The pyrochlore material Nd2Zr2O7 with an "all-in-all-out" (AIAO) magnetic order shows novel quantum moment fragmentation with gapped flat dynamical spin ice modes. The parameterized spin Hamiltonian with a dominant frustrated ferromagnetic transverse term reveals a proximity to a U(1) spin liquid. Here we study magnetic excitations of Nd2Zr2O7 above the ordering temperature (TN) using high-energy-resolution inelastic neutron scattering. We find strong spin ice correlations at zero energy with the disappearance of gapped magnon excitations of the AIAO order. It seems that the gap to the dynamical spin ice closes above TN and the system enters a quantum spin ice state competing with and suppressing the AIAO order. Classical Monte Carlo, molecular dynamics and quantum boson calculations support the existence of a Coulombic phase above TN. Our findings relate the magnetic ordering of Nd2Zr2O7 with the Higgs mechanism and provide explanations for several previously reported experimental features.Competing interactions and geometrical frustration support highly degenerate states which suppress conventional magnetic order and lead to novel emergent states [1]. Classical spin ice (CSI) is a prominent example which is realized in (Dy/Ho) 2 Ti 2 O 7 pyrochlores consisting of a network of corner-sharing tetrahedra [2][3][4][5][6]. In the CSI, the single-ion Ising anisotropy due to the crystal electric field (CEF) interactions frustrates the ferromagnetic (FM) interactions between the spins. This creates the "2-in-2-out" (2I2O) local constraint (ice rule) on the spin configuration leading to infinite degeneracy on the pyrochlore lattice [5]. However, an antiferromagnetic (AFM) interaction is not frustrated resulting in a long-range "all-in-all-out" (AIAO) order [1].With the introduction of transverse spin couplings, CSI transforms to quantum spin ice (QSI) allowing quantum tunnelling between the degenerate ice-rule states which realizes a type of U(1) quantum spin liquid [7][8][9][10][11][12][13][14][15]. Recently, there has been a tremendous effort aimed at finding materials supporting QSI [16]. Several materials have been examined in the search for QSI including, for example, Yb 2 Ti 2 O 7 [17], Pr 2 (Zr/Hf) 2 O 7 [18, 19], and Tb 2 Ti 2 O 7 [20], but the evidence so far is ambiguous, complicated by multi-phase competitions, structural defects and low-lying crystal field levels [21-26]. As a QSI candidate, Nd 2 Zr 2 O 7 is an ideal material for modelling, having well-isolated, Kramers, Ising anisotropic, dipolar-octupolar CEF ground doublets and a clean, well-ordered structure and it has been under * jianhui.xu@helmholtz-berlin.de † john.benton@riken.jp ‡ bella.lake@helmholtz-berlin.de intensive study [27-37]. Although it has an AIAO order as the ground state below T N ∼ 0.4 K [29, 30], it shows remarkably persistent spin dynamics [31], quantum moment fragmentation, gapped dynamical spin ice [32, 35], gapped kagome spin ice in (111) fields [36] and quantum spin-1/2 chains in (110) fields [37]. The parameterized anisotropic...