The present invention relates to a method for pre-processing semiconducting thermoelectric materials for metallization, interconnection and bonding to form a thermoelectric device, and thermoelectric devices utilising the pre-processed processing semiconducting thermoelectric materials made by the method.
The Seebeck effect is one of three possible expressions of the thermoelectric effect, namely the direct conversion of thermal energy to electric energy found in some materials when subject to a temperature gradient creating a heat flux through the material. The Seebeck effect will when connecting the material to a heat sink on one side and a heat source on the opposite side, create an electric potential which may be utilised for driving an electrical device or charging a battery. The thermoelectric conversion efficiency is dependent on the ratio electric over thermal conductivity and is usually defined as the dimensionless figure of merit, ZT:
where σ is electric conductivity, S is a thermoelectric coefficient often termed the Seebeck-coefficient, κ is thermal conductivity, and T is absolute temperature.
Skutterudite is a class of minerals discovered at Skutterud in Norway in 1827, often denoted by the general formula TPn3, where T is a transition metal such as i.e.; Co, Rh, In, Fe, and Pn is one of the pnictogens (member of the nitrogen group in the periodic table); P, As or Sb.
The unit cell of the skutterudite structure contains 32 atoms arranged into the symmetry group Im3 as shown schematically in
The skutterudite is semiconducting when electric neutral, that is, maintains a ratio of T:[Pn4]=4:3. Further, due to its covalent bonding structure, the skutterudite crystal lattice has a high carrier mobility. At the same time, the complexity of the crystal lattice combined with the heavy atoms results in a relatively low thermal conductivity, so that semiconducting skutterudites often have a favourable electric over thermal conductivity ratio and thus promising figures of merit, ZT.
Semiconducting materials conduct electricity by using two types of charge carriers; electrons and holes (vacant electron sites in the crystal lattice atoms). By doping, i.e. substituting one or more of the T atoms in the crystal lattice with an atom of another element, the semiconducting material can be made to dominantly conduct electric charges by either electrons (n-type conductivity) or holes (p-type conductivity), depending on which dopant (substitute element) being introduced.
An n-type and a p-type semiconductor may be electrically connected to form an electric circuit as schematically illustrated in
The configuration shown in
A thermoelectric device of this kind may provide a compact, highly reliable, long lasting, and noiseless and pollution free manner of generating electric power from a heat source.
U.S. Pat. No. 6,660,926 discloses that the thermal conductivity of skutterudite can be reduced, and thus obtain a higher figure of merit, by filling the two vacant smaller cubes of the 32-atom unit cell with a binary compound and in addition substituting elements to replace part of the original transition metal and/or pnictogen elements to conserve the valence electron count of the unit cell. The document discloses several examples of such materials having high ZT-values, of which one is CeFe4-xCoxSb12.
From WO 2011/014479 it is known that owing to its large crystal cells, heavy atomic mass, large carrier mobility and disturbance of filled atoms in the Sb-dodecahedron, thermoelectric materials of CoSb3 based skutterudite exhibit superior thermoelectric properties at temperatures in the range from 500 to 850 K. The document discloses that the n-type skutterudite YbyCo4Sb12 has a ZT of 1.4 and that p-type skutterudite CaxCeyCo2.5Fe1.5Sb12 has a ZT of 1.2. The document discloses further that at 850 K, the vapour pressure of Sb is about 10 Pa, leading to a serious degradation of the semiconductor due to loss of the element Sb. The solution to this problem according to WO 2011/014479 is to coat the skutterudite material with a first metal layer and a second metal oxide layer. The metal layer may be one of; Ta, Nb, Ti, Mo, V, Al, Zr, Ni, NiAl, TiAl, NiCr, or an alloy of two or more of them; and the metal oxide may be one of TiO2, Ta2O5, Al2O3, ZrO2, NiO2, SiO2, or a composite of two or more of them, or a multi-layer of two or more of them.
According to U.S. Pat. No. 6,673,996, skutterudite is the only known single thermoelectric material suitable for use over the temperature range from room temperature up to about 700° C. The document describes CeFe4Sb12 based alloys and CoSb3 based alloys as suited materials for p-type and n-type thermoelectric materials, respectively. On the cold side, the thermoelectric materials are connected to a cold shoe made of Al2O3 coated with a layer of Cu to provide the electric and thermal contact. In order to protect the thermoelectric material from in-diffusion of Cu, there is employed a diffusion barrier of Ni which is formed onto the Cu-layer by electroplating.
