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 (Li,Fe)OHFeSe. SC-I and SC-II represents two distinct superconducting regions. The contour color plot of the normal-state resistivity exponent α illustrates a sharp transition of the normal state from the Fermi liquid for SC-I to the non-Fermi liquid for the SC-II phase. This figure is reproduced from Ref. [38].