An embodiment of the present invention relates generally to a high voltage switch, and more particularly, to a high voltage switch utilizing low voltage metal-oxide-semiconductor (MOS) transistors with high voltage breakdown isolation junctions.
As complementary metal-oxide-semiconductor (CMOS) technology advances, channel lengths are reduced, thereby enabling high frequency operations. While it is possible to accommodate more functionality into a smaller area, short-channel transistors present a disadvantage in that limits to the source-drain voltage restrict the ability to apply high supply voltages. This issue is particularly manifested proximate interface sections, such as input/output (I/O) pads.
Unlike the system of
It is desirable to provide a circuit utilizing low voltage transistors for high voltage needs without an expensive and complex design that is unduly limited by the breakdown voltages of the transistors.
Briefly stated, an embodiment of the present invention comprises a high voltage switch that has first and second states and includes an input receiving an input voltage that is greater than a supply voltage. Each of first, second, and third MOS structures of a first conductivity type has a gate, a source, and a drain. The sources and drains of each of the MOS structures are electrically coupled in series between the input and ground. An output is electrically coupled to the input. When the switch is in the first state, the gate of the first MOS structure is pulled to ground, the gate of the second MOS structure is pulled to the supply voltage, and the gate of the third MOS structure is pulled to a voltage greater than the supply voltage and less than the input voltage. When the switch is in the second state, the gates of all of the MOS structures are pulled to the supply voltage.
Another embodiment of the present invention comprises a high voltage switch that has first and second states and includes an input receiving an input voltage that is greater than a supply voltage. Each of first, second, third, and fourth MOS structures of a first conductivity type has a gate, a source, and a drain. The sources and drains of each of the MOS structures are electrically coupled in series between the input and ground. The gate of the second MOS structure is electrically coupled directly to the supply voltage. An output is electrically coupled to the input. A voltage divider is electrically coupled between the input and the supply voltage and has a first output coupled to the gate of the fourth MOS structure and a second output coupled to the gate of the third MOS structure. A reverse-biased diode is electrically coupled between the input and the voltage divider. When the switch is in the first state, the gate of the fourth MOS structure is pulled to a first voltage, the gate of the third MOS structure is pulled to a second voltage, and the gate of the first MOS structure is pulled to ground. The first gate voltage is less than the input voltage and greater than the second voltage. The second voltage is greater than the supply voltage. When the switch is in the second state, the gates of the first, third, and fourth MOS structures are pulled to the supply voltage.
Still another embodiment of the present invention comprises a high voltage switch including first, second, and third MOS structures of a first conductivity type, each having a gate, a source, and a drain. The sources and drains of each of the MOS structures are electrically coupled in series between an input and ground. When the switch is in an on state, the gates of all of the MOS structures are pulled to a supply voltage. When the switch is in an off state, the gate of the first MOS structure is pulled to ground, the gate of the second MOS structure is pulled to the supply voltage, and the gate of the third MOS structure is pulled to a voltage greater than the supply voltage and less than an input voltage received by the input. The input voltage is greater than the supply voltage. An output is electrically coupled to the input. Voltage of the output is generally equal to a total saturation voltage of the first, second, and third MOS structures when the switch is in the off state.
The foregoing summary, as well as the following detailed description of preferred embodiments of the invention, will be better understood when read in conjunction with the appended drawings. For the purpose of illustration, there are shown in the drawings embodiments which are presently preferred. It should be understood, however, that the invention is not limited to the precise arrangements and instrumentalities shown.
Certain terminology is used in the following description for convenience only and is not limiting. The words “right”, “left”, “lower”, and “upper” designate directions in the drawings to which reference is made. The words “inwardly” and “outwardly” refer to directions toward and away from, respectively, the geometric center of the apparatus and designated parts thereof. The terminology includes the above-listed words, derivatives thereof, and words of similar import. Additionally, the words “a” and “an”, as used in the claims and in the corresponding portions of the specification, mean “at least one.”
As used herein, reference to conductivity will be limited to the embodiment described. However, those skilled in the art know that p-type conductivity can be switched with n-type conductivity and the device would still be functionally correct (i.e., a first or a second conductivity type). Therefore, where used herein, reference to n or p can also mean either n or p or p and n can be substituted therefor.
Current technology enables the isolation of transistors from one another using various techniques. One preferred technique utilizes a single crystal semiconductor-on-insulator (SOI), as shown in
Embodiments of the present invention are directed to a topology of devices, such as the device shown in
The switch 100 includes a number of semiconductor MOS structures (preferably transistors) of a first conductivity type (preferably n-type), each having a gate, a source, a drain, and a bulk connection. The sources and drains of the MOS structures are electrically coupled in series between the input 102 and ground GND.
