Data read-out circuit, data read-out method, and data...

Static information storage and retrieval – Systems using particular element – Ferroelectric

Reexamination Certificate

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C365S189120

Reexamination Certificate

active

06487103

ABSTRACT:

BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to a data readout circuit, a data readout method, and a data storage device.
2. Description of the Related Art
FIG. 1
is a circuit diagram showing the structure of a conventional ferroelectric memory. As shown in
FIG. 1
, the conventional ferroelectric memory comprises a word line WL, a bit line BL, a ferroelectric capacitor CF, n-channel MOS transistors
12
,
14
,
17
A,
17
B,
18
A,
18
B, and Ti, p-channel MOS transistors T
8
to T
10
, capacitors
19
and
22
, and nodes NA and NB. The bit line BL has a bit line stray capacitance CBL.
Here, the gate of the n-channel MOS transistor
14
is connected to the word line WL. One terminal of the source/drain of the n-channel MOS transistor
14
is connected to the bit line BL, while the other terminal is connected to the ferroelectric capacitor CF. A plate line CP is connected to one terminal of the ferroelectric capacitor CF.
A voltage V
CON
is supplied to the n-channel MOS transistors
17
A and
17
B, while a reference voltage V
ref
is supplied to the source/drain of the n-channel MOS transistor
17
A. A voltage VN is supplied to the gate of the n-channel MOS transistor
12
, and a voltage RES is supplied to the gate of the n-channel MOS transistor T
1
. A voltage VP is supplied to the gate of the p-channel MOS transistor T
8
.
In the above ferroelectric memory, the single n-channel MOS transistor
14
and the single ferroelectric capacitor CF constitute one ferroelectric memory cell, as shown in FIG.
1
. This ferroelectric capacitor CF holds digital information consisting of 1 or 0 in a non-volatile state by taking a reverse polarized state.
Next, an operation to write the data in the ferroelectric memory cell will be described. When the information of “1” is written in the ferroelectric memory cell, the potential of the bit line BL serves as a ground potential. When the information of “0” is written in the ferroelectric memory cell, the potential of the bit line BL serves as a power potential Vcc. The word line WL is then activated, so that the n-channel MOS transistor
14
is energized and that the potential of the plate line CP changes from the ground potential to the power source potential Vcc and returns to the ground potential. Receiving the voltage, the ferroelectric capacitor CF shifts to a predetermined polarized state, and holds the information of “1” or “0”. When the data write operation is completed, the potential of the bit line BL is returned to the ground potential.
Next, an operation to read out data from the ferroelectric memory cell will be described. In this case, the potential of the bit line BL serves as the ground potential. The word line WL is activated, so that the n-channel MOS transistor
14
is energized, and that the potential of the plate line CP shifts from the ground potential to the power source potential Vcc, thereby moving the charges polarized to the ferroelectric capacitor CF to the bit line BL. Here, the potential of the bit line BL greatly or slightly rises depending on the polarized state of the ferroelectric capacitor CF.
For instance, a latched sense amplifier circuit compares the potential of the bit line BL with the reference potential. In the initial state, the power source to the sense amplifier circuit is off, and when voltage is applied to the two input terminals, the power is supplied to the sense amplifier circuit. At this point, the input terminal having the potential higher than the other rises to the power source potential Vcc, and the input terminal having the potential lower than the other drops to the ground potential. By this sense amplifier circuit, data held by the ferroelectric capacitor CF can be read out.
FIGS. 2A
to
2
I are timing charts showing the data read-out operation performed by the conventional ferroelectric memory shown in FIG.
1
. As shown in
FIGS. 2A and 2B
, a voltage V
CON
and a signal RES are activated from 0 V (low level) to 3 V (high level) at time t
1
. By doing so, the potential of the bit line BL is initialized to 0 V, as shown in FIG.
2
G. As shown in
FIG. 2A
, the voltage VCON is high until time t
4
.
As shown in
FIG. 2C
, the word line WL is activated at time t
2
, and the n-channel MOS transistor
14
is switched on. As shown in
FIG. 2D
, the potential of the plate line CP rises from 0 V to the power source potential (3 V) at time t
3
. Here, the potential of the bit line BL rises depending on the polarized charge amount of the ferroelectric capacitor CF, as shown in FIG.
2
G.
In
FIGS. 2G
to
2
I, each converted capacitance value, 0.2 pF, of the ferroelectric capacitor CF is indicated by a solid line, while each converted capacitance value, 0.05 pF, is indicated by a broken line. As can be seen from the timing charts, the larger the polarized charge amount, the higher the potential of the bit line BL. When the converted capacitance value of the ferroelectric capacitor CF is 0.2 pF, the potential of the bit line BL rises up to 0.5 V, which will be described more later.
Next, as shown in
FIG. 2E
, the voltage VN to be supplied to the gate of the n-channel MOS transistor
12
that serves as a power switch for a sense amplifier is shifted to the high level at time t
5
. Here, as shown in
FIGS. 2H and 2I
, if the potential of the node NA (the potential of the bit line BL) is lower than the potential of the node NB (the reference voltage V
ref
), the potential of the node NA becomes 0 V while the potential of the node NB becomes equal to the reference voltage V
ref
, as indicated by the broken lines. On the other hand, the potential of the node NA is higher than the potential of the node NB, the potential of the node NA does not fluctuate, but the potential of the node NB shifts to 0 V, as indicated by the solid lines.
Next, as shown in
FIG. 2F
, a voltage VP to be supplied to the gate of the p-channel MOS transistor T
8
that serves as a VCC power switch for a sense amplifier is shifted to the low level at time t
6
. As shown in
FIGS. 2H and 2I
, if the potential of the node NA is lower than the potential of the node NB, the potential of the node NA is 0 V while the potential of the node NB becomes 3 V, as indicated by the broken lines. On the other hand, if the potential of the node NA is higher than the potential of the mode NB, the potential of the node NA becomes 3V while the potential of the node NB remains 0 V, as indicated by the solid lines.
As described above, after one of the potentials of the node NA and the node NB is shifted to 0 V while the other one of the potentials is shifted to 3 V, the potential of the node NA is transmitted via the bit line BL, so that the information stored in the ferroelectric memory cell is read out.
In the process of reading out information from the conventional ferroelectric memory shown in
FIG. 1
, the potential of the bit line rises depending on the polarization of the ferroelectric capacitor. Assuming that a cell capacitance value determined from the polarized charge amount of the ferroelectric capacitor and the voltage supplied between the electrodes is about 0.2 pF, the parasitic capacitance of the bit line is 1 pF, and the power source voltage is 3 V, the voltage of the bit line rises, by 0.5 V, which is calculated by 3 V×0.2 pF/(0.2 pF +1pF), when the plate line rises from 0 V to 3 V. The potential of the bit line is shown in FIG.
2
G. Accordingly, the voltage to be supplied to the ferroelectric capacitor becomes 2.5 V, which is calculated by 3 V−0.5 V.
Intensive studies have been made on lowering the read-out voltage of the properties of the ferroelectric capacitor. However, polarized electric charge cannot adequately read out with a low read-out voltage, which results in inaccurate information read-out and reduction of read-out margins.
Meanwhile, to reduce the power consumption of portable telephones and mobile electronic equipment, there has been a strong demand for lowering the power source voltage as well. If the bit line capacitance is increased, a rise of the voltage

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