Optical coupler provided with a structuration

The invention relates to an optical coupler (10) in a vertical configuration, capable of working for a wavelength and comprising a first waveguide (12) and a second waveguide (14). The second waveguide (14) has a patterning (33) in the form of a series of patterns (36), the patterns (36) extending along a transverse direction (X) perpendicular to the longitudinal direction (Z), being parallel to each other and orthogonal to the general direction of the first waveguide (12), each pattern (36) being arranged both in the core (30) and the cladding (32) of the second waveguide (14) and having parameters influencing the evanescent wave coupling between the first waveguide (12) and the second waveguide (14), said parameters being chosen such that the coupling (C) is greater than 15%.

FIELD OF THE INVENTION

The present invention relates to an optical coupler, a component comprising such an optical coupler, a determination method, and a method for manufacturing such an optical coupler.

BACKGROUND OF THE INVENTION

The invention is situated in the field of the heterogeneous integration of laser sources on an integrated optical structure. Such integrations are applicable in various fields using components from integrated photonics. Applications include optical telecommunications, optical sensors and biophotonics. For these different applications, there is a need for structures making it possible to guide the light effectively.

Integrated photonics developed on substrates such as glass, silicon or III-V materials. It will be recalled that a semiconductor of type “III-V” is a composite semiconductor manufactured from one or more elements from column III of the periodic table of elements (boron, aluminum, gallium, indium, etc.) and one or more elements from column V or pnictogens (nitrogen, phosphorus, arsenic, antimony, etc.). It is desirable instead to use silicon substrates, since silicon substrates make it possible to integrate both optical components and electronic components.

However, no monolithic laser source effective on silicon yet exists. To offset this problem, heterogeneous laser source integrations using III-V materials on a silicon substrate are generally used.

To obtain effective coupling of the laser light created by the laser source in the III-V material with a silicon guiding structure, it has been proposed to use evanescent waves to couple a passive waveguide of the silicon guide structure with the laser source. The coupling is related to the ratio between the amplitude of the electric field of the wave circulating in the passive waveguide and the amplitude of the electric field of the wave emitted by the laser source. More specifically, the coupling is defined by formula C=I2/(I1+I2), where C is the coupling, I1 is the intensity of the electric field in the laser, and I2 is the intensity of the electric field in the passive waveguide. Furthermore, it will be recalled that a passive waveguide is a waveguide with no active element.

The obtainment of the coupling between the laser source and the passive waveguide requires that the laser source be very close to the passive waveguide. The coupling in fact greatly depends on the spacing between the laser source and the passive waveguide. This proximity is often difficult to obtain in practice, since the passive waveguide should be protected by depositing an insulating layer degrading the laser source, in particular due to the temperature at which the deposition is done.

To avoid this problem, document WO-A-03/054,596 proposes producing a passive waveguide including an optical relief with gradual efficiency.

However, this type of structure is difficult to produce in a technology involving silicon.

SUMMARY OF THE INVENTION

There is therefore a need for an optical coupler having good coupling efficiency and that is easier to manufacture.

To that end, the invention relates to an optical coupler in a vertical configuration, capable of working for a wavelength and comprising a first waveguide extending in a longitudinal direction and capable of propagating a first propagation mode of the light having a first effective index, a second waveguide distinct from the first waveguide, parallel to the first waveguide, having a core and a cladding and capable of propagating a second propagation mode of the light having a second effective index, the second effective index being different from the first effective index. The second waveguide having a patterning, the patterning having a period along the longitudinal direction below the ratio between the wavelength at which the optical coupler is capable of operating and the product of two by the second effective index, the patterning being in the form of a series of patterns, the patterns extending along a transverse direction perpendicular to the longitudinal direction, being parallel to each other and orthogonal to the general direction of the first waveguide, each pattern having parameters influencing the evanescent wave coupling between the first waveguide and the second waveguide, said parameters being chosen such that the coupling is greater than 15%.

Such an optical coupler makes it possible to obtain better coupling. The optical coupler is easy to manufacture, since only techniques from microelectronics are used.

