This disclosure generally relates to methods of manufacturing semiconductor devices, and more particularly relates to methods of bonding of multiple substrates.
Wafer to wafer bonding, chip to chip bonding, and chip to wafer bonding (generally substrate to substrate bonding) are being implemented to continue Power-Performance-Area-Cost (PPAC) scaling for complex circuits such as are implemented in Systems on Chip (SOCs). Conventional bonding techniques, such as direct bonding and hybrid bonding, utilize high pressure and/or high temperature to achieve reliable oxide-to-oxide bonding adhesion between the substrates. Typically, conventional technologies or processes of bonding two substrates may have a high penetration depth into a bonding interface and may damage the materials at this interface through physical sputtering. For example, the materials at this interface may have their chemical states and compositions modified during this penetration. Improved lower temperature bonding technologies with excellent adhesion are thus desired.
According to one implementation, a method of bonding a first surface for bonding to a second surface may include exposing the first surface to a plasma having an electron density in a range between 1×109 cm−3 and 1×1012 cm−3, and including a reducing agent; and bonding the first surface to the second surface. In other embodiments, the electron density of the plasma is in a range between 1×1010 cm−3 and 1×1011 cm−3.
The plasma may have an electron temperature of less than 1 eV. The electron temperature may be in a range between 0.2 eV and 0.8 eV. The electron temperature may be in a range between 0.3 eV and 0.7 eV. The method may include, before bonding the first surface to the second surface, exposing the second surface to the plasma. The method may include, after bonding the first surface to the second surface, annealing a bond interface between the first surface and the second surface.
According to another implementation, a method of activating a first surface for bonding to a second surface may include exposing the first surface to a plasma having an electron density in a range between 1×109 cm−3 and 1×1012 cm−3; and bonding the first surface to the second surface, and the plasma is generated by a plasma generator using a slot-plane-antenna (SPA) technique. In other embodiments, the electron density of the plasma is in a range between 1×1010 cm−3 and 1×1011 cm−3.
The plasma may have an electron temperature of less than 1 eV. The electron temperature may be in a range between 0.2 eV and 0.8 eV. Before bonding the first surface to the second surface, the second surface may be also exposed to the plasma. After bonding the first surface to the second surface, a bond interface between the first surface and the second surface may be annealed.
According to yet another implementation, a method of activating a first surface for bonding to a second surface includes exposing the first surface to a plasma including a reducing agent; and bonding the first surface to the second surface. The plasma is generated by a plasma generator using a slot-plane-antenna (SPA) technique.
The reducing agent may be selected from a group consisting of H2, H2O, H2O2, CO, CO2, NH3, CH4, SO2, H2S, and NO. The reducing agent may be selected from a group consisting of volatile organic compounds. One of the volatile organic compounds may be selected from a group consisting of C2H6, C3H8, C4H10, C2H4 and C2H2.
According to still yet another implementation, a chamber for activating a surface includes a first wafer carrier configured to hold a first wafer having a first surface facing up; a plasma generator configured to generate a plasma using a slot-plane-antenna (SPA) technique; a plasma inlet port connected to the plasma generator and configured to direct the plasma toward the first surface of the first wafer; and a reducing agent inlet port connected to a reducing agent supply to supply a reducing agent into the chamber. The plasma has an electron density in a range between 1×109 cm−3 and 1×1012 cm−3 and an electron temperature of less than 1 eV.
The plasma may have an electron temperature of less than 1 eV. The reducing agent may be selected from a group consisting of H2, H2O, H2O2, CO, CO2, NH3, CH4, SO2, H2S, NO, and a volatile organic compound.
Non-limiting embodiments of the present disclosure are described by way of example with reference to the accompanying figures, which are schematic and are not intended to be drawn to scale. Unless indicated as representing the background art, the figures represent aspects of the disclosure. For purposes of clarity, not every component may be labeled in every drawing. In the drawings:
Reference will now be made to the illustrative embodiments depicted in the drawings, and specific language will be used here to describe the same. It will nevertheless be understood that no limitation of the scope of the claims or this disclosure is thereby intended. Alterations and further modifications of the inventive features illustrated herein, and additional applications of the principles of the subject matter illustrated herein, which would occur to one skilled in the relevant art and having possession of this disclosure, are to be considered within the scope of the subject matter disclosed herein. Other embodiments may be used, or other changes may be made without departing from the spirit or scope of the present disclosure. The illustrative embodiments described in the detailed description are not meant to be limiting of the subject matter presented.
According to some embodiments, before bonding (e.g., fusion or hybrid bonding) a first bonding surface of a first wafer and a second bonding surface of a second wafer, at least the first bonding surface is activated by utilizing a plasma. The plasma may have a high electron density and low electron temperature. In some embodiments, a reducing agent is added to the plasma. After at least the first bonding surface is activated, the first and the second bonding surfaces can be brought together and bonded.
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In some embodiments, the plasma 201 has a high electron density in a range between 1×109 cm−3 and 1×1012 cm−3, and in other embodiments, the plasma 201 has a high electron density in a range between 1×1010 cm−3 and 1×1011 cm−3.
