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Chikina A, Matic Vignjevic D. At the right time in the right place: How do luminal gradients position the microbiota along the gut? Cells Dev 2021; 168:203712. [PMID: 34174490 DOI: 10.1016/j.cdev.2021.203712] [Citation(s) in RCA: 8] [Impact Index Per Article: 2.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 04/18/2021] [Revised: 06/16/2021] [Accepted: 06/21/2021] [Indexed: 01/02/2023]
Abstract
The gastrointestinal system is highly compartmentalized, where individual segments perform separate tasks to achieve common physiological goals. The gut luminal content, chyme, changes its chemical and physical properties as it passes through different intestinal segments. Together, the chyme composition, mucus, pH and oxygen gradients along the gut create a variety of highly distinct ecological niches that form, maintain and reinforce the symbiosis with the particular microbiota. Hosting different microbiota members at specific locations creates one of the most complex and sophisticated gradient - gradient of the local ecosystems that live and interact with each other, providing advantages and challenges to the host and creating our microbial self. Here, we discuss how intestinal luminal gradients are created and maintained in homeostasis, their role in a correct microbiota positioning, and their change upon inflammation and cancer.
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Affiliation(s)
- Aleksandra Chikina
- Institut Curie, PSL Research University, CNRS UMR 144, F-75005 Paris, France.
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2
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Ma JZ, Nie SM, Yi CJ, Jandke J, Shang T, Yao MY, Naamneh M, Yan LQ, Sun Y, Chikina A, Strocov VN, Medarde M, Song M, Xiong YM, Xu G, Wulfhekel W, Mesot J, Reticcioli M, Franchini C, Mudry C, Müller M, Shi YG, Qian T, Ding H, Shi M. Spin fluctuation induced Weyl semimetal state in the paramagnetic phase of EuCd 2As 2. Sci Adv 2019; 5:eaaw4718. [PMID: 31309151 PMCID: PMC6625818 DOI: 10.1126/sciadv.aaw4718] [Citation(s) in RCA: 10] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/22/2018] [Accepted: 06/10/2019] [Indexed: 05/22/2023]
Abstract
Weyl fermions as emergent quasiparticles can arise in Weyl semimetals (WSMs) in which the energy bands are nondegenerate, resulting from inversion or time-reversal symmetry breaking. Nevertheless, experimental evidence for magnetically induced WSMs is scarce. Here, using photoemission spectroscopy, we observe that the degeneracy of Bloch bands is already lifted in the paramagnetic phase of EuCd2As2. We attribute this effect to the itinerant electrons experiencing quasi-static and quasi-long-range ferromagnetic fluctuations. Moreover, the spin-nondegenerate band structure harbors a pair of ideal Weyl nodes near the Fermi level. Hence, we show that long-range magnetic order and the spontaneous breaking of time-reversal symmetry are not essential requirements for WSM states in centrosymmetric systems and that WSM states can emerge in a wider range of condensed matter systems than previously thought.
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Affiliation(s)
- J.-Z. Ma
- Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
- Institute of Condensed Matter Physics, École Polytechnique Fédérale de Lausanne, CH-10 15 Lausanne, Switzerland
| | - S. M. Nie
- Department of Materials Science and Engineering, Stanford University, Stanford, CA 94305, USA
| | - C. J. Yi
- Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
- School of Physics, University of Chinese Academy of Sciences, Beijing 100190, China
| | - J. Jandke
- Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - T. Shang
- Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
- Institute of Condensed Matter Physics, École Polytechnique Fédérale de Lausanne, CH-10 15 Lausanne, Switzerland
- Laboratory for Multiscale Materials Experiments, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - M. Y. Yao
- Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - M. Naamneh
- Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - L. Q. Yan
- Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
| | - Y. Sun
- Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
- School of Physics, University of Chinese Academy of Sciences, Beijing 100190, China
