The field of the invention is that of assembly, or hybridization, of two microelectronic chips with each other, comprising the application of a so-called hybridization temperature.
The invention more precisely relates to the production of a first microelectronic chip intended to be hybridized with a second microelectronic chip, and to a method for hybridizing the two microelectronic chips.
The invention is applicable to the assembly of chips made of different materials, such as for example an optoelectronic chip comprising a matrix array of light-emitting diodes or photodiodes based on GaN on a chip comprising a readout circuit based on silicon.
It is often necessary to hybridize two microelectronic chips with each other, i.e. to join them mechanically by applying a so-called hybridization temperature, while ensuring electrical and mechanical interconnection therebetween.
The microelectronic chips may equally well be electronic devices such as an integrated circuit for reading and/or processing electrical signals, as optoelectronic devices such as a matrix array of light-emitting diodes or photodiodes.
The microelectronic chips are joined via their respective connection faces, on which faces each chip comprises a matrix array of N*M electrical interconnection pads. The assembly method then comprises a step of aligning and bringing into contact the interconnection pads pairwise, then a step of applying a so-called hybridization temperature, thus forming a mechanical link between the two chips by fusion or inter-diffusion of the interconnection pads of each microelectronic chip or both microelectronic chips.
As schematically illustrated in
As illustrated in
By way of illustration, for ΔT equal to about 200° C. and Δα equal to about 4×10−6K−1, and for chips P1, P2 each having a matrix array of 1280×1024 interconnection pads 12, 22 spaced apart by a pitch of 50 μm, the relative misalignment ΔL may reach half the pitch p, i.e. here about 25 μm, or more. The relative misalignment may lead, notably in the case of small pitches and large interconnection matrix arrays, to a loss of mechanical contact and therefore to an electrical connection fault between the respective interconnection pads.
The objective of the invention is to at least partially remedy the drawbacks of the prior art, and more particularly to propose a method for producing a first microelectronic chip intended to be hybridized with a second microelectronic chip in such a way that, in the subsequent hybridization phase, the relative misalignment between the respective interconnection pads is smaller than a preset threshold value.
To achieve it, one subject of the invention is a method for producing a first microelectronic chip comprising a layer, called the layer of interest, having a first face, called the connection face, on which electrical interconnection pads are located, and having a thermal expansion coefficient αci, and intended to be joined, at a temperature called the hybridization temperature Th, to a second microelectronic chip having a second face, called the connection face, on which electrical interconnection pads are located, and having a thermal expansion coefficient {tilde over (∝)}P2, called the apparent thermal expansion coefficient, at the second connection face, lower than the thermal expansion coefficient αci.
According to the invention, the method comprises the following steps:
The following are certain preferred but nonlimiting aspects of this method.
The method may comprise a step of defining a maximum value {tilde over (α)}P1max of the so-called apparent thermal expansion coefficient {tilde over (α)}P1 of the first chip at the first connection face so that the relative misalignment ΔL is substantially equal to the preset threshold value ΔLmax.
The interconnection pads may be distributed periodically with a pitch p, and the preset threshold value ΔLmax may be lower than or equal to p/2.
The layer of adhesive may have a thermal expansion coefficient αcc higher than that αci of the layer of interest and than that αcp of the handle layer.
The method may comprise a prior step of growing the layer of interest from a growth substrate made of a material having a thermal expansion coefficient higher than the apparent thermal expansion coefficient {tilde over (∝)}P2 of the second chip.
The layer of interest of the first chip may comprise light-emitting diodes or photodiodes.
The layer of interest of the first chip may be based on a III-V semiconductor compound or a II-VI semiconductor compound.
The second chip may comprise a so-called carrier layer and an integrated-circuit layer that is located between the second connection face and the carrier layer, the apparent thermal expansion coefficient {tilde over (∝)}P2 being substantially equal to the thermal expansion coefficient of the carrier layer.
The carrier layer may be made of silicon.
The layer of adhesive may have a thickness ecc smaller than or equal to 4 times the thickness eci of the layer of interest.
