Ultrasensitive electrolyte-assisted temperature sensor


Heat sensors form an important class of devices that are used across multiple fields and sectors. For applications such as electronic skin and health monitoring, it is particularly advantageous if the output electronic signals are not only high, stable, and reproducible, but also self-generated to minimize power consumption. Here, we present an ultrasensitive heat sensing concept that fulfills these criteria while also being compatible with scalable low-cost manufacturing on flexible substrates. The concept resembles a traditional thermocouple, but with separated electrodes bridged by a gel-like electrolyte and with orders of magnitudes higher signals (around 11 mV K−1). The sensor pixels provide stable and reproducible signals upon heating, which, for example, could be used for heat mapping. Further modification to plasmonic nanohole metasurface electrodes made the sensors capable of also detecting light-induced heating. Finally, we present devices on flexible substrates and show that they can be used to detect human touch.


The ability to detect heat and temperature is essential in nature, and has aided animals, plants, and microorganisms to find their optimal conditions to grow and avoid damaging extremes1,2. For humans, our skin allows detection of local temperature changes induced both by contact with warm objects and via exposure to light radiation3,4. Heat sensing thereby forms an essential part of the skin’s integrated network of sensors, which aid our interaction with the outside world by enabling detection of external stimuli4. Motivated by applications such as humanoid robotics, prosthetics, and wearable electronics, recent research has devoted significant efforts to develop electronic skin (e-skin) that can mimic the functionalities of human skin5,6,7,8,9. For such e-skin, augmentation with heat sensing is one of the critical requirements10,11,12,13. Previous research has explored different heat sensing principles for e-skin, including heat-induced resistance changes of conducting materials14, variations in source–drain current of transistors15, and frequency-changes in piezoelectric devices16. Achieving high sensitivity for such sensors often involves microfabrication or patterning that are rather complicated and expensive in terms of large-scale production of low-cost sensors14. Furthermore, the above examples require an external electrical current to be applied through the devices in order to generate the sensor signal, which means consumption of energy14. Interestingly, human skin itself is a low-energy consuming sensory system8, which can inspire the design of self-powered sensors that generate output signals without external power17,18.

Pyroelectric systems are known to self-generate electrical signals during changes in temperature. A change in temperature affects the self-polarization over the pyroelectric material, leading to electrical currents to compensate for those changes19,20,21. However, pyroelectric signals are transient and quickly decay to zero after a change in temperature has taken place, which is not suitable for long-term temperature monitoring22,23,24,25. By contrast, recently developed ionic thermoelectric sensors26 can provide self-generated open-circuit voltages that are stable over time. A drawback is that ionic thermoelectric voltages do not correspond only to the temperature of a single target sensor spot, but they are induced by a temperature gradient between two different positions27. No signal is obtained upon uniform heating of the whole material or device. The requirement of a difference in temperature over the material poses challenges in terms of monitoring absolute temperatures of single spots, in particular for small dimensions and thicknesses where the whole material is heated. So far, the most commonly used self-powered temperature sensor is the thermocouple (TC), which provides thermovoltages based on the difference in Seebeck coefficients of two electronic conductors forming a junction28. However, the sensitivity of TCs is limited to tens of microvolts per kelvin due to low electronic Seebeck coefficients29. Sensors that provide higher signals for the same heat stimulus could not only improve resolution, but also open up for concepts that benefit from large absolute changes in voltage, such as heat-gated transistors30.

Here, we present a concept for self-powered heat sensing that resembles a traditional TC, but with orders of magnitude higher sensitivity. The so-called electrolyte-assisted temperature sensor (EATS) does not require any spatial temperature differences and can therefore be thin. EATS provides large and stable signals (not only transient signals) that are proportional to changes in temperature (from 14 to 55 °C). The large signals make EATS suitable for detection of small temperature changes (0.1 °C), with response better than commercial TCs. The sensor signals are reproducible and the devices are stable over long periods (at least 6 months). The concept has a simple structure composed of two different metals connected by a printable gel-like electrolyte, and is suitable to be applied on various rigid or flexible substrates by low-cost manufacturing methods. Furthermore, we present a modified type of EATS for detection of light-induced heating. For these modified devices, the metal electrodes are perforated with nanoholes, which make them interact strongly with light by conversion of incident light to plasmons (collective charge oscillations in the metal). A significant fraction of the plasmons decay via absorption and local heat generation31,32, which increases the temperature and induces signals in the sensor. The principle of using thermoplasmonic nanohole films to convert light to electrical signals follows our previous work on radiation-induced heat sensing33,34,35. Finally, we evaluate the EATS concept for heat mapping using sensor pixel arrays, and demonstrate its capability to detect human touch.

