c and is blocked by the second aperture 14c. That is, the second polarized light P2 cannot pass through the polarization direction discriminator 10 and is blocked.

In the case of FIG. 3B, the first polarized light P1 and the second polarized light P2 enter the polarization direction discriminator 10 from the right side. The first polarized light P1 and the second polarized light P2 that have passed through the aperture 14o of the second diaphragm 14c pass through the second Faraday rotator 12, so that their polarization directions are rotated by 45 degrees clockwise. In other words, the first polarized light P1 becomes the second intermediate polarized light P13 having a polarization direction in a +45° tilt direction which is rotated by 45° clockwise. On the other hand, when the second polarized light P2 passes through the second Faraday rotator 12, the polarization direction is rotated by 45° clockwise. In other words, the second polarized light P2 becomes the first intermediate polarized light P23 having a polarization direction in a -45° tilt direction which is rotated by 45° counterclockwise. The second intermediate polarized light P13 derived from the first polarized light P1 and the first intermediate polarized light P23 derived from the second polarized light P2 enter the birefringent element 14a. The polarization direction of the second intermediate polarized light P13 derived from the first polarized light P1 is parallel to the paper surface and deviates from the optical axis AX. On the other hand, the polarization direction of the first intermediate polarized light P23 derived from the second polarized light P2 is perpendicular to the plane of the paper, and travels straight through the birefringent element 14a. The first intermediate polarized light P23 emitted from the birefringent element 14a goes straight along the optical axis AX and enters the first Faraday rotator 11, and the second intermediate polarized light P13 emitted from the birefringent element 14a is a light It is refracted in a direction parallel to the axis AX and enters the first Faraday rotator 11. When the first intermediate polarized light P23 passes through the first Faraday rotator 11, the plane of polarization is rotated by -45° counterclockwise. In other words, the first intermediate polarized light P23 has a polarization plane parallel to the +x direction from the −45° tilted direction with the +y direction as a reference, and is returned to the original second polarized light P2. As a result, the second polarized light P2 passes through the polarization direction discriminator 10 in one direction, i.e., the -Z direction, while maintaining its polarization state. The second intermediate polarized light P13 is returned to the first polarized light P1, but enters outside the aperture 14o of the first aperture 14b and is blocked by the first aperture 14b. That is, the first polarized light P1 cannot pass through the polarization direction discriminator 10 and is blocked.

In the polarization direction discriminator 10 of the second embodiment described above, the polarization selection device 115 includes the birefringent element 14a, which is an optical element, and the birefringence element 14a, which is an optical element, and a birefringent element 14a, which is an optical element, and a birefringent element 14a, which is an optical element, and a second port PO1, which is disposed outside the first Faraday rotator 11. 1 aperture 14b, and a second aperture 14c disposed outside the second Faraday rotator 12 as a second port PO2. In the case of the second embodiment, reliable light blocking using the first aperture 14b and the second aperture 14c is possible, and it becomes easy to improve the accuracy of the polarization direction discriminator 10.

[Third embodiment]
A mode-locked laser according to the third embodiment will be described below. Note that the mode-locked laser of the third embodiment incorporates the polarization direction discriminator of the first embodiment or the second embodiment.

The mode-locked laser 100 shown in FIG. 4 is a dual output laser. More specifically, the mode-locked laser 100 is a dual comb laser, and is a dual comb light source that generates two optical frequency combs within a single optical resonator. The mode-locked laser 100 outputs a pair of optical combs having different polarization directions as a dual output laser. The mode-locked laser 100 is a passive mode-locked laser that performs a passive mode-locking operation, and includes a resonator 100a, a polarization direction discriminator 10, an optical amplification section 20, a first transmission adjustment section 31, and a second transmission adjustment section 31. It includes a transmission adjustment section 32 and an output coupler 50. The mode-locked laser 100 includes a polarization-maintaining ring-shaped resonator 100a, an optical amplification section 20, a first transmission adjustment section 31, a second transmission adjustment section 32, a polarization direction discriminator 10, and an output. A coupler 50 is provided, and these are joined by fusion or the like.

In the mode-locked laser 100, the resonator 100a is formed into a ring shape by the optical fiber 2. The optical fiber 2 is a polarization maintaining optical fiber (PMF).

