The pyrochlore magnet Yb2Ti2O7 has been proposed as a quantum spin ice candidate, a spin liquid state expected to display emergent quantum electrodynamics with gauge photons among its elementary excitations. However, Yb2Ti2O7's ground state is known to be very sensitive to its precise stoichiometry. Powder samples, produced by solid state synthesis at relatively low temperatures, tend to be stoichiometric, while single crystals grown from the melt tend to display weak "stuffing" wherein ∼ 2% of the Yb 3+ , normally at the A site of the A2B2O7 pyrochlore structure, reside as well at the B site. In such samples Yb 3+ ions should exist in defective environments at low levels, and be subjected to crystalline electric fields (CEFs) very different from those at the stoichiometric A sites. New neutron scattering measurements of Yb 3+ in four compositions of Yb2+xTi2−xO7−y, show the spectroscopic signatures for these defective Yb 3+ ions and explicitly demonstrate that the spin anisotropy of the Yb 3+ moment changes from XY-like for stoichiometric Yb 3+ , to Ising-like for "stuffed" B-site Yb 3+ , or for A-site Yb 3+ in the presence of an oxygen vacancy.Exotic magnetic ground states of cubic pyrochlore magnets, with composition A 2 B 2 O 7 , are of great topical interest, as the pyrochlore lattice is one of the canonical architectures supporting geometrical frustration in three dimensions [1,2]. Magnetism can reside at either the A 3+ site or the B 4+ site, and the magnetic moments' anisotropy and the interactions between the moments conspire to give rise to rich ground state selection. Among the states and materials that have been of recent interest have been the classical spin ice states in Dy and Ho titanate pyrochlores [3][4][5][6][7], spin liquid and spin glass states in molybdate pyrochlores [8], and spin fragmentation in Nd based zirconate pyrochlores [9]. The possibility that a quantum analogue of the spin ice ground state, i.e. quantum spin ice (QSI), may exist in certain low moment pyrochlore magnets, including Yb 2 Ti 2 O 7 and Pr 2 Zr 2 O 7 , has generated much excitement [10][11][12][13][14][15][16][17][18][19][20][21][22][23][24].At low temperatures Yb 2 Ti 2 O 7 displays two magnetic heat capacity anomalies: a broad one near 2 K and a sharp anomaly signifying a thermodynamic phase transition near T C = 0.26 K [25][26][27][28][29]. Below T C , the ordered structure is thought to be a splayed ferromagnet with moments pointing close to the (100) directions [30][31][32][33][34]. However, surprising sample variability has been reported in this phase transition, with some studies not seeing direct evidence for the ferromagnetic ordered state [18,[35][36][37][38][39][40][41]. Using the sharp anomaly in C P as the figure-ofmerit for the phase transition, interesting systematics have been observed [28,29,42,43]. Powder samples grown by solid state synthesis at relatively low temperatures show a sharp C P anomaly and a high T C . usually ∼ 0.26 K [28,29,42,44]; however most single crystal studies display broader the...