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<table>Dynamical response (resistance versus time) of S1 after changing the vacuum into air flux  <svg height="15.0875" id="M22" style="vertical-align:-2.3205pt" version="1.1" viewbox="0 0 45.262501 15.0875" width="45.262501" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg> and back into vacuum.  (a) <svg height="11.825" id="M23" style="vertical-align:-0.1638pt" version="1.1" viewbox="0 0 55.349998 11.825" width="55.349998" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg>°C. (b) <svg height="11.825" id="M24" style="vertical-align:-0.1638pt" version="1.1" viewbox="0 0 55.349998 11.825" width="55.349998" xmlns="http://www.w3.org/2000/svg" xmlns:xlink="http://www.w3.org/1999/xlink">
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</svg>°C.</table>

Journal of Sensors

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Figure 3

Figure 3: Field-Assisted and Thermionic Contributions to Conductance in <svg style="vertical-align:-4.50008pt;width:48.450001px;" id="M1" height="20.887501" version="1.1" viewBox="0 0 48.450001 20.887501" width="48.450001"  xmlns="http://www.w3.org/2000/svg">
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Figure 3 | Field-Assisted and Thermionic Contributions to Conductance in 
	
		
			
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Journal of Sensors

Field-Assisted and Thermionic Contributions to Conductance in S n O 𝟐 Thick-Films

Figure 3

Field-Assisted and Thermionic Contributions to Conductance in Thick-Films