As shown in FIG. 5, the polarization direction discriminator 10 is inserted onto the optical path of the optical fiber 2 of the resonator 100a via the connectors 3a and 3b. The connectors 3a and 3b can include lenses and the like, and can collimate the circulating lights OL1 and OL2. The polarization direction discriminator 10 has a structure illustrated in FIG. 1A and the like. The first Faraday rotator 11, the polarizing plate 14, and the second Faraday rotator 12 constituting the polarization direction discriminator 10 are positioned and fixed in a light-shielding holder 18.

Returning to FIG. 4, the optical amplification section 20 is disposed in the resonator 100a along with the resonator 100a, and includes a first light supply section 21, a second light supply section 22, and a gain fiber 23.

The first light supply section 21 has a first excitation light source 21a and a first multiplexing coupler 21b. The first light supply section 21 supplies the excitation light PL of the first polarized light P1 to the resonator 100a from one direction. The first polarized light P1, that is, the excitation light PL, propagates in the first rotation direction (specifically, in the clockwise direction of the loop of the resonator 100a). The first excitation light source 21a is composed of, for example, a semiconductor laser, and outputs excitation light having a wavelength of, for example, 980 nm. The first multiplexing coupler 21b does not prevent light having a wavelength of, for example, 1550 nm from propagating and circulating in the resonator 100a. The excitation light introduced into the resonator 100a from the first light supply unit 21 excites the dopant added to the doped fiber, which is the gain fiber 23, and enables stimulated emission at the wavelength of the output resonant light.

The second light supply section 22 has a second excitation light source 22a and a second multiplexing coupler 22b. The second light supply section 22 supplies the excitation light PL of the second polarized light P2 to the gain fiber 23 from the other direction. The second polarized light P2, that is, the excitation light PL, propagates in the second circulation direction (specifically, in the counterclockwise direction of the loop of the resonator 100a). The first excitation light source 21a is similar to the first excitation light source 21a, and outputs excitation light having a wavelength of 980 nm, for example. The second multiplexing coupler 22b does not prevent light with a wavelength of, for example, 1550 nm from propagating and circulating in the resonator 100a. The optical fiber extending between the second excitation light source 22a and the second multiplexing coupler 22b has a splice connection 22s, and enables rotation of the polarization direction of the excitation light PL output from the second excitation light source 22a. There is. The excitation light introduced into the resonator 100a from the second light supply section 22 excites the dopant added to the doped fiber, which is the gain fiber 23, and enables stimulated emission at the wavelength of the output resonant light.

The gain fiber 23 is an optical gain section placed in the resonator 100a. The gain fiber 23 is connected in-line to the optical fiber 2 that constitutes the resonator 100a. The gain fiber 23 is a polarization-maintaining optical fiber doped to have an amplification function. Specifically, the gain fiber 23 is a doped fiber doped with a rare earth element such as erbium (Er), and the first circulating light OL1 circulates clockwise around the resonator 100a, and the second circulating light OL1 circulates counterclockwise. The circulating light OL2 is amplified.

The first transmission adjustment section 31 and the second transmission adjustment section 32 are arranged in the resonator 100a, and enable generation of ultrashort pulses using saturable absorption characteristics in which the transmittance changes nonlinearly. The first transmission adjustment section 31 and the second transmission adjustment section 32 have a saturable absorber 30a arranged on the optical path, and carbon nanotubes, graphene, etc. can be used as the saturable absorber 30a.

The output coupler 50 is coupled to the resonator 100a and takes out the first polarized light P1 and the second polarized light P2. Output coupler 50 has two

output ports

51a and 51b and is coupled to resonator 100a. The first output light Q1 is output from the first output port 51a of the output coupler 50 via the first isolator 61 as pulsed light of the second polarization P2, and the second output light Q1 is output from the second output port 51b of the output coupler 50 via the first isolator 61. A second output light Q2 is outputted as a pulsed light of the first polarized light P1.

