Change of delay time is measured: material constant is temperature coefficient of delay (TCD) |
Frequency shift is measured: material constant is temperature coefficient of frequency (TCF = −TCD) |
Wide band device: sharp peaks in time-domain |
High Q-factor needed for sharp peaks in frequency-domain -> narrow resonance. |
Differential measurement is easy due to multi peak design |
Differential measurement requires multiple resonators |
Wide band operations allow for wide temperature shift |
Too wide temperature shifts might shift the sensor’s resonance frequency out of the dedicated ISM-band |
Devices are relatively long ~>4–6 mm, measurement corresponds to mean value over delay path ~2 mm |
Resonators can be small and allow point-like measurements |
Sophisticated phase tracking required |
High resolution frequency reading needed |