The layer of adhesive may have a Young's modulus Ecc comprised between 90 MPa and 40 GPa.
The thickness ecp of the handle layer may be larger than or equal to 20 times the thickness eci of the layer of interest.
The invention also relates to a method for hybridizing a first microelectronic chip with a second microelectronic chip having a second face, called the connection face, on which electrical interconnection pads are located, and having a thermal expansion coefficient {tilde over (∝)}P2, called the apparent thermal expansion coefficient, the method comprising the following steps:
Other aspects, aims, advantages and features of the invention will become more clearly apparent on reading the following detailed description of preferred embodiments thereof, which description is given, by way of nonlimiting example, with reference to the appended drawings, in which:
In the figures and in the rest of the description, elements that are identical or similar have been referenced with the same references. In addition, the various elements are not shown to scale to make the figures clearer. Moreover, the various embodiments and variants are not exclusive from one another and may be combined together. Unless otherwise indicated, the terms “substantially”, “about” and “of the order of” mean to within 10%.
The invention relates to a method for producing a first microelectronic chip intended to be hybridized with a second microelectronic chip at a hybridization temperature Th higher than room temperature. By hybridization, what is meant is an assembly of two microelectronic chips so as to mechanically fasten the chips to each other, and to achieve an electrical connection.
The microelectronic chips may comprise integrated circuits and/or optically active elements such as light-emitting diodes or photodiodes. Preferably, the first chip is an optoelectronic chip comprising a matrix array of light-emitting diodes or photodiodes, and the second microelectronic chip comprises an integrated circuit forming a readout circuit intended to apply a control signal or read signal to the light-emitting diodes or to the photodiodes. A chip may be produced from a semiconductor wafer and have dimensions of width, length or diameter, substantially equal to those of the semiconductor wafer. It may also have dimensions smaller than those of the semiconductor wafer.
Each microelectronic chip may comprise one or more layers of various materials each having a specific thermal expansion coefficient. The thermal expansion coefficient of a material expresses the relative elongation (l2−l1)/l1 of the material for a given temperature difference T2−T1. In other words:
α=(l2−l1)/(l1·(T2−T1)),
where l1 is the length of the material at the temperature T1, and l2 is the length at a temperature T2 higher than T1.
In the case of a chip comprising a plurality of layers of different materials, the apparent thermal expansion coefficient {tilde over (α)} at a given face of the chip is defined as being the relative elongation ({tilde over (l)}2−{tilde over (l)}1)/{tilde over (l)}1 of the chip at the face in question for the given temperature difference T2−T1. In other words: α=({tilde over (l)}2−{tilde over (l)}1)/({tilde over (l)}1·(T2−T1)), where {tilde over (l)}1 and {tilde over (l)}2 are here lengths measured at the face in question. The apparent thermal expansion coefficient may therefore be measured simply, at the face in question of the chip.
The apparent thermal expansion coefficient of a chip, when the latter is formed from a plurality of layers of different materials, differs from the average thermal expansion coefficient of the chip, which essentially corresponds to a weighting of the thermal expansion coefficients of each layer of the chip depending on their volume fraction, thickness and/or coefficients of elasticity (Young's modulus and Poisson's ratio). Thus, the average thermal expansion coefficient of a layer comprising a plurality of different materials may be expressed as: <α>=Σiαiνi, where αi is the thermal expansion coefficient of the ith material and νi is the volume fraction of the ith material in the layer. In addition, the average thermal expansion coefficient of a chip comprising a plurality of layers of different materials may be expressed as:
<α>=(ΣiαieiEi/[(1−νi)·(1−αiΔT)])/(ΣieiEi/[(1−νi)·(1−αiΔT)]),
where αi is the thermal expansion coefficient of the material of the ith layer, ei is the thickness of the ith layer, and Ei and νi are the Young's modulus and the Poisson's ratio of the material of the ith layer.
