This application is a national phase entry under 35 U.S.C. § 371 of International Patent Application PCT/FR2019/051515, filed Jun. 21, 2019, designating the United States of America and published as International Patent Publication WO 2019/243751 A1 on Dec. 26, 2019, which claims the benefit under Article 8 of the Patent Cooperation Treaty to French Patent Application Serial No. 1855540, filed Jun. 21, 2018.
This disclosure relates to a front-side imager, and to a process for manufacturing such an imager.
Document US 2016/0118431 describes a front-side imager.
As illustrated in
According to one embodiment, the buried oxide is chosen to be relatively thin (i.e., to have a thickness smaller than 100 nm and, in particular, of about 20 nm) in order to play the role of the dielectric of a capacitor. That portion of the substrate that is located below the buried oxide is biased to a voltage different from the voltage of the active layer, thus allowing the interface between the dielectric layer and this active layer to be passivated.
The voltage to be applied to that portion of the substrate that is located under the BOX depends on the thickness of the latter. The potential difference to be applied is proportional to the thickness of the buried oxide.
Inversely, if the buried oxide is chosen to be relatively thick (i.e., to have a thickness of about 100 to 200 nm or more), it has reflective optical properties and allows incident photons to be reflected so as to confine them in the active layer, in particular, in the case of photons the wavelength of which is in the range of the near infrared.
The optimal thickness ranges for each of these two functions do not coincide, and the skilled person is required to make a compromise between the reflectivity of the buried oxide and his ability to polarize each pixel by applying a low potential difference between the active layer and the substrate.
One aim of the present disclosure is to design a front-side imager that performs better than existing imagers and, in particular, a substrate from which the imager may be obtained.
This substrate is able to be fabricated at a low cost.
To this end, a first subject of the present disclosure relates to a front-side imager comprising in succession:
The term “front side,” as used herein, means that side of the imager that is intended to be exposed to light radiation, which side is located on the same side of the structure as the associated electronic components.
The first separating layer advantageously has a thickness between 10 and 100 nm.
The second separating layer advantageously has a thickness between 100 and 300 nm.
According to one embodiment, the intermediate layer is made of a doped polycrystalline or amorphous material.
According to one embodiment, the intermediate layer is made of doped silicon.
Alternatively, the intermediate layer is made of a metal.
The intermediate layer advantageously has a thickness between 20 and 150 nm.
According to one embodiment, the active layer comprises a silicon seed layer.
According to another embodiment, the active layer is a silicon-germanium layer.
According to one embodiment, the active layer further comprises a single-crystal layer of silicon-germanium on the seed layer.
Particularly advantageously, the germanium content in the silicon-germanium layer is lower than or equal to 10%.
Preferably, the thickness of the silicon-germanium layer is smaller than a critical thickness defined as being a thickness beyond which the silicon-germanium relaxes.
According to another embodiment, the active layer further comprises a single-crystal layer of silicon on the seed layer.
According to one embodiment, the substrate further comprises, on the active layer, a layer referred to herein as the optical confinement layer having a coefficient of optical reflection from the front side toward the active layer higher than the coefficient of reflection from the active layer toward the front side.
Advantageously, the optical confinement layer comprises a layer of titanium nitride between two layers of silicon oxide.
According to one embodiment, each photodiode is separated from an adjacent photodiode by at least one electrically isolating trench extending up to the first electrically insulating layer.
Advantageously, the trench comprises an electrically conductive or semiconductor via extending up to the intermediate layer between walls made of an electrically insulating material.
According to one embodiment, the at least one trench extends through the optical confinement layer.
According to one embodiment, each trench comprises a first wall extending up to the intermediate layer and a second wall extending at least partially into the second separating layer so as to electrically isolate a segment of the intermediate layer, the electrically conductive or semiconductor via being electrically connected to the segment of the intermediate layer.
The imager such as described above is formed from a substrate for a front-side imager, comprising in succession:
According to one embodiment, the seed layer is a silicon layer.
According to another embodiment, the seed layer is a silicon-germanium layer.
According to one embodiment, the substrate further comprises a silicon-germanium single-crystal layer on the seed layer, the silicon-germanium layer forming, with the seed layer, the active layer of the imager.
According to another embodiment, the substrate further comprises a silicon single-crystal layer on the seed layer, the silicon layer forming, with the seed layer, the active layer of the imager.
According to one embodiment, the substrate may be fabricated using a process comprising the following steps:
According to one alternative embodiment, the substrate may be fabricated using a process comprising the following steps:
Another subject of the present disclosure relates to a process for fabricating a front-side imager such as described above.
According to one embodiment, the fabricating process comprises the following steps:
According to one alternative embodiment, the fabricating process comprises the following steps:
The processes further comprise a step of forming a matrix array of photodiodes in the active layer.
Moreover, a layer referred to herein as the optical confinement layer may be formed on the active layer, the optical confinement layer having a coefficient of optical reflection from the front side toward the active layer higher than the coefficient of reflection from the active layer toward the front side.
Other features and advantages of the present disclosure are described in the detailed description that follows, with reference to the accompanying drawings in which:
To make the drawings more clear, the various layers have not necessarily been shown to scale.
