I. Introduction
Biomagnetic field measurement methods such as magnetoencephalography (MEG) and magnetic resonance imaging (MRI) are of considerable practical concern from the standpoint of non-invasive analysis of human brain function. Superconducting quantum interference devices (SQUIDs), which have ultra-high sensitivity to magnetic fields in the femtotesla range, have been recently used to detect biomagnetic fields. However, these tools are extremely expensive to maintain because they require cryogenic cooling to sustain the superconductivity state regardless of whether they are in operation. Alternative sensors are therefore desirable for the development and spread of biomagnetic field measurements. The most remarkable of these are optically pumped atomic magnetometers, which were chiefly developed by the Romalis group at Princeton University [1]–[3]. These magnetometers have high sensitivity, which has been theoretically estimated to be 0.01 under spin-relaxation free (SERF) conditions [2]. Several research groups have empirically applied optically pumped atomic magnetometers to biomagnetic field measurements [3]–[6]. Therefore, we have investigated their properties and reported the suitability of the potassium atomic magnetometer for biomagnetic field measurements by use of a phantom model of the human head [7].