The invention relates to the field of optoelectronics.
The subject of the invention is more particularly an optoelectronic arrangement comprising a semiconductor nanowire.
Semiconductor-based nanowires are recognized as being good candidates when it comes to producing optoelectronic devices.
This is because the thread-like geometry of a nanowire makes it possible to construct a wide variety of nano-heterostructures, and to act, widely, on their electronic and optical properties.
It will be noted that there are two main approaches for the fabrication of nanowires, the approach based on epitaxial growth (referred to as “bottom-up” growth) and the nanofabrication-based approach (known as “top-down” fabrication) based among other things on lithography and etching.
For mass applications, for which reducing the fabrication cost is a major issue, the epitaxial growth approach is much more attractive.
Among the numerous potential applications of nanowires in optoelectronics and photonics, there are mainly:
For these applications, the integration of a mirror at the level of the base of the nanowires is particularly desirable to maximize the effectiveness of extraction (in the light-emitting diodes and the single photon sources), or reinforce the absorption in the photovoltaic cells.
In this regard, it is known practice to use a planar mirror which ensures a good reflectivity. As an example, a horizontal film of gold, placed under a set of vertical nanowires of small diameter d, makes it possible to reflect more than 90% of the light at normal incidence. A diameter is considered to be “small” if it is significantly less than the length of the radiation wave concerned, for example d<0.3λ/n, where n designates the refractive index of the material forming the nanowire.
Another particular case is that of the larger diameter nanowires, optimized for effective light guidance. Such guidance can be implemented when the diameter of the nanowire is approximately of the order of λ/n, with λ being the wavelength concerned and n the refractive index of the nanowire material. Such a nanowire supports only a guided mode, which plays a predominant role in its optical properties. The aim is then to find a mirror which provides a high reflection coefficient for the guided mode. The best solution known at the present time consists of a hybrid planar mirror, formed by a layer of silver covered with a thin layer of dielectric as described in the document “Efficient photonic mirrors for semiconductor nanowires” by I. Friedler at al. published in OPTICS LETTERS on 15 Nov. 2008 Vol. 33, No. 22, pages 2635 to 2637.
The great drawback with these planar mirrors has in the fact that they have to be integrated via a complex and costly step of mounting on a substrate other than that used to grow the nanowires (step known to those skilled in the art as “flip-chip”). Furthermore, such an approach does not currently make it possible to mount large surface areas (300 mm diameter in the microelectronics standards) reliably and reproducibly.
The aim of the present invention is to propose a solution that makes it possible to form an optoelectronic arrangement that is compact, highly reproducible, and compatible with fabrication in large surface areas.
Efforts are being made to achieve this aim notably by virtue of an optoelectronic arrangement comprising a semiconductor nanowire intended to participate in the processing, notably in a reception and/or an emission, of a light concerned and a mirror reflecting the light concerned, the semiconductor nanowire comprising a first section and a second section, and in which the mirror surrounds at least longitudinally, the first section of the semiconductor nanowire, said second section extending out of the mirror. Furthermore, an aperture of the mirror wholly or partly filled by the first section has lateral aperture dimensions less than λ/5n, with n being the refractive index of the material of the first section of the semiconductor nanowire, and λ being the wavelength of the light concerned. The arrangement comprises a substrate on which the mirror rests.
Advantageously, the semiconductor nanowire extends, via its first section, from said substrate.
Preferably, the mirror comprises a layer that is reflective to the light concerned, notably the reflecting layer comprises a material with a coefficient of reflection in terms of intensity, at the wavelength concerned and for a planar wave at normal incidence, that is greater than or equal to 60%, such as, for example, gold, aluminium, copper or silver.
Moreover, the mirror may comprise a buffer layer that is transparent to the light concerned increasing the reflectivity of the mirror, notably the buffer layer is made of a dielectric material comprising SiO2 or Si3N4, or of an electrically conductive transparent material such as indium-tin oxide or zinc oxide, the reflecting layer being arranged between the substrate and the buffer layer.
Preferentially, the reflecting layer has a thickness greater than 30 nm, and the buffer layer has a thickness between 2 nm and 20 nm.
According to a particular implementation, the cross sections of the first and second sections are substantially identical.
According to another implementation, the second section, arranged in continuity with the first section, has a cross section whose surface area is greater than the surface area of the cross section of the first section so as to form a shoulder with said first section.
Advantageously, the cross section of the second section at its interface with the mirror has dimensions greater than those of the aperture of the mirror wholly or partly filled by the first section.
The invention also relates to an optoelectronic device which comprises a plurality of arrangements as described, notably sharing one and the same mirror, and each semiconductor nanowire is coupled to means that make it possible, with said semiconductor nanowire, to emit or receive the light concerned.
