Pump circuits using flyback effect from integrated inductance

Miscellaneous active electrical nonlinear devices – circuits – and – Specific identifiable device – circuit – or system – With specific source of supply or bias voltage

Reexamination Certificate

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C327S536000

Reexamination Certificate

active

06538494

ABSTRACT:

FIELD OF THE INVENTION
The present invention relates to generating a larger magnitude output voltage from an input voltage, and more particularly, to on-chip charge pumps.
BACKGROUND OF THE INVENTION
Many electronic devices require a plurality of operating voltages. However, the power supply which furnishes power to electronic devices often only have a rather limited number of different output voltages. Thus, many electronic devices include power conversion circuitry to ensure the availability of the required voltages.
In many instances, the magnitude of an input power signal must be converted to a power signal having a voltage with a higher magnitude. Devices which perform this type of power conversion are known as charge pumps. For example, if a charge pump is provided with a positive input voltage, it may generate an output voltage which is more positive than the input voltage. Alternatively, if a charge pump is provided with a negative input voltage, it may generate an output voltage which is more negative than the input voltage.
One example of an electronic device which requires a charge pump is a dynamic random access memory (DRAM) device. DRAM devices typically include a large plurality (e.g., millions) of DRAM cells arranged in one or more arrays. A typical DRAM cell
100
is illustrated in FIG.
1
. The information stored in a DRAM cell
100
is written to or read from a capacitor
102
. The capacitor
102
is coupled to a potential source
105
and a source
101
s
of a transistor
101
. The transistor
101
is used to control access to the capacitor, and is itself coupled to a word line
104
via gate
101
g
, as well as bit line
103
via drain
101
d
. The DRAM cell
100
is said to store a logical 0 if the amount of charge stored within the capacitor is such that node
102
a
is at a potential less than a reference potential, for example, ground potential. If the amount of charge stored in the capacitor
102
is such that the potential at node
102
a
is greater than the reference potential, the DRAM cell
100
is said to store a logical 1, for example Vcc potential. The reference potential corresponds to the potential of a reference capacitor (not shown) having an equilibrated charge, and typically corresponds to ½ Vcc. Typical values for Vcc include 5.0 volts and 3.3 volts. However, there is a trend towards using smaller voltages for Vcc, since reducing the magnitude of Vcc is advantageous for reducing power consumption, thereby permitting higher density and/or higher speed DRAM devices. DRAM devices are ordinarily coupled to power line(s) having a potential of Vcc. Many portions of a DRAM device require a voltage Vpp which is greater than Vcc. The DRAM device must therefore use a charge pump to create the higher Vpp and Vccp potentials from Vcc.
FIG. 2
is an illustration of a semiconductor device
200
which includes an integrated charge pump
202
. The charge pump
202
and the operational circuit
203
are coupled to a ground potential GND via ground signal line
206
and to Vcc via signal line
205
. The operational circuit
203
may include a variety of circuits. If the semiconductor device
200
is a DRAM, then the operational circuit would include portions of the DRAM circuitry. The semiconductor device
200
may alternatively be any number of other devices which may require the use of a charge pump
202
to generate a higher potential from base potential.
FIG. 3
is an illustration of a simple prior art pump circuit
300
. The pump circuit
300
comprises an oscillator
301
which produces a square wave (or pulse train) which swings between ground potential and Vcc. An inverter
302
may be used to condition the square wave. The oscillator
301
produces a signal having a potential Vcc during a first phase. After the signal passes through inverter
302
, it arrives at node
303
having ground potential. Meanwhile, transistor
306
, which has a drain coupled to a power source having a potential of Vcc, is conducting, while transistor
307
is non-conducting. Thus, node
305
has a potential somewhat lower than Vcc and charge from the power source Vcc is being stored into capacitor
304
. As charge is stored in capacitor
304
, the potential at node
305
increases.
During the second phase of the oscillator
301
, the oscillator
301
produces a signal at ground potential, which is transformed by the inverter
302
into a signal having a potential of Vcc. This further charges capacitor
304
and further raises the voltage at node
305
. As the potential at node
305
builds, transistor
306
becomes non-conducting while transistor
307
becomes conducting. This causes the charge stored in capacitor
304
to be shared with the loading capacitor
308
, thereby raising the voltage at the output terminal
309
. During subsequent clock cycles, the charge stored in capacitor
304
during the first phase of the oscillator is transferred to the loading capacitor
308
during the second phase, resulting in a elevated voltage Vccp at the output terminal
309
.
The prior art pump circuit
300
is dependent upon the capacitor
304
to generate the boosted voltage Vccp. This limits the operating frequency of the prior art pump circuit to the rate at which the capacitor
304
can be charged and discharged. As semiconductor devices such as DRAMs increase in frequency, it becomes increasingly difficult to charge and discharge the capacitor
304
at a corresponding higher rate. Thus, the prior art pump circuit
300
is unsuitable for use in high speed memory devices. Accordingly, there is a need for an apparatus and a method for a charge pump which is suitable for operation in high speed and/or low powered semiconductor devices.
SUMMARY OF THE INVENTION
The present invention is directed at an on-chip charge pump capable of supplying the boosted voltage required in a high speed semiconductor device such as a high speed dynamic random access memory (DRAM). The charge pump of the present invention is powered by the flyback effect of an inductor. The use of an inductor's flyback effect for the purpose of generating a boosted voltage is known. For example, the flyback effect is routinely used to generate the 10 kV high anode voltage in televisions and other cathode ray tube devices. However, semiconductor devices have traditionally used capacitor based charge pumps. In the present invention, a flyback based charge pump and its associated inductor are integrated into the semiconductor device. In the high speed semiconductor device, such as a DRAM, an inductor based charge pump may be operated at higher frequency than a traditional capacitor based charge pump.


REFERENCES:
patent: 5126590 (1992-06-01), Chern
patent: 5267218 (1993-11-01), Elbert
patent: 5367489 (1994-11-01), Park et al.
patent: 5721509 (1998-02-01), Taft et al.
patent: 5939866 (1999-08-01), Biorkengen
patent: 6011743 (2000-01-01), Khang
patent: 6091613 (2000-07-01), Yang et al.
patent: 6160440 (2000-12-01), Javanifard et al.
patent: 6160749 (2000-12-01), Pinkham et al.
patent: 406045148 (1994-02-01), None
Arcioni et al., “Design and Characterization of Si Integrated Inductors”, IEEE Instumentation and Measurement Technology Conference, 5/98.
Chap. 1, An Introduction to DRAM, Sec. 1.2 DRAM Basics, pp. 24-29.
28V, Low-Power, High Voltage, Boost or Inverting DC-DC Converter.
Chap. 6, Voltage Converters, Sec. 6.2 Pumps and Generators, pp. 166-171.
Brent Keeth, “A DRAM Circuit Design Tutorial”, Micron Technology, Inc., 12/95, pp. 75-79.

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