Crystal structures and sign reversal Hall resistivities in iron-based superconductors Lix(C3H10N2)0.32FeSe <inline-formula> <tex-math> <?CDATA $(0.15\lt x\lt 0.4$?> </tex-math><mml:math> <mml:mo stretchy="false">(</mml:mo> <mml:mn>0.15</mml:mn> <mml:mo><</mml:mo> <mml:mi>x</mml:mi> <mml:mo><</mml:mo> <mml:mn>0.4</mml:mn> </mml:math> <inline-graphic xmlns:xlink="http://www.w3.org/1999/xlink" xlink:href="cpb_28_6_067401

Crystal structures and sign reversal Hall resistivities in iron-based superconductors Li_x(C₃H₁₀N₂)_0.32FeSe

( 0.15 < x < 0.4

)

Sun Rui-Jin^{1, 2}, Jin Shi-Feng^{1, 3, †}, Deng Jun^{1, 2}, Hao Mu-Nan^{1, 2}, Zhao Lin-Lin^{1, 2}, Fan Xiao^{1, 2}, Sun Xiao-Ning^{1, 2}, Guo Jian-Gang^{1, 2}, Gu Lin^{1, 2, ‡}

Response of lattice parameters, anionic Se height, Fe–Se bond length and Se–Fe–Se bond angles of Li_0.15(C₃H₁₀N₂)_0.32FeSe to elevating temperature at 85 K, 110 K, 130 K, 150 K, 170 K, 200 K, and 295 K, respectively. Dashed lines are guides for the eyes.