The invention also relates to a method for fabricating at least one arrangement as described, said method comprising the following steps:
Moreover, the method may comprise the formation of an aperture in the mirror, the step of formation of the semiconductor nanowire being performed by growth, notably by epitaxy, from the aperture.
Preferably, the aperture is formed in such a way as to have a bottom delimited by the substrate, or by a part of the mirror, the growth of the semiconductor nanowire being performed from said bottom.
Advantageously, the step of formation of the mirror, performed before the step of formation of the semiconductor nanowire, comprises the deposition of a first layer of a material suitable for catalysing the growth of the semiconductor nanowire and the deposition of one or more second layers on the first layer in such a way that the bottom of the aperture is formed by a part of the first layer and that the internal side wall of the aperture is delimited at least partly by the second layer or layers.
According to one implementation, the first section is obtained by axial growth and the second section is obtained by axial and/or radial growth.
According to a particular implementation, the method comprises the following successive steps:
Other advantages and features will become more clearly apparent from the following description of particular embodiments of the invention given as nonlimiting examples and represented in the attached drawings, in which:
The present optoelectronic arrangement differs from the prior art notably in that the mirror surrounds a section of the semiconductor nanowire situated between its two opposite longitudinal ends.
As illustrated in
“Processing of a light concerned” should be understood to mean that the semiconductor nanowire 2 can participate in a reception (for example in the context of a use of the semiconductor nanowire 2 in a photovoltaic cell) and/or an emission (for example in the context of a use of a semiconductor nanowire 2 in a light-emitting diode) of the light concerned. Typically, the semiconductor nanowire 2 will be able to be electrically doped, wholly or partly, by a first type, notably p type, and will at least partly form a p/n junction of a light-emitting diode or of a photodiode.
Advantageously, the semiconductor nanowire 2 is formed from one or more semiconductor materials belonging, for example, to the families (Si, Ge) or III-V (such as GaAs, InAs, GaP InP, GaSb, GaN, AlN, InN) or II-VI (such as CdTe, CdSe, ZnTe, ZnSe, ZnO, MgO) and their alloys.
Moreover, the arrangement comprises a mirror 3 that is reflective to the light concerned. The semiconductor nanowire 2 comprising a first section 2a and a second section 2b, the mirror 3 surrounds, at least longitudinally, the first section 2a of the semiconductor nanowire 2, said second section 2b extending out of the mirror 3.
More particularly, the semiconductor nanowire 2 extends between two opposite longitudinal ends 4a and 4b of the semiconductor nanowire 2, and the second section 2b is in continuity with the first section 2a. In fact, the limit between the first section 2a and the second section 2b is represented by the broken line I1 in
The fact that “the mirror 3 surrounds at least longitudinally, the first section 2a of the semiconductor nanowire 2” should be understood to mean that the mirror possesses a through aperture within which the first section 2a is arranged.
In
“Aperture wholly or partly filled by the first section 2a” should be understood to mean that the lateral dimensions of the first section 2a can be less than or equal to the lateral dimensions of the aperture. In other words, between the two ends 4a, 4b of the semiconductor nanowire 2, the mirror 3 surrounds the first section 2a with or without contact (in
In
The semiconductor nanowire 2 is advantageously a vertical structure relative to the mirror which is considered as a planar structure.
Preferably, the aperture of the mirror 3 wholly or partly fined by the first section 2a has lateral aperture dimensions less than λ/5n, with n being the refractive index of the first section 2a of the semiconductor nanowire 2, and λ being the wavelength of the light concerned. Advantageously, the aperture has a disc-shaped section, so it is considered that the diameter of the aperture is less than λ/5n. These dimensions make it possible to prevent the light concerned from leaking through the aperture at the level of the mirror and being lost.
Preferably, the lateral dimensions, or, if appropriate, the diameter of the aperture, are between 5 nm and 30 nm.
Preferably, the arrangement comprises a substrate 6 on which the mirror 3 rests.
