JP2007256389A - Optical circuit component and optical element - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To improve the resonator Q value, while keeping a resonator volume V very small. <P>SOLUTION: In a photonic crystal optical circuit component 10, a photonic crystal optical resonator 11 is constituted by providing a dielectric thin film slab 12, having a prescribed refractive index and dielectric pillars 13 which are disposed in the dielectric thin film slab 12 and have a refractive index different from that of the dielectric thin film slab 12, and forming a defect where the same refractive index as the dielectric thin film slab 12 is given to an area, equivalent to one dielectric pillar in periodical arrangement of the dielectric pillars 13 in the dielectric thin film slab 12; and dielectric pillars 13a and 13b in an optical waveguide direction of the photonic crystal optical resonator 11, which are adjacent to the defect, are moved from the periodical array to the optical waveguide direction, and diameters of dielectric pillars 14a, 14b, 14c, 14d in a direction orthogonal to the optical waveguide direction, which are adjacent to the defect, are made smaller than those of the other dielectric pillars 13, 13a, 13b. <P>COPYRIGHT: (C)2008,JPO&INPIT

Description

  The present invention relates to an optical circuit component and an optical element, and more particularly to an optical circuit component and an optical element using a photonic crystal.

  In recent years, in order to further improve characteristics such as information amount and communication speed of a high-speed time division multiplexing element system, a wavelength division multiplexing optical element system, and the like, there is an increasing expectation for practical application of optical devices applicable to them. However, current optical devices have not been put into practical use due to problems such as large power consumption and element dimensions compared to electronic devices.

  For example, with respect to all-optical signal processing in the optical node section of the next-generation optical network, an optical buffer memory is an indispensable development component, so that a flip-flop type 1-bit memory using optical bistable has been developed. However, in the present optical device, in order to confine light, a difference in optical refractive index is used as the principle. For this reason, it is difficult to reduce the light confinement region and the element size cannot be reduced, so that there is no prospect for practical use of the flip-flop type 1-bit memory.

  On the other hand, the photonic crystal has a light band structure similar to an electron band structure. Due to this feature, a forbidden band of light (photonic band) appears in a specific structure, so that strong light confinement and group speed delay / control are possible, and the accompanying non-linear effects can be enhanced. Since the photonic crystal can control light based on a completely different concept from the conventional one, there is an increasing expectation for practical application as a new optical circuit component (see, for example, Non-Patent Document 1).

  In recent years, research on microresonators using slab type two-dimensional photonic crystals has been actively conducted as optical circuit components using photonic crystals. In particular, research related to improvement of the resonator Q value (an index of how much light is confined in the resonator) while the microresonator volume V is maintained is performed (for example, see Non-Patent Document 2). ).

Many of these reports employ a structure in which three to four or more air holes or dielectric pillars constituting a photonic crystal are removed to form a microresonator, and in principle, a slab wire waveguide is used. Research results on a one-dimensional photonic crystal resonator having a structure in which air holes are arranged in a line and one air hole is removed have also been reported (see Non-Patent Document 3).
Susumu Noda, Toshihiko Baba, Masaya Naoki, Yuichi Ono, “Current Status and Future Prospects of Photonic Crystal Research-Aiming for a Technology Roadmap (Revised)” Optoelectronic Technology Promotion Association, 2002 Y. Akahane et al, Nature 425, 944-947 (2003) K. Kanamoto et al, IEICE E87-C, 1142-1147 (2004)

However, the conventional microresonator using a photonic crystal has the following problems.
In the two-dimensional photonic crystal optical resonator, since there are a large number of resonator longitudinal modes, the FSR (Free Spectral Range) cannot be increased, and the resonator volume V cannot be decreased. Even if a resonator having a certain Q value can be realized, coupling with the outside is difficult. On the other hand, even with a one-dimensional photonic crystal, the Q value is low, and a thin waveguide structure having a small cross-sectional area is suspended in the air, so that problems such as poor mechanical stability remain.

