A statistical temperature sensor

M. Hofer, C. Boehm
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引用次数: 1

Abstract

The physical effect which is used in this type of temperature sensor is the temperature coefficient mismatch of transistors. The basic cell for evaluating the effect is a bi-stable cell. For instance this could be an SRAM cell. After powering up the circuit such a cell provides either a 1 or a 0 at its output. In the case that such a bi-stable cell is used as a temperature-sensor, a well-designed cell bases its decision on the mismatch of two NMOS transistors (N1 and N2). The threshold voltage of NMOS transistors is decreasing over temperature. The amount of change is mainly defined by the coefficient KT1 (see BSIM). It turns out that there is a mismatch on KT1 between the different transistors. Thus it may happen that the startup value (or initial value) may change over the temperature. If a huge number of cells is used an accurate value of the temperature can be given. Once a startup vector at a well-defined temperature is defined, the temperature difference can be derived by measuring the Hamming distance (HD) between the reference vector and the output at the actual temperature.
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一种统计温度传感器制造技术
这种类型的温度传感器所使用的物理效应是晶体管的温度系数失配。评价效果的基本单元是双稳态单元。例如,这可能是一个SRAM单元。在给电路通电后,这种电池在其输出端提供1或0。在这种双稳态电池用作温度传感器的情况下,设计良好的电池基于两个NMOS晶体管(N1和N2)的不匹配来做出决定。NMOS晶体管的阈值电压随温度的升高而降低。变化量主要由系数KT1定义(见BSIM)。结果是不同晶体管之间的KT1不匹配。因此,启动值(或初始值)可能会随着温度的变化而变化。如果使用大量的电池,可以给出一个精确的温度值。一旦定义了一个明确温度下的启动矢量,就可以通过测量参考矢量与实际温度下输出之间的汉明距离(HD)来推导温差。
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