In the illustrated polarization direction discriminator 10, the first light supply section 21 and the second light supply section 22 are arranged symmetrically with the output coupler 50 in between, and the gain fiber 23, which is an optical gain section, is arranged symmetrically with the output coupler 50 in between. are arranged symmetrically. Further, the first transmission adjustment section 31 and the second transmission adjustment section 32 are arranged symmetrically with the output coupler 50 in between. In this case, the oscillation state can be stabilized, and the first polarized light P1 and the second polarized light P2 can be generated and extracted with high efficiency.

FIG. 6 is a chart showing the optical spectra of the first output light Q1 and the second output light Q2 of the mode-locked laser 100 shown in FIG. 4. Moreover, FIG. 7 is a chart showing pulse trains of the first output light Q1 and the second output light Q2.

FIG. 6 shows the results of measurement using an optical spectrum analyzer with the resolution bandwidth set to 0.05 nm. The 3-dB optical bandwidths of Output 1 of the first output light Q1 and Output 2 of the second output light Q2 are 4.13 nm and 4.52 nm, respectively. FIG. 7 shows a time waveform measured using an oscilloscope, and repetition frequencies of 20.672968 MHz and 20.678468 MHz were observed.

The mode-locked laser 100 shown in FIG. 4 can be used as a dual comb light source, and can be applied to spectroscopy and distance measurement. Dual comb spectroscopy has applications in smart agriculture and biotechnology, allowing for smaller implementation sizes and faster measurement speeds. Dual-com distance measurement is expected to be applied to the fields of autonomous driving and drones, and can improve measurement accuracy and reduce equipment costs.

In FIG. 5, the polarization direction discriminator 10 is expressed as an integrated device, but the first Faraday rotator 11, the polarizing plate 14, and the second Faraday rotator 12 that constitute this are optical fibers, connectors, and lenses. Even if they are separated via other light guide members, if the polarization state is maintained when passing through the light guide members, they will exhibit the desired function as a non-reciprocal optical element regarding polarization.

The mode-locked laser 100, which is a dual output laser according to the third embodiment described above, includes a polarization-maintaining ring-shaped resonator 100a and a gain fiber 23, which is an optical gain section, arranged in the resonator 100a. , a first light supply unit 21 that supplies the first polarized light P1 to the resonator 100a so as to propagate in the first rotation direction, and a first light supply unit 21 that supplies the second polarized light P2 to the resonator 100a so as to propagate in the second rotation direction. It includes a two-light supply unit 22 and the polarization direction discriminator 10 described above.

In the mode-locked laser 100, the first polarized light P1 propagating in one direction in the resonator 100a and the second polarized light P2 propagating in the other direction in the resonator 100a coexist with high efficiency, thereby reducing polarization crosstalk. and can provide a high-power dual-type light source.

〔others〕
Although the present invention has been described above based on the embodiments, the present invention is not limited to the above embodiments. For example, the rotation of the polarization direction by the first Faraday rotator 11 and the second Faraday rotator 12 is not limited to ±45°, but may be ±45°+180°×n (n is a natural number). Further, the rotation of the polarization direction by the

Faraday rotators

11 and 12 does not have to be strictly ±45°.

Furthermore, in the above embodiment, the rotation of the polarization direction by the first Faraday rotator 11 and the second Faraday rotator 12 is not limited to the opposite direction but may be the same rotation direction as long as the resulting rotation amount of the polarization direction is ±45°. can do.

The first Faraday rotator 11 and the second Faraday rotator 12 can be in the form of optical fibers, and the polarization selection device 15 including the polarizing plate 14 can be integrated into the optical fiber 2.

The first transmission adjustment section 31 and the second transmission adjustment section 32 can be made polarization dependent. For example, the first transmission adjustment section 31 can be given a transmission characteristic suitable for the first polarized light P1, and the second transmission adjustment section 32 can be given a transmission characteristic suitable for the second polarized light P2.

The polarization direction discriminator 10 described in the first embodiment and the second embodiment is not limited to the mode-locked laser 100, but also includes a dual-comb laser that forms an optical comb by a method other than mode-locking, such as a waveguide with a nonlinear effect. can be incorporated into a dual comb laser with a cavity of Specifically, optical combs can be formed by inputting continuous light with different wavelengths into a waveguide, or by inputting a single continuous beam into a waveguide and forming an optical comb through a process similar to the Kerr effect. It is conceivable that this may occur.