According to specific embodiments, the optical coupler comprises one or more of the following features, considered alone or according to any technically possible combinations:the patterns are chosen from the group consisting of openings formed in the second waveguide and blades.the patterns have a dimension along the transverse direction larger than the dimension of the core of the second waveguide along the transverse direction.the core of the second waveguide having an optical index, the second effective index is greater than the first effective index and the patterns are made from a material having an optical index below the optical index of the core of the second waveguide.the patterning has a fill factor, the patterns are made from a material having an optical index, some parameters influencing the evanescent wave coupling between the first waveguide and the second waveguide being the fill factor of the patterning, the optical index of the material from which the patterns are made, and the spacing along the longitudinal direction between each pattern.each pattern is arranged both in the core and the cladding of the second waveguide.each waveguide includes a cladding and a core, the optical index of the core of the first waveguide being below the optical index of the cladding of the second waveguide.the spacing along the longitudinal direction between the patterns is variable in the longitudinal direction.the first waveguide includes a core made from a material belonging to column III of the periodic table formed with a material from column V of the periodic table and two lower and upper layers surrounding the core.the core of the second waveguide has a variable dimension in the transverse direction.the optical coupler includes a substrate, made from a first material, in which the second waveguide is buried, the first waveguide being arranged in contact with the substrate and formed from a material different from the first material.the optical coupler includes a third waveguide distinct from the first and second waveguides and extending parallel to the first and second waveguides, the third waveguide being arranged between the first waveguide and the second waveguide and being capable of propagating a third light propagation mode having a third effective index.a thermal insulation zone of the first waveguide in which the patterning is arranged.

The invention also relates to an optical component including an optical coupler as previously described.

Furthermore, the present invention also relates to a method for determining an optical coupler in a vertical configuration, capable of working for a wavelength and comprising a first waveguide extending in a longitudinal direction and capable of propagating a first propagation mode of the light having a first effective index, and a second waveguide distinct from the first waveguide, parallel to the first waveguide, having a core and a cladding and capable of propagating a second propagation mode of the light having a second effective index, the second effective index being greater than the first effective index, the second waveguide having a patterning, the patterning having a period along the longitudinal direction smaller than the ratio between the wavelength at which the optical coupler is capable of working and the product of two by the second effective index, the patterning being in the form of a series of patterns having parameters influencing the evanescent wave coupling between the first waveguide and the second waveguide, the patterns extending along a transverse direction perpendicular to the longitudinal direction, being parallel to each other and orthogonal to the general direction of the first waveguide, each pattern having parameters influencing the evanescent wave coupling between the first waveguide and the second waveguide. The method comprises a step for choosing a desired evanescent wave coupling between the first waveguide and the second waveguide, the desired coupling being greater than or equal to 15%, and a step for modifying the parameters of the patterning to obtain the desired evanescent wave coupling between the first waveguide and the second waveguide.

Furthermore, the present invention also relates to a method for manufacturing an optical coupler as previously described, in which the manufacturing method comprises steps for manufacturing waveguides and the patterning involving techniques for deposition, epitaxy, polishing, gluing and material removal by etching.

The manufacturing method makes it possible to obtain the optical coupler previously described using only microelectronics techniques. Such techniques are particularly easy to implement.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

In the context of the invention, an optical coupler10is provided that is capable of working for a wavelength λ as shown inFIG. 1.

This coupler10is in a vertical configuration, i.e., a configuration in which this optical coupler10is capable of coupling light between two guides offset in a transverse direction perpendicular to a general propagation direction of the light.

The coupler10comprises a first waveguide12extending in the longitudinal direction Z and capable of propagating a first propagation mode P1of the light having a first effective index NF1. In fact, depending on the field distribution, each propagation mode sees a different index of the materials making up the waveguide depending on each propagation mode. The index seen by each propagation mode defines the effective index.

The coupler10also comprises a second waveguide14distinct from the first waveguide12. The second waveguide14is parallel to the first waveguide12. The second waveguide14has a core30and a cladding32. Furthermore, the second waveguide14is capable of propagating a second propagation mode P2of the light having a second effective index NF2. The second effective index NF2is different from the first effective index NF1.

The second waveguide14has a patterning33in the form of a series of patterns36. The patterning33can also be designated using the generic term “grating”33. However, for clarity reasons, this term is not used in the context of this description, since the patterning33is not a diffraction grating. In particular, the patterning33does not serve to amplify the field in the gain medium. On the contrary, the patterning33makes it possible to extract light by modifying the effective index.

The patterns36extend along a transverse direction X perpendicular to the longitudinal direction Z. The patterns are parallel to each other and orthogonal to the general direction of the first waveguide. The patterning33has a period P along the longitudinal direction Z below the ratio between the wavelength λ at which the optical coupler10is capable of working and the product of two by the second effective index NF2. By definition, the period P is the sum of the spacing between two patterns36and the width of a pattern36.

The patterns36have parameters influencing the evanescent wave coupling C between the first waveguide12and the second waveguide14, these parameters being chosen such that the coupling C is greater than 15%.

