The present invention relates to a method and/or architecture for voltage generators generally and, more particularly, to a method and/or architecture for a proportional to absolute temperature (PTAT) voltage generator.
Data (e.g., a “1” or a “0”) is stored in a 1T memory cell as a voltage level. A “1” is stored as a high voltage level which can decrease due to leakage. A “0” is stored as a voltage level of zero volts which can increase due to leakage. The 1T memory cell requires a periodic refresh to maintain the voltage level stored in the cell. In many applications, a memory chip uses a ring oscillator to control when the refreshes occur. The frequency of a signal generated by a typical ring oscillator decreases with increasing temperature because of CMOS device characteristics. However, the memory cell leakage increases with temperature. As the temperature increases, refresh using a conventional oscillator can occur less frequently than necessary to maintain the voltage level stored in the memory cell. Thus, the oscillator needs to be designed to support the high temperature refresh rate at the expense of more current.
Proportional to absolute temperature(PTAT) voltages and currents are used in temperature monitoring circuits. The monitoring circuits either detect a specific temperature or output a voltage and/or current that increases with temperature. The temperature monitoring circuits can use a PTAT and an inverse PTAT, where the crossing point is a desired temperature. A conventional method of generating PTAT voltage is to use a delta Vbe generator circuit.
Referring to
where T is the absolute temperature in Kelvin, n is the emission coefficient, k is Boltzmann's constant, q is the charge of an electron, Is is the theoretical reverse saturation current, A is the smaller of the areas of diodes 12 and 14, B is the ratio of the areas of the diodes 12 and 14, and R is the resistance of the resistor 16. The resistance R generally has a positive temperature coefficient. The emission coefficient n is related to the doping profile and affects the exponential behavior of the diodes 12 and 14. The value of n is normally approximated to be 1.
The voltage VREF is proportional to the temperature T, ln(T), and 1/R(T). Also, a current I is generated equal to Vt*ln(B)/R which is proportional to temperature since R has a positive temperature coefficient and Vt=k*T/q. The voltage VREF is generated by using a voltage across a diode with the bandgap current I flowing through the diode. The circuit 10 has the following disadvantages: a complex relationship between temperature and the voltage VREF (i.e., the voltage VREF is a function of T, ln(T), and ln(1/R(T)); the value of the voltage VREF is limited when the bandgap current I is also used to generate a PVT compensated voltage; and a larger value for the voltage VREF requires a higher current I.
The present invention concerns a biasing circuit comprising a first circuit and a second circuit. The first circuit may be configured to generate a first bias signal and a second bias signal. The second bias signal may be defined by a threshold voltage and a first resistance. The second circuit may be configured to generate a third bias signal in response to the first and the second bias signals and a second resistance. The third bias signal may have a magnitude that is linearly proportional to absolute temperature (PTAT) and be configured to vary a refresh rate of a memory cell in response to changes in temperature.
The objects, features and advantages of the present invention include providing a method and/or architecture for a proportional to absolute temperature (PTAT) voltage generator that may (i) use a bandgap reference with a current equal to Vt*ln(B)/R, (ii) use one additional resistor to form a linear PTAT voltage reference, and/or (iii) provide a PTAT voltage reference that may be scaled by a ratio of resistor values.
These and other objects, features and advantages of the present invention will be apparent from the following detailed description and the appended claims and drawings in which:
Referring to
The circuit 102 may comprise a transistor 110, a transistor 112, a transistor 114, a transistor 116, a transistor 118, a device 120, a device 122, a device 124, and an amplifier 126. The transistors 110-114 may be implemented as one or more PMOS transistors. The transistors 116 and 118 may be implemented as one or more NMOS transistors. However, other types and/or polarity of transistors may be implemented accordingly to meet the design criteria of a particular application. The devices 120 and 122 may be implemented as base-emitter junction devices (e.g., diodes, diode-connected transistors, etc.). In one example, the devices 120 and 122 may be implemented as forward biased diodes. The device 120 may have an area A. The device 122 generally has an area that is B times A, where B is an integer. The device 124 may be implemented as a resistive circuit. In one example, the device 124 may be implemented as a resistor having a predetermined resistance R. The amplifier 126 may be implemented as an operational amplifier circuit.
The transistors 112-118 and the devices 120-124 may be configured as a delta Vbe generator circuit. A source of the transistor 110 may be connected to a supply voltage (e.g., VCC). A node 128 may be formed by coupling a drain of the transistor 110 with a source of the transistor 112 and the transistor 114. The signal VBIAS may be presented at the node 128. A node 130 may be formed by coupling a gate of the transistor 112, a gate and a drain of the transistor 114, and a drain of the transistor 118. The signal VREF may be presented at the node 130. A node 132 may be formed by coupling a drain of the transistor 112, a drain and a gate of the transistor 116, and a gate of the transistor 118. A source of the transistor 116 may be coupled to a first terminal of the device 120. A second terminal of the device 120 may be connected to a voltage supply ground potential (e.g., VSS). A source of the transistor 118 may be coupled to a first terminal of the device 124. A second terminal of the device 124 may be coupled to a first terminal of the device 122. A second terminal of the device 122 may be connected to the voltage supply ground potential VSS. The first terminals of the devices 120 and 122 may be connected, in one example, to anodes of the devices 120 and 122. The second terminal of the devices 120 and 122 may be connected, in one example, to cathodes of the devices 120 and 122.