The polarization direction discriminator 10 can be incorporated into a continuous wave type dual output laser. In this case, continuous oscillation laser output with bidirectionally transmitted polarized waves can be obtained.

Furthermore, in the above embodiment, the resonator 100a includes the optical fiber 2, but the mode-locked laser 100 can also be applied to other waveguide type optical devices that do not use an optical fiber. Examples of waveguide type optical devices include PLC (Photonics Lightwave Circuits), silicon photonics waveguides, and semiconductor waveguides (InP, GaAs, InGaAsP, etc.).

This application claims priority based on Japanese Patent Application No. 2022-70433 filed on April 21, 2022, and the entire disclosure thereof is incorporated herein by reference.

Claims

a first Faraday rotator disposed on the first port side between a first port provided at one end and a second port provided at the other end;
a second Faraday rotator located between the first port and the second port and on the second port side;
an optical element disposed between the first Faraday rotator and the second Faraday rotator, the optical element restricting passage of one of the first intermediate polarized light and the second intermediate polarized light incident on the optical element; A polarization direction discriminator comprising a polarization selection device.
The polarization direction according to claim 1, wherein the polarization selection device includes, as the optical element, a polarizing plate that relatively suppresses passage of one of the first intermediate polarization and the second intermediate polarization. discriminator.
The polarization direction discriminator according to claim 2, wherein the first Faraday rotator and the second Faraday rotator rotate the polarization direction by 45 degrees in opposite directions.
4. The polarizing axis of the polarizing plate is inclined by 45 degrees with respect to the polarization direction of the first polarized light and the polarization direction of the second polarized light that are input to the first Faraday rotator and the second Faraday rotator. Polarization direction discriminator as described.
The polarization selection device includes a birefringent element as the optical element, a first aperture disposed as the first port outside the first Faraday rotator, and an outside as the second Faraday rotator as the second port. The polarization direction discriminator according to claim 1, further comprising a second diaphragm disposed.
The polarization direction discriminator according to claim 5, wherein the first Faraday rotator and the second Faraday rotator rotate the polarization direction by 45 degrees in opposite directions.
A polarization-maintaining ring-shaped resonator,
an optical gain section disposed in the resonator;
a first light supply unit that supplies first polarized light to the resonator so as to propagate in a first rotation direction;
a second light supply unit that supplies second polarized light to the resonator so as to propagate in a second rotation direction;
A dual output laser comprising a polarization direction discriminator according to any one of claims 1 to 6.
further comprising an output coupler coupled to the resonator and extracting the first polarized light and the second polarized light,
The first light supply section and the second light supply section are arranged symmetrically with the output coupler in between,
8. The dual output laser of claim 7, wherein the optical gain section is arranged symmetrically across the output coupler.
The dual output laser according to claim 8, which outputs a pair of optical combs with different polarization directions.
comprising a transmission adjustment section disposed in the resonator,
A first transmission adjuster and a second transmission adjuster constituting a transmission adjustment section are arranged symmetrically with the output coupler in between,
The dual output laser according to claim 9, which is a mode-locked laser that performs passive mode-locked operation.
A polarization direction discrimination method in which first polarized light and second polarized light are transmitted through a pair of Faraday rotators and a polarization selection device,
A polarization direction discrimination method that limits the passage of a second polarized light while allowing the first polarized light incident from one side to pass, and restricts the passage of the first polarized light while passing the second polarized light incident from the other side.
The polarization selection device includes an optical element disposed between the pair of Faraday rotators, and selects one of a first intermediate polarization that enters the optical element from one side and a second intermediate polarization that enters the optical element from the other side. 12. The polarization direction discrimination method according to claim 11, wherein passage of the polarization direction is restricted.
The polarization direction according to claim 12, wherein the polarization selection device includes, as the optical element, a polarizing plate that relatively suppresses passage of one of the first intermediate polarization and the second intermediate polarization. Discrimination method.
The polarization selection device includes a birefringent element as the optical element, a first aperture disposed outside one of the pair of Faraday rotators as a first port, and a second port disposed outside the other of the pair of Faraday rotators as a second port. 13. The polarization direction discrimination method according to claim 12, further comprising a second aperture disposed on the outside.