| 摘要 |
A measured electron beam (2) having a polarization vector as represented by arrow (1) is irradiated to a ferromagnetic target (7) made of an iron single crystal through a polarization vector rotator (5) comprising a magnetic field generation coil (3) and an electrostatic lens (4). A magnetic field generator (8) is coupled with the target (7) and aligns the direction of magnetization of the target (7) in a direction represented by arrow (6). An oscillator (9) for providing a rotation signal of the polarization vector of the measured electron beam (2) is connected to the polarization vector rotator (5). The current absorbed by the target (7) is detected and amplified by a current amplifier (11). A lock-in amplifier (10) detects the phase and the magnitude of an A.C. component using the signal from the oscillator (9) as a reference signal. The magnitude of the D.C. component of the absorbed current is detected by a D.C. current detector (12). The ratio of the A.C. component of the absorbed current to its D.C. component is calculated by a division circuit (13). When the phase of this A.C. signal (ia) is detected by the lock-in amplifier (10) using the signal (saw tooth wave signal is) from the oscillator (9) as the reference signal, the phase difference DELTA phi between the reference signal and the detected A.C. current corresponds to the angle defined between the polarization vector (arrow 1) of the measured electron beam (1) incident into the detector and the magnetization vector (arrow 6) of the target (7) and in this manner, the direction of the polarization vector can be detected. The magnitude of the polarization vector can be determined by dividing the amplitude (Ia) of the A.C. signal (ia) by the current (Id) detected by the D.C. current detector (12), by the division circuit (13). <IMAGE> |
