Elsevier

Microelectronics Journal

Volume 46, Issue 9, September 2015, Pages 819-824
Microelectronics Journal

Wide-range CTAT and PTAT sensors with second-order calibration for on-chip thermal monitoring

https://doi.org/10.1016/j.mejo.2015.06.004Get rights and content

Abstract

This paper presents wide-range complementary to absolute temperature (CTAT) and proportional to absolute temperature (PTAT) sensors with second-order calibration for on-chip thermal monitoring. Particularly, a current mirror and an n-well resistor are used in these sensors to eliminate the second-order term of the temperature coefficient to linearize the transfer function between the output voltage and the temperature. The proposed CTAT and PTAT sensors are implemented on silicon using a typical 0.18 μm CMOS process. The core area of the CTAT and PTAT sensors is 0.0125 mm2 and 0.0074 mm2, respectively. In the range from 55°C to 155°C, the worst deviation of the CTAT and PTAT temperature sensors is measured to be 3.75°Cto+3.34°C and 3.73°Cto+3.85°C, respectively. The maximum non-linearity reduction of the CTAT and PTAT sensors is 59.84% and 87.48%, respectively, by the proposed second-order calibration. Notably, the overhead area of the CTAT and PTAT sensors is only 0.64% and 1.08%, respectively.

Introduction

It is well known that more transistors have been integrated in a chip by using advanced CMOS technologies. When many transistors are integrated and realized on a single die, the power density as well as the temperature will rise inevitably. Moreover, the chip with high switching activities will generate massive heat (namely hot spot) [1]. Another critical issue is the range of the temperature. The harshest temperature range is demanded by electrical vehicles (EV) and military equipments, which are 40°C to 125°C and 55°C to 125°C, respectively [2], [3], [4]. Temperature sensors are then required to monitor the temperature of those chips in these applications in such a wide temperature range to ensure that no hazards would be caused by over heat problems.

Many prior temperature sensors relied on threshold voltage detection to estimate the temperature [5], [6], [7], [8]. The accuracy in a very wide range is still a challenge regarding on-chip temperature sensing. Vaz et al. proposed a temperature sensor for human body temperature monitoring, where a large resistor is used to cancel temperature non-linearity components of the saturation current [7]. However, this design was meant for low temperature range. Several logic-based design temperature sensors have also been proposed [1], [9]. Chung and Yang proposed an all-digital temperature sensor, where serious process and non-linear effects still exist [1]. The reason is that the process variation and second-order effects of MOSs in all digital circuits are hard to be detected and then calibrated. A few time-domain temperature sensors were also reported [10], [11], [12], [13]. Chen et al. proposed a time-domain temperature sensor based on a successive approximation algorithm [10]. The successive approximation algorithm, however, costs a large area overhead. Meanwhile, the high linearity and second-order effects calibration methods were reported [14], [15], [16], [17], [18]. Lin et al. proposed a non-linear calibration method by isolating body effect. This design, however, did not consider the process variation [14]. Jeong and Ayazi disclosed a process offset cancellation method by applying an identical circuit to realize temperature sensors [17]. The reported process compensation and second-order effects calibrated methods usually need a large area to realize compensation and calibration circuits [10], [11], [12], [13], [14], [15], [16], [17], [18]. Many low-cost calibration methods were also proposed [19], [20], [21]. Fisk and Hasan showed a method using the correlation between pinch-based resistance and substrate bipolar temperature gradient to carry out process-compensation [20]. Besides, Souri et al. also proposed high accuracy and low-power temperature sensors [22], [23], where silicon on insulator (SOI) process was used to attain a much wider temperature range and low power consumption [22]. Another prior design used dynamic threshold MOSTs (DTMOSTs) and an inverter-based second-order zoom analog-to-digital converter (ADC) to achieve high accuracy and low power [23]. However, the SOI process, DTMOSTs, and the other prior calibration technologies must pay high die area and cost [14], [15], [16], [17], [18], [19], [20], [21], [22], [23], [24], [25], [26].

In this study, we propose complementary to absolute temperature (CTAT) and proportional to absolute temperature (PTAT) sensors with low-cost second-order calibration to resolve all the mentioned problems. By using the proposed second-order calibrated CTAT and PTAT sensors consisting of a current mirror and an n-well resistor, the linearity can be enhanced.

Section snippets

Wide-range temperature sensor

Fig. 1(a) shows the schematic of the non-calibrated temperature sensor composed of 2 PMOSs and 2 NMOSs [15]. The non-calibrated temperature sensor will attain a positive or negative T-to-V (temperature-to-voltage) transfer curve by adjusting length and width of MOSs. Since this method is based on threshold voltage detection, the linearity of temperature sensors is affected by threshold voltage and mobility variations. Particularly, a significant second-order effect has been well known to exist

Implementation and measurement results

In this work, the proposed CTAT and PTAT sensors are implemented using a typical 0.18 μm CMOS process. Fig. 4(a) and (b) shows the non-calibration and calibration simulation results of the proposed CTAT sensor, respectively, while Fig. 4(c) and (d) is those of the proposed PTAT sensor. Table 2 compares the non-calibrated and calibrated simulation results, where the maximum non-linearity reduction of the CTAT and PTAT sensors are 59.84% and 87.48%, respectively. Fig. 5 shows the die photo, where

Conclusion

The proposed CTAT and PTAT sensors are calibrated by using a current mirror and an n-well resistor to eliminate the second-order term of the temperature coefficient. Thus, the proposed CTAT and PTAT sensors can be used in a wide temperature range (−55°Cto155°C). The overhead area of the proposed CTAT and PTAT sensors, however, is only 0.64% and 1.08%, respectively. Besides, the same circuit architecture is used to carry out the CTAT and PTAT sensors to attain positive or negative temperature

Acknowledgements

This investigation was partially supported by National Science Council, Taiwan, under Grants NSC102-2221-E-110-081-MY3 and NSC102-3113-P-110-010. The authors would like to express their deepest gratefulness to CIC (Chip Implementation Center) of NARL (Nation Applied Research Laboratories), Taiwan, for their thoughtful chip fabrication service.

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