Composition evolution of crystal structure and negative thermal expansion in pyro-vanadate–phosphate Cu1.8Zn0.2V2–<i>x</i>P<i>x</i>O7

M M. Kawakita (Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,) F F. Ikawa (Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,) K K. Yagi (Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,) M M. Kano (Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,) T T. Kubo (Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,) Y Y. Yokoyama (Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,) N N. Katayama (Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,) Y Y. Okamoto (National Institute of Advanced Industrial Science and Technology (AIST) , 1-1-1 Higashi, Tsukuba, Ibaraki 305-8565,) D D. Hirai (Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,) K K. Takenaka (Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,)

Abstract

We constructed a composition–temperature phase diagram for Cu1.8Zn0.2V2–xPxO7 based on structural analysis conducted using synchrotron radiation over the entire compositional range and a wide temperature (110–760 K) range. As x increases, the structure changes from the β-Cu2V2O7 structure (C2/c) to the α-Cu2P2O7 structure (C2/c), and then to the β-Cu2P2O7 structure (C2/m). Accordingly, the crystallographic negative thermal expansion (NTE) weakens, especially in the β-Cu2P2O7 structure, but it never disappears completely. We also discovered that for x = 0.75–1.0, a phase transition occurs from the α-Cu2P2O7 structure to the β-Cu2P2O7 structure with increasing temperature, accompanied by large volume contraction of at most 1.5%. The anisotropic thermal deformation of the unit cell, which indicates the effectiveness of the microstructural effects enhancing the NTE, also weakens as x increases. Elucidation of NTE requires discussion beyond the crystal structure alone, such as local structure related to the soft linkage between polyhedra.

Article Details

Volume / Issue Vol. 126, Issue 9
Published March 01, 2025
ISSN 0003-6951
Publisher American Institute of Physics

Journal Info

Applied Physics Letters

American Institute of Physics

ISSN: 0003-6951 Physical Sciences

Authors (10)

M

M. Kawakita

Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,

F

F. Ikawa

Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,

K

K. Yagi

Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,

M

M. Kano

Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,

T

T. Kubo

Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,

Y

Y. Yokoyama

Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,

N

N. Katayama

Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,

Y

Y. Okamoto

National Institute of Advanced Industrial Science and Technology (AIST) , 1-1-1 Higashi, Tsukuba, Ibaraki 305-8565,

D

D. Hirai

Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,

K

K. Takenaka

Department of Applied Physics, Nagoya University 1 , Furo-cho, Chikusa-ku, Nagoya 464-8603,