wileyonlinelibrary.comunconventional fractional excitations, [1][2][3][4][5][6] nontrivial scale-invariant quantum excitations at quantum critical points, [7][8][9][10][11][12] and nonresonant absorption in superconductors. [ 13 ] In the context of applications, broadband microwave absorption is highly desirable in microwave fi lters, [ 14 ] signalto-noise enhancers, optical signal processing, [15][16][17] electromagnetic interference shielding, [ 18,19 ] etc. Most of these applications are based on conducting materials, even though normal metals possess relatively narrow absorption ranges (typically 100-1000 MHz). [ 18 ] Hence, composite carbon-based materials, [19][20][21] which extend the absorption range from hundreds of kHz up to hundreds of GHz, [ 18 ] and multilayer magnetic structures that cover the range between several GHz and several THz [22][23][24][25][26] are being developed. However, none of these materials allow for external control of their absorption properties, e.g., by the electric or the magnetic fi eld.A class of materials that could allow for a controllable (ondemand) broadband absorption are metamagnets. These systems are, typically, highly anisotropic and, as a function of the external magnetic fi eld, undergo a fi rst-order phase transition from a state with low magnetization to a state with high magnetization. [ 27 ] Prominent examples are layered metamagnets with perpendicular anisotropy, where ferromagnetic (FM) layers are antiferromagnetically (AFM) aligned. Such systems are not affected by magnetic fi elds perpendicular to the layers until the applied fi eld becomes comparable to the AFM interlayer interaction, when a fi rst-order transition to an FM structure occurs. If a fi nite demagnetization fi eld is present, the high-fi eld FM phase is reached through a "mixed phase," existing in a fi nite range of fi elds. In this phase, AFM and FM orders coexist. [27][28][29][30] There are numerous possible arrangements of FM and AFM domains, [ 29,30 ] and consequently a very rich excitation spectrum can be anticipated. Up to now, studies of the mixed phase have almost exclusively been restricted to ac susceptibility measurements and thus to a frequency range of 0.1-100 kHz. [31][32][33][34][35] Therefore, the intriguing dynamics of the mixed phase have remained elusive.In this paper, we focus on the recently discovered layered metamagnet Cu 3 Bi(SeO 3 ) 2 O 2 Br, with kagome-like Cu layers stacked along the c -axis. [ 36 ] At T N = 27.4 K, the system develops
Controllable Broadband Absorption in the Mixed Phase of MetamagnetsMatej Pregelj , * Oksana Zaharko , Andrej Zorko , Matjaž Gomilšek , Oles Sendetskyi , Axel Günther , Mykhaylo Ozerov , Sergei A. Zvyagin , Hubertus Luetkens , Christopher Baines , Vladimir Tsurkan , and Alois Loidl Materials with broad absorption bands are highly desirable for electromagnetic fi ltering and processing applications, especially if the absorption can be externally controlled. Here, a new class of broadband-absorption materials is introduced. Namely, ...