As a reminder, in the context of the invention, it is chosen to express the coupling as the ratio between the intensity of the electric field of the wave circulating in the second waveguide14and the sum of the intensities of the electric fields of the waves circulating in the first waveguide12and the second waveguide14. Hereinafter, the coupling thus defined is denoted “C”, which is a number with no unit.

When the first waveguide12is supplied with power, the first waveguide12emits light in the form of guided waves.

Part of the waves guided in the first waveguide12then couples with the second waveguide14by evanescent waves. Waves are then guided in the second core30.

The patterning33makes it possible to perform an adaptation of the effective index favoring the coupling between the first waveguide12and the second waveguide14.

This better coupling is obtained while preserving easy manufacturing. In fact, a manufacturing method may be used using only microelectronics techniques. Such a manufacturing method comprises steps for manufacturing waveguides12,14and the patterning33involving techniques for deposition, epitaxy, polishing, gluing and material removal by etching.

The patterns36are for example openings made in the second waveguide14. According to the embodiments, these openings have a square or round shape. Alternatively, the openings are in the shape of a slot, the inside of the slot being a vacuum or air.

According to another example, the patterns36are blades, as illustrated inFIG. 1.

Preferably, the patterns36have a dimension along the transverse direction X larger than the dimension of the core30of the second waveguide14along the transverse direction X. This property makes it possible to increase coupling.

According to one embodiment, the second effective index NF2is greater than the first effective index NF1; the patterns36are then made from a material having an optical index below the optical index of the core30of the second waveguide14. This makes it possible to obtain better coupling more easily.

When the second effective index NF2is lower than the first effective index NF1, the patterns36are then made from a material having an optical index greater than the optical index of the core20of the second waveguide14. This makes it possible to obtain better coupling more easily.

Thus, in the case where the patterning33has a fill factor F and the patterns36are made from a material having an optical index, said parameters influencing the evanescent wave coupling C between the first waveguide12and the second waveguide14are the fill factor of the patterning33, the optical index of the material from which the patterns36are made, and the spacing e along the longitudinal direction Z between each pattern36.

Under these conditions, at the first order, the new effective index NF2′ of the mode of the guide with patterning is given by NF2′=F*n36+(1−F)*NF2and the relationship NF2′≈NF1is also verified.

Preferably, to increase the coupling,

the spacing e along the longitudinal direction Z between the patterns36is variable along the longitudinal direction Z.

In one particular embodiment, the first waveguide12includes a core22made from a material belonging to column III of the periodic table formed with a material according to column V of the periodic table and two lower26and upper28layers surrounding the core20.

Advantageously, to favor coupling, the core30of the second waveguide14has a variable dimension along the transverse direction X.

In order to insulate the second waveguide14from the environment of the first waveguide12, according to one advantageous embodiment, the optical coupler10includes a substrate18, made from a first material, in which the second waveguide14is buried, the first waveguide12being arranged in contact with the substrate18and made from a material different from the first material.

In order to increase this insulation effect with respect to the environment, the optical coupler10includes a third waveguide distinct from the first and second waveguides12,14and extending parallel to the first and second waveguide12,14, the third waveguide being arranged between the first waveguide12and the second waveguide14and being capable of propagating a third light propagation mode P3having a third effective index NF3.

According to one alternative, the optical coupler10includes a thermal insulation zone of the first waveguide12in which the patterning33is arranged. This makes it possible to ensure good management of the heat of the first waveguide12, and in particular to prevent it from heating.

Hereinafter, specific embodiments are described more precisely. This is in particular the case for the optical coupler10ofFIG. 1.

For the rest of the description, a longitudinal direction is defined corresponding to a general propagation direction of the light. A transverse direction is also defined perpendicular to the longitudinal direction and contained in the plane ofFIG. 1. The longitudinal and transverse directions are respectively symbolized by an axis Z and an axis X inFIG. 1.

Furthermore, when the term “index” is used for a medium, that term refers to the refraction index of that medium, which is a property without characteristic dimension of that medium and describing the behavior of the light in that medium. In the event the medium has an index gradient, the term “index” refers to the mean of the index in that medium.

FIG. 1shows an optical coupler10, including a first waveguide12, a second waveguide14and an insulating element16. The optical coupler10also comprises a substrate18in which the second waveguide14is buried, the first waveguide12resting on the substrate18.

The optical coupler10is capable of coupling light from the first waveguide12toward the second waveguide14.