In general, in order to control the spontaneous emission light in a resonator QED (Quantum ElectroDynamics) and to reduce the threshold of optical bistable operation in nonlinear optics, it is desirable to improve the Q value while keeping the resonator volume V small. That is, it is necessary to reduce V / Q ^{2 in order} to reduce the threshold value of an optical switch using optical bistability. Furthermore, it is important that the electric field amplitude is located in the center of the resonator because the resonator utilizes the maximum interaction between the electric field and the medium.

  From the above viewpoint, it can be said that it is most ideal to remove one air hole or dielectric column as a defect constituting the photonic crystal optical resonator. However, until now, no structure has been obtained in which the Q value is improved while the resonator volume V is kept small. Even if a desired microresonator structure is possible, optical coupling with the outside is difficult.

  The present invention has been made in view of the above points, and provides an optical circuit component and an optical element that are capable of performing light control with high accuracy and that are small in size and excellent in optical coupling with the outside. With the goal.

  In the present invention, in order to solve the above problems, in an optical circuit component using a photonic crystal, a dielectric slab having a predetermined refractive index and a refractive index different from that of the dielectric slab disposed in the dielectric slab are used. And forming a defect in which a region corresponding to one dielectric pillar when the dielectric pillars are periodically arranged in the dielectric slab has the same refractive index as that of the dielectric slab. The resonator is configured to move the dielectric column in the optical waveguide direction of the resonator adjacent to the defect from the periodic arrangement in the optical waveguide direction, and in a direction orthogonal to the optical waveguide direction adjacent to the defect. An optical circuit component is provided in which the diameter of the dielectric pillar is different from the diameter of the other dielectric pillars.

  According to such an optical circuit component, a defect corresponding to one dielectric pillar is formed in the dielectric slab to constitute a photonic crystal optical resonator, and the optical resonator optical waveguide direction adjacent to this defect The dielectric pillars of the dielectric are slightly moved out of the periodic array, and the diameter of the dielectric pillars located perpendicular to the optical waveguide direction adjacent to the defect is different from the diameters of the dielectric pillars forming the other gratings. By doing so, it becomes possible to suppress the leakage of light, and the Q value is improved.

  Further, in the present invention, in an optical element including an optical circuit component using a slab type two-dimensional photonic crystal, a dielectric slab having a predetermined refractive index, and the dielectric slab disposed in the dielectric slab A dielectric column having a different refractive index, and a region corresponding to one dielectric column when the dielectric column is periodically arranged in the dielectric slab has the same refractive index as the dielectric slab. And forming a resonator to form a resonator, moving a dielectric column in the optical waveguide direction of the resonator adjacent to the defect from the periodic arrangement in the optical waveguide direction, and an optical waveguide direction adjacent to the defect; There is provided an optical element comprising an optical circuit component configured such that the diameter of the dielectric pillar in the orthogonal direction is different from the diameter of the other dielectric pillar.

  According to such an optical element, a microresonator having a defect corresponding to one dielectric pillar is used, and leakage of light from the resonator is suppressed, and for example, high performance of an optical element such as an optical switch or an optical memory is improved. Become figured.

According to the present invention, when an optical circuit component is periodically arranged with dielectric pillars in the dielectric slab, a defect in which a region corresponding to one dielectric pillar has the same refractive index as that of the dielectric slab is formed. The dielectric column in the optical waveguide direction of the resonator adjacent to the defect is moved from the periodic arrangement to the optical waveguide direction, and the diameter of the dielectric column in the direction perpendicular to the optical waveguide direction adjacent to the defect is The configuration is different from the diameter of other dielectric pillars. As a result, the resonator volume V can be kept small, a high Q value can be obtained, and the V / Q ² value can be further reduced. Therefore, it is possible to realize a very small optical circuit component that operates with lower energy than before.

  In addition, it becomes possible to improve the performance of an optical element using an optical circuit component including a resonator.

Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.
First, the first embodiment will be described. FIG. 1 is a schematic diagram of the configuration of the photonic crystal optical circuit component according to the first embodiment. FIG. 1 shows a two-dimensional slab type photonic crystal composed of a photonic crystal optical resonator 11 having an extremely small volume corresponding to one lattice defect in a photonic crystal optical circuit component 10 regularly arranged regularly. is there. Photonic crystal optical circuit component 10 in which the refractive index of dielectric thin film slab 12 and dielectric cylinder 13 periodically arranged is 3.4 (semiconductor such as silicon (Si) or gallium arsenide (GaAs)) and 1 (air), respectively. And the dielectric cylinder 13 is assumed to be a true cylinder, and its diameter L is L = 0.6a. The thickness t of the dielectric thin film slab 12 was t = 0.6a, and the upper and lower cladding layers were assumed to be air layers. This structure is usually called an air bridge structure. Further, in the photonic crystal optical resonator 11, the dielectric cylinders 13a and 13b constituting the photonic crystal optical resonator 11 are d = 0.2a in the optical waveguide direction from the periodic arrangement (the circle by the broken line is the periodic arrangement). The diameter L1 of the dielectric cylinders 14a, 14b, 14c, and 14d in the direction perpendicular to the optical waveguide direction adjacent to the lattice defects constituting the photonic crystal optical resonator 11 is L1 = 0.4a.

In general, the Q value, which is a photonic crystal optical resonator performance index in a slab type two-dimensional photonic crystal, can be decomposed into 1 / Q = 1 / Q _v + 1 / Q _h , Q _v is the vertical direction of the slab, Q _h indicates the in-plane direction of the slab. Usually, the photonic crystal optical resonator has a higher Q value as the number of lattice defects forming the resonator increases. The result calculated by the three-dimensional FDTD method (Finite Difference Time Domain: Finite Difference Time Domain Method) shows that the lattice diameter and the periodic arrangement are maintained, and when the Q value is 1 defect, Q = 300 and 2 defects. Q = 1200, 3 defects, Q = 1600, 4 defects, Q = 6300.

In the case of FIG. 1, since the photonic crystal optical resonator 11 is assumed to be independent, Q _h of the dielectric thin film slab 12 is infinite, and Q = Q _v. Therefore, in the same state as the above general example, the photonic crystal optical resonator 11 with one defect is Q = 300, which means that the loss in the vertical direction of the dielectric thin film slab 12 is large. This is because, physically, multiple scattering of light occurs in a narrow region of the photonic crystal optical resonator 11, the wave vector is directed in various directions, and a leakage mode in a higher frequency region than the light line is excited. This means that the scattering loss increases. The light line indicates the minimum frequency at which light can propagate in the medium with respect to the propagation constant, and ω = ck / n (ω: angular frequency, c: speed of light, n: refractive index. , K: wave number). Therefore, by using a lower frequency region than the light line, it is possible to suppress leakage of guided light to the upper and lower cladding layers. Further, the dielectric cylinders 13a and 13b are moved d = 0.2a in the optical waveguide direction from the periodic array with respect to the photonic crystal optical resonator 11 composed of one defect, and the dielectric cylinders 14a, 14b, By changing the diameters of 14c and 14d, the light in the region of the photonic crystal optical resonator 11 is reflected by the dielectric cylinders 13a and 13b and the dielectric cylinders 14a, 14b, 14c and 14d. The phase of the reflected light from the dielectric cylinder 13 is shifted. For this reason, multiple scattering of light in the region of the photonic crystal optical resonator 11 is reduced. As a result, light leakage in the vertical direction of the photonic crystal optical circuit component 10 can be reduced. Actually, when the structure of the photonic crystal optical resonator 11 was calculated using the three-dimensional FDTD method, a value of Q = 28000 was obtained. From this, it can be seen that the leakage of light waves in the vertical direction of the slab is very small. FIG. 2 is a diagram showing frequency characteristics of the photonic crystal optical resonator of FIG. The horizontal axis is the normalized frequency (ωα / 2πc = α / λ, λ: wavelength), and the fundamental resonance frequency peak of the resonator is 0.259.