Preferentially, the semiconductor nanowire 2 extends, via its first section 2a, from said substrate 6 (
According to a particular preferred, but optional, implementation, the mirror 3 comprises a reflecting layer 3a to the light concerned. Preferably, the reflecting layer 3a comprises (or consists of) a material with a coefficient of reflection in terms of intensity, at the wavelength concerned and for a planar wave at normal incidence, that is greater than or equal to 60%, such as, for example, gold, aluminium, copper or silver. In order to increase the reflectivity, the mirror 3 may also comprise a buffer layer 3b that is transparent to the light concerned. This buffer layer 3b is, preferably, arranged at the interface between the first section 2a and the second section 2b. Preferably, the buffer layer 3b is made of a dielectric material comprising SiO2 or Si3N4. Alternatively, the buffer layer 3b is made of an electrically conductive transparent material such as zinc oxide or indium-tin oxide (also known by the acronym ITO in the field). The thickness of this buffer layer 3b is preferably such that it eliminates the plasmonic excitation of the reflecting layer 3a when it is reached by the light concerned. Preferably, the thickness d1 of the buffer layer 3b is between 2 nm and 20 nm, and the thickness d2 of the reflecting layer 3a is greater than 30 nm.
The reflecting layer 3a may be formed by a stack of one or more sublayers of identical or different types.
As illustrated in
According to a particular embodiment illustrated in
According to another particular embodiment illustrated in
The section of the section 2b can also vary, for example continually between its value at the level of the mirror and its value (greater or smaller) at its free end. The semiconductor nanowire 2 may also exhibit any other profile.
For its part,
In the examples of
In a way that is applicable to everything stated above, the substrate 6 and at least the base of the semiconductor nanowire 2 in contact with the substrate 6 advantageously have the same type of electrical doping. This makes it possible to functionalize the arrangement by using the substrate 6 as electrical contact element, notably on a rear face of the substrate 6 opposite the face of the substrate on which the mirror 3 is arranged.
The substrate 6 can be made of monocrystalline silicon, of a III-V material such as GaAs, of sapphire, or of a cheaper material such as polycrystalline Si or a metallic alloy.
The invention also relates to an optoelectronic device which comprises a plurality of arrangements as described. In the field, such a device is also referred to as a semiconductor nanowire mat 2. Preferably, the arrangements share one and the same mirror 3 (
It will then be understood that the optoelectronic device can be a photovoltaic cell, a light-emitting diode display, or any other type of optoelectronic device suitable for participating in the emission or the reception of a light concerned.
In the case of the emission of the light concerned, the latter is generated from each semiconductor nanowire and the mirror makes it possible to increase the emission effectiveness by limiting the radiation losses by escape to the substrate and/or makes it possible to make the emission more directional.
In the case of the reception/detection of the light concerned, all the light that has not initially been taken into account by the semiconductor nanowires touches the mirror so as to be then reflected at least towards the semiconductor nanowires. The result of this is that the quantity of radiation absorbed is magnified.
In the context of the optoelectronic device that has a dense network of GaAs nanowires on a GaAs substrate (useful in particular in the context of light-emitting diode or photovoltaic cell applications), in the absence of the mirror, the reflection obtained by the surface area of the substrate is less than (n−1)2/(n+1)2=0.3, in which n designates the refractive index of the substrate at the wavelength concerned (here 1 μm), whereas the presence of the mirror makes it possible to obtain a reflectivity greater than 90% for a wide range of nanowire diameters (nanowire diameter less than 150 nm in the case of the example). “Dense network” should be understood here to mean more than one nanowire per μm2.
The invention also relates to a method for fabricating an optoelectronic arrangement or an optoelectronic device as described. In particular, this method comprises a step of production of a mirror 3 (
The step of formation of the semiconductor nanowire 2 and/or the step of production of the mirror 3 can be configured in such a way as to form the different embodiments of the arrangement, or of the device, described above.
Preferably, the method comprises a step of provision of a substrate 6 and the mirror 3 is produced on said substrate 6 (
According to one embodiment, the method comprises the formation of an aperture 8 in the mirror 3 (
Preferably, the aperture 8 is formed in such a way as to have a bottom 9 delimited by the substrate 6 (
According to a particular execution (
Moreover, the step of formation of the mirror 3 may advantageously comprise a step of formation of the reflecting layer 3a (as described above) on the substrate 6 and a step of formation of the buffer layer 3b as described above) on the reflecting layer 3a (
It is understood that the mirror 3 and the aperture 8 can be formed:
The synthesis of the nanowire, notably semiconductor and advantageously electrically doped, can then be performed from the aperture 8 using different epitaxial growth methods such as organometal vapour phase epitaxy (OMVPE), molecular jet epitaxy (MJE) or, for some materials like ZnO, by low-temperature hydrothermal synthesis.
Depending on the materials and the techniques used, the growth will or will not by catalyst-assisted. Any known method for the growth of semiconductor nanowires is potentially compatible with the use of the mirror 3 as described.
