Silicon-based partially gated tunnel FETs are characterized under optical and electrical excitation. Most significant outcomes of the experiments are (1) unique characteristics, namely, light induced negative transconductance and optically tunable output resistance (photo-resistor), (2) phototransistor operation that is attained when back-gate is used to store optically generated carriers which in return modulate the transconductance of the transistor in on-state. Simulation results show that the investigated devices have the potential to give rise to new circuit topologies exploiting interaction between light and band-to-band tunneling processes, and improve the area efficiency of pixel sensors owing to their optical gain and charge storage mechanism. V C 2014 AIP Publishing LLC.[http://dx.doi.org/10.1063/1.4904026] Tunnel Field Effect Transistor (TFET) which has been singled out by International Technology Roadmap for Semiconductor for low power applications owing to its steeper switching characteristics compared to MOSFET holds great potential for various sensor applications, such as for detection of molecules and light intensity sensing. 1,2 In the recent years, semiconductor optoelectronic devices have been of great interest as they facilitate on-chip optical communication and image processing. 3 In this letter, we investigate silicon-based partially gated TFET as light detection devices and their possible applications.The structure of the TFET used in experiments is shown in Figure 1. The fabrication of investigated devices was carried out by CEA-LETI on an SOI substrate with 145 nm BOX and 20 nm active Si layer using MESA process. 4 The gate stack is composed of 6 nm SiO 2 , 10 nm TiN, and 50 nm Poly Si. The Si 3 N 4 protection layer was deposited and patterned to introduce an intrinsic region (L in ) adjacent to the nþ doped region. This channel extension (underlap) and spacer regions are transparent, unlike the gate stack which reflects a large fraction of the optical power received on the sample at the intermediary interfaces and partially absorbs it.With first order approximations, it is found that the light attaining the channel through the gate stack is 15-90 times weaker, depending on the wavelength, compared to the light intensity obtained in the non-gated region. The experimental results shown in the following parts in this letter belong to a device with gate length (L g ) ¼ 2 lm, spacer length (L spacer ) ¼ 30 nm, gate width (W g ) ¼ 10 lm, and L in ¼ 0.5 lm, and measurements are taken at room temperature and with the back gate grounded unless otherwise mentioned. In a previous study, it has been shown that the impact of light penetrating through the spacer adjacent to the pþ doped region and the gate stack is found to be not negligible yet relatively small, compared to L in . 5 Typical lateral embodiment of a TFET has two features in common with the elementary photosensitive devices, photodiodes: (1) p/i/n structure, (2) operation in reverse bias. In the measured devices, the light absorption in...