A first input (e.g., a non-inverting input) of the amplifier 126 may be coupled to the node 130. A second input (e.g., an inverting input) of the amplifier 126 may be coupled to the node 132. An output of the amplifier 126 may be coupled to a gate of the transistor 110. The amplifier 126 generally forces a current (e.g., I) through the transistors 114 and 118 to be the same as a current through the transistors 112 and 116. The current I may be described by the following equation 2:
The circuit 104 may comprise a transistor 140, a device 142, a transistor 144, a transistor 146, a transistor 148, and a transistor 150. The transistors 140, 148 and 150 may be implemented as one or more PMOS transistors. The transistors 144 and 146 may be implemented as one or more NMOS transistors. However, other types and polarity transistors may be implemented accordingly to meet the design criteria of a particular application. The device 142 may be implemented as a resistive circuit. In one example, the device 142 may be implemented as a resistor having a predetermined resistance R1.
The signal VBIAS may be presented to a source of the transistor 140. The signal VREF may be presented to a gate of the transistor 140. A drain of the transistor 140 may be coupled to a first terminal of the device 142. The signal NCTR may be presented at the drain of the transistor 140. A second terminal of the device 142 may be connected to the voltage supply ground potential VSS. The transistor 140 will generally pass a current equal to the current I in response to the signals VREF and VBIAS. By passing the current I (where I=n*Vt*ln(B)/R, n is the emission coefficient; B is the ratio of diode areas of the devices 120 and 122, R is a predetermined resistance, and Vt is a thermal voltage) through the resistance R1, a voltage may be generated, as shown by the following equation 3:
When the current I is passed through the device 142, the signal NCTR may be generated having a voltage level equal to ln(B) times Vt times R1/R. The voltage level of the signal NCTR is generally proportional to absolute temperature and may be scaled by selecting the ratio R1/R.
The signal NCTR may be presented to a gate of the transistor 144. A source of the transistor 144 and a gate of the transistor 148 may be connected to the voltage supply ground potential VSS. A drain of the transistor 144 may be connected to a source of the transistor 146. A gate of the transistor 146 may be connected to the supply voltage VCC. A drain of the transistor 146 may be connected to a drain of the transistor 148. A source of the transistor 150 may be connected to the supply voltage VCC. A node 152 may be formed by connecting a source of the transistor 148 with a drain and a gate of the transistor 150. The signal PCTR may be presented at the node 152. The signal PCTR may be a mirror of the signal NCTR.
Referring to
The circuit 200 may be implemented as a refresh oscillator of a dynamic memory device. Since the leakage of the memory cells increase with increasing temperature, a PTAT voltage-controlled oscillator in accordance with the present invention may be used to refresh the memory cell more frequently as the temperature increases. The present invention may provide temperature dependent refreshing and also may be used in any application requiring a temperature monitor.
Referring to
While the invention has been particularly shown and described with reference to the preferred embodiments thereof, it will be understood by those skilled in the art that various changes in form and details may be made without departing from the spirit and scope of the invention. For example, any circuit that generates a current equal to a constant times Vt/R may be used to generate the PTAT voltage reference NCTR.
This is a continuation of U.S. Ser. No. 09/885,897 filed Jun. 20, 2001, now U.S. Pat. No. 6,628,558, issued Sep. 30, 2003.
Number | Name | Date | Kind |
---|---|---|---|
4165642 | Lipp | Aug 1979 | A |
4393477 | Murotani | Jul 1983 | A |
4450367 | Whatley | May 1984 | A |
4603291 | Nelson | Jul 1986 | A |
4682306 | Sakurai et al. | Jul 1987 | A |
4716551 | Inagaki | Dec 1987 | A |
4978930 | Suter | Dec 1990 | A |
5072197 | Anderson | Dec 1991 | A |
5175512 | Self | Dec 1992 | A |
5180995 | Hayashi et al. | Jan 1993 | A |
5278796 | Tillinghast et al. | Jan 1994 | A |
5291071 | Allen et al. | Mar 1994 | A |
RE34772 | Bernard et al. | Nov 1994 | E |
5375093 | Hirano | Dec 1994 | A |
5392251 | Manning | Feb 1995 | A |
5428319 | Marvin et al. | Jun 1995 | A |
5434534 | Lucas | Jul 1995 | A |
5440277 | Ewen et al. | Aug 1995 | A |
5444219 | Kelly | Aug 1995 | A |
5495452 | Cha | Feb 1996 | A |
5646518 | Lakshmikumar et al. | Jul 1997 | A |
5774013 | Groe | Jun 1998 | A |
5898343 | Morgan | Apr 1999 | A |
5963103 | Blodgett | Oct 1999 | A |
6016051 | Can | Jan 2000 | A |
6134167 | Atkinson | Oct 2000 | A |
6181121 | Kirkland et al. | Jan 2001 | B1 |
6181191 | Paschal | Jan 2001 | B1 |
6191660 | Mar et al. | Feb 2001 | B1 |
6198356 | Visocchi et al. | Mar 2001 | B1 |
6222399 | Imbornone et al. | Apr 2001 | B1 |
6359809 | Tedrow et al. | Mar 2002 | B1 |
6404690 | Johnson et al. | Jun 2002 | B2 |
Number | Date | Country | |
---|---|---|---|
20030198114 A1 | Oct 2003 | US |
Number | Date | Country | |
---|---|---|---|
Parent | 09885897 | Jun 2001 | US |
Child | 10430971 | US |