Frustrated random-singlet state with ice-type structural fluctuation in spinel titanates

N Noriaki Hanasaki (Department of Physics) T Takayuki Hattori (Department of Physics, University of Osaka) T Takumi Komoda (Department of Physics, University of Osaka) K Kouei Minamoto (Department of Physics, University of Osaka) S Shuhei Torigoe (Department of Physics, University of Osaka) S Satoshi Yamashita Y Yasuhiro Nakazawa T Takehito Nakano (Institute of Quantum Beam Science, Graduate School of Science and Engineering, Ibaraki University) K Kouhei Yoshimi (Graduate School of Engineering Science, University of Osaka) M Mitsuharu Yashima (Graduate School of Engineering Science, University of Osaka) H Hidekazu Mukuda (Graduate School of Engineering Science, University of Osaka) U Utami Widyaiswari (Nuclear Structure Research Group, RIKEN Nishina Center) I Isao Watanabe (Nuclear Structure Research Group, RIKEN Nishina Center) A Akihiro Koda (Institute of Materials Structure Science, High Energy Accelerator Research Organization) T Takashi Honda (J-PARC Center, High Energy Accelerator Research Organization (KEK), Tokai, Ibaraki 319-1106, Japan) T Toshiya Otomo (Institute of Materials Structure Science) H Hajime Sagayama K Katsuaki Kodama (Materials Sciences Research Center, Japan Atomic Energy Agency) H Hiroshi Murakawa (Department of Physics) H Hideaki Sakai (Department of Physics)

Abstract

In ice, it is well known that the orientation of H 2 O molecules is disordered by geometrical frustration. Ice-analogous materials having a pyrochlore lattice display interesting phenomena such as the spin-ice state and the magnetic monopole. In the spinel titanate MgTi 2 O 4 , the Ti ions have a quantum spin in the pyrochlore lattice. The Ti ions are displaced, accompanied by the spin-singlet formation. Since this displacement pattern follows the ice rule, the title compound is a material analogous to ice. When a small quantity of Ti ions are replaced with Mg ions, the ice-type structural fluctuation exists. In this structural ice-type state, the spins are also fluctuating at a nanosecond scale down to 0.3 K. We ascribed this phenomenon to the gapless frustrated random-singlet state, in which the spin-singlet pairs are resonating, and the orphan spins are hopping.

Article Details

Volume / Issue Vol. 123, Issue 1
Published January 06, 2026
ISSN 0027-8424
Publisher National Academy of Sciences

Authors (20)

N

Noriaki Hanasaki

Department of Physics

T

Takayuki Hattori

Department of Physics, University of Osaka

T

Takumi Komoda

Department of Physics, University of Osaka

K

Kouei Minamoto

Department of Physics, University of Osaka

S

Shuhei Torigoe

Department of Physics, University of Osaka

S

Satoshi Yamashita

Y

Yasuhiro Nakazawa

T

Takehito Nakano

Institute of Quantum Beam Science, Graduate School of Science and Engineering, Ibaraki University

K

Kouhei Yoshimi

Graduate School of Engineering Science, University of Osaka

M

Mitsuharu Yashima

Graduate School of Engineering Science, University of Osaka

H

Hidekazu Mukuda

Graduate School of Engineering Science, University of Osaka

U

Utami Widyaiswari

Nuclear Structure Research Group, RIKEN Nishina Center

I

Isao Watanabe

Nuclear Structure Research Group, RIKEN Nishina Center

A

Akihiro Koda

Institute of Materials Structure Science, High Energy Accelerator Research Organization

T

Takashi Honda

J-PARC Center, High Energy Accelerator Research Organization (KEK), Tokai, Ibaraki 319-1106, Japan

T

Toshiya Otomo

Institute of Materials Structure Science

H

Hajime Sagayama

K

Katsuaki Kodama

Materials Sciences Research Center, Japan Atomic Energy Agency

H

Hiroshi Murakawa

Department of Physics

H

Hideaki Sakai

Department of Physics