Tunable Laser

20220077646 · 2022-03-10

    Inventors

    Cpc classification

    International classification

    Abstract

    A wavelength tunable laser includes a filter region having a wavelength selection function on light from a gain region, wherein the filter region is a Sagnac interferometer and includes two ring resonators. The ring resonator has two optical couplers, and first and second curved waveguides that connect the two optical couplers and lengths of which equal to each other, each of the two optical couplers is configured to receive input of the light from the gain region through the input-output port, to couple light of a resonant peak to a bar port of the input-output port, and to couple light except light at a resonant peak wavelength to a cross port of the input-output port, and the first curved waveguide connects the bar ports of the input-output ports of the two optical couplers, and the second curved waveguide connects the cross ports of ports, of the two optical couplers, that the first curved waveguide is connected to.

    Claims

    1. A wavelength tunable laser comprising a filter region having a wavelength selection function on light from a gain region, wherein the filter region is a Sagnac interferometer that functions as a loop mirror, and includes two ring resonators, the ring resonator has two optical couplers, and first and second curved waveguides connecting the two optical couplers, each of the two optical couplers is configured to receive input of the light from the gain region through an input-output port, to split the light into light of a resonant peak and light except light at a resonant peak wavelength, to couple the light of the resonant peak to a bar port of the input-output port, and to couple the light except the light at the resonant peak wavelength to a cross port of the input-output port, and the first curved waveguide connects the bar ports of the input-output ports of the two optical couplers, and the second curved waveguide connects the cross ports of ports, of the two optical couplers, that the first curved waveguide is connected to, the wavelength tunable laser comprising inside a loop of the ring resonator, two radiation waveguides that are connected to the cross ports of the input-output ports of the two optical couplers and discard the light except the light at the resonant peak wavelength, wherein a length of the first curved waveguide and a length of the second curved waveguide equal to each other.

    2. The wavelength tunable laser according to claim 1, wherein each of the two optical couplers is configured such that a ratio of the light, except the light at the resonant peak wavelength, that is coupled to the radiation waveguide is higher than a ratio of the light, of the resonant peak, that is coupled to the first curved waveguide.

    3. The wavelength tunable laser according to claim 1, wherein the optical coupler is a multimode interference coupler.

    4. The wavelength tunable laser according to claim 1, wherein the optical coupler is a directional coupler.

    5. The wavelength tunable laser according to claim 2, wherein the optical coupler is a multimode interference coupler.

    6. The wavelength tunable laser according to claim 2, wherein the optical coupler is a directional coupler.

    7. The wavelength tunable laser according to claim 3, wherein the optical coupler is a directional coupler.

    Description

    BRIEF DESCRIPTION OF DRAWINGS

    [0016] FIG. 1 is a diagram for explaining a conventional wavelength tunable laser.

    [0017] FIG. 2 is a schematic diagram of a sectional view of a high mesa optical waveguide.

    [0018] FIG. 3 is an expanded view of the portion of a ring resonator having MMI couplers with 50:50 of coupling efficiency.

    [0019] FIG. 4 is an expanded view of the portion of a ring resonator having MMI couplers with 85:15 of coupling efficiency.

    [0020] FIG. 5 is an expanded view of the portion of a ring resonator of a wavelength tunable laser according to an embodiment of the present invention.

    [0021] FIG. 6 is an expanded view of the portion of a ring resonator according to Embodiment 1.

    DESCRIPTION OF EMBODIMENTS

    [0022] Embodiments of the invention as claimed in the present application will be hereafter described with reference to the drawings. It is supposed that the same or similar reference numerals denote the same or similar elements, and their duplicated description is omitted.

    [0023] As having been described with reference to FIG. 2 and FIG. 3, in the present embodiment, high mesa optical waveguides, which can realize steep bending radii, are used for a ring waveguide connecting 2×2 optical couplers constituting a ring resonator together. Moreover, MMI optical couplers, which can be easily produced and are low in loss, are used for the 2×2 optical couplers. Although in order to reduce a resonator length L, the lengths of optical coupling units (optical coupling lengths) need to be reduced, known directional couplers constituted of high mesa optical waveguides have some problem in terms of their production. High mesa optical waveguides are small in leakage of light in the traverse direction due to a large specific refractive index relative to the air. While when directional couplers constituted of such high mesa optical waveguides are used for the optical coupling units, the distance between the two high mesa optical waveguides accordingly needs to be 0.1 micrometers or less in order to reduce the optical coupling lengths, a deep trench (its depth is typically three to four micrometers) having about 0.1 micrometers of width is very difficult to form by means of etching or the like in terms of its processing.

    [0024] While MMI optical couplers have an advantage as described above, they have a disadvantage that each of them can obtain only a fixed optical coupling efficiency. In the case of 2×2 MMI optical couplers used for a ring resonator, a length L.sub.MMI, of an MMI optical coupler, which defines an optical coupling efficiency of light entering an input port to a cross port is expressed by expression (1) below.

    [00001] Math . 1 L MMI = M n eq ( 2 W w g + W gap ) 2 λ ( Expression 1 )

    [0025] Herein, n.sub.eq is an equivalent refractive index, W.sub.wg is the width of an input-output waveguide, W.sub.gap is a distance between input-output waveguides, and λ is a wavelength used. In the case of a 50% MMI coupler, by setting M in the expression to 2, an input optical field is equally split, and it operates as a coupler with 50% of coupling efficiency. The ring resonator has a feature that at an optical coupling unit thereof, a smaller optical coupling efficiency to the cross port leads to more improvement of the finesse. Namely, this leads to more circulations of the light in the ring resonator, sharper resonance thereof, and more improvement of wavelength selection performance. Therefore, by changing a splitting ratio from 50%, it is adjusted such that more light circulates in the ring.