Moreover, a layer or chip is said to be based on a material when its average thermal expansion coefficient is substantially equal to the thermal expansion coefficient of the material. By way of example, a layer comprising a plurality of light-emitting diodes made of GaN may comprise segments electrically isolating the diodes from one another made of a dielectric, for example an oxide or nitride of silicon. Such a layer is then said to be based on GaN when its average expansion coefficient is substantially equal to that of GaN.
The first and second microelectronic chips each comprise N×M electrical interconnection pads via which the mechanical assembly of and the electrical connection between the chips are intended to be obtained. The values N and M may be identical or different. The N×M interconnection pads are located on a connection face of the chip, and are spaced apart from one another, preferably periodically with a pitch p. The pitch p is here considered to be identical along the axis of the N pads and along the axis of the M pads, but it may be different. They are made from at least one electrically conductive material. The interconnection pads of the first chip and/or of the second chip, here of the second chip, comprise a meltable material the melting point of which is lower than or equal to the hybridization temperature. By way of example, it may be a question of bumps made of indium or SnAgCu (SAC) or of alloys thereof. The assembly of the microelectronic chips then corresponds to a hybridization achieved by melting.
The invention mainly relates to a method for producing a first microelectronic chip so that, during its hybridization with a second microelectronic chip, the interconnection pads have a relative misalignment smaller than or equal to a preset threshold. By relative misalignment, what is meant is the distance, in the plane parallel to the connection faces, between the center, or barycenter, of an interconnection pad of the first chip and the center, or barycenter, of the interconnection pad, of the second chip, with which it was initially aligned.
The first chip P1 comprises a layer 13, called the layer of interest, having a thermal expansion coefficient αci, a thickness denoted eci, and a Young's modulus Eci. The layer of interest 13 is based on a material of interest, here a crystalline semiconductor material. Thus, the coefficient αci of the layer of interest 13 is substantially equal to the thermal expansion coefficient of the material of interest. The material of interest may be a III-V semiconductor compound, i.e. a compound containing III elements and elements from elements V of the periodic table, for example GaN, or a II-VI semiconductor compound, or even a IV semiconductor compound such as germanium. It may extend continuously in the plane of the layer and through all or some of the thickness of the layer, or, as a variant, may extend so as to form segments or zones that are separate from one another.
In this example, the first chip P1 is an optoelectronic chip the layer of interest 13 of which comprises a matrix array of light-emitting diodes that are based on GaN (not shown). The light-emitting diodes may have an identical or similar structure to that described in patent application FR3023061, or to that described in the publication by Fan et al entitled III-nitride micro-emitter arrays development and applications, J. Phys. D: Appl. Phys. 41 (2008) 094001.
The first chip Pt comprises a so-called connection face 11 at which is located a matrix array of N×M electrical interconnection pads 12. The interconnection pads 12, which are made of a material that is electrically conductive and optionally transparent to the light radiation emitted by the diodes, make electrical contact with the light-emitting diodes. The interconnection pads 12 are spaced apart from one another, preferably periodically with a pitch p.
The second microelectronic chip P2 has a second so-called connection face 21 on which is located a matrix array of N×M electrical interconnection pads 22. The interconnection pads 22 here contain a meltable material that melts at the hybridization temperature Th, and are spaced apart from one another in an identical way to the pads 12 of the chip P1. The chip P2 has a thermal expansion coefficient, called the apparent thermal expansion coefficient, denoted {tilde over (∝)}P2, defined at the connection face 21.
The chip P2 comprises a so-called carrier layer 24 having a thickness ecs and made of a material having a thermal expansion coefficient αcs. By way of example, the carrier layer 24 may be a substrate, or wafer, of silicon of a thickness of 725 m. The thermal expansion coefficient αcs, is then about 2.6×10−6 K−1.
The chip P2 may comprise other layers than the carrier layer 24, notably a layer 23 referred to as the integrated-circuit layer formed from an electrically insulating material, for example a dielectric such as SiO2, in which are found electrical connection lines (not shown) made of an electrically conductive material, for example a metal. This integrated-circuit layer 23 is located between the connection face 21 and the carrier layer 24.
