The properties of materials that we encounter in our daily lives represent only a small part of their full potential. Materials exhibit a wide variety of physical properties depending on their environment—such as temperature, pressure, and magnetic field. In particular, under so-called "extreme conditions" that are far removed from everyday environments, even well-known materials can reveal unexpected and unknown aspects. This is because exotic states that cannot be stabilized under normal conditions may become the most stable under extreme conditions. Thus, the realm of extreme environments, where our everyday assumptions no longer apply, represents a vast unexplored territory for discovering novel physical phenomena.
My research aims to discover new physics and functionalities under extreme conditions by developing precision measurement techniques under ultra-low temperatures (~0.1 K), high pressures (up to 10 GPa), and strong magnetic fields (over 10 T), and using these to study the electronic states of materials. Accurately and comprehensively measuring physical properties under such conditions is far more challenging than in typical settings, which limits the amount of information that can be obtained. I strive to overcome these experimental challenges and develop techniques that enable previously impossible measurements. In my research, I emphasize the importance of interpreting experimental results based on established theoretical frameworks and explaining them quantitatively and thoroughly. Most experiments reveal results where many complex phenomena are intertwined. I believe that by carefully disentangling these phenomena one by one, the unexplained aspects that remain are where truly novel physics resides.
Three-dimensional topological materials with linear band crossings near the Fermi level are of great interest, as their properties are governed by Dirac fermions—particles that obey the laws of relativistic quantum mechanics. Well-known topological materials like Dirac and Weyl semimetals feature linear band crossings at discrete points in momentum space. In contrast, nodal line or nodal ring semimetals, which have recently attracted attention, exhibit band crossings that form continuous lines or rings. Candidate materials with such band structures, including MP3 (where M is an alkaline earth or rare-earth element) based on the black phosphorus structure, have been proposed, and a variety of novel physical properties arising from these features have been theorized. However, it remains challenging to experimentally realize a situation where the physical properties are governed solely by the nodal lines or rings and to reveal their universal behavior.
We addressed this challenge by focusing on black phosphorus, a prototypical elemental semiconductor that can be regarded as the parent compound of the aforementioned MP3 materials. It was known that applying about 1.5 GPa pressure closes the energy gap of black phosphorus, making it semimetallic, but its detailed electronic structure had not been clarified. By using high-quality single crystals synthesized in Japan and a rotatable indenter-type pressure cell in magnetic fields, we performed detailed quantum oscillation measurements under pressure and elucidated the full electronic structure (i.e., the Fermi surface) of semimetallic black phosphorus. The experimentally obtained Fermi surface matched the nodal ring structure predicted by first-principles calculations in remarkable detail, demonstrating that black phosphorus under pressure is indeed a nodal ring semimetal. In this system, only carriers originating from the nodal ring determine the material's properties, and the shape and carrier density of the nodal ring can be easily controlled by pressure, making it unique among known materials. We also found that the large and anisotropic magnetoresistance observed in semimetallic black phosphorus is significantly influenced by a direction-dependent scattering relaxation time along the crystal axes. These results suggest that black phosphorus under pressure can serve as a promising platform for systematic studies of nodal ring semimetal physics. This work was selected as an Editors’ Suggestion in the international journal Physical Review B, published by the American Physical Society.
Many studies, including those on high-temperature superconductors and heavy-fermion systems, have shown that unconventional superconductivity can emerge near quantum critical points associated with magnetic order. However, systematic studies on the relationship between superconductivity and charge order are limited, and many aspects remain unclear. We previously demonstrated that LaAgSb2 serves as a promising platform for exploring novel phenomena near the critical pressure of a charge density wave (CDW). In this study, we further discovered that LaAgSb2 is a superconductor at ambient pressure with a transition temperature Tc = 0.3 K. Electrical resistivity measurements under pressure in the dilution refrigerator temperature range revealed a sharp peak in Tc precisely at the CDW critical pressure, indicating a strong correlation between superconductivity and CDW. The suppression of Tc away from the critical pressure suggests that some superconductivity-enhancing mechanism is active only near the CDW critical point. To understand this behavior, we investigated the superconducting transition temperature Tc expected from the conventional phonon-mediated mechanism, based on first-principles electron-phonon coupling calculations. The results showed that the calculated electron-phonon coupling strength was small, and the theoretical Tc was on the order of a few millikelvin. Therefore, the experimentally observed Tc of around 1 K cannot be explained by this mechanism alone and suggests the involvement of a nontrivial mechanism related to the collapse of CDW order. We also found that carriers with relatively strong electron-phonon coupling are localized on two-dimensional Fermi surfaces formed by px and py orbitals of Sb atoms in the square lattice. This implies that the Sb square lattice plays a crucial role in the formation of CDWs, the emergence of highly mobile carriers, and also in superconductivity.
In addition, we investigated LaCuSb2, which has the same crystal structure as LaAgSb2. Unlike LaAgSb2, LaCuSb2 shows no anomalies indicative of a CDW transition at ambient pressure. Although previous studies were inconclusive, LaCuSb2 has been reported to be a superconductor with Tc ≈ 1 K at ambient pressure. Noting that the unit cell volume of LaCuSb2 is significantly smaller than that of LaAgSb2, we hypothesized that it might already lie near the CDW critical point at ambient pressure and closely examined its electronic state and superconducting properties. From resistivity, magnetization, and specific heat measurements, we established that LaCuSb2 is a bulk superconductor. We also used theoretical calculations to analyze transport phenomena under magnetic fields and determined its Fermi surface. Based on the experimentally determined Fermi surface, we conducted electron-phonon interaction calculations, revealing that: (1) Low-frequency phonon bands exhibit relatively strong electron-phonon coupling, and (2) Carriers interacting strongly with phonons are distributed across the entire Fermi surface. These findings differ from LaAgSb2, where such carriers were localized to specific Fermi surfaces. The theoretical Tc closely matched experimental values, leading us to conclude that LaCuSb2 is a typical phonon-mediated superconductor. The higher Tc compared to LaAgSb2 can be attributed to factors (1) and (2), and no CDW-related critical phenomena appear to be involved in LaCuSb2.
LaAgSb2 is known to exhibit successive charge density wave (CDW) transitions at ambient pressure at TCDW1 = 210 K and TCDW2 = 190 K. Through experiments, we revealed the temperature-pressure phase diagram of CDWs in LaAgSb2 and identified the critical pressures as PCDW1 = 3.2 GPa and PCDW2 = 1.7 GPa for CDW1 and CDW2, respectively. We also found that the Shubnikov–de Haas oscillation patterns changed distinctly at these critical pressures, providing direct evidence of Fermi surface reconstruction associated with the disappearance of the CDWs. In the high-pressure regime above PCDW1, where CDWs are absent, we observed a metallic state with high mobility and conductivity.
Furthermore, we developed a rotatable mechanism for an indenter-type pressure cell, enabling measurement of transport properties with respect to magnetic field direction at pressures up to 4 GPa and temperatures down to 1.6 K. Using this setup, we clarified the Fermi surface anisotropy and magnetoresistance behavior under pressure. By comparing these experimental results with numerical simulations of electrical conductivity based on predicted pressure-induced Fermi surface evolution, we demonstrated that an anisotropic Dirac band originating from the Sb square lattice—hidden under the CDW gap at ambient pressure—emerges above PCDW1 and dominates transport properties in that regime.