We perform an extensive analysis of linear fluctuations during preheating in Higgs inflation in the Einstein frame, where the fields are minimally coupled to gravity, but the field-space metric is nontrivial. The self-resonance of the Higgs and the Higgsed gauge bosons are governed by effective masses that scale differently with the nonminimal couplings and evolve differently in time. Coupled metric perturbations enhance Higgs self-resonance and make it possible for Higgs inflation to preheat solely through this channel. For ξ 100 the total energy of the Higgs-inflaton condensate can be transferred to Higgs particles within 3 efolds after the end of inflation. For smaller values of the nonminimal coupling preheating takes longer, completely shutting off at around ξ 30. The production of gauge bosons is dominated by the gauge boson mass and the field space curvature. For large values of the nonminimal coupling ξ 1000, it is possible for the Higgs condensate to transfer the entirety of its energy into gauge fields within one oscillation. For smaller values of the nonminimal coupling gauge bosons decay very quickly into fermions, thereby shutting off Bose enhancement. Estimates of non-Abelian interactions indicate that they will not suppress preheating into gauge bosons for ξ 1000.1 For inflation on the flat plateau one should consider ξ 440 (e.g. [20]). In models of hilltop or inflection point inflation, smaller values of ξ are possible, although UV corrections are expected to be larger. In order to provide a treatment of Higgs inflation as complete as possible without referring to specific unknown physics, we choose to consider a broad range of non-minimal couplings that go below ξ ≈ 400. 2 See [25] for a way to alter the predictions of α-attractor models through multi-field effects.