Charge trapping memory cell with high speed erase

Abstract

A band gap engineered, charge trapping memory cell includes a charge trapping element that is separated from a metal or metal compound gate, such as a platinum gate, by a blocking layer of material having a high dielectric constant, such as aluminum oxide, and separated from the semiconductor body including the channel by an engineered tunneling dielectric. Fast program and erase speeds with memory window as great as 7 V are achieved.

Description

CROSS REFERENCE TO RELATED APPLICATION[0001]The benefit of U.S. Provisional Patent Application No. 60 / 955,391, filed on 13 Aug. 2007, is hereby claimed.BACKGROUND OF THE INVENTION[0002]1. Field of the Invention[0003]The present invention relates to flash memory technology, and more particularly to scalable charge trapping memory technology adaptable for high speed erase and program operations.[0004]2. Description of Related Art[0005]Flash memory is a class of non-volatile integrated circuit memory technology. Traditional flash memory employs floating gate memory cells. As the density increases in memory devices, and the floating gate memory cells get closer and closer together, interference between the charge stored in adjacent floating gates becomes a problem. This is limiting the ability to increase the density of flash memory based on floating gate memory cells. Another type of memory cell used for flash memory can be referred to as a charge trapping memory cell, which uses a die...

AI Technical Summary

Benefits of technology

[0011]The valence band energy level at the first offset is such that an electric field sufficient to induce hole tunneling through the thin region between the interface with the semiconductor body and the offset, is also sufficient to raise the valence band energy level after the offset to a level that effectively eliminates the hole tunneling barrier in the engineered tunneling dielectric after the offset. This structure enables electric field assisted hole tunneling at high speeds while effectively preventing charge leakage through the engineered tunneling dielectric in the absence of electric fields or in the presence of smaller electric fields induced for the purpose of other operations, such as reading data from the cell or programming adjacent cells.

[0012]In a representative device, the engineered tunneling dielectric layer consists of an ultrathin silicon oxide layer O1 (e.g. <=15 Å), an ultrathin silicon nitride layer N1 (e.g. <=30 Å) and an ultrathin silicon oxide layer O2 (e.g. <=30 Å), which results in an increase in the valence band energy level of about 2.6 eV at an offset 15 Å or less, from the interface with the semiconductor body. The O2 layer separates the N1 layer from the charge trapping layer, at a second offset (e.g. about 35 to 45 A from the interface), by a region of lower valence band energy level (higher hole tunneling barrier). The electric field sufficient to induce hole tunneling between the interface and the first offset also raises the valence band energy level after the second offset to a level that effectively eliminates the hole tunneling barrier, because the second offset is at a greater distance from the interface. Therefore, the O2 layer does not significantly interfere with the electric field assisted hole tunneling, while improving the ability of the engineered tunneling dielectric to block leakage during low fields.

Problems solved by technology

As the density increases in memory devices, and the floating gate memory cells get closer and closer together, interference between the charge stored in adjacent floating gates becomes a problem.

This is limiting the ability to increase the density of flash memory based on floating gate memory cells.

However at that thickness, the endurance and charge retention characteristics of the memory cell are poor relative to traditional floating gate technology.

Also, with relatively thick tunneling dielectric layers, the electric field required for the erase operation also cause electron injection from the gate through the blocking dielectric layer.

However, if the erase saturation level is too high, the cell cannot be erased at all, or the threshold margin between the programmed and erased states becomes too small for many applications.

Decreasing the thickness of the tunneling dielectric layer is limited by issues of charge retention and erase saturation, as mentioned above.

However, the problem of the erase saturation continues to limit operational parameters of the device.

Images