The gates of the MOS structures 1, 2, 3, 4 are each pulled to a particular respective gate voltage VG1, VG2, VG3, VG4. The switch 100 preferably includes two states. In the first state, the gate of the lowest (closest to ground GND) MOS structure 1 is pulled to ground GND, the gate of the second lowest MOS structure 2 is pulled to the supply voltage Vdd, and the gates of the rest of the MOS structures are pulled to respectively higher voltages that are greater than the supply voltage Vdd but less than the voltage at the input 102 so that all of the MOS structures 1, 2, 3, 4 are “off.” Specifically in
The MOS structures 1, 2, 3, 4 are preferably identical. However, to compensate for possible mismatches or for optimum sizing, biasing resistors R1 are connected in parallel with each of the respective MOS structures 1, 2, 3, 4. The biasing resistors R1 preferably each have much higher resistances than the load R0 such that, for example in
It is seen that in both the first and second states, the gate voltage VG2 is equal to the supply voltage Vdd. Thus, the gate of the second MOS structure 2 may be electrically coupled directly to the supply voltage Vdd, as shown in
The voltage divider 206 shown in
When the first MOS structure 1 is turned “on,” the voltage across the MOS structure 1 becomes the saturation voltage VDSSAT1 of the first MOS structure 1, and the voltage between the source and gate of the second MOS structure 2 is sufficient to turn the second MOS structure “on.” The chain reaction continues up to the final MOS structure 4 such that the output voltage VOUT becomes the total saturation voltage VSATTOT, which as described above is much less than the supply voltage Vdd. With the diode D1 being reverse biased, all of the gate voltages VG1, VG2, VG3, and VG4 are pulled to the supply voltage Vdd and the switch 200 is in the second state with all of the MOS structures 1, 2, 3, 4 being “on.”
When the divider resistors R2 are relatively large, the switch 200 may experience a lag due to capacitance at the gates preventing rapid transition between states. To compensate,
Source follower MOS structures are preferably utilized for driving the gates of MOS structures above the second MOS structure 2 having its gate coupled directly to the supply voltage Vdd. For example, a first source follower MOS structure 5 is used to drive the gate of the fourth MOS structure 4, and a second source follower MOS structure 6 is used to drive the gate of the third MOS structure 3. The source follower MOS structures 5, 6 are preferably of the first conductivity type (preferably n-type), each having a gate, a source, a drain, and a bulk connection. Gates of the source follower MOS structures 5, 6 are electrically coupled to respective outputs 308 of the voltage divider 306. The source and drain of the first source follower MOS structure 5 are electrically coupled between the input 302 and the gate of the fourth MOS structure 4, and the source and drain of the second source follower structure are electrically coupled between the respective gates of the third and fourth MOS structures 3, 4. It is thus seen that the first source follower MOS structure 5 and the fourth MOS structure 4 (as well as the second source follower MOS structure 6 and the third MOS structure 3) are configured much like a Darlington pair. As a result, an increase in gain is obtained such that only a small current is required to switch “on” the respective pair, thus reducing delay caused by the divider resistors R2.
Discharge MOS structures are also preferably utilized with respective source follower MOS structures. For example, first discharge and second discharge MOS structures 7, 8 are preferably of a second conductivity type opposite to the first conductivity type (preferably p-type), each having a gate, a source, a drain, and a bulk connection. Gates of the discharge MOS structures 7, 8 are electrically coupled to respective outputs 308 of the voltage divider 306. The source and drain of the first discharge MOS structure 7 are electrically coupled between the respective gates of the third and fourth MOS structures 3, 4. The source and drain of the second discharge MOS structure 8 are electrically coupled between the gate of the third MOS structure 3 and the supply voltage Vdd. Additional resistors R3 may be added to the switch 300 in parallel with each of the discharge MOS structures 7, 8 to prevent gate nodes from leaking high. The discharge MOS structures 7, 8 speed up the gate discharge through the additional resistors R3 by clamping the gate voltages VG3, VG4 to be higher than the respective divider resistor R2 node by the gate voltage of the respective discharge MOS structure 7, 8.
From the foregoing, it can be seen that none of the gate oxides of the MOS structures 1, 2, 3, 4 experiences a voltage higher than the supply voltage Vdd, while an output swing may be between the total saturation voltage VDSSATTOT and the source voltage (e.g., 4×Vdd).
The foregoing examples described and showed the MOS structures 1, 2, 3, 4, as NMOS transistors, but it is understood by those skilled in the art that a similar arrangement may be configured using PMOS transistors.
It will be appreciated by those skilled in the art that changes could be made to the embodiments described above without departing from the broad inventive concept thereof. It is understood, therefore, that the invention is not limited to the particular embodiments disclosed, but it is intended to cover modifications within the spirit and scope of the present invention as defined by the appended claims.