_Applied_  
_sciences_  
A Visible and Near-IR Tunnel Photosensor with a Nanoscale Metal Emitter: The Effect of Matching of Hot Electrons Localization Zones and a Strong Electrostatic Field  
**[PERSON] 1,*+**, **[PERSON] 2**, **[PERSON] 3,4, [PERSON] 4**,  
**[PERSON] 2**, **[PERSON] 4,5, [PERSON] 4**, **[PERSON] 5** and  
**[PERSON] 4,5+**  
\({}^{1}\) Laboratory of System Problems in Control and Automation in Mechanical Engineering, Institute of Precision Mechanics and Control, RAS, 410028 Saratov, Russia  
\({}^{2}\) Volga-Svet Co. Ltd., 410052 Saratov, Russia; [EMAIL_ADDRESS] (N.A.); [EMAIL_ADDRESS] (A.L.)  
\({}^{3}\) Department of Optics and Biophotonics, Faculty of Physics, Saratov State University, 410012 Saratov, Russia; [EMAIL_ADDRESS]  
\({}^{4}\) Laboratory of Laser Diagnostics of Technical and Living Systems, Institute of Precision Mechanics and Control, RAS, 410028 Saratov, Russia; [EMAIL_ADDRESS] (Y.A.); [EMAIL_ADDRESS] (S.Y.); [EMAIL_ADDRESS] (S.Z.); [EMAIL_ADDRESS] (D.Z.)  
\({}^{5}\) Department of Physics, Yury Gagarin State Technical University of Saratov, 410054 Saratov, Russia; [EMAIL_ADDRESS]  
\({}^{*}\) Correspondence: [EMAIL_ADDRESS]; Tel.: +7-845-222-2376  
Footnote †: journal: Applied Physics Letters  
**Abstract:** The results of the research and design of a novel vacuum photosensor with a planar molybdenum blade structure are presented. The advanced prototype implements the principle of an increasing penetrability of the Schottky barrier for the metal-vacuum interfaces under the action of an external strong electrostatic field. Theoretical and experimental substantiation of the photosensor performance in a wide range of wavelengths (from 430 to 680 nm and from 800 to 1064 nm) beyond the threshold of the classical photoelectric effect is given. The finite element method was applied to calculate distribution of the optical and electrostatic fields inside the photosensor structure. The sensor current-to-light response was studied using the periodic pulsed irradiation with the tunable wavelength. It was shown that the nanoscale localization zones of two types are formed near the surface of the blade tip: the zone of an increased concentration of hot electrons localized inside the molybdenum blade, and the zone with an increased strength of the external electrostatic field localized outside the blade. In general, the mutual positions of these zones may not coincide, whereas the position of the first-type localization zone significantly varies with the changes in the wavelength of the irradiating light. This causes features in the spectrum of the quantum yield of the photosensor such as expressed non-monotonic behavior and occurrence of sharp dips. The design of the photosensor that provides matching of the positions for both types of localization zones was proposed; the manufactured prototypes of the designed device were experimentally studied. In the designed photosensor, the ballistic transport of photoelectrons in the vacuum gap with a strong field provides a possibility for the creation of ultra-fast optoelectronic devices, such as modulators, detectors, and generators.  
**Keywords:** tunnel photo emission; hot electrons; vacuum photosensor; quantum yield; wavelength dependence