Another example of employing CoSb3 based skutterudite as thermoelectric material in a thermoelectric device is shown in U.S. Pat. No. 6,759,586. In this document there is disclosed a thermoelectric device comprising a piece of CoSb3 based skutterudite as either n-type or p-type conductivity attached to an electrode made of a Fe-alloy or an Ag-alloy, and which employs a diffusion barrier between the skutterudite and the electrode made of Sb and one of Au, Ag or Cu.
From WO 2012/071173 it is known a thermoelectric device using skutterudite as the thermoelectric conversion material which is covered with a thin barrier layer deposited by atomic layer deposition. Examples of suited barrier layers include metal oxides such as; Al2O3, TiO2, Ta2O5, SnO2, ZnO, ZrO2, and HfO2), and metal nitrides such as; SiNx, TiN, TaN, WN, and NbN).
EP 2 242 121 describes a certain class of filled skutterudite suited for being used as thermoelectric conversion material at temperatures in the range from 20 to 600° C. The group is defined by the general formula: RrTt-mMmXx-nNn (0<r≤1, 3≤t-m≤5, 0≤m≤0.5, 10≤x≤15, 0≤n≤2), where R represents three or more elements selected from the group consisting of rare earth elements, alkali metal elements, alkaline-earth metal elements, group 4 elements, and group 13 elements, T represents at least one element selected from Fe and Co, M represents at least one element selected from the group consisting of Ru, Os, Rh, Ir, Ni, Pd, Pt, Cu, Ag, and Au, X represents at least one element selected from the group consisting of P, As, Sb, and Bi, and N represents at least one element selected from Se and Te. The document discloses further that in order to obtain a good junction between the thermoelectric conversion material end the electrodes of the thermoelectric device, it should be employed a joining layer between these phases comprising an alloy with a composition adjusted to match the thermal expansion coefficient of the thermoelectric conversion material. Examples of suited alloys for use as the joining layer includes titanium alloy of 50 to 100 weight % Ti, and from 0 to 50 weight % of at least one of Al, Ga, In, and Sn. In another example, the joining layer is made of a nickel alloy of 50 to 100 weight % Ni, and from 0 to 50 weight % of Ti. The electrode may be an alloy selected from the group of; titanium alloys, nickel alloys, cobalt alloys, and iron alloys.
Bader et al. 1994 [1] has studied bonding two metals together by use of solid-liquid interdiffusion (SLID) bonding, where a low melting point metal and a high melting point metal are bonded together by forming an intermetallic compound of the two metals at their joint. In one example, the document discloses bonding two pieces of nickel, each having a tin layer on one side, by gently pressing the sides with tin layers against each other and heating the pieces until the tin melts and maintaining the gentle pressure and the temperature until all liquid tin has reacted with the nickel and formed a solid Ni—Sn intermetallic compound which securely bonds the metal pieces together, as illustrated schematically in
US 2013/0152990 discloses use of the SLID-technology for bonding electrodes to thermoelectric conversion materials. The document mentions Bi2Te3, GeTe, PbTe, CoSb3, and Zn4Sb3 as examples of thermoelectric conversion materials, and the thermoelectric conversion material is first coated with a 1 to 5 μm thick barrier layer of Ni or other suited material, then with a 2-10 μm thick Ag, Ni or Cu layer, and finally with 1-10 μm thick Sn layer. The electrode is on one side first coated with a 2-10 μm thick Ag, Ni or Cu layer, and then with 1-10 μm thick Sn layer. The coated thermoelectric conversion material and the electrode are then laid with their Sn layers side by side and pressed together under a gentle heating until the Sn layers melt and react with the Ag, Ni or Cu to form solid intermetallic compounds bonding the electrode to the thermoelectric conversion material.
The main objective of the present invention is to provide a simple, cost-effective and robust method of pre-processing semiconducting thermoelectric materials for metallization, interconnection and bonding to form a thermoelectric device.
A further objective is to provide pre-processed thermoelectric materials made by the method, and in particular, filled and not filled CoSb3-based skutterudite thermoelectric conversion materials.
The invention is based on the realisation that a cost-effective, simple and resilient interconnection and bonding of semiconducting thermoelectric materials to the electrodes of thermoelectric devices, may be obtained by employing the solid-liquid interdiffusion bonding concept in combination with use of an adhesion layer/-diffusion barrier layer/adhesion layer structure (interchangeably also termed as; the ADA-structure) in-between the solid-liquid interdiffusion bonding layers and the semiconducting thermoelectric material.