Hereinafter, “vertical configuration” refers to a configuration in which the optical coupler is capable of coupling light between two guides offset in the transverse direction X. Conversely, “horizontal configuration” refers to a configuration in which the optical coupler is capable of coupling light between two guides aligned along the transverse direction X. In the example ofFIG. 1, the optical coupler10is in a vertical configuration.

The first waveguide12extends in the longitudinal direction Z between a first entry plane12eand a first exit plane12s. Each first plane12eand12sis a plane perpendicular to the longitudinal direction Z.

The first waveguide12includes a first core22and a first cladding24.

The first core22is formed by a layer extending along the longitudinal direction Z. The first core22has a dimension e22along the transverse direction X of 1.5 microns (μm) and a dimension l22along the longitudinal direction Z may be several millimeters, but its dimension along a coupling zone defined by the overlap with the second core30is typically approximately 100 μm.

The first core22is, for example, a hetero structure made from a first material that is a mixture made up of Arsenic, Indium and Aluminum (with formula AlInAs) and a second material that is a mixture made up of Arsenic, Indium and Gallium (with formula GaInAs). Hereinafter, the index nc1of the first core22is equal to 3.3, which mathematically translates to nc1=3.3.

More generally, the first core22is made from a gain material, i.e., a material capable of generating the stimulated emission of photons following an excitation.

The first cladding24has a first upper layer26and a first lower layer28, the first core22being arranged between the first upper layer26and the first lower layer28.

The first lower layer28has a dimension e28along the transverse direction X of 0.5 μm and a dimension l28along the longitudinal direction Z of approximately 100 μm.

According to the example ofFIG. 1, the first upper layer26and the first lower layer28are made from the same material. This material is the material from which the first cladding24is made.

In the illustrated case, the material is indium phosphorus.

Alternatively, the first upper layer26and the first lower layer28are made from two different materials.

The index ng1of the first cladding24is then equal to 3.1, which mathematically translates to ng1=3.1.

The first waveguide12forms an active waveguide. “Active waveguide” refers to a waveguide including at least one layer formed from an active material capable of generating a wave. In the case ofFIG. 1, the first core22is such a layer.

More specifically, the first waveguide12is a laser waveguide, i.e., a laser source. The first waveguide12is for example a so-called quantum cascade laser source (more often designated using its acronym, QCL). Such a waveguide12is capable of generating laser waves with a wavelength of 4.5 μm.

The first waveguide12is capable of propagating the waves according to a first propagation mode P1corresponding to a first effective index NF1. In fact, depending on the field distribution, each propagation mode sees a different index of the materials making up the waveguide depending on each propagation mode. The index seen by each propagation mode defines the effective index. In the present case, the first effective index NF1is equal to 3.21.

The second waveguide14extends in the longitudinal direction Z between a second entry plane14eand a second exit plane14s. Each second plane14eand14sis a plane perpendicular to the longitudinal direction Z. The second entry plane14eis positioned between the first entry plane12eand the first exit plane12s.

The second waveguide14includes a second core30, a second cladding32and a patterning33.

The second core30is formed by a layer extending along the longitudinal direction Z. The second core30has a dimension e30along the transverse direction X of 1.5 μm and a dimension l30along the longitudinal direction Z is several millimeters. However, its dimension along the longitudinal direction Z along the overlap zone with the first core is approximately 100 μm.

The second core30is for example made from silicon-germanium. As a result, the index nc2of the second core30is equal to 3.6, which mathematically translates to nc2=3.6.

The second cladding32includes a second upper layer34and a second lower layer combined with the substrate18.

Alternatively, the second cladding32comprises a second lower layer distinct from the substrate18.

The second upper layer34has a dimension e34along the transverse direction X of 0.75 μm and a dimension l34along the longitudinal direction Z can be several millimeters or centimeters. However, its dimension along the longitudinal direction along the coupling zone defined by the overlap with the second core30is approximately 100 μm.

The second cladding32is for example made from silicon. The index ng2of the second cladding32is then equal to 3.4, which mathematically translates to ng2=3.4.

The second waveguide14is a passive waveguide, i.e., a waveguide not including a layer made from an active material.

The second waveguide14is capable of allowing the propagation of a second propagation mode denoted P2corresponding to a second effective index NF2. In the absence of the patterning33, the second effective index NF2is greater than the first effective index NF1. In that case, the second effective index NF2is equal to 3.51, which mathematically translates to NF2=3.51.

Alternatively, the first waveguide12has a first effective index NF1greater than the second effective index NF2. Only the case where the first effective index NF1is below the second effective index NF2is considered, the transposition being easy for one skilled in the art.

