Origin of the non-Fermi-liquid behavior in CeRh2As2 Article Swipe
P. Khanenko
,
D. Hafner
,
Konstantin Semeniuk
,
Jacintha Banda
,
T. Luehmann
,
F. Baertl
,
Tommy Kotte
,
J. Wosnitza
,
Gertrud Zwicknagl
,
C. Geibel
,
J. F. Landaeta
,
Seunghyun Khim
,
Elena Hassinger
,
M. Brando
·
YOU?
·
· 2024
· Open Access
·
· DOI: https://doi.org/10.48550/arxiv.2409.11894
YOU?
·
· 2024
· Open Access
·
· DOI: https://doi.org/10.48550/arxiv.2409.11894
Unconventional superconductivity in heavy-fermion systems appears often near magnetic quantum critical points (QCPs). This seems to be the case also for CeRh2As2 (Tc $\approx$ 0.31 K). CeRh2As2 shows two superconducting (SC) phases, SC1 and SC2, for a magnetic field along the c axis of the tetragonal unit cell, but only the SC1 phase is observed for a field along the basal plane. Furthermore, another ordered state (phase-I) is observed below T0 $\approx$ 0.48 K whose nature is still unclear: Thermodynamic and magnetic measurements pointed to a non magnetic multipolar state, but recent $μ$SR and NQR/NMR experiments have clearly detected antiferromagnetic (AFM) order below T0 . Also, quasi-two-dimensional AFM fluctuations were observed in NMR and neutron-scattering experiments above T0. The proximity of a QCP is indicated by non-Fermi-liquid (NFL) behavior observed above the ordered states in both specific heat $C(T)/T \propto T^{-0.6}$ and resistivity $ρ(T) \propto T^{0.5}$. These T-dependencies are not compatible with any generic AFM QCP. Because of the strong magnetic-field anisotropy of both the SC phase and phase I, it is possible to study a field-induced SC QCP as well a phase-I QCP by varying the angle $α$ between the field and the c axis. Thus, by examining the behavior of the electronic specific-heat coefficient C(T)/T across these QCPs, we can determine which phase is associated with the NFL behavior. Here, we present low-temperature specific-heat measurements taken in a magnetic field as high as 21 T applied at several angles $α$. We observe that the NFL behavior does very weakly depend on the field and on the angle $α$, a result that is at odd with that observations in standard magnetic QCPs. This suggests a nonmagnetic origin of the quantum critical fluctuations.
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- Type
- preprint
- Language
- en
- Landing Page
- http://arxiv.org/abs/2409.11894
- https://arxiv.org/pdf/2409.11894
- OA Status
- green
- Related Works
- 10
- OpenAlex ID
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https://openalex.org/W4403746450Canonical identifier for this work in OpenAlex
- DOI
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https://doi.org/10.48550/arxiv.2409.11894Digital Object Identifier
- Title
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Origin of the non-Fermi-liquid behavior in CeRh2As2Work title
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preprintOpenAlex work type
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enPrimary language
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2024Year of publication
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2024-09-18Full publication date if available
- Authors
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P. Khanenko, D. Hafner, Konstantin Semeniuk, Jacintha Banda, T. Luehmann, F. Baertl, Tommy Kotte, J. Wosnitza, Gertrud Zwicknagl, C. Geibel, J. F. Landaeta, Seunghyun Khim, Elena Hassinger, M. BrandoList of authors in order
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https://arxiv.org/abs/2409.11894Publisher landing page
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https://arxiv.org/pdf/2409.11894Direct link to full text PDF
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YesWhether a free full text is available
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greenOpen access status per OpenAlex
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https://arxiv.org/pdf/2409.11894Direct OA link when available
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Fermi liquid theory, Fermi Gamma-ray Space Telescope, Physics, Condensed matter physics, SuperconductivityTop concepts (fields/topics) attached by OpenAlex