- Songshan Lake Materials Laboratory, Dongguan, Guangdong 523808, China
| | - A. Chikina
- Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - V. N. Strocov
- Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - M. Medarde
- Laboratory for Multiscale Materials Experiments, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - M. Song
- Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei, Anhui 230031, China
- University of Science and Technology of China, Hefei, Anhui 230026, China
| | - Y.-M. Xiong
- Anhui Province Key Laboratory of Condensed Matter Physics at Extreme Conditions, High Magnetic Field Laboratory, Chinese Academy of Sciences, Hefei, Anhui 230031, China
- Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China
| | - G. Xu
- Wuhan National High Magnetic Field Center and School of Physics, Huazhong University of Science and Technology, Wuhan 430074, China
| | - W. Wulfhekel
- Physikalisches Institut, Karlsruhe Institute of Technology, 76131 Karlsruhe, Germany
| | - J. Mesot
- Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
- Institute of Condensed Matter Physics, École Polytechnique Fédérale de Lausanne, CH-10 15 Lausanne, Switzerland
- Laboratory for Solid State Physics, ETH Zürich, CH-8093 Zürich, Switzerland
| | - M. Reticcioli
- Faculty of Physics, Center for Computational Materials Science, University of Vienna, A-1090 Vienna, Austria
| | - C. Franchini
- Faculty of Physics, Center for Computational Materials Science, University of Vienna, A-1090 Vienna, Austria
- Dipartimento di Fisica e Astronomia, Università di Bologna, 40127 Bologna, Italy
| | - C. Mudry
- Condensed Matter Theory Group, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
- Institute of Physics, Ecole Polytechnique Federale de Lausanne, CH1015 Lausanne, Switzerland
| | - M. Müller
- Condensed Matter Theory Group, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
| | - Y. G. Shi
- Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
- Songshan Lake Materials Laboratory, Dongguan, Guangdong 523808, China
| | - T. Qian
- Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
- Songshan Lake Materials Laboratory, Dongguan, Guangdong 523808, China
- CAS Center for Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences, Beijing 100190, China
| | - H. Ding
- Beijing National Laboratory for Condensed Matter Physics and Institute of Physics, Chinese Academy of Sciences, Beijing 100190, China
- School of Physics, University of Chinese Academy of Sciences, Beijing 100190, China
- Songshan Lake Materials Laboratory, Dongguan, Guangdong 523808, China
- CAS Center for Excellence in Topological Quantum Computation, University of Chinese Academy of Sciences, Beijing 100190, China
| | - M. Shi
- Swiss Light Source, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
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3
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Güttler M, Generalov A, Fujimori SI, Kummer K, Chikina A, Seiro S, Danzenbächer S, Koroteev YM, Chulkov EV, Radovic M, Shi M, Plumb NC, Laubschat C, Allen JW, Krellner C, Geibel C, Vyalikh DV. Divalent EuRh 2Si 2 as a reference for the Luttinger theorem and antiferromagnetism in trivalent heavy-fermion YbRh 2Si 2. Nat Commun 2019; 10:796. [PMID: 30770811 PMCID: PMC6377675 DOI: 10.1038/s41467-019-08688-y] [Citation(s) in RCA: 9] [Impact Index Per Article: 1.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 06/28/2018] [Accepted: 01/25/2019] [Indexed: 11/08/2022] Open
Abstract
Application of the Luttinger theorem to the Kondo lattice YbRh2Si2 suggests that its large 4f-derived Fermi surface (FS) in the paramagnetic (PM) regime should be similar in shape and volume to that of the divalent local-moment antiferromagnet (AFM) EuRh2Si2 in its PM regime. Here we show by angle-resolved photoemission spectroscopy that paramagnetic EuRh2Si2 has a large FS essentially similar to the one seen in YbRh2Si2 down to 1 K. In EuRh2Si2 the onset of AFM order below 24.5 K induces an extensive fragmentation of the FS due to Brillouin zone folding, intersection and resulting hybridization of the Fermi-surface sheets. Our results on EuRh2Si2 indicate that the formation of the AFM state in YbRh2Si2 is very likely also connected with similar changes in the FS, which have to be taken into account in the controversial analysis and discussion of anomalies observed at the quantum critical point in this system.