Results and discussion

Demonstration of the concept and comparison with traditional TCs

Figure 1 demonstrates the concept of the EATS, based on two separated gold (Au) and aluminum (Al) electrodes connected via an electrolyte (see the rightmost sketch in Fig. 1a). We chose a gel electrolyte based on an ionic liquid (1-ethyl-3-methylimidazolium ethylsulfate, [EMIM][ESO4] mixed with 2-hydroxyethyl cellulose (HEC, see Fig. 1b) as the gelling agent. This electrolyte is compatible with screen printing for roll-to-roll device manufacturing and also maintains constant concentration under long-term heating due to its low vapor pressure in the studied temperature range36,37,38.

Fig. 1: Demonstration of the EATS and comparison with traditional TCs.

a Schematic illustration of an Al/Au junction (left) and the EATS device (right). The Al/Au junction device consists of 20 nm-thick aluminum and gold layers overlapping in a 12 mm2 area. For the EATS device, the Au and Al electrodes are separated and bridged by an electrolyte (shaded region, with areas overlapping with the electrodes of 12 mm2). b Schematic illustration of the gel-like electrolyte used in EATS a and the chemical structures of the compositions in the gel. c Variations in open-circuit voltage of an Al/Au junction (bottom panel) upon controlled temperature changes (top panel). d Variation in open-circuit voltage of an EATS (bottom panel) upon controlled temperature changes (top panel). e Change in open-circuit voltage versus temperature for six EATS devices and comparison with the Al/Au junction (black squares) and a commercial TC (red triangles). Different green symbol shapes indicate the results from different samples, and the error is the standard deviation from these six samples. The results were obtained in a cleanroom with relative humidity (RH) of 30%.

As shown in Fig. 1d, varying the temperature (T, top panel) of the EATS led to large changes in the open-circuit potential between the two electrodes (ΔV, bottom panel). These results were reproducible between devices, as clear from Fig. 1e which presents ΔV as a function of T for six different EATS devices. Linear fitting gives an average temperature sensitivity (dV/dT) of 11.5 mV K−1 with standard deviation of 0.5 mV K−1. Likewise, the same EATS device responding to (24) multiple cycles of fixed temperature stimuli showed repeatability of the signals (Supplementary Fig. 1).

As comparison, we prepared simplified TC devices without electrolyte for which the Al and Au electrodes were connected (Al/Au junction) (see the leftmost sketch in Fig. 1a). Such a device provided only small changes in open-circuit voltage upon temperature changes (Fig. 1c), with almost four orders of magnitude lower sensitivity (Fig. 1e). Compared to the commonly used commercial K-type TC (based on NiCr–Ni) with temperature sensitivity of 0.04 mV K−1 (Fig. 1e), the EATS has 275 times higher sensitivity. Monitoring the temperature at equilibrium (without temperature steps) shows that the proof-of-concept EATS sensor provides 4–5 times lower fluctuations than the optimized commercial TC (see Supplementary Fig. 2). The response time for the commercial TC (to reach stable values) varied between 90 and 150 s depending on the magnitude of the temperature change. For the EATS, the response time (to reach the peak value) was around 150–220 s, which we expect can be improved through further optimization of the concept.

Investigation of the heat sensing mechanism

In discussing the mechanism of the sensor concept, we note that the surface potential of metal electrodes can vary with temperature via variations in the electric double-layer at the metal–electrolyte interface, which has been proposed for thermally chargeable supercapacitors39. Aiming to understand the temperature-dependent potentials of the metals involved in our device, we measured changes in the open-circuit voltage for symmetric devices with two electrodes made of the same metals upon changes in temperature in the range from 22 to 38 °C (∆T = 0–16 K). The two identical electrodes were separated by a large distance (circa 5 cm) and connected by an electrolyte bridge such that one electrode could be heated while the other was kept at room temperature. The results show that the surface potential of both Au and Al becomes more negative with increasing temperature (see Fig. 2a), which agrees with previous research40. In the studied temperature range (22–38 °C), the temperature-dependence of the surface potential is similar for the two metals, with values of −3.4 mV K−1 for the Au electrode and −4.7 mV K−1 for the Al electrode. While previous research reported stronger temperature dependence for metals with larger work function (in aqueous solution), that was for a larger temperature range showing clear nonlinear behavior, and less variation between the different metals was reported in the lower temperature range similar to that investigated here40. We also note that there is no large temperature dependence of the capacitance of the Au or Al electrodes, with the Au having around twice capacitance/area (see Supplementary Fig. 4b). The fact that we do not see significant differences between the two metals in terms of change in potential with temperature indicates that alternative effects are responsible for the large signals of the asymmetric EATS.