The second waveguide14is buried in the substrate18, i.e., it is optically insulated from the surrounding medium.

The insulating element16is, according to the example ofFIG. 1, an optical insulating element assuming the form of a parallelepiped element. In the cross-sectional view ofFIG. 1, it extends along the longitudinal direction Z between the first entry plane12eand the second entry plane14e.

The insulating element16is made from a material with an index lower than the effective index NF1of the first waveguide12.

Using the insulating element16makes it possible to avoid evanescent wave coupling between the first waveguide12and the substrate18.

The substrate18is formed by a layer extending along the longitudinal direction Z extending between an entry plane18eand an exit plane18f. According to the example ofFIG. 1, the second exit plane14sis situated between the first exit plane12sand the exit plane18fof the substrate18, while the first entry plane12eis between the entry plane18eof the substrate18and the first exit plane12s.

The substrate18has a dimension e18along the transverse direction X in the vicinity of several hundred μm thick, for example 700 μm, and a dimension l18along the longitudinal direction Z several tens of centimeters wide.

The substrate18is for example made from silicon. The index ns18of the substrate18is then equal to 3.4, which mathematically translates to ns18=3.4.

The patterning33is a series of blades36.

Each blade36extends in a transverse direction X.

According to the example ofFIG. 1, each blade36assumes the form of a rhomb.

Each blade36is parallel to the other blades36.

Each blade36is arranged both in the second core30and in the second cladding32and in the substrate18.

Each blade36has a dimension l36along the transverse direction X and a dimension e36along the longitudinal direction Z.

The patterning33has a spacing e between the blades36along the longitudinal direction Z.

The patterning33also has a fill factor corresponding to the ratio between the dimension e36along the longitudinal direction Z and the sum of the dimension e36along the longitudinal direction Z and the spacing e between the blades36along the longitudinal direction Z.

The index of the material from which the blades36are made is denoted n36. The index n36of the blades36is below the effective index NF1of the first waveguide16.

It appears that the patterning33is characterized by a plurality of parameters that are, for the spacing e between the blades36along the transverse direction X, the fill factor and the index of the material from which the blades36are made. The parameters that characterize the patterning33are parameters influencing the coupling between the first waveguide12and the second waveguide14.

Alternatively, other parameters are used to characterize the patterning33. In particular, a linear combination of the preceding parameters is interesting.

As an example, instead of using the aforementioned dimension, a plurality of dimensions are used, namely the dimension of the blades36in the second upper layer34along the transverse direction X, the dimension of the blades36in the second core30along the transverse direction X, and the dimension of the blades36in the second lower layer along the transverse direction X.

According to one alternative, instead of the fill factor, the dimension along the longitudinal direction Z of the blades36is used.

The parameters characterizing each blade36verify a first property denoted P1. The first property P1is verified when the evanescent wave coupling between the first waveguide12and the second waveguide14is greater than 15%. As a reminder, in the context of the invention, it is chosen to express the coupling as the ratio between the intensity of the electric field of the wave circulating in the second waveguide14and the sum of the intensities of the electric fields of the waves circulating in the first waveguide12and the second waveguide14. Hereinafter, the coupling thus defined is denoted “C”, which is a number with no unit.

In a manner known in itself, for an imposed evanescent wave coupling, one skilled in the art is capable of determining a second waveguide equivalent to the first waveguide14provided with the patterning33. Determining the missing parameters of the patterning33therefore amounts to determining the optimal characteristics of the second equivalent waveguide. The effective index of the mode of the waveguide14provided with the structuring33is then of the first order given by the relationship:
NF2=F*n36+(1−F)*NF2′

where:F is the fill factor of the patterning33.NF2′ is the effective index of the propagation mode of the waveguide14without patterning (without patterning33).

However, the optimization of the evanescent wave coupling between two waveguides is a known problem that one skilled in the art knows how to resolve. In fact, the transfer of light from one waveguide to another waveguide implies that the guided propagation modes of each guide are close enough to each other for their evanescent part to have a non-zero overlap. The optimal coupling length then depends on this overlap, which in turn depends on optogeometric characteristics of the considered waveguides.

