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. 2019 Dec 4;116(51):25530–25534. doi: 10.1073/pnas.1905524116

Fig. 4.

Fig. 4.

Pressure variation of the effective mass. (A) Oscillating component of sample 2 under P = 3 GPa at various temperatures. (B) Temperature dependence of amplitude of SdH oscillations under various pressures. Dashed line represents the fitting by the Lifshitz–Kosevich formula. (C) Pressure variation of the effective mass m normalized by free-electron mass m0. m decreases with pressure, showing the convergent behavior toward P = 2 Gpa.