Abstract

There are two ways of determining polarization of deuteron targets by the deuteron magnetic resonance (DMR) method. One of them (more traditional) is based on directly proportional relation of polarization to the integrated intensity of the DMR absorption spectrum [1]. But in this way calibration of the apparatus against the intensity of the thermal equilibrium spectrum is needed, although the procedure is carried out under low signal-to-noise ratio conditions. A more acceptable way is based on specific features of the DMR spectrum, which can be represented as a superposition of two lines corresponding to the transitions between neighbouring magnetic energy levels.

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