Thus in a first aspect, the present invention relates to a method for forming a pre-processed semiconducting thermoelectric conversion material for metallization, interconnection and bonding, wherein the method comprises the following process steps in successive order:
employing at least one element of a n-type or p-type doped semiconducting thermoelectric conversion material having a first and second surface on opposite sides,
placing the at least one element of semiconducting thermoelectric conversion material into a deposition chamber, and then:
depositing a first bonding layer of a metal A directly onto the second adhesion layer on the first and second surface of element of the semiconducting thermo-electric conversion material, and
depositing a second bonding layer of a metal B directly onto the first bonding layer the on the first and second surface of the element of the semiconducting thermoelectric conversion material,
wherein
the melting point of metal A is higher than metal B and metal B is chemically reactive towards metal A at their common interface when subject to heating above the melting point of metal B forming an intermetallic compound by solid-liquid interdiffusion.
Alternatively, the first and second bonding layers of metal A and B, respectively, may advantageously also be deposited inside the same vapour deposition chamber as the ADA-structure by simply changing to precursor gas(es) forming the first and/or then the second bonding layer. That is, both the adhesion layer/diffusion barrier layer/adhesion layer structure (the ADA-structure) and the solid-liquid interdiffusion bonding layers may be formed in a chemical vapour deposition chamber, a physical deposition chamber, or an atomic deposition chamber, where the deposition of the different layers is obtained by feeding pre-cursor gases with varying chemical composition into the deposition chamber. Alternatively, the element of semiconducting thermoelectric conversion material may be taken out of the vapour deposition chamber after formation of the ADA-structure and then deposit the first and second bonding layers with electroplating or electro-less plating.
In a second aspect, the present invention relates to a thermoelectric device, comprising:
where
characterised in that
each of the N thermoelectric elements of n-type conductivity and the N thermoelectric elements of p-type conductivity have on their first and second surface:
The term “metallization, interconnection and bonding” as used herein means the formation of the mechanical, thermal and electric contacts in a thermoelectric device necessary for collecting and conducting the electric energy produced in the thermoelectric device.
The term “metal” as used in the first and second aspect of the invention is to be interpreted as metal in the generic sense of the term such that it encompasses elementary metal as well as alloys of the same metal. Thus, for example, if the metal in one example embodiment is Ni, the term may be interpreted to be elementary Ni or a Ni-alloy such as i.e. nickel vanadium alloy, nickel silver alloy or other nickel alloys.
The term “pre-processed semiconducting thermoelectric conversion material for metallization, interconnection and bonding” as used herein, means any element of semiconducting thermoelectric material intended to be electrically connected with other elements of semiconducting thermoelectric materials to form a thermoelectric device (interchangeably also termed as: TE-device), and which has been processed such that it is ready to be electrically connected with the other (which are similarly pre-processed) elements of semiconducting thermoelectric material of the TE-device by solid-liquid interdiffusion bonding (interchangeably also termed as: SLID-bonding). The pre-processing of the element of semiconducting thermo-electric material according to the present invention comprises at least depositing on areas on the element where a SLID-bonding is to be formed, in successive order; a first adhesion layer ensuring adequate mechanical bonding to the semiconducting material, a diffusion barrier layer to prevent detrimental inter-diffusion of elements between the semiconducting material and the electrode material, a second adhesion layer to obtain sufficient bonding to the diffusion barrier layer, and then a first and second metal layer which are to form the SLID-bond with corresponding layers on the electrode.
The term “element of semiconducting thermoelectric conversion material (inter-changeably also termed as: TE-element)” as used herein, means any lump, piece or other form of a compact mass of a semiconducting material exhibiting satisfactory ZT-values for being used in thermoelectric devices when doped to p-type or n-type conductivity. The first and second surfaces on opposite sides of the TE-element may advantageously be substantially parallel and planar surfaces on two opposite ends of the element to alleviate use of the SLID-bonding for interconnection of two or more TE-elements into a TE-device having the structures as illustrated in
Many semiconducting thermoelectric conversion materials may leach elements by solid interdiffusion etc. which are detrimental to the thermal and electric properties of the interconnection electrodes (the electric contact elements), such that it should be employed an intermediate diffusion barrier layer between the semiconducting thermoelectric conversion material and the electric contact elements to protect the electrodes. Thus, the invention according to the first and second aspect may advantageously comprise a thin layer of a thickness from 100 nm and above of a metal oxide or a metal nitride is often an excellent diffusion barrier. Examples of preferred diffusion barriers include, but are not limited to 100-1000 nm thick layers of CrNx, TaNx, or TiNx formed by vapour deposition. The thickness of the diffusion barrier layer may advantageously be in one of the following ranges: from, 50 to 5000 nm, from 75 to 3000 nm, from 100 to 2000 nm, from 150 to 1000 nm, from 150 to 750 nm, from 200 to 500 nm, from 200 to 400 nm or from 200 to 300 nm.
