The present invention relates generally to the creation of a diffusion barrier layer. More specifically, the invention relates to the creation of a diffusion barrier layer for copper.
The use of copper interconnects in semiconductor devices may require a barrier layer to surround the copper interconnect to prevent Cu+ ions from diffusing into a silicon oxide dielectric, also called silicon dioxide or oxide. Copper diffusion into an oxide may give rise to various detrimental phenomena, which may include poisoning of an active device. Current barrier layers may include titanium (Ti), tantalum (Ta), and derivatives of these metals such as nitrides and carbides of these metals. Silicon nitrides and carbides are also being employed as effective barriers. One example of a silicon carbide barrier layer would provide a first silicon carbide layer, on which a thick oxide deposition is placed. Another silicon carbide layer is placed over the oxide deposition. Another oxide deposition is placed over the second silicon carbide layer. The silicon carbide acts as a barrier for copper diffusion.
To avoid increasing the dielectric constant of the oxide, barrier layers should be thin. Current methods of forming barrier layers may be too porous or may be difficult to control to provide a thin barrier layer or may not be sufficiently pure.
It would be desirable to create thin barrier layers that have a high purity and low porosity, which may be more effective as barrier layers.
To achieve the foregoing and other objects and in accordance with the purpose of the present invention, a semiconductor device is provided. The semiconductor device comprises a dielectric layer, an electrically conductive copper containing layer, and a barrier layer separating the dielectric layer from the copper containing layer. The barrier layer comprises a silicon oxide layer and a dopant, where the dopant is a divalent ion, which dopes the silicon oxide layer adjacent to the copper containing layer.
In addition, a method of forming a barrier layer is provided. A silicon oxide layer with a surface is provided. The surface of the silicon oxide layer is doped with a divalent ion to form a barrier layer extending to the surface of the silicon oxide layer. An electrically conductive copper containing layer is formed on the surface of the barrier layer, where the barrier layer prevents diffusion of copper into the substrate.
These and other features of the present invention will be described in more detail below in the detailed description of the invention and in conjunction with the following figures.
The present invention is illustrated by way of example, and not by way of limitation, in the figures of the accompanying drawings and in which like reference numerals refer to similar elements and in which:
The present invention will now be described in detail with reference to a few preferred embodiments thereof as illustrated in the accompanying drawings. In the following description, numerous specific details are set forth in order to provide a thorough understanding of the present invention. It will be apparent, however, to one skilled in the art, that the present invention may be practiced without some or all of these specific details. In other instances, well-known process steps and/or structures have not been described in detail in order to not unnecessarily obscure the present invention.
To facilitate understanding,
The first barrier layer 112 and the second barrier layer 116 are formed from silicon oxide doped with a divalent ion dopant. Divalent ions are ions of elements from Groups IIa and IIb of the Periodic Table of Elements, although it is uncertain if all divalent ions would provide the desired barrier. More preferably, the dopant is selected from the group of beryllium, magnesium, calcium, strontium, and barium. In another preferred embodiment, the dopant is calcium. The dopant concentration may be measured by the ratio of dopant ions to silicon atoms in the silicon oxide. It is preferable that the ratio of dopant ions to silicon atoms be in the range from about 1:10 to 1:100. It is more preferable that the ratio of the dopant ions to silicon atoms be in the range from 1:10 to 1:30. Most preferably, the ratio of the dopant ions to silicon atoms is about 1:20. Preferably, the silicon oxide is amorphous silicon oxide.
In other semiconductor devices, the inventive barrier layer may be placed on only one side of a copper containing layer, where another type of barrier layer or no barrier layer may be placed on the other side of the copper containing layer. In addition, another type of dielectric may be used in the place of the undoped areas of silicon oxide.
Without being bound by theory, it is believed that the insertion of a divalent ion, such as calcium, into silicon oxide results in a barrier to Cu+ diffusion through oxide. Analysis based on quantum chemical results showed that interaction of atomic calcium with a siloxane ring leads to insertion of the calcium atom into the ring. Cu+ ions interacting with a siloxane ring containing an inserted calcium atom form several stable structures, which are complexes of Cu+ with the ring or a ring with Cu+ inserted within. The most favorable in energy are four structures, which are three complexes of Cu+ with the ring containing an inserted atom of Ca (I, III, IV) and one (II) with Cu+ inserted into the ring and a Ca atom above the ring.
