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[0001] 1. Field of the Invention
[0002] This invention relates generally to the field of semiconductor memory and logic devices. The invention relates more specifically to a silicon-on-insulator structure, and a method of fabrication therefor.
[0003] 2. Description of the Related Art
[0004] In the field of microelectronics, SOI (Silicon-on-Insulator)-CMOS technology has been demonstrated to have significant speed, power, and radiation immunity advantages over bulk CMOS technology. See, e.g., “Scalability of SOI Technology into 0.13 um 1.2 V CMOS Generation,” E. Leobandung, et al.,
[0005] SOI-CMOS technology, however, has yet to be widely accepted by the systems and circuit design communities because of the complexity of managing an anomalous effect termed the “floating body effect” (hereinafter “FBE”), of the SOI devices, and in particular, of NFET-SOI devices. Unlike bulk NMOSFET devices, in which the body is tied to either a fixed potential or to the source of the device, body potential in NMOSFET-SOI devices is floating, and remains unstable due to the complex dynamics of both positive-charge carrier, or “hole,” generation by impact ionization at the drain edge, and by recombination and diffusion. As a result of this floating potential, NMOSFET-SOI devices exhibit several undesirable characteristics, such as a “kink effect” (current enhancement) in the Id-Vg characteristics of the device, enhanced leakage attributable to parasitic (npn) bipolar junction transistor (BJT) current, and enhanced 1/f noise. In addition, circuit-related drawbacks attributable to FBE include threshold instability, hysterectic behavior in signal input/output, frequency dependent pulse delays, and signal pulse width modulation. The parasitic bipolar current adversely affects memory sense and write operations (in SRAM memory) as well as data retention (in SDRAM memory). “SOI Floating Body, Devices, and Circuit Issues,” J. Cautier, et al.,
[0006] In logic design, such drawbacks can lead to data loss and dynamic circuit failure, as well as timing delays. Additionally, analog circuit applications may be seriously limited due to transistor mismatch and enhanced AC/DC noise. Therefore, overcoming FBE is a major obstacle to the widespread application of SOI-CMOS.
[0007] Several solutions have been proposed to suppress FBE. For example, with field shield isolation technology, FBE has been minimized for SOI-NFET gate arrays by using a field shielded gate and by collecting excess holes via the body contact under the field shield. “CAD-Compatible High-Speed CMOS/SIMOX Gate Array Using Field-Shield Isolation,” T. Iwamatsu, et al.,
[0008] In another approach, a bipolar embedded source structure (BESS) has been employed to suppress FBE. “BESS: A Source Structure that Fully Suppresses the Floating Body Effects in SOI CMOSFETs,” M. Horiuchi, et al.,
[0009] In still another approach, using a Si—Ge inserted SOI, a graded thin layer of Si—Ge is epitaxially inserted into a p-type silicon body toward its bottom, close to the BOX region. “A Novel Si—Ge Inserted SOI Structure for High Performance PDSOI CMOSFET,” G. T. Bae, et al,
[0010] In each of the above-described prior art approaches to overcoming FBE, the central theme is to facilitate the recombination of the excess holes generated by impact ionization. That is, the objective is for the excess holes to be swept away and recombined by a mechanism (or combination of mechanisms) that yields a very small (i.e., a short, or faster) recombination time constant. If a very small time constant could be achieved, the body (e.g., the base of a parasitic BJT bipolar device) would never be charged sufficiently so as to trigger bipolar action. If such a dynamic equilibrium could be achieved for generation and recombination of holes, the body would maintain a constant low body potential regardless of the time constant and the mechanism of hole generation. Consequently, large hole generation would lead to a large recombination current and, therefore, a low gain (i.e., large base current) for a parasitic bipolar device. The resulting device would not exhibit a greater drain induced barrier lowering effect, and would not have reduced source to drain breakdown. Furthermore, circuits employed would not exhibit any hysteretic effects regardless of pulse frequency, or any excessive pass-gate leakage, or any data loss or pulse width modulation.
[0011] Therefore, a need exists for a solution to the floating body effect that can be achieved at the minimum increase in process complexity and the minimum impact on device density and other required device characteristics, such as device current, desired device leakage, and capacitance.
[0012] The present invention provides a silicon-on-insulator structure free from floating body effects, and a method of fabrication therefor. More specifically, the present invention provides a structure capable of facilitating the enhanced recombination of charge carriers, which results in a greatly reduced recombination time constant.