The adherence between the diffusion barrier layer and the semiconducting thermo-electric conversion material has sometimes proven to be insufficient to withstand the shear stresses arising form the thermal expansion involved in thermoelectric devices which may lead to an electrically disconnection between the TED-element and its electrode. It is thus common to increase the adherence between the TED-element and the electrode by applying an intermediate adhesion layer. The invention according to the first and second aspect should thus comprise a first adhesion layer which is deployed directly onto the first and second surface of each TED-element that is to be employed in the TE-device and which forms an intermediate layer between the TE-element and the diffusion barrier layer. Many metals are known to adhere well to both semiconducting materials and typical diffusion barriers and may thus be for being applied as the first adhesion layer. For instance, when the diffusion barrier layer is a metal nitride or metal oxide, any metal known to a person skilled in the art to form excellent bonding with semiconducting materials and metal oxides or metal nitrides may be applied by the first and second aspects of the present invention. The thickness of the first adhesion layer may advantageously be in one of the following ranges; from 20 nm to 2 μm, from 50 nm to 1.5 μm, from 100 nm to 1.5 μm, from 200 nm to 1.5 μm, or from 500 nm to 1.5 μm. The actual choice of which metal to be applied as the first adherence layer is usually dependent upon which materials are being applied in the semiconducting thermoelectric conversion material and in the diffusion barrier layer. However, a person skilled is able to make this selection from her/his general knowledge. Examples of suited metals for use as adhesion layers includes, but is not confined to; Cr, Cu, Sn, Ta, and Ti.
The adherence between the diffusion barrier layer and the first bonding layer of the metal system of the SLID-bonding has also proven to be a possibly problematic due to insufficient resilience towards thermally induces shear stresses. It is thus suggested by the present invention according to the first and second aspect to apply a second adherence layer in-between the diffusion barrier layer and the first bonding layer. The second adherence layer may as the first adherence layer, be a metal layer but not necessarily of the same metal as the first adherence layer. As far as the inventor knows, the use of a second adherence layer is not known in the prior art. The thickness of the second adhesion layer may be in one of the following ranges; from 20 nm to 1000 nm, from 30 nm to 750 nm, from 40 nm to 500 nm, from 100 nm to 400 nm, or from 150 nm to 300 nm. The actual choice of which metal to be applied as the second adherence layer is usually dependent upon which materials are being applied diffusion barrier layer and in the first bonding layer. A person skilled is able to make this selection from her/his general knowledge.
However, a substantial simplifying and work load saving in the production process may be obtained by choosing the same metal in both the first and second adhesion layers as the metal of the metal oxide or metal nitride of the diffusion barrier layer. In this case the ADA-structure is made up of one single metal in elementary form and as an oxide or nitride, such that the entire ADA-structure may be deposited in one single vapour deposition process by simply changing the composition of the pre-cursor gases being fed into the deposition chamber. Thus, if the diffusion barrier layer is made of one of the preferred layers of CrN, TaN, or TiN, both the first and second adhesion layers may advantageously be made of elementary Cr, Ta, or Ti, respectively.
The term “solid-liquid interdiffusion bonding” or “SLID-Bonding” as used herein, is a high temperature technique for interconnection of two metal phases by use of an intermediate metal phase and annealing such as described in i.e. Bader et al. 1994 [1]. The interconnection (bonding) is obtained by employing an intermediate metal phase which in the liquid phase is chemically reactive against the two outer metal phases forming solid intermetallic compounds, and which has a lower melting point than the two metal outer phases that are to be interconnected. SLID-bonding is also denoted as transient liquid phase bonding, isothermal solidification or off-eutectic bonding in the literature. Examples of suited metal systems for SLID-bonding comprise Au—In, Au—Sn, Ag—In, Ag—Sn, Cu—Sn, and Ni—Sn. In principle, any thickness of the layers of the metal system may be applied in a SLID-bonding. This also applies to the method according to the first and second aspect of the invention. However, in practice, it is advantageous that the initial thickness of the first bonding layer of metal A is in one of the following ranges; from 1 μm to 1 cm, from 1 μm to 0.5 cm, from 1 μm to 0.1 cm, from 2 μm to 500 μm, from 2 μm to 100 μm, from 2 μm to 50 μm, or from 3 μm to 10 μm. And the initial thickness of the second bonding layer of metal B may advantageously be in one of the following ranges; from 300 nm to 0.75 cm, 300 nm to 0.3 cm, 300 nm to 750 μm, from 200 nm to 400 μm, from 200 nm to 75 μm, from 200 nm to 30 μm, or from 300 nm to 3 μm. The term “initial thickness” of the bonding first and/or second binding layer is the thickness of the respective bonding layer before annealing and formation of the intermetallic compound(s). Both the chemical structure and physical dimensions of the resulting SLID-bond layers are somewhat changed as compared to the initial (non-reacted) bonding layers involved in the SLID-bonding.