    [0026] FIG. 4 shows an expanded view of the portion of the ring resonator in the case where MMI optical couplers with 85% of coupling efficiency are used. By setting M in expression (1) to 3, 85% of light input to the MMI coupler can be coupled to the bar port. In this case, the length of each MMI optical coupler however is three halves of that of the 50% MMI coupler, and the ratio of the length of the MMI optical couplers relative to the resonator length (length of the waveguides constituting the ring resonator) is high. Accordingly, the optical waveguides connecting the MMI couplers need to be short, and small bending radii are required for the curved waveguides. Since the aforementioned influence is especially large on a ring resonator with a wide FSR, FSRs that can be provided are limited.

    [0027] Therefore, the present embodiment employs a structure using MMI optical couplers with 15% of coupling efficiency, and in the structure, the bar ports are connected together unlike a structure which is generally used for a conventional ring resonator and in which the cross ports of MMI optical couplers are connected together.

    [0028] FIG. 5 shows a configuration of a ring resonator 500 of the present embodiment in which MMI optical couplers with 15% of coupling efficiency are used. The ring resonator 500 includes two MMI optical couplers 50 and 51 each having two inputs and two outputs, and curved waveguides 56 and 57 connecting the two MMI optical couplers 50 and 51. Moreover, the ring resonator 500 further includes a linear waveguide for optical input and a light discarding waveguide 510a which are connected to the MMI optical coupler 51, and a linear waveguide for optical output and a light discarding waveguide 510b which are connected to the MMI optical coupler 50.

    [0029] The linear waveguide for optical input is connected to a first input-output port 52 of the MMI optical coupler 51. The curved waveguide 56 is connected to a bar port 54 with respect to the first input-output port 52 of the MMI optical coupler 51, and a bar port 55 with respect to a first input-output port 53 of the MMI optical coupler 50. The linear waveguide for optical output is connected to a bar port 53 with respect to the first input-output port 55 of the MMI optical coupler 50. The curved waveguide 57 is connected to a cross port 509 with respect to the first input-output port 55 of the MMI optical coupler 50, and a second input-output port 508 of the MMI optical coupler 51. The light discarding waveguide 510a is connected to a cross port 58 with respect to the first input-output port 52 of the MMI optical coupler 51 (bar port with respect to the second input-output port 508). The light discarding waveguide 510b is connected to a second input-output port 59 of the MMI optical coupler 50.

    [0030] For the MMI optical couplers 50 and 51, by setting M in expression (1) to 1, 15% of light input to the MMI coupler is coupled to the bar port. When 15% of the light is coupled to the bar port of the MMI optical coupler, 85% of the light is connected to the cross port, hence, the cross ports of the MMI optical couplers are connected together with the waveguides to form a ring resonator, and the waveguide of the cross port from an input 1 is set to be a discarding waveguide inside the ring resonator.

    Embodiment 1

    [0031] FIG. 6 is a configuration diagram of a ring resonator 600 according to Embodiment 1. The waveguide for the input 1 is input to the 15:85 MMI optical coupler 51, 15% of light is coupled to a ring waveguide of the ring resonator 600 (curved waveguide 56), and 85% of the light is coupled to a discarding waveguide inside the ring resonator (light discarding waveguide 510a). In the structure of the ring resonator, the curved waveguide 56 connecting the MMI coupler 51 and the MMI coupler 50 together connects the outer ports 54 and 55 of the respective MMI couplers together, and the curved waveguide 57 connecting the MMI coupler 50 and the MMI coupler 51 together connects the inner ports 509 and 508 of the respective MMI couplers together. Bending radii are adjusted as to the two curved waveguides 56 and 57 to make lengths of those equal to each other. Thereby, both portions on the curved waveguide 57 side and the curved waveguide 56 side relative to the MMI couplers 51 and 50 of the ring resonator 600 are maintained to be symmetric, and fluctuation, in interference, which occurs due to production errors and the like can be reduced.

    REFERENCE SIGNS LIST

    [0032] 1 Monolithically integrated wavelength tunable laser [0033] 10a, 10b Curved waveguide [0034] 11, 12 Linear waveguide [0035] 13 Input-output waveguide [0036] 14, 15 Optical coupling unit [0037] 16 Optical splitting and combining unit [0038] 17, 18 2×2 optical coupler [0039] 19 1×2 optical coupler [0040] 2 High mesa optical waveguide [0041] 20 Substrate [0042] 22 Lower cladding [0043] 23 Core layer [0044] 24 Upper cladding [0045] 25a Upper electrode [0046] 25b Lower electrode [0047] 3, 4 Ring resonator [0048] 40, 41 2×2 optical coupler [0049] 50, 51 MMI optical coupler with 15:85 of splitting ratio [0050] 500 Ring resonator [0051] 52, 55 First input-output port [0052] 53, 54 Bar port [0053] 56, 57 Curved waveguide [0054] 58, 509 Cross port [0055] 59, 508 Second input-output port [0056] 510a, 510b Light discarding waveguide