Monopnictides of rare earth elements (LnY, where Ln are lanthanides; Y = N, P, As, Sb, Bi) [1] have recently attracted attention of researchers due to the improvement of the technology of their preparation.According to the data available in the literature, experimental studies of the aforementioned materials under uniform compression have been predominantly focused on pressure dependences of their elastic mod uli and unit cell parameters, while theoretical studies have been focused primarily on calculations of elec tronic structures of the initial and high pressure phases [2][3][4][5][6][7][8][9]. There are no experimental studies of the effect of uniform compression on the electron sub system of rare earth element (REE) monopnictides. At the same time, it is obvious that changes in elec tronic structures of the materials studied under pres sure are primarily responsible for the phase transitions in them. This stipulates interest in systematic studies of the effect of uniform compression on the electron transfer in REE monopnictides and on the transfor mation of their electronic structure. A rather informa tive technique in this aspect is the method of measur ing thermopower under uniform compression, because this quantity is very sensitive to anomalies in pressure induced density of states g(E) at the level of the chemical potential μ.The lanthanum monobismuthide LaBi was chosen for the studies owing to the following reasons. First, it has a relatively low pressure of the structural phase transition [4], and second, it has the unfilled 4f shell of the free La ion.The samples used in our studies consisted of a poly crystalline substance prepared by melting elements (La, Bi) in a stoichiometric proportion, followed by homogenizing annealing [10]. The X ray diffraction analysis showed that LaBi crystallizes in the B1 struc tural type (space group Fm3m), has the unit cell parameter a = 6.57(1) Å, and the X ray coherent scat tering region L ≈ 320 Å. At room temperature and under atmospheric pressure, the Hall constant R H = ⎯1.067 cm 3 /C was obtained at the induction of mag netic field H = 13.6 T and electrical resistivity ρ ≈ 130 μΩ cm; in this case, we have ∂ρ/∂T < 0. 1The electrical resistance R and thermopower S were measured at room temperature in a high pressure apparatus with diamond anvils at a pressure up to 22 GPa. The medium transmitting the pressure on the sample was a lithographic stone (species of calcite). The measurement technique was described in detail in [11].The dependences of R and S on the pressure for LaBi are shown in Figs. 1 and 2. It should be noted immediately that, in the measurement of the depen dence of the electrical resistance on the pressure, no phase transition in LaBi at ~10 GPa was revealed. Only the dependence lnR(P) exhibits a slight anomaly in the pressure region of ~11 GPa (marked by the arrow in inset to Fig. 1), which is probably associated 1 The results of the studies of the temperature and field depen dences of the Hall constant R H and electrical resistivity ρ of LaBi in ...