The electronic structure of magnetically-doped TI with stoichiometry Bi1.09Gd0.06Sb0.85Te3
in the region of the Dirac point has been studied in detail by angle-resolved photoelectron
spectroscopy (ARPES) at various temperatures (above and below the Néel temperature, 1-35 K)
and different polarizations of synchrotron radiation. It has shown that the energy gap in
photoemission spectra opens at the Dirac point and remains open above the temperature of the
long-range magnetic ordering, Tn. Measurements of magnetic properties by the superconducting
magnetometry method (SQUID) have shown antiferromagnetic ordering with a transition
temperature to the paramagnetic phase equal to 8.3 K. Study of the temperature dependence of
the Dirac cone state intensity at the Г point by ARPES has confirmed the magnetic transition
and has shown a possibility of its indication directly from photoemission spectra. A more
detailed analysis of the splitting between the upper and lower Dirac cone states (i.e. the energy
gap) at the Dirac point in the photoelectron spectra has shown the dependence of the measured
gap on the synchrotron radiation polarization (about 28-30 meV for p-polarization and 22-25
meV for circularly polarized radiation of opposite chirality). The mechanism of opening the gap
at a Dirac point above the Tn was proposed due to the “pairing” of the Dirac fermions with
opposite momentum and spin orientation as a result of their interaction with the spin texture
generated by photoemission in the region of the photoemission hole on a magnetic impurity atom
(Gd). It was shown that the gap at the Dirac point, measured above Tn, is dynamic and is formed
directly during photoemission process. At the same time, the origin of the gap remains magnetic
(even when the long-range magnetic ordering is destroyed) and is associated with the properties
of the magnetic topological insulator that determines a practically unchanged size of the gap
above Tn. The dynamic origin of the generated gap is confirmed by the dependence
of its magnitude on the polarization of synchrotron radiation.