Abstract:Optical properties of nodal-line semimetal ZrSiS are studied using first-principles calculations. Frequency-independent optical conductivity is a fingerprint of the infrared optical response in ZrSiS. We find that this characteristic feature is robust with respect to external pressure of up to 10 GPa, yet with the flat region being narrowed with increasing pressure. Upon tensile stress of 2 GPa, the Fermi surface undergoes a topological transition accompanied by a weakening of the interband screening, which re… Show more
“…For both directions, σ 1 consists of a Drude term at low energies due to itinerant charge carriers. From the spectral weight analysis of the Drude contribution we obtain a plasma frequency ω p of 3.17 eV for E ab and 1.08 eV for E c, in agreement with the results of first-principles calculations [20]. The ratio of dc conductivities σ ab /σ c amounts to ∼16, which lies in between the values 8 and 30 given in Refs.…”
The anisotropic optical response of the layered, nodal-line semimetal ZrSiS at ambient and high pressure is investigated by frequency-dependent reflectivity measurements for the polarization along and perpendicular to the layers. The highly anisotropic optical conductivity is in very good agreement with results from density functional theory calculations and confirms the anisotropic character of ZrSiS. Whereas the in-plane optical conductivity shows only modest pressure-induced changes, we found strong effects on the out-of-plane optical conductivity spectrum of ZrSiS, with the appearance of two prominent excitations. These pronounced pressure-induced effects can neither be attributed to a structural phase transition according to our single-crystal x-ray diffraction measurements, nor can they be explained by electronic correlation and electron-hole pairing effects, as revealed by theoretical calculations. Our findings are discussed in the context of the recently proposed excitonic insulator phase in ZrSiS.
“…For both directions, σ 1 consists of a Drude term at low energies due to itinerant charge carriers. From the spectral weight analysis of the Drude contribution we obtain a plasma frequency ω p of 3.17 eV for E ab and 1.08 eV for E c, in agreement with the results of first-principles calculations [20]. The ratio of dc conductivities σ ab /σ c amounts to ∼16, which lies in between the values 8 and 30 given in Refs.…”
The anisotropic optical response of the layered, nodal-line semimetal ZrSiS at ambient and high pressure is investigated by frequency-dependent reflectivity measurements for the polarization along and perpendicular to the layers. The highly anisotropic optical conductivity is in very good agreement with results from density functional theory calculations and confirms the anisotropic character of ZrSiS. Whereas the in-plane optical conductivity shows only modest pressure-induced changes, we found strong effects on the out-of-plane optical conductivity spectrum of ZrSiS, with the appearance of two prominent excitations. These pronounced pressure-induced effects can neither be attributed to a structural phase transition according to our single-crystal x-ray diffraction measurements, nor can they be explained by electronic correlation and electron-hole pairing effects, as revealed by theoretical calculations. Our findings are discussed in the context of the recently proposed excitonic insulator phase in ZrSiS.
“…The sharp VHS adjacent to the protected nodal line implies that additional electronic features relying upon the enhanced g(E) could be engineered into this system [26][27][28][29][30], by tuning E F to the VHS. Tuning could be accomplished by chemical pressure [43], physical pressure or strain [16,44], and light activation [17] with the re-quired energy difference being quite small. This could be another avenue for switching the topological behavior for quantum computing applications.…”
Section: B Van Hove Singularity and Nodal Networkmentioning
We have applied nuclear magnetic resonance spectroscopy to study the distinctive network of nodal lines in the Dirac semimetal ZrSiTe. The low-T behavior is dominated by a symmetry-protected nodal line, with NMR providing a sensitive probe of the diamagnetic response of the associated carriers. A sharp low-T minimum in NMR shift and (T1T ) −1 provides a quantitative measure of the dispersionless, quasi-2D behavior of this nodal line. We also identify a van Hove singularity closely connected to this nodal line, and an associated T -induced Lifshitz transition. A disconnect in the NMR shift and line width at this temperature indicates the change in electronic behavior associated with this topological change. These features have an orientation-dependent behavior indicating a field-dependent scaling of the associated band energies.
“…The sharp VHS adjacent to the protected nodal line implies that additional electronic features relying upon the enhanced g(E ) could be engineered into this system [26][27][28][29][30], by tuning E F to the VHS. Tuning could be accomplished by chemical pressure [43], physical pressure or strain [16,44], and light activation [17] with the required energy difference being quite small. This could be another avenue for switching the topological behavior for quantum computing applications.…”
We have applied nuclear magnetic resonance spectroscopy to study the distinctive network of nodal lines in the Dirac semimetal ZrSiTe. The low-T behavior is dominated by a symmetry-protected nodal line, with NMR providing a sensitive probe of the diamagnetic response of the associated carriers. A sharp low-T minimum in the NMR shift and (T 1 T ) −1 provides a quantitative measure of the dispersionless, quasi-two-dimensional behavior of this nodal line. We also identify a Van Hove singularity closely connected to this nodal line, and an associated T -induced Lifshitz transition. A disconnect in the NMR shift and linewidth at this temperature indicates the change in electronic behavior associated with this topological change. These features have an orientation-dependent behavior indicating a field-dependent scaling of the associated band energies.
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