Fig. 2: Investigation of sensor mechanism by heating only one of the electrodes (heating is depicted by the orange shading).

a Change in surface potential upon heating one of the electrodes for symmetric devices composed of two gold electrodes (yellow symbol shapes, results for four devices) or two aluminum electrodes (gray symbol shapes, results for three devices). b Same as in a but for an asymmetric device upon heating either the gold electrode (yellow) or the aluminum electrode (gray). c Controlled temperature changes applied to an EATS with a different electrolyte based on 3% NaSCN in PEG (inset). d Open-circuit potential variations of the same device upon the heat cycles presented in c. All measurements were performed in a cleanroom at RH = 30%.

In that respect, we note that the EATS resembles a galvanic cell41, although without any redox couples added to the electrolyte. In order to investigate if the sensor signals of such non-ideal galvanic system depend on the electrolyte, we repeated the measurement using the same type of EATS device, but using a very different type of electrolyte (see the inset in Fig. 2c). This electrolyte was composed of sodium thiocyanate (NaSCN) in polyethylene glycol (PEG, Mw = 300), which is also stable during heating. Interestingly, we observed remarkably similar results when using the NaSCN:PEG electrolyte as when using the ionic liquid-based electrolyte, both in terms of sensitivity and time response (Fig. 2d). One thing that both electrolytes have in common is the presence of water and oxygen at small concentrations adsorbed from the atmosphere42,43, which could be related to the generated sensor signals. Regarding possible galvanic contribution to the signals, we note that EATS devices were stable for at least half a year (see Supplementary Figs. 5 and 11) and, hence, are not based on rapid consumption of the Al due to oxidation. Such long-term stability is advantageous for the concept to be used in practical applications.

The devices could also recover their open-circuit voltage after being electrically shorted for extended periods of time. In most galvanic cells, such action would quickly deplete the device and reduce the voltage to zero44. Another possibility is that the device functions as a hybrid supercapacitor45, with the Al electrode being most susceptible to electrochemical reactions while the Au acts more as a blocking electrode. Indeed, equivalent circuit analysis (see Supplementary Fig. 6) of impedance spectroscopy data for an EATS shows that the Al electrode provides a three orders of magnitude lower charge transfer resistance compared with the Au electrode in the studied temperature range (see Supplementary Table 1). Also, the Au electrode is almost purely capacitive while the Al electrode has a significant contribution from resistive processes (see details in Supplementary Note 2). To further elucidate this possible function of the EATS, we made asymmetric Au–Al devices (with similar electrode areas as for EATS) that were compatible with heating of only one of the electrodes at a time (see schematics in Fig. 2b). As shown in Fig. 2b, heating the Au electrode only resulted in modest changes in the open-circuit potential (−2.7 mV K−1). By contrast, heating the Al electrode induced large signals, with a sensitivity of −11.3 mV K−1. This value is very similar to the response upon heating both electrodes of the full devices. Hence, these results confirm that the sensor signal is related to variation in temperature of the redox-active Al electrode in combination with being connected via the electrolyte to the more inert Au electrode.

Heat mapping by pixel arrays and plasmonic metasurfaces

Motivated by good performance in terms of sensitivity, reproducibility, and stability, we investigate the EATS for heat mapping. Heat mapping could find use in many applications, including for e-skin7,12,46, and we here demonstrate the concept for rectangular arrays with four sensor pixels.