The second chip P2 is based on the material of the carrier layer 24, so that it has an apparent thermal expansion coefficient {tilde over (∝)}P2, at the connection face 21, substantially equal to the thermal expansion coefficient αcs of the carrier layer 24, in other words: {tilde over (∝)}P2˜αcs.
However, the apparent thermal expansion coefficient {tilde over (∝)}P2 of the chip P2 is lower than the thermal expansion coefficient αci of the layer of interest 13 of the chip P1. By way of example, the coefficient αci is about 5.6×10−6 K−1 for a layer of interest 13 based on GaN and the apparent coefficient {tilde over (∝)}P2 is about 2.6×10−6 K−1 for a chip P2 based on silicon. According to the invention, it is sought to mechanically constrain the layer of interest 13 of the chip P1 in order to control and limit the relative misalignment ΔL of the interconnection pads 12 with respect to those 22 of the chip P2.
To do this, a first step consists in considering, on the one hand, the thermomechanical properties of the layer of interest 13 of the chip P1 and, on the other hand, the thermomechanical properties of the second chip P2. Thus an input dataset is obtained, namely:
A second step consists in determining a maximum threshold value ΔLmax for the relative misalignment ΔL between the interconnection pads 12 of the chip P1 and the interconnection pads 22 of the chip P2, so as to limit or even avoid the risk of loss of mechanical and therefore electrical contact between the interconnection pads.
This maximum threshold value ΔLmax notably depends on the spacing between adjacent interconnection pads 12, 22 of a given connection face 11, 21. Thus, in the case where the N*M interconnection pads are spaced apart from one another periodically with a pitch p, the maximum threshold value ΔLmax of the relative misalignment ΔL may be lower than or equal to p/2, and preferably be lower than or equal to p/4. The pads may have an average dimension, in the XY plane, substantially equal to p/2. Preferably, the maximum threshold value ΔLmax of the relative misalignment ΔL may be lower than or equal to the average dimension of the pads, for example equal to p/2, and preferably be lower than or equal to half the average dimension of the pads, for example equal to p/4. By average dimension of a pad, what is meant is the dimension of width or of length of the pad, or even of diameter, along an axis passing through the N or M interconnection pads.
Advantageously, the maximum threshold value ΔLmax may be expressed in terms of the apparent thermal expansion coefficient {tilde over (α)}P1 of the chip P1 at its connection face 11. Thus, the maximum threshold value ΔLmax of the relative misalignment is reached, for a maximum value {tilde over (α)}P1max of the apparent expansion coefficient {tilde over (α)}P1 of the chip P1 at its connection face 11, using the relationship: {tilde over (α)}P1max˜2·ΔLmax/(L·ΔT)+{tilde over (α)}P2. For example, in the case of an N×N matrix array of interconnection pads spaced apart periodically by a pitch p, and for a maximum relative misalignment ΔLmax substantially equal to p/2, the length L being able to be estimated to be N·p, a maximum value {tilde over (α)}P1max substantially equal to 1/(N·ΔT)+αP2 is obtained.
Thus, for a matrix array of N×N interconnection pads to be hybridized and a given temperature increase ΔT, the maximum value {tilde over (α)}P1max of the apparent thermal expansion coefficient of the chip P1 at the connection face 11 is determined.
Thus, if it is desired to be able to hybridize chips P1 and P2 having a matrix array of N×N=4000×4000 interconnection pads, the maximum value {tilde over (α)}P1max is about 3×10−6 K−1.
A third step consists in determining threshold values for thermomechanical and dimensional characteristics of the chip P1, the latter then being formed from the layer of interest 13 to which is fastened a layer 15, called the handle layer, by means of an intermediate layer of adhesive 14, in such a way that, during the hybridization of the chips P1 and P2, the relative misalignment ΔL is substantially equal to the maximum threshold value ΔLmax. This is achieved when the apparent expansion coefficient {tilde over (α)}P1 of the chip P1 is substantially equal to the maximum value {tilde over (α)}P1max.