The electric contact elements that are to be applied for electrically connecting the TE-elements into a TE-device should be a stratified layered element comprising two metal layers of the same metals as the stratified metal layers of the first and second bonding layer, respectively. That is, the electric contact element comprises a first bonding layer of metal A and a second bonding layer of metal B. The thickness of the second metal layer of the electric contact element may advantageously be the same as the thickness of the second boundary layer deposited on the TE-element; however this is not mandatory, other thicknesses may be applied if convenient. The same applies for the first boundary layer of the electric contact element, this may have the same thickness as the first boundary layer of the TE-element, but this is not mandatory, other thicknesses may be applied. It might i.e. be found advantageous to apply a thicker first boundary layer of the electric contact element to obtain mechanical strength. Thus any thickness within reasonable practical limits may be applied as the first boundary layer of the electric contact element.
The principle of forming a SLID-bonding is illustrated schematically in
The method according to the first aspect of the invention produces one TE-element, of either p-type conductivity or n-type conductivity, having the structure schematically illustrated in
In
The ADA/SLID-structure provides a very strong and resilient bonding between the electric contact elements and the TE-elements of the TE-device, and is thus especially suited for use in high-temperature appliances which involve relatively strong shear stresses at the bonding interfaces due to differences in the thermal expansions of the materials of the different layers, TE-element and electrode. Even though, the present invention may use any semiconducting thermoelectric conversion material, it is preferred to employ filled or non-filled CoSb3-based skutterudite thermoelectric conversion materials due to their promising figure of merit, ZT, at temperatures up to about 800° C. It is advantageous to employ a metal system with a thermal expansion as equal as the TE-element as possible. Thus, in the case of employing TE-elements of filled or non-filled CoSb3-based skutterudite thermoelectric conversion materials, it is preferred to employ the metal system Ni—Sn for the SLID-bonding.
The invention is described in more detail by way of example embodiments of a thermoelectric device with a similar construction as illustrated in figures.
The first example embodiment utilises a filled or non-filled CoSb3-based skutterudite as the semiconducting thermoelectric conversion material intended to operate at high temperatures, i.e. at temperatures in the range from about 0° C. to about 800° C.
Thus in the first example embodiment of the invention according to the first aspect, the invention is a method for forming a pre-processed semiconducting thermo-electric conversion material for metallization, interconnection and bonding, wherein the method comprises the following process steps in successive order:
employing at least one element of a n-type or p-type doped semiconducting thermoelectric conversion material of a filled or non-filled CoSb3-based skutterudite having a first and second surface on opposite sides,
placing the at least one element of semiconducting thermoelectric conversion material into a deposition chamber, and then:
wherein
the deposition chamber is either a chemical vapour deposition chamber, a physical deposition chamber, or an atomic deposition chamber, and the deposition of the different layers of steps i) to v) is obtained by feeding pre-cursor gases with varying chemical composition into the deposition chamber,
the non-metallic compound of the second metal is either a nitride or an oxide of the second metal, and
the melting point of metal A is higher than metal B and metal B is chemically reactive towards metal A at their common interface when subject to heating above the melting point of metal B forming an intermetallic compound by solid-liquid interdiffusion.
