Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode
Reexamination Certificate
2001-10-03
2002-09-24
Christianson, Keith (Department: 2813)
Active solid-state devices (e.g., transistors, solid-state diode
Field effect device
Having insulated electrode
C257S700000, C257S724000, C257S920000
Reexamination Certificate
active
06455885
ABSTRACT:
BACKGROUND OF THE INVENTION
(1) Field of the Invention
The invention relates to the manufacturing of high performance Integrated Circuit (IC's), and, more specifically, to methods of creating high performance electrical components (such as an inductor) on the surface of a semiconductor substrate by reducing the electromagnetic losses that are typically incurred in the surface of the substrate.
(2) Description of the Prior Art
The continued emphasis in the semiconductor technology is to create improved performance semiconductor devices at competitive prices. This emphasis over the years has resulted in extreme miniaturization of semiconductor devices, made possible by continued advances of semiconductor processes and materials in combination with new and sophisticated device designs. Most of the semiconductor devices that are at this time being created are aimed at processing digital data. There are however also numerous semiconductor designs that are aimed at incorporating analog functions into devices that simultaneously process digital and analog data, or devices that can be used for the processing of only analog data. One of the major challenges in the creation of analog processing circuitry (using digital processing procedures and equipment) is that a number of the components that are used for analog circuitry are large in size and are therefore not readily integrated into devices that typically have feature sizes that approach the sub-micron range. The main components that offer a challenge in this respect are capacitors and inductors, since both these components are, for typical analog processing circuits, of considerable size.
A typical application for inductors of the invention is in the field of modern mobile communication applications that make use of compact, high-frequency equipment. Continued improvements in the performance characteristics of this equipment has over the years been achieved, further improvements will place continued emphasis on lowering the power consumption of the equipment, on reducing the size of the equipment, on increasing the operational frequency of the applications and on creating low noise levels. One of the main applications of semiconductor devices in the field of mobile communication is the creation of Radio Frequency (RF) amplifiers. RF amplifiers contain a number of standard components, a major component of a typical RF amplifier is a tuned circuit that contains inductive and capacitive components. Tuned circuits form, dependent on and determined by the values of their inductive and capacitive components, an impedance that is frequency dependent, enabling the tuned circuit to either present a high or a low impedance for signals of a certain frequency. The tuned circuit can therefore either reject or pass and further amplify components of an analog signal, based on the frequency of that component. The tuned circuit can in this manner be used as a filter to filter out or remove signals of certain frequencies or to remove noise from a circuit configuration that is aimed at processing analog signals. The tuned circuit can also be used to form a high electrical impedance by using the LC resonance of the circuit and to thereby counteract the effects of parasitic capacitances that are part of a circuit. One of the problems that is encountered when creating an inductor on the surface of a semiconductor substrate is that the self-resonance that is caused by the parasitic capacitance between the (spiral) inductor and the underlying substrate will limit the use of the inductor at high frequencies. As part of the design of such an inductor it is therefore of importance to reduce the capacitive coupling between the created inductor and the underlying substrate.
At high frequencies, the electromagnetic field that is generated by the inductor induces eddy currents in the underlying silicon substrate. Since the silicon substrate is a resistive conductor, the eddy currents will consume electromagnetic energy resulting in significant energy loss, resulting in a low Q capacitor. This is the main reason for a low Q value of a capacitor, whereby the resonant frequency of 1/(LC) limits the upper boundary of the frequency. In addition, the eddy currents that are induced by the inductor will interfere with the performance of circuitry that is in close physical proximity to the capacitor.
It has already been pointed out that one of the key components that are used in creating high frequency analog semiconductor devices is the inductor that forms part of an LC resonance circuit. In view of the high device density that is typically encountered in semiconductor devices and the therefrom following intense use of the substrate surface area, the creation of the inductor must incorporate the minimization of the surface area that is required for the inductor, while at the same time maintaining a high Q value for the inductor. Typically, inductors that are created on the surface of a substrate are of a spiral shape whereby the spiral is created in a plane that is parallel with the plane of the surface of the substrate. Conventional methods that are used to create the inductor on the surface of a substrate suffer several limitations. Most high Q inductors form part of a hybrid device configuration or of Monolithic Microwave Integrated Circuits (MMIC's) or are created as discrete components, the creation of which is not readily integratable into a typical process of Integrated Circuit manufacturing. It is clear that, by combining the creation on one semiconductor monolithic substrate of circuitry that is aimed at the functions of analog data manipulation and analog data storage with the functions of digital data manipulation and digital data storage, a number of significant advantages can be achieved. Such advantages include the reduction of manufacturing costs and the reduction of power consumption by the combined functions. The spiral form of the inductor that is created on the surface of a semiconductor substrate however results, due to the physical size of the inductor, in parasitic capacitances between the inductor wiring and the underlying substrate and causes electromagnetic energy losses in the underlying resistive silicon substrate. These parasitic capacitances have a serious negative effect on the functionality of the created LC circuit by sharply reducing the frequency of resonance of the tuned circuit of the application. More seriously, the inductor-generated electromagnetic field will induce eddy currents in the underlying resistive silicon substrate, causing a significant energy loss that results in low Q inductors.
The performance parameter of an inductor is typically indicated is the Quality (Q) factor of the inductor. The quality factor Q of an inductor is defined as Q=Es/El, wherein Es is the energy that is stored in the reactive portion of the component while El is the energy that is lost in the reactive portion of the component. The higher the quality of the component, the closer the resistive value of the component approaches zero while the Q factor of the component approaches infinity. For inductors that are created overlying a silicon substrate, the electromagnetic energy that is created by the inductor will primarily be lost in the resistive silicon of the underlying substrate and in the metal lines that are created to form the inductor. The quality factor for components differs from the quality that is associated with filters or resonators.
For components, the quality factor serves as a measure of the purity of the reactance (or the susceptance) of the component, which can be degraded due to the resistive silicon substrate, the resistance of the metal lines and dielectric losses. In an actual configuration, there are always some physical resistors that will dissipate power, thereby decreasing the power that can be recovered. The quality factor Q is dimensionless. A Q value of greater than 100 is considered very high for discrete inductors that are mounted on the surface of Printed Circuit Boards. For inductors that form part of
Ackerman Stephen B.
Christianson Keith
Huynh Yennhu
Megic Corporation
Saile George O.
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