In recent years, the terahertz frequency range has been extensively explored, including a short wave length part of the millimeter band, namely, the 2 mm (100-150 GHz) and 1 mm (150-300 GHz) intervals. At present, the task of increasing the radiation power that can be generated in these wavelength intervals by microwave O type devices with working voltages up to 20 kV is topical. One possible way of solving this task is offered by orotrons with a double row periodic struc ture (DPS), where the goal can be achieved by increas ing the width of a planar electron beam.The orotron was originally proposed in 1966 by Rusin and Bogomolov [1]. A distinctive feature of this device is the presence of a comb like periodic stricture situated on a plane mirror in an open resonator (OR). A planar electron beam, which propagates over the ripples of this structure, is focused by an external mag netic field. Since then, a large number of devices with ORs have been developed, which are known both as orotrons (see, e.g., [2]) and under other names (see, e.g., [3]). In an orotron with DPS [2], in contrast to a single row comb like structure [1], there is a planar gap for the electron beam propagation between rows. Orotrons with DPS have been extensively studied at the Kotel'nikov Institute of Radio Engineering and Electronics since their invention (see, e.g., [4]). Pres ently these investigations are aimed at using the advan tages of these devices in the terahertz frequency range [5].Previously, it was theoretically predicted [6] that, in orotrons with DPS and a hemispherical OR for the centimeter wavelength range, the width (2C) of the planar electron beam can be increased up to at least two caustic radii (r c ) without decreasing efficiency of the electron-wave interaction. This possibility is related to the fact that the RF field amplitude distribu tion for the main mode (TEM 00q ) is Gaussian both along and across the electron beam. However, in the existing devices with 2C ≤ 2r c , a decrease in the field amplitude at the boundaries of the electron beam compensates for the increase in the working current achieved by increasing the beam width at a constant current density in the flight channel.In orotrons with DPS for the aforementioned fre quency range, especially for the 1 mm wavelength interval, a decrease in the generation startup current is achieved by using a DPS with the number of periods increased up to N > 100. This DPS has a greater length than that in orotrons for the centimeter and millimeter range with N ≈ 20. For this reason, it is impossible to create a desired field amplitude distribution along the interaction space using a hemispherical mirror. Hence, orotrons for the 1 mm range should employ ORs with focusing mirrors of some other shapes.This Letter presents some results of the first exper iments with an orotron for the 140-300 GHz range based on a DPS having a sphero cylindrical focusing mirror, the generatrix of which is parallel to the elec tron beam.A detailed design of the experimental prototype orotron, whi...