  Therefore, in the first embodiment, as described above, in the photonic crystal optical resonator 11 composed of one defect, the dielectric cylinders 13a and 13b in the optical waveguide direction are changed from the periodic arrangement to the optical waveguide direction. The diameters of the dielectric cylinders 14a, 14b, 14c, and 14d in the direction perpendicular to the optical waveguide direction adjacent to the lattice defects constituting the photonic crystal optical resonator 11 are slightly different from each other. The diameter of the dielectric cylinder 13 is smaller. As a result, the leakage of light in the vertical direction is reduced, and the Q value can be improved while the resonator volume V is reduced.

The photonic crystal optical circuit component 10 having the above configuration can be applied to, for example, an optical switch or an optical memory.
3 and 4 are diagrams showing a switching principle using a photonic crystal optical resonator. FIG. 3 shows an optical bistable history curve. When light energy is accumulated in the resonator, the refractive index n in the resonator changes according to the relationship n = n ₀ + n ₂ I. Here, n ₀ is the linear refractive index, n ₂ is the third-order nonlinear refractive index, and I is the intracavity light intensity. The above relational expression indicates a change in refractive index due to the so-called optical Kerr effect. When the input power is increased, output light is generated when the changed refractive index satisfies the phase condition in the resonator. This represents that the output power in FIG. 3 shifts from the A value to the B value. When the input power is lowered, the output power shifts from the B value to the C value and falls to the D value state. Thus, the output power has two values with respect to the input power, and has a history. This is called optical bistability. FIG. 4 is a diagram for explaining an optical switch using the optical bistability of FIG. First, holding light having input power is inserted between the A value and the D value. When the set pulse is applied, the input power increases rapidly, so that the output power state shifts from the A value to the B value and switches. When returning, when a reset pulse is input, the state shifts from the C value to the D value. The time of the set pulse and the reset pulse can be freely controlled, and the photonic crystal optical resonator 11 can be applied as an optical memory. In addition, as the application of photonic crystals to optical switches and optical memories progresses, expectations for application to various other optical elements also increase. Although the present embodiment shows the case where the diameter L of the dielectric cylinder 13 is L = 0.6a, the same effect can be expected as long as L has a photonic band gap.

  Next, a second embodiment will be described. FIG. 5 is a schematic diagram of the configuration of the optical circuit component of the second embodiment. In the photonic crystal optical circuit component 20, the photonic crystal optical resonator 21 (the region between the broken line X2 and the broken line Y2) has the same structure as the photonic crystal optical resonator 11 in the first embodiment. In the second embodiment, the photonic crystal optical waveguides 25 (regions on the left side of the broken line X2) and 26 (right sides of the broken line Y2) are disposed through the dielectric cylinders arranged on both sides of the photonic crystal optical resonator 21. Area). In order to improve the optical coupling between the photonic crystal optical waveguides 25 and 26 and the photonic crystal optical resonator 21 (in other words, to improve the transmittance of the entire optical circuit component), both sides of the photonic crystal optical waveguides 25 and 26 are provided. The diameter L2 of the arranged dielectric cylinders 27a to 27h and 28a to 28h is L2 = 0.5a, and the width of the dielectric cylinders 27a to 27h and 28a to 28h is w1 (w1 = 1.73a). However, the dielectric cylinders 23a and 23b constituting the photonic crystal optical resonator 21 are deviated by d = 0.2a in the optical waveguide direction from the periodic arrangement (the circle by the broken line is the periodic arrangement). The diameter L1 of the dielectric cylinders 24a, 24b, 24c and 24d in the direction perpendicular to the optical waveguide direction adjacent to the lattice defect constituting the vessel 21 is L1 = 0.4a, and the thickness t of the dielectric thin film slab 22 is t = 0. .6a.

