Abstract
Magnetic-field-induced semimetal-insulator phase transition in graphite has regained attention, although its mechanism is not fully understood. Recently, a study performed under the pulsed magnetic field discovered that this phase transition depends on thickness even in a relatively thick system of the order of 100 nm and suggested that the electronic state in the insulating phase has an order along the stacking direction. Here we report the thickness dependence observed under dc magnetic fields, which nicely reproduces the previous results obtained under the pulsed magnetic field. In order to look into the critical condition to control the phase transition, the effect of electrostatic gating is also studied in a field-effect transistor structure since it will introduce a spatial modulation along the stacking direction. Magnetoresistance, measured up to 35 T, is prominently enhanced by the gate voltage in spite of the fact that the underlying electronic state is not largely changed owing to the charge-screening effect. On the other hand, the critical magnetic field of the semimetal-insulator transition is found to be insensitive to gate voltages, whereas its thickness dependence is fairly confirmed. By applying positive gate voltages, a prominent oscillation pattern, periodic in magnetic field, becomes apparent, the origin of which is not clear at this stage. Although electrostatic control of the phase transition is not realized in this study, the findings of gate-voltage tunability will help determine the electronic state in the quantum limit in graphite.
Original language | English |
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Article number | 155136 |
Journal | Physical Review B |
Volume | 94 |
Issue number | 15 |
DOIs | |
State | Published - 23 Oct 2018 |
Bibliographical note
Funding Information:A portion of this work was performed at the National High Magnetic Field Laboratory, which is supported by National Science Foundation Cooperative Agreement No. DMR-1157490 and the state of Florida. This work was partially supported by JSPS KAKENHI Grants No. JP15K21722, No. JP25107003, No. JP16H03999, and No. JP16K17739. W.K. was also supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (No. 2018R1D1A1B07050087 and No. 2018R1A6A1A03025340).
Funding Information:
The authors acknowledge Dr. E S. Choi for technical support and discussions. The authors also thank to Dr. B. Fauqué for fruitful discussions. A portion of this work was performed at the National High Magnetic Field Laboratory, which is supported by National Science Foundation Cooperative Agreement No. DMR-1157490 and the state of Florida. This work was partially supported by JSPS KAKENHI Grants No. JP15K21722, No. JP25107003, No. JP16H03999, and No. JP16K17739. W.K. was also supported by Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (No. 2018R1D1A1B07050087 and No. 2018R1A6A1A03025340).
Publisher Copyright:
© 2018 American Physical Society.