For example, it is known from the book entitledOptical wave guide theoryby A. W. Sneider and J. D. Love, published by Chapman and Hall in 1983, that for two waveguides A and B close enough for the evanescent part of the propagation modes of the waves circulating in those two guides to overlap, the length LCcorresponding to the maximum coupling from the waveguide A toward the waveguide B to the other may be written:

Lc=πK2+δ2Where⁢:δ=πλ⁢(neffA-neffB)
whereλ is the length in the vacuum,neffAis the effective index of the considered propagation mode circulating in the waveguide A, andneffBis the effective index of the considered propagation mode circulating in the waveguide B,

K=ɛ0μ0⁢k4⁢∫SB⁢Δ⁡(n2)⁢Ea⁢Eb*⁢⁢dA
whereε0is the dielectric permeability in the vacuum,μ0is the magnetic permeability in the vacuum,k is the number of waves associated with the wavelength λ,Δ(n2) is the squared index difference between the index of the core of the waveguide B and the index of the cladding of the waveguide A,Eais the electric field of the considered propagation mode in the waveguide A,Ebis the electric field of the considered propagation mode in the waveguide B,“*” designates the mathematical conjugation operation, andSBis the core section of the waveguide of B.

In order to perform the calculations, one skilled in the art usually uses digital simulation tools in particular to calculate the fields of the propagation modes of the waveguides A and B.

Thus, one skilled in the art manages to obtain the characteristics of the patterning33. Implementing such an optimization leads, in the case ofFIG. 1, for example, to the following choice.

Furthermore, each pattern36is arranged both in the core30and in the cladding32of the second waveguide14.

According to the example ofFIG. 1, each blade36extends from the second upper layer34while passing through all of the second core30as far as the second lower layer. More specifically, each blade36has a same dimension l36of 3 μm in the transverse direction X, distributed in 0.75 μm in the second upper layer34, 1.5 microns in the second core30and 0.75 μm in the second lower layer.

As a result, the blades36are in contact with the first lower layer28.

The blades36are made from silicon oxide (with chemical formula SiO2). The index n36of the blades36then reaches 1.5, which automatically translates to n36=1.5. The index n36of the blades36is below the effective index NF1of the first waveguide16.

The patterning33has a spacing e between the blades36such that the period P of the patterning33, i.e., the sum of the spacing e and the thickness of the blade e36, is less than or equal to the ratio of the working wavelength of the optical coupler and the product of two by the second effective index NF2. The spacing between the blades36is the distance separating two blades36along the longitudinal direction Z. This mathematically translates to:

The simulations done by the applicant have shown that the shorter the period P is, the better the coupling is.

According to the example ofFIG. 1, the period P between the blades is strictly less than 0.65 μm.

Preferably, the fill factor is comprised between 10 and 30%.

In the example ofFIG. 1, the fill factor is 14%.

The operation of the optical coupler10according to the invention will now be described.

When the first waveguide12is supplied with power, the first waveguide12emits light in the form of waves guided in the first core22.

Part of the waves guided in the first core22then couples with the second waveguide16by evanescent waves. Waves are then guided in the second core30.

The patterning33makes it possible to perform an adaptation of the effective index favoring the coupling between the first waveguide12and the second waveguide16.

FIGS. 2 and 3are simulations showing the distribution of the light energy in the optical coupler10according toFIG. 1. Upon observingFIG. 3, it appears that on the entry plane12eof the first waveguide12, the intensity of the electric field is 100%, whereas on the exit plane12sof the second waveguide14, the intensity of the electric field is 80%, which shows that the coupling C is approximately 80%.

This shows that the parameters chosen for the coupler10ofFIG. 1, i.e., for each of the three layers (third core26, upper layer40and lower layer42), the dimension along the longitudinal direction Z of the considered player, the dimension along the transverse direction X of the considered layer and the optical index in which the considered layer is made, verify the property P1.

The coupling C obtained upon studyingFIG. 3should be compared to the coupling obtained with an optical coupler according to the state of the art.

Such an optical coupler according to the state of the art is a coupler representing the same characteristics, but without patterning.

In that case,FIGS. 4 and 5are obtained by simulation. Upon studyingFIG. 5, it is observed that the coupling C is low, approximately 5%. In other words, using the coupler10according to the invention makes it possible to obtain a gain by a factor16in terms of coupling.

The optical coupler10according to the invention therefore makes it possible, owing to the presence of the patterning33, to perform an effective index adaptation making it possible to ensure a transition from a first propagation mode P1to a second propagation mode P2of better quality than in the state of the art. This leads to increasing the observed coupling C.

This better coupling is obtained while preserving easy manufacturing. To illustrate this advantage, it is now described in reference toFIGS. 6 to 11.

As appears upon studying the values of the example ofFIG. 1, in the absence of the third waveguide14, since the index ng2of the second gain is greater than the index nc1of the first core20, the coupling is physically impossible. The introduction of the third waveguide14makes it possible, for each waveguide, for the index of the cladding of the waveguide to be below the indices of the core(s) of each adjacent waveguide.