We created a temperature gradient over the whole device by heating from one side while keeping the other side fixed at room temperature (22 °C, illustrated in Fig. 3a). The different pixels show different signal responses (Fig. 3b) and could accurately capture the respective local temperature variations as verified by commercial TCs close to (but not on) the pixels (Fig. 3c). We modified the device structure by replacing the flat metal film electrodes with the same type of electrodes but perforated with nanoholes. Using colloidal lithography47, we made sensor devices with 20 nm thick Al and Au nanohole electrodes, with 107 nm in diameter holes (see scanning electron microscopy (SEM) images in Fig. 3e). Such metal nanohole films strongly interact with and absorb light via excitation of plasmons (see absorption spectra in Supplementary Fig. 7)48, while their continuous metal structure still allows them to be used as electrodes33,49,50. The strong light absorption results in local heat generation, which makes the sensor pixels sensitive to light stimuli33,35,51. We used this light-sensitivity to individually stimulate different pixels by light, as an alternative methodology to heat mapping to evaluate the concept. We made 2 by 2 pixel arrays of plasmonic EATS (see Fig. 3d) and measured the response of one pixel (pixel 1) while varying which pixel that was illuminated (by a solar simulator, see Fig. 3f). As expected, the sensor signal was largest when illuminating the measured pixel (pixel 1) and decreased with distance between the measured and illuminated plasmonic pixels. This reflects the temperature distribution over the sample upon illumination at different positions. We also note that the sensor responded more rapidly for the illuminated pixel, which may be due to more rapid increase in temperature of the illuminated metasurface pixel compared to nearby areas.

Fig. 3: Heat mapping using arrays of EATS and metasurface-based pixel arrays.

a Schematic illustration of the sensor device and setup for non-uniform heating of the sample using two Peltier elements. The effective size of each Al/Au pixel is 24 mm2. b Voltage variations of the different pixels (V1–V4), at RH = 30%. c Temperature evolution of the pixels in b monitored by traditional TC placed close to the pixels (T1–T4). d Photograph of a 2 by 2 array of metasurface-modified pixels. e SEM images of a gold metasurface nanohole electrode (left) and an aluminum metasurface nanohole electrode (right). The scale bars represent 200 nm. f Sensor response for pixel 1 upon illumination of the different plasmonic EATS by a solar simulator (at room humidity without control).

Mitigating humidity effects and application as e-skin

For many applications, including e-skin, it is important to be able to decouple signals induced by different types of stimuli, such as changes in temperature and humidity. Measurements for heat cycles at different relative humidity (Fig. 4a) show that the sensitivity of the EATS remained high at both high (RH = 30%, green) and low (RH = 4%, blue) relative humidity, with higher temperature response at low humidity. The sensor kinetics varied with humidity. At higher relative humidity, changes in temperature induced clear transient peaks (increase in T) and dips (decrease in T) before saturation at somewhat lower signals. This behavior was less pronounced at low relative humidity. Furthermore, changes in relative humidity also caused significant changes in the open-circuit voltage when maintaining the device at a fixed temperature (dashed line in Fig. 4b). To further understand these effects, we performed impedance spectroscopy of an EATS at high and low relative humidities. Supplementary Fig. 8 presents the experimental results, which clearly show large variations in the electrical properties at different relative humidities. In particular, we found a large increase in the total resistance of the sensor when decreasing the relative humidity, indicating that an increase in the electrolyte bulk resistance and/or charge transfer resistance by lowering the relative humidity induces changes in the open-circuit potential of the sensor.

Fig. 4: Humidity response of EATS and mitigating the effect by encapsulation.

a Temporal changes in open-circuit voltage of an EATS on a glass substrate during heat cycles (from 22 to 26 °C, 30, 34, and 38 °C, respectively) at high humidity (green) and low humidity (blue). b Variation in open-circuit potential upon changes in humidity (alternating between RH = 30% and RH = 4%) at 22 °C, for an open EATS (dashed line) and for an encapsulated EATS (solid line). c Changes in open-circuit voltage versus temperature at high (green) and low (blue) humidity for open (unfilled markers and dashed lines) and encapsulated EATS (filled markers and solid lines). Each data point (error bar) represents the average value (standard deviation) from three series of measurements. The inset shows a photograph of an encapsulated EATS device. d Change in open-circuit voltage generated by an encapsulated EATS (green) and a commercial TC (red) upon touch by a human hand (yellow shaded areas).

To decouple the signals induced by heat from those induced by relative humidity changes, we prepared a new type of encapsulated EATS. The metal electrodes were deposited on flexible polyethylene terephthalate (PET) foil, and after applying the electrolyte the whole device structure was encapsulated between two barrier films. As shown in Fig. 4b, the dependence of the open-circuit voltage to changes in relative humidity could be efficiently mitigated by encapsulation (solid line), showing no observable variations when alternating between relative humidity of 30% and 4%.