The handle layer 15 is based on a material that is preferably identical to the material of the carrier layer 24 of the chip P2, and hence:
The layer of adhesive 14 has the following characteristics:
The minimum thickness ecpmin of the handle layer 15, on the one hand, and the maximum value eccmax, the minimum value Eccmin and the maximum value Eccmax of the layer of adhesive 14, on the other hand, may be determined via a parametric study carried out by numerical simulation, in particular by means of the software package ANSYS®, of the thermomechanical behavior of the chip P1 modelled using a finite element method.
In this example, the variables that are the thickness ecp of the handle layer 15, and the thickness ecc and the Young's modulus Ecc of the layer of adhesive 14, are varied so that the apparent expansion coefficient {tilde over (α)}P1 of the chip P1 at its connection face 11 has a value equal to the maximum value {tilde over (α)}P1max.
The chip P1 comprises a layer of interest 13 based on GaN, and has a thermal expansion coefficient αci equal to about 5.6×10−6 K−1, a thickness eci of about 5 μm, a Young's modulus Eci equal to about 390 GPa and a Poisson's ratio νci equal to about 0.33. The layer of adhesive 14 has a thermal expansion coefficient αcc equal to about 86×10−6 K−1, a thickness ecc the maximum value of which is to be determined, a Young's modulus Ecc the minimum and maximum values of which are to be determined, and a Poisson's ratio of about 0.35, here in the case of an epoxy adhesive, for example the adhesive EPO-TEK E360. The handle layer 15 is based on silicon. It has a thermal expansion coefficient αcp equal to about 2.6×10−6 K−1, a thickness ecp the minimum value of which is to be determined, a Young's modulus Ecp equal to about 130 GPa, and a Poisson's ratio of about 0.28.
As illustrated in
The inventors have demonstrated that, generally, the value of the apparent thermal expansion coefficient {tilde over (α)}P1 of the chip P1 at the connection face 11 is lower than or equal to the maximum value {tilde over (α)}P1max when the value of the Young's modulus Ecc of the layer of adhesive 14 belongs to an interval bounded by a minimum value Eccmin and a maximum value Eccmax, the limits being included.
Specifically, it would appear that, when the Young's modulus Ecc has a value lower than the minimum value Eccmin, the apparent thermal expansion coefficient {tilde over (α)}P1 is higher than the maximum value {tilde over (α)}P1max. Specifically, there is then a mechanical decoupling, in terms of transmission of mechanical stresses, between the layer of interest 13 of high thermal expansion coefficient and the handle layer 15 of low thermal expansion coefficient. In other words, during the application of the hybridization temperature Th, there is a lack of transmission of mechanical stresses between the handle layer 15 and the layer of interest 13 at the layer of adhesive 14, so that the layer of interest 13 is then not or hardly stressed by the handle layer 15.
It would furthermore appear that, when the Young's modulus has a value higher than the maximum value Eccmax, the apparent thermal expansion coefficient {tilde over (α)}P1 also becomes higher than the maximum value {tilde over (α)}P1max. In this case, there is also a decoupling of mechanical stresses between the handle layer 15 and the layer of interest 13. However, on application of the hybridization temperature Th, the layer of interest 13 is essentially coupled to the layer of adhesive 14, which has a very high thermal expansion coefficient, and not to the handle layer 15.
It would therefore appear that a satisfactory coupling of mechanical stresses between the handle layer 15 and the layer of interest 13 is possible when the value of the Young's modulus Ecc of the adhesive is comprised between the minimum value Eccmin and the maximum value Eccmax. This is particularly surprising in so far as the adhesive has a high thermal expansion coefficient, here 85×10−6 K−1, much higher than that of the handle layer 15 and than that of the layer of interest 13. Now, document WO 2013/068891 teaches that an adhesive of high thermal expansion coefficient prevents satisfactory transmission of mechanical stresses between two substrates. Those skilled in the art would therefore have considered that adhesively bonding the layer of interest 13 to a handle layer 15 of low thermal expansion coefficient would not have allowed the maximum value {tilde over (α)}P1max of the apparent thermal expansion coefficient {tilde over (α)}P1 to be reached in so far as the thermal expansion coefficients of adhesives generally have very high values.