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Affiliation(s)
- M Güttler
- Institut für Festkörper- und Materialphysik, Technische Universität Dresden, D-01062, Dresden, Germany
| | - A Generalov
- MAX IV Laboratory, Lund University, Box 118, 22100, Lund, Sweden
| | - S I Fujimori
- Materials Sciences Research Center, Japan Atomic Energy Agency, Sayo, Hyogo, 679-5148, Japan
| | - K Kummer
- European Synchrotron Radiation Facility, 71 Avenue des Martyrs, 38043 Grenoble, France
| | - A Chikina
- Swiss Light Source and Swiss FEL, Paul Scherrer Institute, CH-5232, Villigen-PSI, Switzerland
| | - S Seiro
- IFW Dresden, Helmholtzstr. 20, 01069, Dresden, Germany
- Max-Planck-Institut für Chemische Physik fester Stoffe, 01187, Dresden, Germany
| | - S Danzenbächer
- Institut für Festkörper- und Materialphysik, Technische Universität Dresden, D-01062, Dresden, Germany
| | - Yu M Koroteev
- Tomsk State University, Lenina Av., 36, Tomsk, Russia, 634050
- Institute of Strength Physics and Materials Science, RAS, Tomsk, Russia, 634055
| | - E V Chulkov
- Tomsk State University, Lenina Av., 36, Tomsk, Russia, 634050
- Centro de Física de Materiales CFM-MPC and Centro Mixto CSIC-UPV/EHU, 20018, San Sebastián/Donostia, Spain
- Donostia International Physics Center (DIPC), 20080, San Sebastian, Spain
- Saint Petersburg State University, Saint Petersburg, Russia, 198504
| | - M Radovic
- Swiss Light Source and Swiss FEL, Paul Scherrer Institute, CH-5232, Villigen-PSI, Switzerland
| | - M Shi
- Swiss Light Source and Swiss FEL, Paul Scherrer Institute, CH-5232, Villigen-PSI, Switzerland
| | - N C Plumb
- Swiss Light Source and Swiss FEL, Paul Scherrer Institute, CH-5232, Villigen-PSI, Switzerland
| | - C Laubschat
- Institut für Festkörper- und Materialphysik, Technische Universität Dresden, D-01062, Dresden, Germany
| | - J W Allen
- Randall Laboratory, University of Michigan, 450 Church St, Ann Arbor, MI, 48109-1040, USA
| | - C Krellner
- Kristall- und Materiallabor, Physikalisches Institut, Goethe-Universität Frankfurt, Max-von-Laue Strasse 1, 60438, Frankfurt am Main, Germany
| | - C Geibel
- Max-Planck-Institut für Chemische Physik fester Stoffe, 01187, Dresden, Germany
| | - D V Vyalikh
- Donostia International Physics Center (DIPC), 20080, San Sebastian, Spain.
- IKERBASQUE, Basque Foundation for Science, 48011, Bilbao, Spain.
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4
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Horio M, Hauser K, Sassa Y, Mingazheva Z, Sutter D, Kramer K, Cook A, Nocerino E, Forslund OK, Tjernberg O, Kobayashi M, Chikina A, Schröter NBM, Krieger JA, Schmitt T, Strocov VN, Pyon S, Takayama T, Takagi H, Lipscombe OJ, Hayden SM, Ishikado M, Eisaki H, Neupert T, Månsson M, Matt CE, Chang J. Three-Dimensional Fermi Surface of Overdoped La-Based Cuprates. Phys Rev Lett 2018; 121:077004. [PMID: 30169083 DOI: 10.1103/physrevlett.121.077004] [Citation(s) in RCA: 4] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/12/2018] [Indexed: 06/08/2023]
Abstract
We present a soft x-ray angle-resolved photoemission spectroscopy study of overdoped high-temperature superconductors. In-plane and out-of-plane components of the Fermi surface are mapped by varying the photoemission angle and the incident photon energy. No k_{z} dispersion is observed along the nodal direction, whereas a significant antinodal k_{z} dispersion is identified for La-based cuprates. Based on a tight-binding parametrization, we discuss the implications for the density of states near the van Hove singularity. Our results suggest that the large electronic specific heat found in overdoped La_{2-x}Sr_{x}CuO_{4} cannot be assigned to the van Hove singularity alone. We therefore propose quantum criticality induced by a collapsing pseudogap phase as a plausible explanation for observed enhancement of electronic specific heat.
