1. Technical Field
The present invention relates generally to semiconductor interconnect structures, and more particularly, to methods of forming a gas dielectric structure for a semiconductor interconnect structure using radiation.
2. Related Art
In order to enhance semiconductor chip operational speed, semiconductor devices have been continuously scaled down in size. Unfortunately, as semiconductor device size is decreased, the capacitive coupling between conductors in a circuit tends to increase since the capacitive coupling is inversely proportional to the distance between the conductors. This coupling may ultimately limit the speed of the chip or otherwise inhibit proper chip operation if steps are not taken to reduce the capacitive coupling.
The capacitance between conductors is also dependent on the insulator, or dielectric, used to separate the conductors. Traditional semiconductor fabrication commonly employs silicon dioxide (SiO2) as a dielectric, which has a dielectric constant (k) of approximately 3.9. One challenge facing further development is finding materials with a lower dielectric constant that can be used between the conductors. As the dielectric constant of such materials is decreased, the speed of performance of the chip is increased. Some new low-k dielectric materials that have been used to provide a lower dielectric constant between conductors include, for example, fluorinated glass and organic materials. Unfortunately, provision of newer low-k dielectric materials presents a number of new challenges, which increase process complexity and cost.
Implementation of organic materials to reduce the dielectric constant also reduces the overall back-end-of-line (BEOL) capacitance. Unfortunately, organic materials suffer from temperature limitations, shrinkage or swelling during manufacturing or chip operation, and poor structural integrity. Instead of using silicon dioxide (SiO2), another approach is to implement gas, such as air, which is provided in the form of a gas dielectric structure in a semiconductor structure. Air has the lowest effective dielectric constant. Simple capacitance modeling of parallel wires shows that even a small air-gap near the wires results in a significant improvement in the overall dielectric constant (k) for a structure, e.g., a 10% air gap per edge will reduce the effective dielectric constant of a dielectric by approximately 15%. Current processing for implementing gas dielectric structures, however, is fairly complex and cannot be easily integrated. As a result, completely new integration schemes have been developed, which are more complex and more costly. For example, typical gas dielectric structure formation requires additional masking layers for reactive ion etching (RIE) processing steps relative to damascene wire formation.
In view of the foregoing, there is a need for an improved solution for forming a gas dielectric structure for a semiconductor interconnect structure.
Methods and resulting structure of forming a gas dielectric structure in an interconnect structure are disclosed. In one embodiment, the method includes providing the interconnect structure including at least one interconnect layer having a dielectric, at least one conductor and a first cap layer; and causing the dielectric to contract to form the gas dielectric structure by exposing the interconnect structure to radiation. The radiation can be electron beam radiation or ultraviolet (UV) radiation. In one embodiment, an interface-breaking enhancing film can be used to selectively locate the gas dielectric structures formed.
A first aspect of the invention is directed to a method of forming a gas dielectric structure in an interconnect structure, the method comprising the steps of: providing the interconnect structure including at least one interconnect layer having a dielectric, at least one conductor and a first cap layer; and causing the dielectric to contract to form the gas dielectric structure by exposing the interconnect structure to radiation.
A second aspect of the invention includes a method of forming a gas dielectric structure in an interconnect structure, the method comprising the steps of: providing the interconnect structure including an interlevel dielectric, at least one conductor and a first cap layer above the interlevel dielectric and a second cap layer below the interlevel dielectric; and causing the interlevel dielectric to contract from at least one of the first cap layer, the second cap layer and the at least one conductor to form the gas dielectric structure by exposing the interconnect structure to electron beam radiation.
A third aspect of the invention related to an interconnect structure comprising: a dielectric layer including at least one conductor positioned therein; at least one cap layer adjacent the dielectric layer; and at least one gas dielectric structure positioned within the dielectric layer, wherein the gas dielectric structure has a substantially arcuate shape extending from the at least one cap layer.
The foregoing and other features of the invention will be apparent from the following more particular description of embodiments of the invention.
The embodiments of this invention will be described in detail, with reference to the following figures, wherein like designations denote like elements, and wherein:
With reference to the accompanying drawings, various embodiments of methods of forming a gas dielectric structure in an interconnect structure will now be described.
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In any event, the exposure must be sufficiently long enough and have energy (e.g., acceleration voltage for e-beam) sufficient to pierce cap layer 108 to interact with dielectric 104. Where electron beam radiation is used, a dose of approximately 300 micro-Coulombs/cm2 has been found advantageous. In one embodiment, this dose may be achieved using electron beam radiation of no less than approximately 2 KeV and no greater than approximately 10 KeV, for no less than approximately 1 minute and no greater than approximately 8 minutes. In addition, electron beam radiation preferably has an energy of no less than approximately 300 Pascal and no greater than 1 giga-Pascal. In one particular example, a silicon nitride (Si3N4) cap layer having a thickness of approximately 3000 Å and a density of approximately 1.3 g/cm3, was exposed to electron beam radiation of approximately 3 KeV for approximately 2-3 minutes, which resulted in the above-described dose. The above-described parameters may vary, however, depending on the type of cap layer 108 used and its thickness.
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The above-described methodology can be carried out after each cap layer is formed and at each level.
The resulting interconnect structure 200 (
While this invention has been described in conjunction with the specific embodiments outlined above, it is evident that many alternatives, modifications and variations will be apparent to those skilled in the art. Accordingly, the embodiments of the invention as set forth above are intended to be illustrative, not limiting. Various changes may be made without departing from the spirit and scope of the invention as defined in the following claims.