Contrary to the substrate of
The carrier substrate is generally obtained by slicing a single-crystal ingot. The substrate essentially plays the role of mechanical carrier of the imager. The carrier substrate may comprise a material chosen from silicon, III-V semiconductors, glass, silica, sapphire, alumina, aluminum nitride, silicon carbide or even a ceramic or a metal alloy. Advantageously, the carrier substrate is made of silicon. Its doping (if it is a question of silicon), nature and characteristics may be optimized in order to integrate, in a hybrid way, in the form of a system-on-chip, electronic devices other than the imager. The doping of the substrate may be uniform throughout the thickness of the material or limited to one segment thereof. Preferably, the doped zone is adjacent to one of the two separating layers.
The active layer comprises a single-crystal semiconductor and is intended to receive a matrix array of photodiodes that allow images to be captured.
The two separating layers on either side of the intermediate layer have different thicknesses and play different roles in the operation of the imager.
The first separating layer is located on the side of the front side, and it is thinner than the second separating layer, which is located on the side of the back side.
The role of the first separating layer is to allow a bias to be transferred from the intermediate layer to the active layer. The role of the second separating layer is to electrically insulate the intermediate layer from the substrate, and to allow the stack of the layers separating the active layer from the carrier substrate to have a suitable reflectivity with respect to photons coming from the active layer.
Each of the two separating layers is made from an electrically insulating material, such as a dielectric material, for example, an oxide, such as a thermal or deposited silicon oxide, or even an oxynitride. The structure comprising these two electrically insulating separating layers may then be qualified a “double BOX,” i.e., a “double buried oxide.”
On the side of its front side, the substrate comprises a seed layer on the first separating layer, the seed layer being a single-crystal semiconductor layer suitable for the epitaxial growth of a single-crystal semiconductor layer intended to form, with the seed layer, the active layer of the imager.
The material of the seed layer is chosen depending on the material of the epitaxial layer and, in particular, has a lattice parameter suitable for allowing the growth of the epitaxial layer while preventing or at the very least minimizing the generation of crystal defects such as dislocations.
The seed layer and the epitaxial layer may be made of the same material (homoepitaxy) or two different materials (heteroepitaxy).
The epitaxial layer may be made of silicon. In this case, the seed layer is advantageously made of silicon.
Preferably, the epitaxial layer is made of silicon-germanium (SiGe) because silicon-germanium has an optical absorption coefficient higher than that of silicon, in particular, in the infrared, this absorption coefficient being proportional to the concentration of germanium. The seed layer may then be made of silicon-germanium or of silicon. In the latter case, the design of the epitaxial layer must not take into account only the concentration of germanium but also the thickness of the layer. Specifically, if the SiGe layer is formed by epitaxy on a silicon seed layer, the lattice parameter of which is different from that of the silicon-germanium, the SiGe layer relaxes beyond a certain thickness, called the critical thickness. This relaxation results in the formation of dislocations within the SiGe layer. Such dislocations make the SiGe layer unsuitable for use as active layer, in particular, in an imager and must, therefore, be avoided. Now, the critical thickness is inversely proportional to the concentration of germanium. The thickness of the epitaxial layer and the concentration of germanium in the layer, therefore, result from a compromise between:
Typically, it is sought to maximize the thickness and the concentration of germanium of the epitaxial layer in order to obtain the best possible absorption in the infrared. Preferably, the germanium content of the active layer is lower than or equal to 10%. Specifically, the critical thickness of a layer of Si0.9Ge0.1 is about a few microns, this being suitable for the active layer of a front-side imager.
The intermediate layer may be a semiconductor or even an electrically conductive material. Specifically, the role of this intermediate layer is to allow the active layer to be biased from behind, in other words, via a zone placed between the carrier substrate and the second electrically insulating layer. Such a bias allows a potential difference to be applied between the active layer and the buried intermediate layer.
The intermediate layer may be single-crystal but this is not indispensable because it is neither sought to achieve the ability to conduct electrons through this layer, nor any other electronic property such as commonly considered for applications other than that of imagers, but merely to achieve the ability to modify the electrical potential of the active layer on the periphery of the first separating layer.
The intermediate layer may thus be polycrystalline and/or amorphous, this making it less expensive to fabricate, and/or a metal. This layer may be doped to a greater or lesser extent so as to ensure it is able to be biased. A semiconductor intermediate layer is advantageously made of silicon. The layer then typically has a thickness between 20 nm and 150 nm.
The first electrically insulating separating layer, which is interposed between the active layer and the intermediate layer, plays the role of the dielectric of a capacitor, and thus allows the active layer to be biased on the periphery of the electrically insulating material. To this end, the first separating layer is chosen to be sufficiently thin to minimize the potential difference to be applied between the intermediate layer and the active layer. Typically, the thickness of the first separating layer is between 10 nm and 100 nm.
The thickness of the first separating layer is in contrast too small to allow all the photons that pass through the active layer and, in particular, photons the wavelength of which is in the range of the near infrared, to be reflected. Therefore, photons that pass through the active layer are liable to pass through the first separating layer and the intermediate layer.