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Affiliation(s)
- M Horio
- Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
| | - K Hauser
- Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
| | - Y Sassa
- Department of Physics and Astronomy, Uppsala University, SE-75121 Uppsala, Sweden
| | - Z Mingazheva
- Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
| | - D Sutter
- Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
| | - K Kramer
- Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
| | - A Cook
- Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
| | - E Nocerino
- Department of Applied Physics, KTH Royal Institute of Technology, Electrum 229, SE-16440 Stockholm Kista, Sweden
| | - O K Forslund
- Department of Applied Physics, KTH Royal Institute of Technology, Electrum 229, SE-16440 Stockholm Kista, Sweden
| | - O Tjernberg
- Department of Applied Physics, KTH Royal Institute of Technology, Electrum 229, SE-16440 Stockholm Kista, Sweden
| | - M Kobayashi
- Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
| | - A Chikina
- Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
| | - N B M Schröter
- Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
| | - J A Krieger
- Laboratory for Muon Spin Spectroscopy, Paul Scherrer Institute, CH-5232 Villigen PSI, Switzerland
- Laboratorium für Festkörperphysik, ETH Zürich, CH-8093 Zürich, Switzerland
| | - T Schmitt
- Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
| | - V N Strocov
- Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
| | - S Pyon
- Department of Advanced Materials, University of Tokyo, Kashiwa 277-8561, Japan
| | - T Takayama
- Department of Advanced Materials, University of Tokyo, Kashiwa 277-8561, Japan
| | - H Takagi
- Department of Advanced Materials, University of Tokyo, Kashiwa 277-8561, Japan
| | - O J Lipscombe
- H. H. Wills Physics Laboratory, University of Bristol, Bristol BS8 1TL, United Kingdom
| | - S M Hayden
- H. H. Wills Physics Laboratory, University of Bristol, Bristol BS8 1TL, United Kingdom
| | - M Ishikado
- Comprehensive Research Organization for Science and Society (CROSS), Tokai, Ibaraki 319-1106, Japan
| | - H Eisaki
- Electronics and Photonics Research Institute, National Institute of Advanced Industrial Science and Technology, Ibaraki 305-8568, Japan
| | - T Neupert
- Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
| | - M Månsson
- Department of Applied Physics, KTH Royal Institute of Technology, Electrum 229, SE-16440 Stockholm Kista, Sweden
| | - C E Matt
- Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
- Swiss Light Source, Paul Scherrer Institut, CH-5232 Villigen PSI, Switzerland
- Department of Physics, Harvard University, Cambridge, MA 02138, USA
| | - J Chang
- Physik-Institut, Universität Zürich, Winterthurerstrasse 190, CH-8057 Zürich, Switzerland
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5
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Yamada A, Renault R, Chikina A, Venzac B, Pereiro I, Coscoy S, Verhulsel M, Parrini MC, Villard C, Viovy JL, Descroix S. Transient microfluidic compartmentalization using actionable microfilaments for biochemical assays, cell culture and organs-on-chip. Lab Chip 2016; 16:4691-4701. [PMID: 27797384 DOI: 10.1039/c6lc01143h] [Citation(s) in RCA: 11] [Impact Index Per Article: 1.4] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/24/2023]
Abstract
We report here a simple yet robust transient compartmentalization system for microfluidic platforms. Cylindrical microfilaments made of commercially available fishing lines are embedded in a microfluidic chamber and employed as removable walls, dividing the chamber into several compartments. These partitions allow tight sealing for hours, and can be removed at any time by longitudinal sliding with minimal hydrodynamic perturbation. This allows the easy implementation of various functions, previously impossible or requiring more complex instrumentation. In this study, we demonstrate the applications of our strategy, firstly to trigger chemical diffusion, then to make surface co-coating or cell co-culture on a two-dimensional substrate, and finally to form multiple cell-laden hydrogel compartments for three-dimensional cell co-culture in a microfluidic device. This technology provides easy and low-cost solutions, without the use of pneumatic valves or external equipment, for constructing well-controlled microenvironments for biochemical and cellular assays.