The results obtained for Cu+ interaction with pure oxide and pure nitride rings confirm that the energy difference between states for the above case is sufficient for preventing Cu+ diffusion. In the case of oxide and nitride, Cu+ forms two stable complexes with basic ring units. Copper diffusion is determined on a microscopic level by the energy Ea for Cu+ jump from a more stable complex to a less stable one. Values of ΔE for these jumps are 0.37 and 1.57 eV for oxide and nitride, respectively. These values correlate with experimental data that nitride is a good barrier for Cu+ diffusion in contrast with oxide for which ΔE is quite small. ΔE for Cu+ interaction with Ca containing oxide rings being calculated to be 1.6-1.7 eV, indicates that an oxide with Ca inserted should serve as a barrier for Cu+ diffusion. The other possible dopants described above are also considered as candidates for implantation into silicon oxide for generating barriers for Cu+ diffusion.
Without wishing to be bound by theory, silicon oxide forms a ring of alternating silicon and oxygen atoms. There may be from about two to six silicon atoms in the ring. Normally without a divalent dopant, a Cu+ ion sits above a ring and jumps from ring to ring to diffuse into the silicon oxide and poison it. However, by placing a Ca ion in about one ring for every two or four adjacent rings, a Cu+ ion will tend to replace the Ca in the ring and the Ca ion will be placed above the ring. It is believed that such a configuration provides energy level structure II. Such a configuration having an energy level so much lower than the other energy level structures traps the Cu+. It is believed that a single Ca ion is sufficient for two or three rings.
An alternative method of forming the barrier layers may be performed by exposing the silicon oxide layers to plasmas of the dopant ion. A calcium ion plasma would provide a lower energy Ca implantation with a higher flux. The lower energy may provide a thinner barrier layer. In other embodiments, a combination of implantations and plasma may be used to more easily create the inventive barrier layer on the side walls of the vias and trenches of a dual damascene process. Other methods may also be used to create the inventive barrier layer.
Copper interconnects may be used in a damascene type structure. In damascene structures, a via, trench, or both via and trench may be etched in a dielectric. It may be desirable to place the barrier layer on both horizontal surfaces of a dielectric and vertical surfaces forming sidewalls of vias and trenches.
A divalent ion dopant is then implanted into horizontal surfaces of the silicon oxide (step 404). Such a doping may be performed using any of the above-described methods, such as a 10-20 keV ion implantation or plasma implantation.
A deep implant of a divalent ion is then provided (step 412) forming an implant region 704 within the parts of the silicon oxide 508 exposed by the via patterned photoresist 608, as shown in
The photoresist 608 is then removed (step 418). The horizontal barrier layer 604 and the sidewall barrier layer 808 may be covered with a copper layer 904 (step 420), as shown in
These methods provide a thin barrier layer with low porosity and high purity. By use of a silicon oxide layer doped with a divalent ion with low porosity and high purity, a thin barrier layer is provided which is able to be an effective barrier layer.
In another embodiment of the invention, the deep implant of step 412 may be performed before the patterned mask is placed (step 408). This would cause the entire silicon oxide layer 508 to become a barrier layer. The remaining steps are performed. Since the entire silicon oxide layer 508 is doped with a divalent ion, the entire silicon oxide layer 508 may be a copper barrier.
While this invention has been described in terms of several preferred embodiments, there are alterations, modifications, permutations, and substitute equivalents, which fall within the scope of this invention. It should also be noted that there are many alternative ways of implementing the methods and apparatuses of the present invention. It is therefore intended that the following appended claims be interpreted as including all such alterations, permutations, and substitute equivalents as fall within the true spirit and scope of the present invention.
This application is a continuation application of prior application Ser. No. 10/044,864, filed on Oct. 22, 2001 now U.S. Pat. No. 7,115,991, by Vladimir Zubkov et al. and entitled “Method for Creating Barriers for Copper Diffusion”, from which priority under 35 U.S.C. §120 is claimed, and which is incorporated by reference herein for all purposes.
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Number | Date | Country | |
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Parent | 10044864 | Oct 2001 | US |
Child | 11104763 | US |