The manufacturing method first includes the deposition of a silicon substrate18. For example, the deposition step102is for example implemented using a technique known in itself for chemical vapor deposition (CVD) or physical vapor deposition (PVD). The obtained substrate layer18is diagrammatically illustrated inFIG. 6.

The manufacturing method next includes manufacturing a silicon and germanium layer100on the silicon substrate18. According to the proposed example, the manufacturing is implemented using silicon and crystalline germanium epitaxy. Epitaxy is an ordered growth technique of two materials (in this case, silicon and germanium) relative to one another that have a certain number of shared symmetrical elements in their crystalline networks. The assembly of the substrate layer18and the silicon and germanium layer100obtained at the end of this step of the method is diagrammatically illustrated inFIG. 7.

The method next comprises a lithography step done in the silicon-germanium layer so as to cut out a part of the layer100to obtain a layer forming the second core30of the second waveguide14. The assembly of the substrate layer18and the second core30obtained at the end of this step of the method is diagrammatically illustrated inFIG. 8.

The method subsequently includes a step for manufacturing a silicon layer so as to form the upper layer32of the second waveguide14. This manufacturing step successively includes an epitaxy step of the layer and polishing step of the layer in order to flatten the surface. According to the illustrated method example, the polishing step is carried out using a chemical mechanical polishing (CMP) technique. The assembly of the substrate18and the second waveguide14obtained at the end of this step of the method is diagrammatically illustrated inFIG. 9.

The method next includes a step for manufacturing the patterning33comprising a lithography sub-step making it possible to produce holes in the second waveguide14, those holes next being filled with the material forming the blades36, in this case silicon oxide. The lithography sub-step is followed by a new polishing sub-step. The assembly of the substrate18and the second waveguide14provided with the patterning33obtained at the end of this step of the method is directly illustrated inFIG. 10.

The method lastly includes a step for gluing the first waveguide12, the result of which is illustrated byFIG. 11. The gluing step may be gluing by molecular adhesion. It is also possible to perform gluing by simple epitaxy (thin layers), then produce the waveguides12using techniques similar to those used for the waveguide14.

The method therefore makes it possible to obtain the optical coupler10. Implementing this method involves only the use of proven technologies in the context of the manufacture of planar components, and more particularly components made from a semiconductor material. In particular, such a manufacturing method does not involve implementing a technology for immersion in molten salt baths, which is a delicate technology to carry out. As a result, the method according to the invention is particularly easy to implement.

Furthermore, the optical coupler10has the advantage of not imposing constraints on the shape of the first waveguide12and the second waveguide14. The first waveguide12and the second waveguide14can therefore be optimized to provide an optimal output (ratio between the output power of the considered device and the incident power on the considered device) without deteriorating the coupling C.

Alternatively, it should be noted that it is possible to design multiple optical couplers10whereof the parameters of the patterning33verify the property P1relative to the coupling C.

In particular, different materials can be considered to produce the patterning33. In particular, semiconductor materials of type “III-V” can be considered.

These remarks on the materials apply to the materials of all of the layers involved in the coupler10.

As an illustration, a coupler10according to a second embodiment is considered. The identical elements between the coupler10according to the second embodiment and the coupler10according to the first embodiment are not repeated. Only the differences are highlighted.

In that case, the blades36are made from zinc sulfide (with chemical formula ZnS). The index n36in this case is equal to 2.25, which mathematically translates to n36=2.25. Furthermore, the fill factor is 23%.

FIGS. 12 and 13are simulations showing the distribution of the light energy in the optical coupler10according to the second embodiment. Upon observingFIG. 13, it appears that the intensity of the electric field is 100% in the entry plane12eof the first waveguide12, while in the exit plane14sof the second waveguide14, the intensity of the electric field is 80%, which shows that the coupling C is approximately 80%.

This example also illustrates that preferably, to obtain the best coupling, the parameters characterizing the patterning33alternatively verify a second property denoted P2. The second property P2is verified when the evanescent wave coupling C between the first waveguide12and the second waveguide14is greater than 30%.

Still more advantageously, alternatively, the parameters characterizing the patterning33verify a third property denoted P3. The third property P3is verified when the evanescent wave coupling C between the first waveguide12and the second waveguide14is greater than 50%.

Other, more complex patterns are also advantageous for the optical coupler10.FIGS. 14 and 15illustrate two examples of this.