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0Total citation count in OpenAlex
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10Other works algorithmically related by OpenAlex
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| abstract_inverted_index.depend | 251 |
| abstract_inverted_index.nature | 75 |
| abstract_inverted_index.origin | 277 |
| abstract_inverted_index.plane. | 61 |
| abstract_inverted_index.points | 11 |
| abstract_inverted_index.recent | 91 |
| abstract_inverted_index.result | 261 |
| abstract_inverted_index.state, | 89 |
| abstract_inverted_index.states | 133 |
| abstract_inverted_index.strong | 159 |
| abstract_inverted_index.weakly | 250 |
| abstract_inverted_index.$C(T)/T | 138 |
| abstract_inverted_index.(QCPs). | 12 |
| abstract_inverted_index.Because | 156 |
| abstract_inverted_index.NQR/NMR | 94 |
| abstract_inverted_index.\propto | 139, 144 |
| abstract_inverted_index.another | 63 |
| abstract_inverted_index.appears | 5 |
| abstract_inverted_index.applied | 237 |
| abstract_inverted_index.between | 189 |
| abstract_inverted_index.clearly | 97 |
| abstract_inverted_index.generic | 153 |
| abstract_inverted_index.observe | 243 |
| abstract_inverted_index.ordered | 64, 132 |
| abstract_inverted_index.phase-I | 182 |
| abstract_inverted_index.phases, | 31 |
| abstract_inverted_index.pointed | 83 |
| abstract_inverted_index.present | 223 |
| abstract_inverted_index.quantum | 9, 280 |
| abstract_inverted_index.several | 239 |
| abstract_inverted_index.systems | 4 |
| abstract_inverted_index.varying | 185 |
| abstract_inverted_index.CeRh2As2 | 21, 26 |
| abstract_inverted_index.behavior | 128, 200, 247 |
| abstract_inverted_index.critical | 10, 281 |
| abstract_inverted_index.detected | 98 |
| abstract_inverted_index.magnetic | 8, 37, 81, 87, 230, 271 |
| abstract_inverted_index.observed | 54, 68, 110, 129 |
| abstract_inverted_index.possible | 172 |
| abstract_inverted_index.specific | 136 |
| abstract_inverted_index.standard | 270 |
| abstract_inverted_index.suggests | 274 |
| abstract_inverted_index.unclear: | 78 |
| abstract_inverted_index.$\approx$ | 23, 71 |
| abstract_inverted_index.(phase-I) | 66 |
| abstract_inverted_index.T^{-0.6}$ | 140 |
| abstract_inverted_index.T^{0.5}$. | 145 |
| abstract_inverted_index.behavior. | 220 |
| abstract_inverted_index.determine | 212 |
| abstract_inverted_index.examining | 198 |
| abstract_inverted_index.indicated | 124 |
| abstract_inverted_index.proximity | 119 |
| abstract_inverted_index.anisotropy | 161 |
| abstract_inverted_index.associated | 216 |
| abstract_inverted_index.compatible | 150 |
| abstract_inverted_index.electronic | 203 |
| abstract_inverted_index.multipolar | 88 |
| abstract_inverted_index.tetragonal | 45 |
| abstract_inverted_index.coefficient | 205 |
| abstract_inverted_index.experiments | 95, 115 |
| abstract_inverted_index.nonmagnetic | 276 |
| abstract_inverted_index.resistivity | 142 |
| abstract_inverted_index.Furthermore, | 62 |
| abstract_inverted_index.fluctuations | 108 |
| abstract_inverted_index.measurements | 82, 226 |
| abstract_inverted_index.observations | 268 |
| abstract_inverted_index.Thermodynamic | 79 |
| abstract_inverted_index.field-induced | 176 |
| abstract_inverted_index.fluctuations. | 282 |
| abstract_inverted_index.heavy-fermion | 3 |
| abstract_inverted_index.specific-heat | 204, 225 |
| abstract_inverted_index.T-dependencies | 147 |
| abstract_inverted_index.Unconventional | 0 |
| abstract_inverted_index.magnetic-field | 160 |
| abstract_inverted_index.low-temperature | 224 |
| abstract_inverted_index.superconducting | 29 |
| abstract_inverted_index.non-Fermi-liquid | 126 |
| abstract_inverted_index.antiferromagnetic | 99 |
| abstract_inverted_index.superconductivity | 1 |
| abstract_inverted_index.neutron-scattering | 114 |
| abstract_inverted_index.quasi-two-dimensional | 106 |
| cited_by_percentile_year | |
| countries_distinct_count | 0 |
| institutions_distinct_count | 14 |
| citation_normalized_percentile.value | 0.16442142 |
| citation_normalized_percentile.is_in_top_1_percent | False |
| citation_normalized_percentile.is_in_top_10_percent | False |