  6 and 7 are dispersion diagrams showing the waveguide mode of the optical waveguide. FIG. 6 shows the relationship between the wave number and the frequency when L = L2 = 0.6a and t = 0.6a. This shows that there are two waveguide modes # 1 and # 2 in the photonic band gap. Of these guided modes, guided mode # 1 has a symmetric mode in a mirror plane parallel to the propagation direction, and is called an even mode. On the other hand, waveguide mode # 2 has an antisymmetric mode and is called an odd mode. Since a general single mode is an even mode, waveguide mode # 1 is usually used for light propagation in a photonic crystal optical waveguide. FIG. 6 shows a waveguide mode in such a waveguide, and the light transmission band is a region from a normalized frequency of 0.261 to 0.277 from the mode end to the light line. 8 shows the normalized frequency characteristics of the photonic crystal optical resonator 11 shown in FIG. 2, and also shows the waveguide band of the photonic crystal optical waveguide shown in FIG. 6 (broken line B1 in FIG. 8). To the broken line B2). It can be seen that the resonant frequency of the photonic crystal optical resonator 21 does not match the waveguide band of the photonic crystal optical waveguide of FIG.

  Therefore, in order to achieve resonance frequency matching between the photonic crystal optical resonator and the photonic crystal optical waveguide, one of the effective refractive indexes may be changed. Here, the effective refractive index is changed by modifying the structure of the photonic crystal optical waveguide without changing the structure of the photonic crystal optical resonator. FIG. 7 shows the relationship between the wave number and the frequency when the diameter L2 of the dielectric cylinders 27a to 27h and 28a to 28h arranged on both sides of the photonic crystal optical waveguides 25 and 26 is L2 = 0.5a. By reducing the hole diameter, the effective refractive index can be increased and the normalized frequency corresponding to the waveguide mode can be decreased. The obtained waveguide mode # 1 has a waveguide band with a normalized frequency of 0.253 to 0.272, and from FIG. 8, the resonance frequency of the photonic crystal optical resonator 21 exists within the waveguide band. Is clear (frequency between solid line A1 and solid line A2 in FIG. 8). By using this photonic crystal optical waveguide, it is possible to excite the photonic crystal optical resonator from the outside. In view of the above, the form of FIG. 5 can be taken.

  FIG. 9 is a schematic diagram of a configuration of a modification of the optical circuit component according to the second embodiment. In FIG. 9, in the photonic crystal optical circuit component 30, the photonic crystal optical resonator 31 (region between the broken line X3 and the broken line Y3) and the photonic crystal optical waveguide 35 (region on the left side of the broken line X3), 36 (broken line) The region on the right side of Y3) is connected via four dielectric cylinders 33a to 33d and 33e to 33h, respectively.

  At this time, the dielectric cylinders 33a and 33h constituting the photonic crystal optical resonator 31 are deviated by d = 0.2a in the optical waveguide direction from the periodic arrangement (the position of the circle by the broken line is the periodic arrangement). The diameter L1 of the dielectric cylinders 34a, 34b, 34c, and 34d in the direction orthogonal to the optical waveguide direction adjacent to the lattice defects constituting the nick crystal optical resonator 31 is set to L1 = 0.4a. Further, the dielectric cylinders 37a to 37f and 38a to 38f arranged on both sides of the photonic crystal optical waveguides 35 and 36 have a diameter L2 of L2 = 0.5a and a width w1, thereby constituting other photonic crystals. The diameter L of the dielectric cylinders 33 and 33a to 33h is L = 0.6a, and the thickness t of the dielectric thin film slab 32 is t = 0.6a.

  10 and 11 are diagrams showing the transmission characteristics of the photonic crystal optical circuit component. FIG. 10 shows a case where the photonic crystal optical resonator 21 and the photonic crystal optical waveguides 25 and 26 are connected via three dielectric cylinders in the photonic crystal optical circuit component 20, whereas FIG. In the photonic crystal optical circuit component 30, the photonic crystal optical resonator 31 and the photonic crystal optical waveguides 35 and 36 are connected via four dielectric cylinders. The transmission characteristics in FIGS. 10 and 11 are calculated by the two-dimensional FDTD method. The horizontal axis is the normalized frequency. 10 and 11, it can be seen that there is a very sharp peak near the normalized frequency of 0.264. The difference in resonance frequency is due to the difference between the three-dimensional and two-dimensional FDTD methods. And it turns out that the direction of FIG. 11 has a sharper resonance peak compared with FIG. This is because the photonic crystal optical resonator 31 configured via four dielectric cylinders has a higher Q value than the photonic crystal optical resonator 21 configured via three dielectric cylinders. It is shown that. Thus, the overall Q value can be changed by changing the number of dielectric cylinders between the photonic crystal optical resonator and the photonic crystal optical waveguide. Although the present embodiment shows the case of L = 0.6a, the same effect can be expected even with a combination different from this as long as L has a photonic band gap.

