Abstract:
A radiation measuring technique includes adjusting a threshold level of a radiation sensor in a radiation-measuring circuit and obtaining an output signal based on radiation dose sensed by the radiation sensor.

Description:
BACKGROUND  
         [0001]    This invention relates to a CMOS radiation-measuring circuit with a variable threshold.  
           [0002]    A complementary-symmetry MOSFET (CMOS) radiation-measuring circuit may include transistors configured to provide a digital output that changes from one state to another when the radiation dose absorbed by the circuit exceeds a threshold. The size of the devices used in the CMOS radiation-measuring circuit determines the radiation dosage that will cause the digital output of the CMOS radiation-measuring circuit to change from one digital state to another digital state. Hence, the design of a CMOS radiation-measuring circuit requires careful consideration of the size of transistors in the circuit.  
           [0003]    When the voltage applied between the gate and source terminals of a MOSFET exceeds a certain voltage, the MOSFET turns on. This voltage is referred to as the threshold voltage. The threshold voltages of p-channel type MOSFET (pMOS) and n-channel type MOSFET (nMOS) devices are sensitive to ionizing radiation. Generally, the threshold voltage of an irradiated MOSFET device shifts due to an increase of trapped charge in the oxide and interface states. 
       
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0004]    [0004]FIG. 1 illustrates a system that includes a radiation sensor.  
         [0005]    [0005]FIG. 2 is a schematic of a radiation sensor with a variable threshold. 
     
