†Effect of uniaxial stress on helimagnetic phases in the square-lattice itinerant magnet <math> <msub> <mi>EuAl</mi> <mn>4</mn> </msub> </math>: M. Gen, T. Nomoto, H. Saito, T. Nakajima, Y. Tokunaga, R. Takagi, S. Seki and T.-H. Arima, Phys. Rev. B 113, L100406 (2026).
Long-period incommensurate magnetic orderings associated with the large magnetocaloric effect in <math> <mrow> <msub> <mi>GdCo</mi> <mn>2</mn> </msub> <msub> <mi mathvariant="normal">B</mi> <mn>2</mn> </msub> </mrow> </math>: S. R. Larsen, N. Terada, H. Mamiya, H. Saito, T. Nakajima, S. Itoh, P. Manuel, D. Khalyavin, F. Orlandi and H. Kitazawa, Phys. Rev. B 113, 104411 (2026).
Emergent electric field induced by dissipative sliding dynamics of domain walls in a Weyl magnet: R. Yamada, D. Kurebayashi, Y. Fujishiro, S. Okumura, D. Nakamura, F. S. Yasin, T. Nakajima, T. Yokouchi, A. Kikkawa, Y. Taguchi, Y. Tokura, O. A. Tretiakov and M. Hirschberger, Nat. Phys. 22, 239 (2026).
†Phase Stability and Site Occupancy in Ba 12 Fe 28 Ti 15 O 84 : Insights from Fe 2+ –Ti 4+ Substitution and Neutron Diffraction Studies: H. Onuma, K. Kakizaki, K. Kamishima, H. Saito and T. Nakajima, J. Phys. Soc. Jpn. 94, 104804 (2025).
†Fermi surface reconstruction due to orthorhombic distortion in the Dirac semimetal <math> <msub> <mi mathvariant="normal">YbMnSb</mi> <mn>2</mn> </msub> </math>: D. Bhoi, F. Ye, H. Ma, X. Shen, A. Maurya, S. Kasamatsu, T. Misawa, K. Yoshimi, T. Nakajima, M. Kondo, Y. Kinoshita, M. Tokunaga, M. Matsuda and Y. Uwatoko, Phys. Rev. B 111, 214115 (2025).
