“…The electron beam was transported to the target 7 which was fixed into the vacuum cham ber 6 by means of three rotating magnets 4, two pairs of magnetic quadrupole lenses 5, and a corrector 6, which made it possible to focus the electron beam on the place where the target was located with a size of up to 3 mm and with a divergence of, at most, 5 mrad. These values satisfied the PB measurement conditions in the backscattering geometry, which were limited by the dimensions of the transverse cross section of the electron beam and its divergence [7][8][9]. The trans verse size, the position in the vacuum channel, and the current of the electron beam were controlled by the proportional chamber 11 and a Faraday cylinder 12.…”