The origin of the spin liquid state in Tb2Ti2O7 has challenged experimentalists and theorists alike for nearly 20 years. To improve our understanding of the exotic magnetism in Tb2Ti2O7, we have synthesized a chemical pressure analog, Tb2Ge2O7. Germanium substitution results in a lattice contraction and enhanced exchange interactions. We have characterized the magnetic ground state of Tb2Ge2O7 with specific heat, ac and dc magnetic susceptibility, and polarized neutron scattering measurements. Akin to Tb2Ti2O7, there is no long-range order in Tb2Ge2O7 down to 20 mK. The Weiss temperature of −19.2(1) K, which is more negative than that of Tb2Ti2O7, supports the picture of stronger antiferromagnetic exchange. Polarized neutron scattering of Tb2Ge2O7 reveals that at 3.5 K liquid-like correlations dominate in this system. However, below 1 K, the liquid-like correlations give way to intense short-range ferromagnetic correlations with a length scale related to the Tb-Tb nearest neighbor distance. Despite stronger antiferromagnetic exchange, the ground state of Tb2Ge2O7 has ferromagnetic character, in stark contrast to the pressure-induced antiferromagnetic order observed in Tb2Ti2O7.Geometrically frustrated pyrochlores, R 2 M 2 O 7 , exhibit a diverse array of exotic magnetic behaviors [1]. The ground states in these materials are dictated by a complex, and often delicate balance of exchange, dipolar, and crystal field energies. Tb 2 Ti 2 O 7 is one of the most remarkable of these frustrated pyrochlores; strong antiferromagnetic exchange and Ising-like spins led to predictions of an antiferromagnetic Néel state below ∼1 K for this material [2]. However, experimental studies revealed a lack of static order or spin freezing in Tb 2 Ti 2 O 7 down to 70 mK [3,4], and more recently 57 mK [5]. Subsequently, enormous efforts have been undertaken to uncover the origin of the spin liquid state in Tb 2 Ti 2 O 7 .A further complication in Tb 2 Ti 2 O 7 is the coupling of magnetic and lattice degrees of freedom [6][7][8][9]. It has been suggested that hybridized magnetoelastic excitations may be responsible for the suppression of magnetic order in Tb 2 Ti 2 O 7 [10]. Another theoretical construct that attempts to account for the lack of static order in Tb 2 Ti 2 O 7 is a quantum spin ice state [11][12][13][14][15]. A third proposed scenario is that the non-Kramers doublet ground state of Tb 2 Ti 2 O 7 is split into two non-magnetic singlets through a symmetry reducing structural distortion [16][17][18].Other studies sought to uncover the origin of the spin liquid state in Tb 2 Ti 2 O 7 by focusing on mechanisms of its destruction, such as: external pressure [19], magnetic fields [18,20,21], and a combination of the two [22]. Partial antiferromagnetic order is induced in Tb 2 Ti 2 O 7 with external hydrostatic pressures of 8.6 GPa, resulting in a 1% compression of the lattice [19]. Another means of destroying the spin liquid state is chemical pressure: substitution of the non-magnetic titanium cation for an iso-electronic cation w...