The role of the second separating layer is to induce a reflection of the photons, in particular, photons the wavelength of which is in the range of the near infrared, toward the pixel formed in the active layer through the stack comprising: the second separating layer, the intermediate layer and the first separating layer. To this end, this second separating layer has a sufficiently large thickness to have a high reflectivity (or optical reflection coefficient), in particular, in the field of the near infrared. Typically, the thickness of the second separating layer, which is, for example, made of silicon oxide, is between 100 nm and 300 nm.
The substrate comprises in succession, from its back side to its front side:
Examples of processes for fabricating the substrate illustrated in
According to a first embodiment, which is illustrated in
On the one hand, with reference to
On the other hand, with reference to
Next, the first donor substrate is thinned so as to transfer a layer 4 of the semiconductor to the receiver substrate. This thinning may be carried out by polishing or etching of the semiconductor from the side opposite to the bonding interface. However, advantageously, before the bonding step, a weakened zone 41 is advantageously formed in the semiconductor so as to delineate a surface layer 4 to be transferred; the weakened zone may be formed by implanting atomic species such as hydrogen and/or helium (implantation being schematically shown by arrows in
Moreover, with reference to
With reference to
Next, the second donor substrate is thinned so as to transfer a layer 3a of the semiconductor to the receiver substrate, thus allowing the substrate shown in
According to a second embodiment, illustrated in
This second embodiment of the process takes advantage of the fact that the semiconductor intermediate layer does not have an optical or electronic function and may, therefore, be made from a material that is not single-crystal but polycrystalline and/or amorphous. Thus, the intermediate layer may be formed by deposition on the subjacent second electrically insulating layer 2b.
With reference to
With reference to
With reference to
With reference to
Next, the donor substrate 30 is thinned so as to transfer the layer 3a to the intermediate layer 4, this allowing the substrate shown in
This second embodiment of the process is particularly advantageous in that it is less expensive since it involves a single layer-transfer step instead of two.
Whatever the process for fabricating the structure illustrated in
The seed layer 3a and the epitaxial layer 3b together form the active layer 3. Since the thickness of the epitaxial layer 3b is clearly larger than the thickness of the seed layer 3a, the optical properties of the active layer are considered to be essentially those of the epitaxial layer 3b, even if the layers 3a and 3b are made of different materials.
Thus, for example, if the epitaxial layer is made of SiGe but the seed layer is not made of SiGe, for example, when it is made of silicon, the silicon layer is sufficiently thin (of a thickness smaller than or equal to 300 nm) with respect to the thickness of the SiGe layer to not notably affect the properties of the active layer in terms of absorption in the infrared.
However, it is possible to modify the nature of the seed layer, for example, by means of a thermal-mixing process. As known per se, the process comprises oxidizing a SiGe layer epitaxially grown on a silicon layer, the oxidation having the effect of consuming only the silicon (to form silicon oxide) and of making the germanium migrate toward the face opposite to the free surface of the SiGe layer. An SiO2 layer is then obtained on the surface, which may then be removed by etching.
With reference to
According to one optional but advantageous embodiment, with reference to
The optical confinement layer 6 lets the radiation incident on the surface of the imager pass substantially without reflecting it, but, in contrast, reflects photons present in the active layer and reflected by the double BOX structure, this having the effect of trapping the photons in the active layer and of increasing their path length in the active layer. The optical confinement layer thus allows the optical absorption of the active layer to be increased.
According to one embodiment illustrated in
According to one embodiment illustrated in
Lastly, according to one embodiment illustrated in
Although not shown in
Numerical simulations of optical absorption have been carried out for various substrates, according to the prior art (with a single layer of silicon oxide between the carrier substrate and the active layer, as illustrated in
The reflectivity of such a stack is about 72% for an incident wavelength of 940 nm.
In these simulations, certain substrates were covered with an optical confinement layer having a reflectivity from the front side toward the active layer higher than the reflectivity from the active layer toward the front side. The optical confinement layer consisted of the following stack, from the front side toward the back side of the substrate: SiO2, 100 nm/TiN, 10 nm/SiO2, 200 nm.
The active layer consisted either of a silicon layer of 6 μm thickness, or of a SiGe layer of 2 μm thickness having a concentration of germanium equal to 10%.
The table below indicates the optical absorption coefficient in the active layer, for radiation of normal incidence (i.e., incidence perpendicular to the front side of the substrate) and having a wavelength of 940 nm. The simulation does not take into account the influence of diffraction or of refraction from the trenches separating the various pixels.
A significant improvement in absorption is observed when a double BOX structure is used instead of a single layer of SiO2. The optical absorption is further improved when the active layer is made of SiGe instead of silicon, and/or when an optical confinement layer that confines the photons in the active layer is added.
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1855540 | Jun 2018 | FR | national |
Filing Document | Filing Date | Country | Kind |
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PCT/FR2019/051515 | 6/21/2019 | WO |
Publishing Document | Publishing Date | Country | Kind |
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WO2019/243751 | 12/26/2019 | WO | A |
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