Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode
Reexamination Certificate
1998-10-01
2001-06-19
Lee, Eddie C. (Department: 2815)
Active solid-state devices (e.g., transistors, solid-state diode
Field effect device
Having insulated electrode
C257S295000, C257S296000, C257S306000, C257S310000
Reexamination Certificate
active
06249014
ABSTRACT:
BACKGROUND OF THE INVENTION
The present invention relates, in general, to the field of integrated circuit (“IC”) manufacturing processes. More particularly, the present invention relates to hydrogen barrier encapsulation techniques for the control of hydrogen induced degradation of ferroelectric memory devices, in particular with respect to multi-level metal IC processing.
Certain memory devices, such as the FRAM® (FRAM is a registered trademark of Ramtron International Corporation, Colorado Springs, Colo.) family of solid state, random access memory integrated circuits, provide non-volatile data storage through the use of a ferroelectric dielectric material which may be polarized in one direction or another in order to store a binary value representative of a logic level “one” or “zero”. The ferroelectric effect allows for the retention of a stable polarization in the absence of an applied electric field due to the alignment of internal dipoles within the Perovskite crystals in the dielectric material. This alignment may be selectively achieved by application of an electric field which exceeds the coercive field of the material. Conversely, reversal of the applied field reverses the internal dipoles.
A hysteresis curve, wherein the abscissa and ordinate represent the applied voltage (“V”) and resulting polarization (“Q”) states respectively, may be plotted to represent the response of the polarization of a ferroelectric capacitor to the applied voltage. A more complete description of this characteristic hysteresis curve is disclosed, for example, in U.S. Pat. Nos. 4,914,627 and 4,888,733 assigned to the assignee of the present invention, the disclosures of which are herein specifically incorporated by this reference.
Data stored in a ferroelectric memory cell is “read” by applying an electric field to the cell capacitor. If the field is applied in a direction to switch the internal dipoles, more charge will be moved than if the dipoles are not reversed. As a result, sense amplifiers can measure the charge applied to the cell bit lines and produce either a logic “one” or “zero” at the IC output pins provided that “Q” is sufficiently large. In a conventional two transistor/two capacitor (“2C/2T”) ferroelectric memory cell, (one transistor/one capacitor “1T/1C” devices have also been described) a pair of two data storage elements are utilized, each polarized in opposite directions. To “read” the state of a 2T/2C memory cell, both elements are polarized in the same direction and the sense amps measure the difference between the amount of charge transferred from the cells to a pair of complementary bit lines. In either case, since a “read” to a ferroelectric memory is a destructive operation, the correct data is then restored to the cell during a precharge operation.
In a simple “write” operation, an electric field is applied to the cell capacitor to polarize it to the desired state. Briefly, the conventional write mechanism for a 2T/2C memory cell includes inverting the dipoles on one cell capacitor and holding the electrode, or plate, to a positive potential greater than the coercive voltage for a nominal 100 nanosecond (“nsec.”) time period. The electrode is then brought back to circuit ground for the other cell capacitor to be written for an additional nominal 100 nsec. In any event, the switching polarization (“Q
SW
”, where Q
SW
=2Pr, the remnant polarization) of the device must be sufficiently large for the signal presented to the sense amplifiers to be accurately read or the performance of the device is severely degraded should Q
SW
be too low for reliable operation.
It has been observed that when a ferroelectric capacitor is exposed to hydrogen species, the ferroelectric properties of the capacitor are severely degraded. The rate at which this degradation occurs is a function of the flux of hydrogen which comes in direct contact with the ferroelectric capacitor and temperature although the type of hydrogen species, (i.e. monatomic vs. diatomic) is also a factor. Diffusion of hydrogen through conductive and non-conductive layers surrounding the ferroelectric capacitor is a function of hydrogen concentration, temperature, time and the diffusivity of hydrogen through a given material in accordance with Fick's laws of diffusion. As a consequence, control of these factors can be used to ameliorate or reduce ferroelectric device degradation due to the presence of hydrogen.
Following the formation of the ferroelectric capacitor structures on an integrated circuit (“IC”) device, some type of electrical interconnect is required to couple the transistor and capacitor components of the IC device. Typical IC interconnect materials include alloys of aluminum, tungsten and oxide non-conductive layers. Most of the industry standard process steps used for such interconnect processing contain hydrogen species or require process temperatures at or above 400° C. or both.
Recently, two mechanisms for hydrogen induced degradation in IC devices have been identified:
1) Hydrogen generated external to the die due to process steps which contain hydrogen (either deliberately introduced into the process-step or as a byproduct of the process step). These process steps may include chemical vapor deposition (“CVD”) of oxides or refractory materials, anneals or etch process steps; and
2) Hydrogen generated within the body or structure of the die. For example, water adsorbed within oxide layers has been shown to diffuse through the oxide layer at fairly low temperatures (~400° C.) and react with metals within the die structure which cause the dissociation of the water molecule and subsequently generate hydrogen species which in turn degrade ferroelectric device performance.
Multilevel metal processes for standard memory, embedded or logic devices using design rules of 0.5 &mgr;m or smaller commonly include process steps such as tungsten plug deposition, high density plasma (“HDP”, silane based) interlevel oxide deposition or plasma tetraethyloxysilicate (“TEOS”) oxide deposition, chemical mechanical polishing (“CMP”) for planarization of oxide or tungsten plug layers and hot metal reflow (420° C. up to 520° C. wafer substrate temperature) aluminum deposition. All of these process steps generate hydrogen either directly or through various secondary mechanisms. CVD tungsten plug deposition, for example, uses roughly 3% (or higher) hydrogen (at 400° C. to 500° C.) for the carrier gas, and HDP oxide deposition uses silane which reacts to form SIO
2
, water and hydrogen. CMP utilizes a water slurry which causes water adsorption into the oxide films. Subsequently, during any process step using temperatures of 400° C. or greater (tungsten plug deposition, interlevel dielectric (“ILD”) oxide deposition or hot aluminum reflow deposition), water will diffuse through the oxide layer and disassociate at metal interfaces to form hydrogen and oxygen as previously noted.
Therefore, in order to successfully integrate ferroelectric capacitors with multilevel metal process steps it is necessary to either: 1) remove the hydrogen from the multilevel metal process steps altogether; or 2) to make the ferroelectric device more immune to hydrogen degradation.
Completely removing the hydrogen from industry standard process steps would, naturally, require a great deal of new process development. If such were even possible to achieve, it would likely result in many non-standard processes and equipment configurations which would increase the cost and complexity of manufacturing ferroelectric IC's.
A more desirable method, therefore would be to somehow render the ferroelectric capacitor more immune to hydrogen degradation. Improving the hydrogen immunity of ferroelectric capacitors, however, has long been a major impediment to ferroelectric process integration. In this regard, various methods have been reported including doping the ferroelectric material itself to make it less susceptible to hydrogen damage (often at the compromise of other ferroelectric electrical properties) or the use of compound or exotic ele
Burton Carol W.
Hogan & Hartson LLP
Kubida William J.
Lee Eddie C.
Ortiz Edgardo
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