In an embodiment, the electron temperature of the plasma 201 is less than 1 eV. In another embodiment, the electron temperature of the plasma 201 is in a range between 0.2 eV and 0.8 eV. In yet another embodiment, the electron temperature of the plasma 201 is in a range between 0.3 eV and 0.7 eV. In still yet another embodiment, the electron temperature of the plasma 201 is in a range between 0.4 eV and 0.6 eV.
In some embodiments, the low ion energy plasma 201 can be e.g., an inductively coupled plasma (ICP), a capacitively coupled plasma (CCP), and a slotted plane antenna (SPA) plasma, and can be generated by using any plasma generating systems. As such, the surface 208A over the dielectric layer 204A is made ready for bonding.
By minimizing the ion energy of the plasma 201, ion bombardment and plasma penetration depth into a bonding interface 210 between the wafers 200A and 200B are minimized. By lowering the penetration depth into the bonding interface 210, the amount of conductive material that can be damaged or modified is limited or restricted to the top surface (e.g., 208A). While there may still be some resistive species present, the quantity will be much lower than that which would be present after a conventional plasma activation. Since bonding strength is primarily dependent on the surface quality, lowering the penetration depth will not lower the bond strength of the dielectric bond layer 204A at bond surface 208A.
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During the activation, the plasma gas 301 can advantageously modify the bonding layer material to improve bonding strength thereof, however, may also disadvantageously modify the conductive material to create more resistive species. If only reducing agent gas 303 is used, all the materials on the bonding interface 310A will be reduced to their initial state, which can advantageously improve conductivity of the electrical contacts, however, may also disadvantageously reduce the bond strength of the material. By adding the reducing agent gas 303 to the plasma gas 301, through either a pulsed addition or a simultaneous addition, the strength of the bonding interface 310A can be advantageously increased, while advantageously minimizing the creation of high resistivity species at the surface of the conductive material 306A of the wafer 300A that receives a surface activation operation.
As such, by using such a plasma having a low ion energy and high electron density, the thickness of the modified surface is very thin. By introducing such a reducing agent gas, the surface of the conductive material will be reduced. Through the combination of using such a plasma and adding such a reducing agent gas, bonding strength of the bonding surface (e.g., 408A) that receives a surface activation operation is improved, and all high resistive species can be eliminated from the surface of a conductive material after the activation process.
In some embodiments, the first wafer carrier 510 is configured to hold and move a first wafer 502A that has a first surface 508A facing up. In some embodiments, the second wafer carrier 512 is configured to hold and move a second wafer 502B that has a second surface 508B facing down.
In some embodiments, the plasma generator 522 generates a plasma (or plasma gas) 501 by using a slot-plane-antenna (SPA) technique. In some embodiments, the plasma inlet port 520 is connected to the plasma generator 522, and configured to supply the plasma 501 into the chamber 500 and to direct the plasma 501 toward the first surface 508A of the first wafer 502A. In some embodiments, the plasma 501 generated by using the SPA technique has a high electron density and a low electron temperature in the chamber 500. In some embodiments, the plasma 501 has a high electron density in a range between 1×109 cm−3 and 1×1012 cm−3, and in other embodiments, the plasma 501 has a high electron density in a range between 1×1010 cm−3 and 1×1011 cm−3. In an embodiment, the electron temperature of the plasma 501 is less than 1 eV. In another embodiment, the electron temperature of the plasma 501 is in a range between 0.2 eV and 0.8 eV. In yet another embodiment, the electron temperature of the plasma 501 is in a range between 0.3 eV and 0.7 eV. In still yet another embodiment, the electron temperature of the plasma 501 is in a range between 0.4 eV and 0.6 eV.
In some embodiments, the reducing agent inlet port 530 is connected to a reducing agent supply 532 and configured to supply a reducing agent (or reducing agent gas) 503 into the chamber 500. As such, the reducing agent gas 503 is combined with the plasma gas 501 within the chamber 500 to activate at least the first surface 508A of the first wafer 502A.
After performing a surface activation to at least the first surface 508A of the first wafer 502A, the first wafer 502A and the second wafer 502B are brought together and aligned each other, and then bonded each other in accordance with some embodiments. In some embodiments, the surface 508B of the second wafer 502B is similarly activated as the surface 508A of the first wafer 502A. In some embodiments, thermal energy is applied to the first wafer 502A and the second wafer 502B to anneal a bond interface formed therebetween.
What has been described and illustrated herein is an example along with some of its variations. The terms, descriptions and figures used herein are set forth by way of illustration only and are not meant as limitations. Many variations are possible within the spirit and scope of the subject matter, which is intended to be defined by the following claims 1-20 and their equivalents, in which all terms are meant in their broadest reasonable sense unless otherwise indicated.
This application claims priority to and the benefit of U.S. Provisional Application No. 63/447,693, filed Feb. 23, 2023, entitled “BONDING LAYER AND PROCESS,” which is incorporated herein by reference in its entirety for all purposes.
Number | Date | Country | |
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63447693 | Feb 2023 | US |