A fourth step consists in depositing the layer of adhesive 14 on the face 13a of the layer of interest 13 opposite to the connection face 11, then in fastening the handle layer 15 to the layer of adhesive 14.
The layer of adhesive 14 is chosen so that, on the one hand, its thickness ecc is smaller than or equal to the maximum value eccmax determined beforehand, and, on the other hand, so that its Young's modulus Ecc is comprised between the minimum value Eccmin and maximum value Eccmax determined beforehand.
The handle layer 15 is chosen so that, on the one hand, its thickness ecp is larger than or equal to the minimum value ecpmin determined beforehand, and, on the other hand, so that its thermal expansion coefficient αcp is lower than or equal to the apparent coefficient {tilde over (∝)}P2 of the chip P2.
The layer of adhesive 14 may have a thermal expansion coefficient αcc higher than the coefficient αci of the layer of interest 13 and than the coefficient αcp of the handle layer 15. As mentioned above, the inventors have demonstrated the satisfactory transmission of mechanical stresses between the handle layer 15 and the layer of interest 13 during the hybridization at the temperature Th, thus allowing the expansion of the layer of interest 13 to be limited with the aim of controlling the relative misalignment between the interconnection pads.
Generally, but in particular in the case of a chip P1, comprising a layer of interest 13 based on GaN adhesively bonded to a handle layer 15 made of silicon, hybridized with a chip P2 based on silicon, it is advantageous for the layer of adhesive 14 to have a thickness ecc smaller than or equal to 4 times the thickness eci of the layer of interest 13, and preferably smaller than or equal to 2 times this thickness eci. It is also advantageous for the layer of adhesive 14 to have a Young's modulus Ecc comprised between 90 MPa and 40 GPa. In addition, it is advantageous for the thickness ecp of the handle layer 15 to be at least 20 times larger than the thickness eci of the layer of interest 13. A relative misalignment smaller than or equal to p/2 is then obtained between the chips P1 and P2 each of which has N×M interconnection pads, the highest of N and M being lower than or equal to about 4000.
Here and for the rest of the description a direct three-dimensional coordinate system (X, Y, Z) is defined where the X and Y axes form a plane parallel to the main plane of the layer of interest 13, and where the Z axis is oriented substantially orthogonally to the main plane of the layer of interest 13. In the rest of the description, the terms “vertical” and “vertically” are understood to be relative to an orientation substantially parallel to the Z axis, and the terms “horizontal” and “horizontally” as being relative to an orientation substantially parallel to the (X, Y) plane.
With reference to
Here a matrix array (not shown) of light-emitting diodes is produced, for example using the method described in patent application FR3023061. Next, the N×N or N×M interconnection pads 12 are produced on the connection face 11 of the layer of interest 13. The interconnection pads 12 are here segments of an electrically conductive and transparent material, such as ITO, that are electrically connected to the light-emitting diodes.
A temporary layer of adhesive 17, for example of an epoxy adhesive, is deposited so as to cover the connection face 11 of the layer of interest 13, then a temporary handle layer 18, for example a substrate or wafer, of silicon or of a material the thermal expansion coefficient of which is close to that of Si, is affixed (
With reference to
Next, the layer of adhesive 17 and the temporary handle layer 18 are removed so as to free, i.e. to uncover, the connection face 11 of the chip P1 and the interconnection pads 12 (
With reference to
It is then possible to thin the carrier layer 24 of the chip P2 (
It is also possible to remove the handle layer 15 and the layer of adhesive 14 of the chip P1 (
Particular embodiments have just been described. Various variants and modifications will appear obvious to those skilled in the art.
Number | Date | Country | Kind |
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16 60118 | Oct 2016 | FR | national |
Filing Document | Filing Date | Country | Kind |
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PCT/FR2017/052828 | 10/16/2017 | WO | 00 |
Publishing Document | Publishing Date | Country | Kind |
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WO2018/073517 | 4/26/2018 | WO | A |
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20200058837 A1 | Feb 2020 | US |