  Next, a third embodiment will be described. FIG. 12 is a schematic diagram of the configuration of the optical circuit component according to the third embodiment. FIG. 12 shows photonic crystal optical circuit components 40 in which photonic crystal optical waveguides 45 (regions on the left side of the broken line X4) and 46 are provided on both sides of a photonic crystal optical resonator 41 (region between the broken line X4 and the broken line Y4). Similarly to FIG. 9 of the second embodiment in which (the region on the right side of the broken line Y4) is coupled, the photonic crystal optical resonator 41 has four dielectric cylinders 43a to 43d and 43e to 43 arranged on both sides. The photonic crystal optical waveguides 45 and 46 are connected via 43h. However, in FIG. 12, the width of the photonic crystal optical waveguides 45 and 46 is different from the width w 1 of the photonic crystal optical resonator 41.

  The dielectric cylinders 43a and 43h constituting the photonic crystal optical resonator 41 are deviated by d = 0.2a in the optical waveguide direction from the periodic arrangement (the circle by the broken line is the periodic arrangement). Dielectric cylinders 44a, 44b, 44c, and 44d in the direction perpendicular to the optical waveguide direction adjacent to the lattice defects constituting the diameter L1 of L1 = 0.4a, and other dielectric cylinders 43 constituting the photonic crystal, The diameter L of 43a to 43h is L = 0.6a, and the thickness t of the dielectric thin film slab 42 is t = 0.6a.

  In FIG. 12, the width of the photonic crystal optical waveguide is given by the modes of the photonic crystal optical resonators 21 and 31 and the photonic crystal optical waveguides 25, 26, 35, and 36 as in the second embodiment. It provides frequency matching and improves the Q value.

Next, a fourth embodiment will be described. FIG. 13 is a schematic diagram of the configuration of the optical circuit component of the fourth embodiment.
In FIG. 13, in a photonic crystal optical circuit component 50, photonic crystal optical waveguides 55 and 56 are continuously connected, and a photonic crystal optical resonator 51 is present on the side.

  The dielectric cylinders 53a and 53b constituting the photonic crystal optical resonator 51 are shifted by d = 0.2a in the optical waveguide direction from the periodic arrangement (the circle by the broken line is the original position). The diameter L1 of the dielectric cylinders 54a, 54b, 54c, 54d in the direction perpendicular to the optical waveguide direction adjacent to the lattice defects constituting the L1 = 0.4a, and the thickness t of the dielectric thin film slab 52 is t = 0.6a. And

  The radius L2 of the dielectric cylinders 57a to 57n and 58a to 58n arranged on both sides of the photonic crystal optical waveguides 55 and 56 is L2 = 0.5a, the width of the photonic crystal optical waveguides 55 and 56 is w1, and other photo The diameter L of the dielectric cylinder 53 constituting the nick crystal was set to L = 0.6a. The number of rows of dielectric columns between the photonic crystal optical resonator 51 and the photonic crystal optical waveguides 55 and 56 is 1 to 5.

  In FIG. 13, the widths of the photonic crystal optical waveguides 55 and 56 are set in the same manner as in the first, second, and third embodiments, and the photonic crystal optical resonator 51 and the photonic crystal optical waveguide. The mode frequency matching of the waveguides 55 and 56 is given, and the Q value is improved.

  In the above description, silicon or gallium / arsenic is used as the material of the dielectric thin film slabs 12, 22, 32, 42, 52, and the material other than the dielectric thin film slabs 12, 22, 32, 42, 52 is used. Although the case of using air has been described, other materials can also be used. For example, silicon, germanium, gallium / arsenic compound, indium / phosphorus compound, or indium / antimony compound can be used for the material of the dielectric thin film slabs 12, 22, 32, 42, 52, and the dielectric thin film For materials other than the slabs 12, 22, 32, 42, 52, use polyimide organic compounds, epoxy organic compounds, acrylic organic compounds, air, vacuum, or oxides of the above dielectric thin film slab materials. Can do. Even when such a material is used, the same effect as described above can be obtained.