FIG. 14shows an optical coupler10according to a third embodiment. The elements that are identical between the third embodiment and the coupler10according to the first embodiment are not repeated. Only the differences are highlighted.

In this third embodiment, the dimension e36along the longitudinal direction Z of each blade varies. More specifically, depending on the propagation direction of the light, the dimension e36along the longitudinal direction Z of a blade is smaller than the dimension e36along the longitudinal direction Z of the preceding blade.

This makes it possible to obtain a patterning33ensuring adiabatic coupling of the waves. As a result, the fill factor goes from a minimum value to a maximum value, passing through the resonant coupling value mentioned in the previous embodiment. If this variation is slow enough, optimal coupling is obtained, equivalent to that of the coupling by the periodic patterning of the preceding embodiment. The primary interest lies in the robustness to technological imperfections. In fact, for a very specific targeted fill factor, it is possible that the technological patterning33manufacturing may not be perfect, which causes the coupling to be poor. With a fill factor gradient, while therefore being sure to go through the proper value, the coupling is then ensured.

FIG. 15shows an optical coupler10according to a fourth embodiment. The elements that are identical between the coupler10according to the fourth embodiment and the coupler10according to the third embodiment are not repeated. Only the differences are highlighted.

In the case ofFIG. 15, it is assumed that the heat conductivity of the material from which the insulating element16is made is lower than that of the substrate18. In order to improve the heat conductivity, it is proposed that the insulating element16be provided with openings or assume the form of blades like the patterning33to benefit from the best heat release properties for the substrate18.

According to other alternatives, it is also possible to consider more complex patterns. As an example, the optical coupler10includes a third waveguide distinct from the first and second waveguides12,14and extending parallel to the first and second wave guides12,14, the third waveguide being arranged between the first waveguide12and the second waveguide14and be capable of propagating a third light propagation mode P3having a third effective index NF3.

In that case, all of the parameters characterizing the third waveguide and the patterning33are such that the evanescent wave coupling between the first waveguide12and the second waveguide14is greater than 15% (30%, 50%, respectively, depending on the selected property).

Due to the multiplicity of the optical couplers10meeting properties P1, P2or P3, it is also proposed, in the context of this invention, to have a method for determining parameters including a step for choosing parameters such that the coupling C is greater than 15%, 30% or 50%.

The optical coupler10obtained is in particular especially interesting in the case of an integrated gas sensor. More generally, such an optical coupler10can be used in any optical component for which it is favorable to implement a heterogeneous integration.

It should also be noted that the optical coupler10is also applicable in the case where the first waveguide12is not an active waveguide. As an example, the first waveguide12is an infrared detector comprising an absorbing material at the wavelength of interest with a waveguide14that is transparent at that same wavelength of interest. Thus, the guide12detects the light coming from the guide14in the opposite direction.

The proposed optical coupler10especially pertains to the field of the middle infrared.

“Middle infrared” refers to a spectral band grouping together waves whereof the wavelength is comprised between 2 μm and 10 μm.

Preferably, the preceding spectral band is limited to the band comprised between 2 μm and 7 μm, in particular if SiO2 is used, since SiO2 has a high absorption for radiations whereof the wavelength is greater than 7 μm.

In particular, in the case where the second waveguide is made from a Si (cladding)/SiGe (core) or SiGe (cladding)/Ge (core), a leak problem of the laser field appears once the index nc1of the first core22is below the optical index ng2of the second cladding32. The patterning33makes it possible to limit that leak.

It should be noted that for a radiation below 2 μm, the leak problem is generally absent, since the index nc1of the first core22is greater than the optical index ng2of the second cladding32.

Furthermore, it should also be noted that the coupling zone of the coupler10has an effective index.

When the effective index of the coupling zone of the coupler10is constant, the effective index of the coupling zone is such that the optical index of the second cladding with patterning33is below the first effective index NF1(to avoid the leak of the mode in the cladding). Thus, the optical index of the coupling zone is, for example, below or preferably equal to the first effective index NF1.

When the effective index of the coupling zone is not constant, the effective index varies gradually from a value below or equal to the first effective index NF1to a value equal to the second effective index NF1. In the coupling zone, the condition according to which the optical index of the second cladding with patterning33is below the first effective index NF1is respected to prevent the mode from leaking in the cladding. Beyond the coupling zone, the light that is propagating is essentially contained in one or more modes guided by the second waveguide. As a result, the condition according to which the optical index of the second cladding with patterning33is below the first effective index NF1can no longer be respected, and that non-respect does not cause a leak.