Importantly, the encapsulated EATS devices provided high temperature response independent of relative humidity level, with sensitivity measured to 13.5 mV K−1 at high relative humidity (RH = 30%, green filled markers in Fig. 4c) and 13.4 mV K−1 at low humidity (RH = 4%, blue filled markers). The open markers and dashed lines in Fig. 4c correspond to three measurements from two open EATS devices (without encapsulation). These open EATS devices exhibited different sensitivity at different humidity (11.5 mV K−1 at RH = 30% and 13.8 mV K−1 at RH = 4%), while the encapsulated devices successfully eliminated the relative humidity dependence. In addition, the flexible encapsulated EATS also provided reproducible signals before and after repeated bending of the device (bent over a cylinder with diameter of 40 mm, see details in Supplementary Note 7). Notably, some of these results were obtained 6 months after device preparation, demonstrating good long-term stability and mechanical properties of the encapsulated EATS devices.

Finally, we put our concept to practical test by evaluating its capability of detecting human touch, which forms one of the essential features when used in e-skin applications. Temperature changes from touch can be small, and we first investigated the response of EATS to small temperature changes and compared the results with those of a commercial TC. As shown in Supplementary Fig. 10, EATS could provide clear signals with high signal-to-noise ratios for small changes in temperature (0.1 °C), while the traditional TC was more limited and showed lower signal-to-noise ratios. Figure 4d presents the variation in open-circuit voltage upon touch by a human hand (yellow shaded areas), both for an encapsulated EATS (green) and for a commercial TC (red). The commercial TC could only produce small signals on the order of 0.2 mV, while the EATS provided sensor signals of several millivolts, despite having more material to heat up. In terms of temperature range, the encapsulated EATS maintained its linear response also in a larger range from 14 to 55 °C (Supplementary Fig. 11), making it suitable for many applications such as health-monitoring systems, and monitoring the temperature in packaging within this range.

In summary, we have reported a concept for ultrasensitive temperature sensing. The sensor signals are self-generated in analogy with traditional TCs, but with almost 300 times higher sensitivity. We show that the concept is applicable for heat mapping and that it can be made light-sensitive by modifying the sensor with light-absorbing plasmonic metasurfaces. While the sensor could also react to changes in humidity, we show that this feature can be eliminated by encapsulation when desired. The sensors were stable for at least several months and show good reproducibility between samples. Combined, the features and performance of the sensor make it suitable for use in applications such as e-skin, where the simplistic structure can be particularly useful for low-cost manufacturing at large scale.


Fabrication of TC and (plasmonic/bendable) EATS

Glass wafers and 0.25 mm-thick PET sheets were used as substrates for different devices. Glass wafers were rubbed in soap water and then ultrasonicated in soap water once and two times in deionized (DI) water for 5 min each. They were rinsed with acetone and isopropanol and dried with N2 stream. To remove organic contamination the glass substrates were surface-treated by UV-ozone for 15 min. PET sheets were rinsed with DI water, acetone, and isopropanol and after drying with a N2 stream they were baked for 30 min at 130 °C in an oven. Shadow mask evaporation was used to evaporate 20 nm Al and 20 nm Au electrodes on the clean glass and PET substrates. For plasmonic EATS, we used colloidal lithography described elsewhere52 to fabricate Al and Au metasurface electrodes with thickness of 20 nm and nanohole dimeter of 107 nm. To prepare the ionic liquid electrolyte for (plasmonic) EATS, 1-ethyl-3-methylimidazolium ethyl sulfate ([EMIM][ESO4]) was mixed with HEC (7.5 wt%) while heated to 100 °C on a hotplate until forming a gel. Both chemicals were purchased from Sigma Aldrich. The electrolyte was then applied via a brush onto the electrodes, with thicknesses on the order of 300 µm (measured for three samples by analyzing images taken using an optical contact angle and surface tension meter [KSV Instruments, CAM 200]).

NaSCN in PEG (Mw = 300) was another electrolyte that we used to compare the function of the device with that of the [EMIM][ESO4] electrolyte. NaSCN was purchased from Sigma-Aldrich and mixed with PEG with 3 wt%. It was applied on the devices in similar way as the[EMIM][ESO4] electrolyte.

