Memory cell configuration and method for its production

Active solid-state devices (e.g. – transistors – solid-state diode – Field effect device – Having insulated electrode

Reexamination Certificate

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C257S303000, C257S306000

Reexamination Certificate

active

06300652

ABSTRACT:

BACKGROUND OF THE INVENTION
Field of the Invention
The invention relates to a memory cell configuration and a method for producing the memory cell configuration.
Memory cell configurations, both for DRAM applications and for non-volatile memories, have an increased storage density from generation to generation.
In DRAM cell configurations, use is made almost exclusively of so-called single-transistor memory cells. A single-transistor memory cell includes a read-out transistor and a storage capacitor. The information is stored in the storage capacitor in the form of an electric charge, which represents a logic value, zero or one. That information can be read out through a bit line by driving the read-out transistor through a word line. The storage capacitor must have a minimum capacitance in order to reliably store the charge and at the same time be able to distinguish between the information read out. The lower limit for the capacitance of the storage capacitor is currently regarded as 20 fF.
Since the storage density increases from memory generation to memory generation, the required area of the single-transistor memory cell must be reduced from generation to generation. At the same time, the minimum capacitance of the storage capacitor must be maintained.
Up until the 1 Mbit generation, both the read-out transistor and the storage capacitor were realized as planar components. Starting with the 4 Mbit memory generation, a further deduction in the area of the memory cell was achieved through the use of a three-dimensional configuration of the read-out transistor and the storage capacitor. One possibility is to realize the storage capacitor in a trench. In that case, the electrodes of the storage capacitor are disposed along the surface of the trench. That increases the effective area of the storage capacitor, upon which the capacitance depends, as compared with the space requirement at the surface of the substrate for the storage capacitor, which corresponds to the cross-section of the trench.
A further possibility for increasing the storage capacitance with the space requirement of the storage capacitor remaining the same or being reduced is constructing the storage capacitor as a stacked capacitor. In that case, a polysilicon structure, for example a cylinder, a crown structure or a rib structure (FIN), is formed over the word lines and makes contact with the substrate. That polysilicon structure forms the storage node. It is provided with a capacitor dielectric and a capacitor plate. In that case, the free space above the substrate surface is utilized for the storage capacitor. The entire cell area can be covered by the polysilicon structure as long as the polysilicon structures for adjacent memory cells are insulated with respect to one another. That concept has the advantage of being largely compatible with a logic process.
The area for a memory cell of a DRAM belonging to the 1 Gbit generation should only be about 0.2 &mgr;m
2
. In order to realize the minimum capacitance for the storage capacitor of approximately 25 fF on an area of that type, it is necessary, in the case of a trench capacitor concept, for the active trench depth to be at least 8 &mgr;m in conjunction with a trench width of 0.3 &mgr;m and a dielectric having an oxide-equivalent thickness of 4 nm. Trenches having dimensions of that type can only be realized by using complicated etching processes with long etching times. In a stacked capacitor concept, those demands on the area requirement of a memory cell can only be realized with a relatively complicated structure of the polysilicon structure. In addition, those complicated structures are more and more difficult to produce due to their topology.
A further increase in the capacitance that can be attained per unit of area is achieved by the use of so-called high-epsilon dielectrics as a storage dielectric in the storage capacitor (see, for example, the paper by P. C. Fazan, entitled: Trends in, the Development of ULSI DRAM Capacitors, in Integrated Ferroelectrics, Volume 4 (1994), pages 247 to 256). High-epsilon dielectrics are ferroelectric or paraelectric materials. The capacitor is constructed as a stacked capacitor in those concepts. To that end, a lower electrode is first produced by layer deposition and structuring. The high-epsilon dielectric is deposited thereon. Finally, an upper capacitor electrode is applied, structured and provided with an electrical contact. Since high-epsilon dielectrics are deposited at temperatures in the range of 700 to 800° C., at which many electrode materials react, only specific materials, for example TiN, Pt, W, RuO
2
, Ir
2
O
3
or Pd, are suitable for the lower electrodes. The search for further materials which are suitable for the lower electrode is the subject of worldwide research activity.
SUMMARY OF THE INVENTION
It is accordingly an object of the invention to provide a memory cell configuration and a method for its production, which overcome the hereinafore-mentioned disadvantages of the heretofore-known devices and methods of this general type and in which the memory cell configuration is suitable for large scale integrated DRAMs belonging to the 1 Gbit and subsequent generations and can be produced with reduced process complexity as compared with known solutions.
With the foregoing and other objects in view there is provided, in accordance with the invention, a memory cell configuration, comprising a multiplicity of individual memory cells each including a selection transistor and a storage capacitor in a semiconductor layer structure; substantially parallel bit lines and substantially parallel word lines, the bit lines and the word lines extending transversely relative to one another; an insulating layer; at least the selection transistors being disposed below the insulating layer; the storage capacitors being disposed on the insulating layer; each of the storage capacitors including a first electrode, a storage dielectric and a second electrode; the storage dielectric having ferroelectric or paraelectric material; and the first electrode, the storage dielectric and the second electrode each being disposed next to one another above the insulating layer.
The memory cell configuration according to the invention includes a multiplicity of individual memory cells, each of which include a selection transistor and a storage capacitor. In this case, the storage capacitors are disposed according to the manner of stacked capacitors in a plane above the selection transistors. The selection transistors are covered with an insulating layer.
The storage capacitors each include a first electrode, a storage dielectric and a second electrode. In this case, the first electrode, the storage dielectric and the second electrode are each disposed next to one another above the insulating layer. The capacitance of the storage capacitor is determined by the area between the first electrode and the storage dielectric, and the second electrode and the storage dielectric. This area and therefore the capacitance of the storage capacitor can be adjusted in the configuration according to the invention by way of the height of the first and second electrodes and of the storage dielectric.
Although a capacitor configuration for memories with a vertical capacitor has already been proposed in German Published, Non-Prosecuted Patent Application DE 43 36 001 A1, the storage dielectric used therein is a monocrystalline, ferroelectric layer, with the result that the capacitor can only be produced on a monocrystalline substrate. The known capacitor configuration is therefore unsuitable for a stacked capacitor configuration.
Ferroelectric and/or paraelectric material is used as the storage dielectric. Ferroelectric and paraelectric material are crystalline materials having a polar lattice. The ionic bond is predominant in these materials. They have a high dielectric constant ∈. The dielectric constant ∈ of many ferroelectric and paraelectric material is between 300 and 1000. In contrast, amorphous dielectrics, such as, for example, SiO

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