(Appendix 1) In optical circuit parts using photonic crystals,
A dielectric slab having a predetermined refractive index and a dielectric pillar having a refractive index different from that of the dielectric slab disposed in the dielectric slab,
A resonator is formed by forming a defect in which a region corresponding to one dielectric column when the dielectric columns are periodically arranged in the dielectric slab has the same refractive index as that of the dielectric slab, and The dielectric column in the optical waveguide direction of the resonator adjacent to the defect is moved from the periodic arrangement in the optical waveguide direction, and the diameter of the dielectric column in the direction orthogonal to the optical waveguide direction adjacent to the defect is other dielectric material. An optical circuit component characterized by being different from the diameter of a pillar.

  (Supplementary Note 2) A linear region corresponding to a plurality of dielectric pillars when connected to the resonator and periodically arranging the dielectric pillars in the dielectric slab has the same refractive index as the dielectric slab. 2. The optical circuit component according to appendix 1, wherein the optical circuit component has an optical waveguide provided with a linear defect serving as a light propagation path.

(Supplementary note 3) The optical circuit component according to supplementary note 2, wherein a plurality of the dielectric pillars are arranged in a connection region of the resonator with the optical waveguide.
(Supplementary note 4) The optical circuit component according to supplementary note 3, wherein the number of the dielectric pillars arranged in the connection region is variable.

  (Supplementary note 5) The optical circuit component according to supplementary note 2, wherein the optical waveguide is connected to the resonator so that an optical waveguide direction of the optical waveguide coincides with an optical waveguide direction of the resonator. .

  (Additional remark 6) The said optical waveguide is characterized by the diameter of the dielectric pillar arrange | positioned on the both sides of the said linear defect among the said dielectric pillars differing from the diameter of the other dielectric pillar of the said optical waveguide. The optical circuit component according to Appendix 2.

  (Additional remark 7) The said optical waveguide moved the dielectric pillar arranged on the both sides of the said linear defect among the said dielectric pillars from the periodic arrangement to the direction orthogonal to an optical waveguide direction. 2. The optical circuit component according to 2.

(Supplementary note 8) The optical circuit component according to supplementary note 2, wherein the optical waveguide is connected to both sides of the resonator in the optical waveguide direction with the resonator interposed therebetween.
(Supplementary note 9) The optical circuit component according to supplementary note 2, wherein the resonator is provided at a side of the linear defect region of the optical waveguide.

  (Supplementary note 10) The optical circuit component according to supplementary note 1, wherein the dielectric slab is formed using silicon, germanium, a gallium / arsenic compound, an indium / phosphorus compound, or an indium / antimony compound.

  (Supplementary Note 11) The dielectric pillar is formed using silicon dioxide, polyimide organic compound, epoxy organic compound, acrylic organic compound, air, vacuum, or an oxide of the dielectric slab material. The optical circuit component according to appendix 1.

(Supplementary Note 12) In an optical element including an optical circuit component using a slab type two-dimensional photonic crystal,
A dielectric slab having a predetermined refractive index, and a dielectric pillar having a refractive index different from that of the dielectric slab disposed in the dielectric slab, and the dielectric pillar is placed in the dielectric slab. A resonator is formed by forming a defect in which a region corresponding to one dielectric pillar when arranged periodically has the same refractive index as that of the dielectric slab, and an optical waveguide direction of the resonator adjacent to the defect. An optical circuit configured such that the diameter of the dielectric column in the direction perpendicular to the optical waveguide direction adjacent to the defect is different from the diameter of the other dielectric columns An optical element comprising a component.