[0013] Accordingly, the present invention relates to a structure having a field shield integration configuration that provides an effective drift field for holes and simultaneously enhanced recombination centers for positive-charge carriers (holes) and negative-charge carriers (electrons). The effective drift field and the enhanced recombination centers facilitate the rapid recombination of the charge carriers, leading to a very small recombination time constant. The structure comprises a silicon substrate, an oxide insulation layer disposed above the silicon substrate, a silicon body layer disposed above the oxide insulation layer, and a field shield gate disposed above the silicon body layer. The field shield gate includes a conductor portion, and an alumina insulation layer disposed beneath the conductor portion. The oxide insulation layer and the silicon body layer each include at least one channel stop region, and at least one recombination center for the recombination of positive- and negative-charge carriers.
[0014] The present invention also relates to a method of fabricating the above-described silicon-on-insulator structure. The method comprises providing an oxide insulation layer on a silicon substrate; providing on the oxide insulation layer a shallow trench isolation configuration of a silicon body layer; providing on a portion of the silicon body layer an alumina insulation layer of a field shield gate; providing on the alumina insulation layer a conductor portion of the field shield gate; and providing through ion implantation at least one channel stop region and at least one recombination center in each of the silicon body layer and the oxide insulation layer. By conducting the oxidation of the alumina insulation formation layer in a moist environment, a highly controlled negative charge at the alumina insulation layer-silicon body layer interface can be achieved, which provides an effective drift field. The enhanced recombination center is produced by ion implantation of either silicon, nickel, or cobalt deep inside the silicon body layer. The elements silicon, nickel, or cobalt provide deep electron and hole energy states within the bandgap of the silicon body layer, thereby creating deep recombination centers for electrons and holes.
[0015] By virtue of the aforementioned features and other features described herein, the present invention provides a silicon-on-insulator structure with a recombination time constant substantially smaller than that associated with conventional structures and methods, thereby overcoming the floating body effect.
[0016] Other features and advantages of the present invention will become more fully apparent from the following detailed description of the exemplary embodiments of the invention which are provided in connection with the accompanying drawings.
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[0024] The present invention will be understood from the exemplary embodiments described herein.
[0025] The present invention provides a field shield integration configuration that offers simultaneously enhanced recombination centers for positive-charge carriers (holes) and negative-charge carriers (electrons), and an effective drift field for holes (not required for electrons due to their inherent high mobility). The effective drift field and the enhanced recombination centers facilitate the rapid recombination of the charge carriers, leading to a very small recombination time constant. The present invention, therefore, overcomes the conventional slow thermal recombination mechanism or the diffusion time constant associated with hole recombination at the body contact.
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[0027] In an active device region
[0028] The method of fabricating structure
[0029] The presence of the channel stop region
[0030] In the present invention, two factors determine the ability of the holes to recombine with a small recombination time constant. The first factor is the presence of an effective drift field, and the second factor is the presence of the enhanced recombination center
[0031] The second factor, the presence of the enhanced recombination center
[0032] The presence of the enhanced deep recombination center
[0033] The ion implantation to produce the recombination center
[0034] The recombination center
[0035] The ability of the charge carriers to recombine with a small recombination time constant is attributable to the interaction between the negative interface charge at the alumina insulation layer
[0036] As indicated above, in the active device region
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[0040] A chip produced from the structure
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[0042] In still another embodiment of the invention, a chip produced from the structure
[0043] The present invention, therefore, provides a structure capable of facilitating the enhanced recombination of charge carriers, which results in a recombination time constant that is substantially smaller than that associated with conventional structures and methods. By virtue of the features described herein, the invention provides scalability, performance and circuit designability over a wide range of application frequencies and power supplies. The invention also facilitates mixed signal circuit design (e.g., phase-locked loop), and can be used for memory and logic applications.
[0044] Although the invention has been described and illustrated as being suitable for use in a processor applications, for example, computer control systems, the invention is not limited to these embodiments. Rather, the invention could be employed in any system in which a small recombination time constant is desirable.
[0045] Accordingly, the above description and accompanying drawings are only illustrative of exemplary embodiments that can achieve the features and advantages of the present invention. It is not intended that the invention be limited to the embodiments shown and described in detail herein. The invention is limited only by the scope of the following claims.