    
     DETAILED DESCRIPTION  
       [0006]    As shown in FIG. 1, a CMOS radiation-measuring circuit  1  with a variable threshold may be exposed to a source of radiation  2  to determine when a threshold radiation dose has been reached. The radiation-measuring circuit  1  includes a radiation sensor  3  and an auxiliary circuit  4 . The radiation-measuring circuit  1  may be used, for example, as a built-in radiation-measuring circuit in standard circuits to prevent malfunction due to radiation hazards. The CMOS radiation-measuring circuit with a variable threshold may have a wide range of applications in spacecraft design, medicine, nuclear plant and personal dosimetry. The radiation-measuring circuit may be used as or incorporated in a dosimeter. Depending on its specific application, dose ranges from millirads to tens of megarads may be detected by the circuit.  
         [0007]    [0007]FIG. 2 illustrates details of a CMOS radiation-measuring circuit that may be used to measure a variable radiation dose. A pMOS transistor P 1  serves as the radiation sensor  3 . This transistor is coupled to the auxiliary circuit  4  that includes a current mirror with pMOS transistors P 2  and P 3 . The pMOS current mirror generates a current that is a multiple of the reference current source (I sens ). For example, in one implementation, the current through the second side of the current mirror (transistor P 3 ) is ten times the reference current (I sens ) through the first side of the current mirror (transistor P 2 ). The source terminal of the radiation-sensing transistor P 1  is coupled to a first side of the current mirror (transistor P 2 ) through a resistive element N 1 . Thus, the radiation-sensing transistor P 1  is biased through the resistive element N 1  and the transistor P 2 .  
         [0008]    The resistive element N 1  causes the voltage at the drain terminal of the transistor P 2  to differ from the voltage (V a ) at the source terminal of the radiation-sensing transistor P 1 . The resistance of the element N 1  should not be affected by radiation. In some implementations, the resistive element N 1  may include a resistor. However, the use of a transistor as the resistive element N 1  can provide better efficiency and better control because it uses less silicon area. In one embodiment, the resistive element N 1  includes an nMOS transistor with its gate terminal shorted to its drain terminal. The transistor P 2  that forms the first side of the current mirror may have its gate terminal shorted to its drain terminal. The source terminal of the sensing transistor P 1  also is coupled to an output load nMOS transistor N 2  that is coupled to the second side of the current mirror (transistor P 3 ).  
         [0009]    The width (W) and length (L) of a channel region of a pMOS transistor affects its behavior. The current through the left-hand side of the circuit (I sens ) may be approximated by:  
           I   sens   =μpC   ox ( W/L )( V   a   −|V   tP1 |) 2    
         [0010]    where μp is the hole mobility, C ox  is the gate oxide capacitance, and V tP1  is the threshold voltage of transistor P 1 . The dimensions of the devices used in the radiation-measuring circuit can be selected so that when the circuit is not exposed to radiation and the input voltage (V in ) across the body terminal and the source terminal of the radiation-sensing transistor P 1  is zero, the gate-source voltage of the radiation-sensing transistor P 1  is slightly beyond its non-irradiated threshold voltage value. Therefore, even when the radiation-measuring circuit is not exposed to radiation, the radiation-sensing transistor P 1  is enabled.  
         [0011]    Additionally, when the circuit is not exposed to radiation, the current I sens  is magnified by the current mirror (transistors P 2  and P 3 ). The circuit is designed so that the voltage (V a ) is above the threshold voltage of transistor P 1  (V tP1 ). That voltage, which appears at the gate terminal of the output load transistor N 2 , is not large enough to sufficiently turn on the output load transistor. In summary, when the CMOS radiation-measuring circuit is not exposed to radiation, the second side of the current mirror (transistor P 3 ) is on, the output load transistor N 2  is almost turned off, and the current that flows through the second side of the current mirror is much larger than I sens . The value of the output voltage (V out ) is pulled to the supply voltage V dd  through the transistor P 3 . In that mode of operation, the output voltage (V out ) represents a high digital state.  
         [0012]    However, when the circuit is irradiated, the absolute value of the threshold voltage for the radiation-sensing transistor P 1  increases, as described above. Once the threshold voltage increases above the value of the voltage (V a ), the radiation-sensing transistor P 1  turns off. As can be seen from the approximation for I sens  in the above equation, when P 1  is turned off, the current (I sens ) through the first side of the current mirror (transistor P 2 ) will drop to zero. As a result, the current that flows into the output load transistor N 2  also decreases. At this point, the voltage (V a ) is only slightly less than the supply voltage V dd  as a result of the voltage drop across the resistive element N 1  and the transistor P 2 . This voltage (V a ), which also appears at the gate terminal of the output load transistor N 2 , causes the output load transistor N 2  to turn on. The output voltage (V out ) of the CMOS radiation-measuring circuit is, thus, coupled to ground through the output load transistor N 2 . In that mode of operation, the output voltage (V out ) represents a digital low state. Therefore, the radiation-measuring circuit provides a digital output.  
         [0013]    To allow the radiation-measuring circuit to sense different radiation doses, the threshold voltage of the radiation-sensing transistor P 1  can be modified by changing the body bias of the transistor through the input voltage (V in ). The body bias is the voltage between the body terminal and the source terminal of the transistor V bs . The voltage used to adjust the body bias may be applied, for example, from an external source that allows a user to adjust the value of V in  when the CMOS radiation-measuring circuit is exposed to radiation. Alternatively, the voltage used to adjust the body bias may be an integrated voltage source based on bandgap or charge pump circuits that a user may adjust using software.  
         [0014]    As discussed earlier, changing the threshold voltage of the radiation-sensing transistor P 1  changes the dose required to turn off that transistor. Therefore, the dose required to change the output of the CMOS radiation-measuring circuit from one digital state to another can be altered by changing the body bias of the radiation-sensing transistor P 1 . A single radiation-measuring circuit can, therefore, be used to measure different dose values that the circuit may be exposed to.  
         [0015]    The auxiliary circuit to which the radiation-sensing transistor P 1  is coupled preferably is composed of components that, as a whole, are insensitive to threshold voltage shift due to radiation exposure. Preferably, pMOS transistors are used in the current mirror because this configuration tends to be less sensitive to threshold voltage shifts provided the threshold voltages of each pMOS transistor shift by the same amount. Resistive element N 1  and the output load transistor N 2  preferably are nMOS transistors because the absolute value of the threshold voltage shift in an nMOS transistor remains substantially unchanged. More specifically, the charge trapped in the oxide is positive for both nMOS and pMOS devices, whereas the interface state charge is positive for a pMOS and negative for an nMOS. Because these charge components have the same sign in a pMOS device, the threshold voltage of the pMOS device is shifted toward a more negative value. In contrast, because these charge components have opposite signs in an nMOS device, they induce a competing effect in threshold voltage shift and the resulting sign of the threshold voltage shift in an nMOS device depends on which charge component&#39;s contribution is dominant. Therefore, the absolute value of the threshold voltage shift is usually much higher in pMOS transistors than nMOS transistors.  
         [0016]    An advantage of the foregoing techniques is the radiation dose that may be measured by the radiation-measuring circuit  1  need not be fixed. Therefore, CMOS radiation-measuring circuits need not incorporate several radiation-measuring circuits to measure different radiation doses. Also, the auxiliary circuit, used in the radiation-measuring circuit can be relatively impervious to radiation-induced changes.  
         [0017]    Various modifications may be made. For example, the radiation-measuring circuit can include an nMOS current mirror, an nMOS radiation-sensing transistor, a pMOS resistive element coupled to the radiation-sensing transistor and a pMOS output load. Other implementations are within the scope of the following claims.