The anapole, a non-radiating charge-current configuration, was recently observed in a variety of artificial materials and nanostructures. We provide a brief overview of this rapidly developing field and discuss implications for spectroscopy, energy materials, electromagnetics, as well as quantum and nonlinear optics. Toroidal electrodynamics, a new chapter of electromagnetics research is currently attracting considerable and growing attention 1-4. It includes the study of toroidal multipoles and anapoles (see Fig. 1). The recent surge of interest in toroidal multipoles is driven by the emerging understanding that alongside the well-known electric and magnetic multipoles they are necessary for a complete characterization of the electromagnetic properties of matter 2. Indeed, while electromagnetic fields in free-space can be fully characterized with transverse electric (TE) and transverse magnetic (TM) multipoles 5 , the characterization of current density requires three multipole series, the electric, magnetic, and toroidal multipoles 6,7 (see Fig. 2). The distinctive role of toroidal multipoles is particularly apparent in the optical properties of matter containing large molecules or structural elements of toroidal symmetry and of size comparable to the electromagnetic wavelength. Dynamic toroidal response of metamaterials had been the subject of intense discussions since 2007 8,9 , but the first unambiguous experimental demonstration of dominant toroidal response in matter was recorded in a microwave metamaterial in 2010 1 (see Fig. 3). Subsequently, dynamic toroidal response has been observed in metallic 10-15 , plasmonic 16-22 , and dielectric metamaterials 23,24 at frequencies ranging from microwave through to terahertz and up to near-infrared/visible parts of the spectrum (see Fig. 3). The analysis of transmission, reflection 12 , and polarization phenomena 13 in complex molecular systems and metamaterials is incomplete without account of the dynamic toroidal response. Toroidal resonances could play a role in nano-lasers 19 , sensors 25 , and data storage devices 3,26. We shall also note that static toroidal dipoles, also known as 'static anapoles' introduced by Ya. B. Zeldovich in the context of parity violation in nuclear physics 27 , have been observed in magnetism 26 and could be the only allowed electromagnetic form-factor for dark matter candidate particles 28. An electric dipole (a pair of oscillating charges) together with a toroidal dipole (oscillating poloidal current on a torus (see Fig. 1)) can form a non-radiating charge-current configuration,