The first example embodiment also includes a thermo electric device utilising a filled or non-filled CoSb3-based skutterudite as the semiconducting thermoelectric conversion material. Thus, the example embodiment of the invention also comprises a thermoelectric device, comprising:
where
characterised in that
each of the N thermoelectric elements of n-type conductivity and the N thermoelectric elements of p-type conductivity have on their first and second surface:
Every layer of the ADA/SLID-structure of the first example embodiment may have the same thicknesses as given above in section “Description of the invention”. Also, in an especially preferred alternative of the example embodiment, the first metal of the first adhesion layer and the third metal of second adhesion layer is the same metal, and may be one of Cr, Ta or Ti. Further, the non-metallic compound of the second metal of the diffusion barrier layer is in this example embodiment a nitride of the same metal as employed in the adhesion layers, i.e. one of CrN, TaN or TiN, respectively. And further, the metal A of the first bonding layer is one of Au, Ag, Cu, Ni, a Ni—V alloy with from 6.5 to 7.5 atomic % V, and metal B is one of; In or Sn.
In a more preferred alternative of the first example embodiment, the first and second adhesion layers is a layer of at least 99.5 weight % pure Ti, the diffusion barrier layer is TiN, the metal A of the first bonding layer of both the TE-element and the electric contact element is Ni, and the metal B of the second bonding layer of both the TE-element and the electric contact element is Sn.
The combination of employing an adhesion layer of pure Ti having a more than 99.5% purity based on the total weight of the Ti-phase, a diffusion barrier layer of TiN and a contact layer of Ni has proven to provide an especially robust metalli-sation exhibiting excellent electric and thermal conductivities of CoSb3-based skutterudite thermoelectric conversion materials, which may easily and securely be bonded to the electrodes of the thermoelectric device by use of the SLID-technology. That is, the electrode may be bonded to the CoSb3-based skutterudite thermoelectric conversion material by depositing a contact layer of Ni and then a bonding layer of Sn on the electrode, and then bonding them together by pressing the bonding layers of Sn together and heating them until the Sn reacts with the Ni and forms one or more of the following intermetallic compounds; Ni3Sn, Ni3Sn2, or Ni3Sn4.
The inventor has discovered that the bonding strength and the electric and thermal conductivity of the layers forming the metallisation structure may be significantly improved by practically avoiding any oxidation of the metal phases (Ti, Ni or Sn) during and after deposition. That is, the deposition process should advantageously be performed in a protected atmosphere practically void of oxygen (i.e. having less than 50 ppm oxygen) or made under a vacuum (i.e. at a pressure of less than 1000 Pa). Alternatively, if the handling of the thermoelectric material after formation of the metallisation involves exposure to air/oxygen, the metallic surfaces deposition proves may include depositing 10 to 50 nm of Au on top of the metal layer as an oxidation resistance layer. The oxidation resistance layer may be applied onto either the Ti layer (the adhesion layer), the contact layer (Ni) or the bonding layer (Sn), or one two or more of these.
The thermoelectric elements of the second example embodiment are formed by depositing a Ti layer having a thickness of approximately 200 nm, a TiN layer having a thickness of approximately 1000 nm and a Ni layer having a thickness of approximately 1000 nm on p- and n-type thermoelectric elements (doped CoSb3) with a size of 4.5×4.5×3.5 mm3. The adhesion between the TE material and the metallization was then quantified by pull-testing before and after thermal aging. The pull-strength was above 20 MPa both for reference samples and thermally aged samples, and the fractures were cohesive TE material fractures (i.e. inside the bulk of the TE material), meaning that the adhesion strength between the TE material and the metallization is higher than the tensile bulk strength of the TE material.
The thermoelectric module of the third example embodiment is formed by depositing a Ti layer having a thickness of approximately 200 nm, a TiN layer having a thickness of approximately 1000 nm and a Ni layer having a thickness of approximately 2000 nm on p- and n-type thermoelectric elements (doped CoSb3) with a size of 4.5×4.5×3.5 mm3. Furthermore, a Cu layer with a thickness of approximately 20 μm, a Ni layer with a thickness of approximately 5 μm and a Sn layer with a thickness of approximately 2 μm is deposited on an alumina substrate. The functionalized TE elements are then placed on the substrate, and a thermos-compression bonding is performed in an inert atmosphere. The bonding is performed with a pressure of 2 MPa at 300° C. for 20 minutes forming a Ni—Sn SLID bond. The Ni—Sn SLID bond consist of pure Ni and Ni3Sn4, where the latter has a melting point close to 800° C., giving and high operating temperature. The bond also has high mechanical strength. Shear strength tests show that the bond strength is above 60 MPa, well above other known techniques stating bond strengths of approximately 10 MPa.
Number | Date | Country | Kind |
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20141357 | Nov 2014 | NO | national |
Filing Document | Filing Date | Country | Kind |
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PCT/EP2015/076291 | 11/11/2015 | WO | 00 |