| human | Q5 |
| P6178 | Dimensions author ID | 011471663200.95 |
| P496 | ORCID iD | 0000-0001-5456-7756 |
| P108 | employer | Los Alamos National Laboratory | Q379848 |
| P734 | family name | Harrison | Q2712864 |
| Harrison | Q2712864 | ||
| Harrison | Q2712864 | ||
| P735 | given name | Neil | Q5570878 |
| Neil | Q5570878 | ||
| P106 | occupation | researcher | Q1650915 |
| P21 | sex or gender | male | Q6581097 |
| Q59090640 | A multi-component Fermi surface in the vortex state of an underdoped high-Tc superconductor |
| Q62679444 | AnisotropicHc2up to 92 T and the signature of multiband superconductivity in Ca10(Pt4As8)((Fe1−xPtx)2As2)5 |
| Q62579225 | Bose-Einstein Condensation ofS=1Nickel Spin Degrees of Freedom inNiCl2−4SC(NH2)2 |
| Q84726199 | Cascade of magnetic field induced spin transitions in LaCoO3 |
| Q61198269 | Chemical potential oscillations from nodal Fermi surface pocket in the underdoped high-temperature superconductor YBa2Cu3O6+x |
| Q83376468 | Comment on "Bose-Einstein condensation of magnons in Cs(2)CuCl(4)" |
| Q80588079 | Cuprate Fermi orbits and Fermi arcs: the effect of short-range antiferromagnetic order |
| Q84721188 | Determining the in-plane Fermi surface topology in high T(c) superconductors using angle-dependent magnetic quantum oscillations |
| Q46208379 | Dimensional reduction at a quantum critical point |
| Q89766775 | Electronically driven collapse of the bulk modulus in δ-plutonium |
| Q45820314 | Exact mapping of the d(x(2)-y(2)) Cooper-pair wavefunction onto the spin fluctuations in cuprates: the Fermi surface as a driver for 'high T(c)' superconductivity |
| Q92129053 | Extent of Fermi-surface reconstruction in the high-temperature superconductor HgBa2CuO4+δ |
| Q79417297 | Fermi surface changes across the Néel phase boundary of NdB6 |
| Q54188775 | Fermi surface of CeIn3 above the Néel critical field. |
| Q62140585 | Fermi surface of CePt2In7: A two-dimensional analog of CeIn3 |
| Q53527106 | Formation of pancakelike Ising domains and giant magnetic coercivity in ferrimagnetic LuFe2O4. |
| Q37068532 | Fractalization drives crystalline states in a frustrated spin system. |
| Q80745359 | Geometric frustration and dimensional reduction at a quantum critical point |
| Q55059187 | Heavy fermions. Unconventional Fermi surface in an insulating state. |
| Q37194795 | Heavy holes as a precursor to superconductivity in antiferromagnetic CeIn3 |
| Q86026332 | High-magnetic-field lattice length changes in URu2Si2 |
| Q79941014 | Interplay between fermi surface topology and ordering in URu2Si2 revealed through abrupt hall coefficient changes in strong magnetic fields |
| Q83374087 | Irreversible dynamics of the phase boundary in U(Ru0.96Rh0.04)2Si2 and implications for ordering |
| Q33687514 | Magnetic field tuning of an excitonic insulator between the weak and strong coupling regimes in quantum limit graphite |
| Q62140520 | Magnetic field-tuned localization of the5f-electrons in URu2Si2 |
| Q87465212 | Manifestation of magnetic quantum fluctuations in the dielectric properties of a multiferroic |
| Q33778877 | Metal-insulator quantum critical point beneath the high Tc superconducting dome. |
| Q119796873 | Multiferroicity with coexisting isotropic and anisotropic spins in Ca 3 Co 2 − x Mn x O 6 |
| Q82632684 | Near doping-independent pocket area from an antinodal Fermi surface instability in underdoped high temperature superconductors |
| Q35679344 | Nodal bilayer-splitting controlled by spin-orbit interactions in underdoped high-Tc cuprates |
| Q79797980 | Nonlocal magnetic field-tuned quantum criticality in cubic CeIn(3-x)Sn(x) (x = 0.25) |
| Q55058333 | Normal-state nodal electronic structure in underdoped high-Tc copper oxides. |
| Q37320755 | Observation of a multiferroic critical end point. |
| Q79417573 | Phonon thermal transport of URu2Si2: broken translational symmetry and strong-coupling of the "hidden order" to the lattice |
| Q61068141 | Protected Nodal Electron Pocket from Multiple-QOrdering in Underdoped High Temperature Superconductors |
| Q87016424 | Pulsed field magnetization in rare-earth kagome systems |
| Q59781181 | Quantum Spin Correlations in an Organometallic Alternating-Sign Chain |
| Q80107004 | Quantum criticality in an organic magnet |
| Q87357815 | Quantum oscillations from nodal bilayer magnetic breakdown in the underdoped high temperature superconductor YBa2Cu3O(6+x) |
| Q62140664 | Quantum oscillations in antiferromagnetic CaFe2As2on the brink of superconductivity |
| Q80905892 | Quantum oscillations in the underdoped cuprate YBa2Cu4O8 |
| Q84054987 | Role of f electrons in the Fermi surface of the heavy fermion superconductor beta-YbAlB4 |
| Q62140597 | Sequential Spin Polarization of the Fermi Surface Pockets inURu2Si2and Its Implications for the Hidden Order |
| Q37128049 | Single reconstructed Fermi surface pocket in an underdoped single-layer cuprate superconductor. |
| Q84054721 | Spin-density wave fermi surface reconstruction in underdoped YBa2Cu3O6+x |
| Q83995628 | Spin-order driven Fermi surface reconstruction revealed by quantum oscillations in an underdoped high Tc superconductor |
| Q86428932 | Successive Magnetic-Field-Induced Transitions and Colossal Magnetoelectric Effect in Ni_{3}TeO_{6} |
| Q62140563 | Superconducting Pairs with Extreme Uniaxial Anisotropy inURu2Si2 |
| Q86999976 | Superconductivity. Quasiparticle mass enhancement approaching optimal doping in a high-T(c) superconductor |
| Q63366976 | Two-dimensionalXYbehavior observed in quasi-two-dimensional quantum Heisenberg antiferromagnets |
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