Read operation scheme for a high-density, low voltage, and...

Static information storage and retrieval – Floating gate – Particular biasing

Reexamination Certificate

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C365S185170

Reexamination Certificate

active

06175522

ABSTRACT:

FIELD OF THE INVENTION
The present invention relates to non-volatile semiconductor flash memory devices and, more particularly, to a scalable, lower voltage NAND flash memory device.
BACKGROUND OF THE INVENTION
Conventional flash memory devices, otherwise known as flash electrically erasable programmable read only memories (FLASH EEPROMs), typically include a two-dimensional array of floating gate memory transistors, or “cells,” formed on a semiconductor substrate. These cells are arranged into strings, known as NAND strings, to form bit lines, wherein each cell is coupled to the next cell in the string by coupling the source of one transistor to the drain of another transistor. Word lines, disposed perpendicularly to the bit lines, connect to the control gate of one transistor in each NAND string.
A portion of a flash memory circuit, including three bit lines
302
,
304
, and
306
and four of sixteen word lines, is depicted in FIG.
3
. Each bit line, e.g. bit line
304
, comprises a NAND string of floating gate transistors coupled in series source to drain, for example, transistors
310
,
312
, and
314
for bit line
304
.
FIG. 4
shows a cross-section of floating gate transistors
310
,
312
, and
314
on bit line
304
. Floating gate transistor
312
is formed on a substrate
400
, having a source region
402
(which is a drain region for neighboring transistor
314
), a drain region
404
(which is a source region for neighboring transistor
310
), and a doped channel region
406
. A gate oxide
408
is formed on the channel region
406
to insulate the floating gate
410
from the channel region
406
. An insulating layer
412
physically and electrically separates the floating gate
410
from a control gate
414
, which is coupled to an appropriate word line, e.g., word line
2
for floating gate transistor
312
.
Initially, the cells in a flash memory are erased so that the floating gate memory transistors are at a certain threshold voltage, such as about −2V. Selected cells are programmed by applying a high voltage, such as about 18V-23V, to the word lines of the selected cells. For example, selected cell
312
is programmed by applying a high voltage to word line
2
. Applying the programming voltage causes electrons tunneling from the silicon substrate to the floating gate
410
of a selected flash memory transistor
312
, thereby increasing the threshold voltage of the selected flash memory transistor
312
to a positive voltage, such as about +1V. By adjusting the threshold voltage of selected floating gate memory transistors, flash memory cells are programmed to store data.
A conventional approach for reading data from a selected memory cell involves selecting a bit line by applying a IV bias to the drain end of a selected bit line and grounding the drain ends of unselected bit lines and the source ends of both selected and unselected bit lines. A memory cell on a particular word line is selected by applying a gate voltage (V
GATE
) of about 0V to the word line and by applying a pass voltage (V
PASS
) of about 4.5V to the other word lines. The pass voltage is sufficient to cause unselected cells on the selected bit line to turn on. Referring to
FIG. 3
, if the floating gate transistor
312
of a selected cell has been programmed to a 1V threshold voltage, then the gate voltage V
GATE
=0 is insufficient to turn the floating transistor
312
on and very little drive current is produced from the selected transistor for the selected bit line indicating that the selected cell is programmed. On the other hand, if the floating gate transistor
312
of the selected cell is still at the erased threshold voltage (e.g. at −2V), then the floating gate transistor
312
is on, since the gate voltage V
GATE
=0 is greater than the threshold voltage (−2V). Accordingly, a drive current is produced for the selected bit line indicating that the selected cell is erased.
Escalating demands for high density and performance associated with flash memory devices challenge the limitations of conventional flash memory technology. For example, it is desirable to reduce the channel length of the floating gate transistor to pack the transistors more densely. However, merely shortening the channel length from a conventional 0.25 &mgr;m to produce smaller transistors creates a “punchthrough” condition. Referring again to
FIG. 4
, punchthrough is a malfunction which occurs when the depletion region
420
caused by a source-drain bias extends through the entirety of the channel region
406
and short-circuits the transistor. Consequently, the transistor is always turned on and thus appears to be always erased even though it is programmed.
Furthermore, the conventional flash memory device depicted in
FIG. 3
requires a 4.5V pass voltage. As lower power supply voltages, e.g. 3.3V, become more popular, however, it is desirable to use a lower pass voltage, commensurate with the power voltage, and to reduce the silicon substrate doping concentration for improved tunnel oxide integrity and product reliability. However, merely reducing the doping level of the channel region to reduce the threshold voltage for the lower pass voltage exacerbates the punchthrough problem. Consequently, conventional flash memory devices employ additional voltage boosting circuitry, such as a charge pump, to provide a 4.5V pass voltage from a 3.3V power supply. This additional circuitry increases the die size and hinders scalability.
When the pass voltage on the unselected cell in the selected bit line is increased, however, the electric field across the tunnel oxide is also increased. This electric field encourages electrons to leak into the floating gate from the silicon substrate through trap assisted tunneling processes. Since the rate of charge leakage is exponentially proportional to the electric field, a high pass voltage results in a greater occurrence of a charge gain error and impairs device reliability. Therefore, it is also desirable to lower the pass voltage to reduce the occurrence of “read disturb,” an error condition in which a cell is accidentally programmed during a read operation.
SUMMARY OF THE INVENTION
There exists a need for scalable flash memory device in which the channel length of the floating gate transistors can be smaller than 0.25 &mgr;m, especially without the problems of punchthrough associated with conventional devices. There is also a need for a flash memory that can use a lower power supply voltage, eg. 3.3V, without requiring additional voltage boosting circuitry or encountering the problems associated with punchthrough and read disturb.
This and other needs are addressed by the present invention in which the source end of the NAND string is biased with a voltage of at least about 0.5V, preferably from about 0.1V to about 1.5V. Biasing the source end of a floating transistor in accordance with the present invention raises the potential batter at the source side and reduces the extent of the depletion region and, hence, the occurrence of punchthrough. Consequently, the channel length can be decreased to improve scalability and the doping level of the channel region can be reduced to enable the use of lower pass voltages commensurate with smaller power supply voltages. As a result, the charge retention and reliability of a memory cell be significantly improved.
Accordingly, one aspect of the invention relates to a method of reading a selected memory cell in a bit line including a string of memory transistors coupled drain to source in series. Each of the memory transistors has a gate coupled to a respective word line. The method includes applying a source end potential about 0.5V to a source end of the string of memory transistors and reading the selected memory cell while the source end is biased to about 0.5V. Preferably, the source end potential is in the range from about 0.1V to about 1.5V, the potential at the drain end of the selected string is at least about 1.0V higher than the source end potential, and a pass voltage is about 3.0V to abo

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