As an example, gold is traditionally used for the growth by OMVPE of Si nanowires. This catalyst will be provided in this case by the first layer 10, and the etching of the mirror 3 will be conducted in such a way as to retain, in this case, the first layer 10. During the growth, the gold present initially at the bottom of the aperture 8 forms a small drop which remains at the top of the nanowire. The rest of the mirror 3 is chosen in such a way as to remain inert during the growth, while having good optical properties (for example, aluminium is a good choice).
Alternatively, a nanowire of GaN can be obtained with no additional catalyst element, by MJE and by OMVPE. In this case, the mirror will be made of materials that are inert with respect to the growth of the nanowire, and a selective epitaxy of the nanowire will be obtained in the aperture of the mirror.
Once the growth of the semiconductor nanowire is sufficient for it to emerge from the hole, a radial and/or axial heterostructure of this semiconductor nanowire can be produced.
In a general manner applicable to the different implementations of the method, the first section 2a of the semiconductor nanowire 2 is obtained by axial growth and the second section 2b of the semiconductor nanowire 2 is obtained by axial and/or radial growth.
“Axial growth” should be understood to mean that the semiconductor nanowire increases its length without increasing its diameter (or its lateral dimensions), or increases its length much faster (more than ten times faster) than its diameter (or its lateral dimensions). This axial growth makes it possible to modulate the nature, composition or doping of the semiconductor obtained by axial growth of the semiconductor nanowire and to define, along the axis of the semiconductor nanowire passing through its two opposite longitudinal ends, quantum barriers or boxes.
“Radial growth” should be understood to mean that the semiconductor nanowire increases in diameter (or in lateral dimensions) between one and ten times faster than in length, that is to say that it increases little or not at all in length. This radial growth makes it possible to define lateral quantum wells or even radial p/n junctions.
During the step of growth of the semiconductor nanowire 2, it is possible to switch over from one growth (radial/axial) to the other by adjusting the growth conditions, in order to fabricate more complex structures. As an example, photonic wire-based single-photon sources have been fabricated by defining a quantum box by axial growth, then by using a step of radial growth to incorporate it in a cylindrical waveguide of controlled size. A person skilled in the art will therefore be able to implement an appropriate growth of the semiconductor nanowire according to the desired optoelectronic device.
In the preceding examples, use is made of metals that are suited by their optical properties to the fabrication of the mirror, and inert during the growth of the semiconductor nanowire. If such materials do not exist because of a fixed choice of one of them, or if the aim is simply to minimize the contamination of the semiconductor nanowires by the materials forming the mirror during their growths, an alternative strategy will preferentially be used.
In this alternative strategy, the method comprises the following successive steps:
The outer surface 14 of the mirror 13 is intended to be arranged facing the light concerned. In other words, the outer surface 14 is opposite the substrate 6. It will then be understood that, in the arrangement, the first section 2a can be formed wholly or partly by a part of the substrate 6.
It is understood that all the materials targeted above in the context of the optoelectronic arrangement can be used in the context of the method in order to form an element of the arrangement with which they are associated.
The method described above can also make it possible to fabricate a plurality of arrangements sharing one and the same mirror (thus forming the optoelectronic device). In this case, the apertures within this mirror or the initials sections produced before forming the mirror, make it possible to form all or part of the semiconductor nanowires by using the apertures as growth mask for the nanowires or the initials sections as starting point for the growth of the rest of the semiconductor nanowires. Thus, the result is a high degree of reproducibility inasmuch as the semiconductor nanowires do not grow randomly but at perfectly defined prioritized sites.
One of the many advantages of the method as described is that it allows for a growth of the semiconductor nanowire at the level of the mirror, thus avoiding the mounting of the nanowire structure on another substrate as in the prior art. The result thereof is that this method can be implemented with significantly lower fabrication costs while favouring reproducibility.
Number | Date | Country | Kind |
---|---|---|---|
13 54060 | May 2013 | FR | national |
Number | Name | Date | Kind |
---|---|---|---|
20080149944 | Samuelson et al. | Jun 2008 | A1 |
20100276664 | Hersee | Nov 2010 | A1 |
20140301420 | Kawaguchi et al. | Oct 2014 | A1 |
Entry |
---|
Niels Gregersen et al., Designs for High-Efficiency Electrically Pumped Photonic Nanowire Single-Photon Sources, Optics Express, Sep. 27, 2010, vol. 18, No. 20, Department of Photonics Engineering, Technical University of Denmark. |
I. Friedler et al., Efficient Photonic Mirrors for Semiconductor Nanowires, Nov. 15, 2008, 2635-2637, vol. 33, No. 22, Optics Letters. |
French Search Report dated Jan. 23, 2014. |
Number | Date | Country | |
---|---|---|---|
20140326945 A1 | Nov 2014 | US |