It is a schematic diagram of the structure of the photonic crystal optical circuit component of 1st Embodiment. It is a figure which shows the frequency characteristic of the photonic crystal optical resonator of FIG. It is FIG. (1) which shows the switch principle using a photonic crystal optical resonator. It is FIG. (2) which shows the switch principle using a photonic crystal optical resonator. It is a schematic diagram of a structure of the optical circuit component of 2nd Embodiment. It is a dispersion | distribution figure (the 1) which shows the waveguide mode of an optical waveguide. It is a dispersion | distribution figure (the 2) which shows the waveguide mode of an optical waveguide. It is a dispersion | distribution figure (the 3) which shows the waveguide mode of an optical waveguide. It is a schematic diagram of the structure of the modification of the optical circuit component of 2nd Embodiment. It is the figure (the 1) which showed the transmission characteristic of the photonic crystal optical circuit. It is the figure (the 2) which showed the transmission characteristic of the photonic crystal optical circuit. It is a schematic diagram of a structure of the optical circuit component of 3rd Embodiment. It is a schematic diagram of a structure of the optical circuit component of 4th Embodiment.

Explanation of symbols

DESCRIPTION OF SYMBOLS 10 Photonic crystal optical circuit component 11 Photonic crystal optical resonator 12 Dielectric thin film slab 13, 13a, 13b, 14a-14d Dielectric cylinder a Lattice constant L, L1 Diameter of dielectric cylinder

Claims (10)

In optical circuit components using photonic crystals,
A dielectric slab having a predetermined refractive index and a dielectric pillar having a refractive index different from that of the dielectric slab disposed in the dielectric slab,
A resonator is formed by forming a defect in which a region corresponding to one dielectric column when the dielectric columns are periodically arranged in the dielectric slab has the same refractive index as that of the dielectric slab, and The dielectric column in the optical waveguide direction of the resonator adjacent to the defect is moved from the periodic arrangement in the optical waveguide direction, and the diameter of the dielectric column in the direction orthogonal to the optical waveguide direction adjacent to the defect is other dielectric material. An optical circuit component characterized by being different from the diameter of a pillar.   Propagation of light, which is connected to the resonator and has the same refractive index as that of the dielectric slab in a linear region corresponding to a plurality of dielectric columns when the dielectric columns are periodically arranged in the dielectric slab. 2. The optical circuit component according to claim 1, further comprising an optical waveguide provided with a linear defect serving as a path.   The optical circuit component according to claim 2, wherein a plurality of the dielectric pillars are arranged in a connection region of the resonator with the optical waveguide.   4. The optical circuit component according to claim 3, wherein the number of the dielectric pillars arranged in the connection region is variable.   The optical circuit component according to claim 2, wherein the optical waveguide is connected to the resonator so that an optical waveguide direction of the optical waveguide coincides with an optical waveguide direction of the resonator.   3. The optical waveguide according to claim 2, wherein a diameter of a dielectric column arranged on both sides of the linear defect in the dielectric column is different from a diameter of another dielectric column of the optical waveguide. Optical circuit components.   3. The optical waveguide according to claim 2, wherein the dielectric pillars arranged on both sides of the linear defect in the dielectric pillars are moved from the periodic array in a direction perpendicular to the optical waveguide direction. Optical circuit components.   3. The optical circuit component according to claim 2, wherein the optical waveguide is connected to both sides of the resonator in the optical waveguide direction with the resonator interposed therebetween.   The optical circuit component according to claim 2, wherein the resonator is provided beside a region of the linear defect of the optical waveguide. In an optical element including an optical circuit component using a slab type two-dimensional photonic crystal,
A dielectric slab having a predetermined refractive index, and a dielectric pillar having a refractive index different from that of the dielectric slab disposed in the dielectric slab, and the dielectric pillar is placed in the dielectric slab. A resonator is formed by forming a defect in which a region corresponding to one dielectric pillar when arranged periodically has the same refractive index as that of the dielectric slab, and an optical waveguide direction of the resonator adjacent to the defect. An optical circuit configured such that the diameter of the dielectric column in the direction perpendicular to the optical waveguide direction adjacent to the defect is different from the diameter of the other dielectric columns An optical element comprising a component.

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