Cubic anvil cell apparatus for high-pressure and low-temperature physical property measurements<xref rid="cpb_27_7_077403fn1" ref-type="fn">*</xref><fn id="cpb_27_7_077403fn1"> <label>*</label><p>Project supported by the National Natural Science Foundation of China (Grant No. 11574377), the State Key Development Program for Basic Research of China (Grant Nos. 2018YFA0305700 and 2014CB921500), the Key Research Program of Frontier Sciences of the Chinese Academy of Sciences (Grant No. QYZDB-SSW-SLH013), and the JSPS KAKENHI (Grant No. 15H03681).</p></fn>

Cubic anvil cell apparatus for high-pressure and low-temperature physical property measurements* *

Project supported by the National Natural Science Foundation of China (Grant No. 11574377), the State Key Development Program for Basic Research of China (Grant Nos. 2018YFA0305700 and 2014CB921500), the Key Research Program of Frontier Sciences of the Chinese Academy of Sciences (Grant No. QYZDB-SSW-SLH013), and the JSPS KAKENHI (Grant No. 15H03681).

Cheng Jin-Guang^{1, 2, †}, Wang Bo-Sen^{1, 2}, Sun Jian-Ping^{1, 2}, Uwatoko Yoshiya³

(color online) T–P phase diagram of MnP. PM: paramagnetic, FM: ferromagnetic, AFM: antiferromagnetic, SC: superconductivity; T_c: PM–FM transition temperature, T_s: FM–Screw transition temperature, T^*: FM–AFM transition temperature, T_m: PM–AFM transition temperature, T_sc: superconducting transition temperature. This figure is reproduced from Ref. [18] .