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Affiliation(s)
- Ayako Yamada
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France and Institut Pierre-Gilles de Gennes, 75005, Paris, France
| | - Renaud Renault
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France and Institut Pierre-Gilles de Gennes, 75005, Paris, France
| | - Aleksandra Chikina
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France and Institut Pierre-Gilles de Gennes, 75005, Paris, France
| | - Bastien Venzac
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France and Institut Pierre-Gilles de Gennes, 75005, Paris, France
| | - Iago Pereiro
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France and Institut Pierre-Gilles de Gennes, 75005, Paris, France
| | - Sylvie Coscoy
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France
| | - Marine Verhulsel
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France and Institut Pierre-Gilles de Gennes, 75005, Paris, France
| | - Maria Carla Parrini
- Institut Curie, Centre de Recherche, PSL Research University, 75005, Paris, France and ART group, Inserm U830, 75248 Paris, France
| | - Catherine Villard
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France and Institut Pierre-Gilles de Gennes, 75005, Paris, France
| | - Jean-Louis Viovy
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France and Institut Pierre-Gilles de Gennes, 75005, Paris, France
| | - Stéphanie Descroix
- Laboratoire Physico Chimie Curie, Institut Curie, PSL Research University, CNRS UMR168, 75005, Paris, France. and Sorbonne Universités, UPMC Univ Paris 06, 75005, Paris, France and Institut Pierre-Gilles de Gennes, 75005, Paris, France
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6
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7
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Gofryk K, Saparov B, Durakiewicz T, Chikina A, Danzenbächer S, Vyalikh DV, Graf MJ, Sefat AS. Fermi-surface reconstruction and complex phase equilibria in CaFe2As2. Phys Rev Lett 2014; 112:186401. [PMID: 24856707 DOI: 10.1103/physrevlett.112.186401] [Citation(s) in RCA: 7] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/19/2013] [Indexed: 06/03/2023]
Abstract
Fermi-surface topology governs the relationship between magnetism and superconductivity in iron-based materials. Using low-temperature transport, angle-resolved photoemission, and x-ray diffraction, we show unambiguous evidence of large Fermi-surface reconstruction in CaFe2As2 at magnetic spin-density-wave and nonmagnetic collapsed-tetragonal (cT) transitions. For the cT transition, the change in the Fermi-surface topology has a different character with no contribution from the hole part of the Fermi surface. In addition, the results suggest that the pressure effect in CaFe2As2 is mainly leading to a rigid-band-like change of the valence electronic structure. We discuss these results and their implications for magnetism and superconductivity in this material.
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Affiliation(s)
- K Gofryk
- Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
| | - B Saparov
- Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
| | - T Durakiewicz
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - A Chikina
- Department of Physics, St. Petersburg State University, St. Petersburg 198504, Russia and Institute of Solid State Physics, Dresden University of Technology, Zellescher Weg 16, D-01062 Dresden, Germany
| | - S Danzenbächer
- Institute of Solid State Physics, Dresden University of Technology, Zellescher Weg 16, D-01062 Dresden, Germany
| | - D V Vyalikh
- Department of Physics, St. Petersburg State University, St. Petersburg 198504, Russia and Institute of Solid State Physics, Dresden University of Technology, Zellescher Weg 16, D-01062 Dresden, Germany
| | - M J Graf
- Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
| | - A S Sefat
- Oak Ridge National Laboratory, Oak Ridge, Tennessee 37831, USA
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8
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Höppner M, Seiro S, Chikina A, Fedorov A, Güttler M, Danzenbächer S, Generalov A, Kummer K, Patil S, Molodtsov SL, Kucherenko Y, Geibel C, Strocov VN, Shi M, Radovic M, Schmitt T, Laubschat C, Vyalikh DV. Interplay of Dirac fermions and heavy quasiparticles in solids. Nat Commun 2013; 4:1646. [PMID: 23552061 DOI: 10.1038/ncomms2654] [Citation(s) in RCA: 24] [Impact Index Per Article: 2.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 12/20/2012] [Accepted: 02/26/2013] [Indexed: 11/09/2022] Open
Abstract
Many-body interactions in crystalline solids can be conveniently described in terms of quasiparticles with strongly renormalized masses as compared with those of non-interacting particles. Examples of extreme mass renormalization are on the one hand graphene, where the charge carriers obey the linear dispersion relation of massless Dirac fermions, and on the other hand heavy-fermion materials where the effective electron mass approaches the mass of a proton. Here we show that both extremes, Dirac fermions, like they are found in graphene and extremely heavy quasiparticles characteristic for Kondo materials, may not only coexist in a solid but can also undergo strong mutual interactions. Using the example of EuRh₂Si₂, we explicitly demonstrate that these interactions can take place at the surface and in the bulk. The presence of the linear dispersion is imposed solely by the crystal symmetry, whereas the existence of heavy quasiparticles is caused by the localized nature of the 4f states.
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Affiliation(s)
- M Höppner
- Max Planck Institute for Solid State Research, Heisenbergstrasse 1, D-70569 Stuttgart, Germany
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