Encapsulated devices were used to minimize the humidity dependence. The encapsulation was obtained by first attaching an adhesive barrier film to the back side of the device substrate. Al and Au electrodes were then deposited on PET substrate using shadow-mask thermal evaporation, with an electrode area of 5 × 7 mm2. An adhesive plastic sheet was cut into the shape of a frame and attached on top of the device substrate, with the opening of the frame aligned to the Al and Au electrodes. The cavity inside the frame was filled with the ionic liquid electrolyte and the encapsulated device structure was completed by attaching another layer of the adhesive barrier film on top of the areas covered by electrodes and electrolyte on the front side of the device substrate. The adhesive polymer-based barrier film used for the encapsulation, HydroBlock AG2500, was purchased from Honeywell.

Microstructure and optical characterization

SEM (Zeiss, Sigma 500 Gemini) was used to study the distribution and quality of the Au and Al nanoholes. Absorption spectra of (plasmonic) EATS were evaluated using a custom-built setup consisting of a white light source (300 W, Xe lamp, Newport), an integrating sphere (Labsphere), and an optical light guide connected to a spectrograph (Andor Shamrock 303i, Newton CCD detector).

Impedance characterization

The impedance measurements were carried out using an impedance spectrometer (Alpha high-resolution dielectric analyzer, Novocontrol Technologies GmbH, Hundsangen, Germany). An AC voltage of 100 mV was applied while sweeping the frequency from 1 × 106 to 1 × 10−1 Hz.

Heat and radiation sensing evaluation

Direct heat sensing measurements were performed by controlled heating of the samples from the bottom side via a Labview-controlled Peltier element (22–40 °C) and simultaneously monitoring the temperature on top of the devices using a TC. The open-circuit voltage generated by the devices was measured using a Keithley 2182A nanovoltmeter set to autorange. The Au electrodes were always connected to the positive measurement terminal of the nanovoltmeter if not stated otherwise. The temperature cycles were applied through a Labview program. Open-circuit voltage measurements throughout this work were performed in a cleanroom with relative humidity of 30% unless otherwise stated. To study the effect of humidity on the response of the devices, the humidity of the measurement chamber was reduced to ~4% by constant purging of N2. Monitoring of the radiation-induced heating was carried out using a solar simulator (LCS-100, Oriel Instruments, 300 W Xe lamp, AM1.5Gfilter) calibrated to an irradiance of 1 Sun (1000 W m−2) and a custom-designed aperture to only illuminate only one pixel at time. Using an optical beam shutter (SH, Thorlabs), light on and off states were controlled. Via a Labview-controlled Keithley 2182A nanovoltmeter, the open-circuit voltage generated by the devices was measured.

Evaluating effects on bending

The sensor response of an encapsulated EATS was acquired before and after repeated bending of the device around a rod with diameter of 40 mm. For each bending cycle, the device was bent and unbent 10 times before being placed on the Peltier element to measure the open-circuit potential upon temperature cycles. This whole bending and measurement procedure was repeated on three consecutive days.

Data availability

The data that support the findings of this study are available from the corresponding authors upon reasonable request.


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The authors gratefully acknowledge financial support from the Swedish Foundation for Strategic Research, the Swedish Research Council, the Wenner-Gren Foundations, Essity, the Swedish Government Strategic Research Area in Materials Science on Functional Materials at Linköping University (Faculty Grant SFO-Mat-LiU No. 2009 00971) and the Vinnova Digital Cellulose Competence Center (DCC), Diary number 2016-05193. The work was also supported by Treesearch.se. Open access funding provided by Linköping University.

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M.P.J. and D.Z. conceived the project and supervised the research. M.S.C. performed the device fabrication and took part in measurements and data analysis. P.A.E. and M.S.C. performed sample preparations on flexible substrates and encapsulation of the devices. D.Z. and M.S.C. performed experiments on the humidity and temperature sensing properties of the devices. J.E. conducted the impedance spectroscopy measurements and corresponding data analysis. M.S.C. wrote the paper with contributions from all authors.

Corresponding authors

Correspondence to Dan Zhao or Magnus P. Jonsson.

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Shiran Chaharsoughi, M., Edberg, J., Andersson Ersman, P. et al. Ultrasensitive electrolyte-assisted temperature sensor. npj Flex Electron 4, 23 (2020). https://doi.org/10.1038/s41528-020-00086-5

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