Spin-polarized Weyl cones and giant anomalous Nernst effect in ferromagnetic Heusler films

強磁性ホイスラー薄膜におけるスピン偏極ワイルコーンと巨大異常ネルンスト効果

角田 一樹   ; 桜庭 裕弥*; 増田 啓介*; 河野 嵩*; 鹿子木 将明*; 後藤 一希*; Zhou, W.*; 宮本 幸治*; 三浦 良雄*; 奥田 太一*; 木村 昭夫*

Sumida, Kazuki; Sakuraba, Yuya*; Masuda, Keisuke*; Kono, Takashi*; Kakoki, Masaaki*; Goto, Kazuki*; Zhou, W.*; Miyamoto, Koji*; Miura, Yoshio*; Okuda, Taiichi*; Kimura, Akio*

Weyl semimetals are characterized by the presence of massless band dispersion in momentum space. When a Weyl semimetal meets magnetism, large anomalous transport properties emerge as a consequence of its topological nature. Here, using in-situ spin- and angle-resolved photoelectron spectroscopy combined with ab initio calculations, we visualize the spin-polarized Weyl cone and flat-band surface states of ferromagnetic CoMnGa films with full remanent magnetization. We demonstrate that the anomalous Hall and Nernst conductivities systematically grow when the magnetization-induced massive Weyl cone at a Lifshitz quantum critical point approaches the Fermi energy, until a high anomalous Nernst thermopower of 6.2 VK is realized at room temperature. Given this topological quantum state and full remanent magnetization, CoMnGa films are promising for realizing high efficiency heat flux and magnetic field sensing devices operable at room temperature and zero-field.