We report the results of 153 Eu and 11 B nuclear magnetic resonance (NMR) studies of EuB 6 at temperatures above 0.04 K and in magnetic fields between 0 and 7 T. We have observed a surprising evolution of the 153 Eu NMR spectrum at very low temperatures, which we interpret as evidence for a complex electronic ground state of EuB 6 , involving the coexistence of two magnetically very similar, but electronically inequivalent, phases. The low temperature 11 B NMR spectra reveal two inequivalent boron sites with internal fields of 20.02 and 20.35 T. [S0031-9007 (98)07982-4] PACS numbers: 75.30.Kz, 76.60.CqFrom the results of early work, EuB 6 was thought to be a ferromagnetic semiconductor [1] with a Curie temperature of approximately 13 K involving the ordering of well-localized Eu 21 moments. However, this simple picture could not account for magnetic and electronic properties of this material [2][3][4]. For example, at low temperatures no insulating but rather a metallic behavior has been observed [5]. Also the magnetically ordered state of EuB 6 has proven to be difficult to understand. Previous and more recent results [6,7] on the temperature dependence of the specific heat C p ͑T ͒ indicate that two consecutive phase transitions occur with onsets at 16 and 14 K, respectively. In an effort to add microscopic information to the database concerning the low-temperature behavior of EuB 6 , we have made 153 Eu and 11 B NMR experiments on a EuB 6 sample which has been characterized by structural, thermal, transport, and optical properties [6].As the most surprising result we note an anomalous evolution of the 153 Eu NMR spectrum at low temperatures, which implies the gradual development of a new ordered phase in EuB 6 and the coexistence of two magnetically inequivalent phases in the ground state of this material. The differences appear to be minute and to consist of a rather subtle but distinct variation in the electronic environment at the Eu sites. Our 11 B NMR results are consistent with a slight distortion of the crystal structure below the Curie temperature, but we have no evidence for moment reorientation phenomena at lower temperatures [7].For our NMR experiments we used standard spin-echo techniques with external magnetic fields between 0 and 7 T, at temperatures between 0.04 and 300 K. The NMR spectra were measured at a fixed frequency by monitoring the spin-echo signal at a given frequency and varying stepwise the applied magnetic field. The spin-lattice relaxation time was measured by destroying the nuclear magnetization with a comb of rf pulses and observing the nuclear magnetization recovery towards thermal equilibrium. The spin-spin relaxation time T 2 was obtained by analyzing the decay of the spin echo as a function of the separation between the rf pulses, using a model suggested for the case of EuO by . Prior to the actual NMR measurements we applied magnetic fields of the order of a few tesla at low temperatures, which, in the presence of even weak magnetic anisotropy, results in a very good alignme...