Spin-Orbit Coupling and Topological
Systems
Phase transitions in condensed matter physics generally have been identified
with an order parameter that spontaneously breaks the symmetry of the system and
develops long range order, such as for the magnetization that develops in a
ferromagnet below the Curie temperature or the staggered magnetization below the
Néel temperature in an antiferromagnet. With the discovery of
the Integer Quantum Hall Effect, and now for Topological Insulators (TI), the
traditional classification of quantum phases of matter has expanded. These
latter systems lack the concept of spontaneous symmetry breaking, rather
exhibiting topological order associated with the presence of nontrivial
topological components that lead to gapless boundary modes with chirality. One
of the essential properties of TI's is a strong spin-orbit interaction, which
interaction becomes larger the heavier the element. For the well-studied 3d
systems the spin-order interaction typically does not play an essential role,
which is one of the reasons attention in the condensed matter community has
turned to 4d, 5d, and 5f systems.
Further expansion of these new and fascinating systems now includes Topological
Semimetals. In the Weyl semimetal CeAlGe, Joe Checkelsky's group at M.I.T.
has discovered the particularly interesting phenomenon of Singular Angular
MagnetoResistance (SAMR). For a general explanation please see the news
item at
https://news.mit.edu/2019/approaching-magnetic-singularity-0620, while the
publication can be found at
Science
365, 377 (2019); (perspectivve
by Hassinger and Meng).
Half-Heusler Topological Insulators and Related
In the so-called Z2 two-dimensional and three-dimensional systems,
these topologically protected metallic states are of interest not only from a
fundamental point of view, but also because they have the technological
potential to transform spintronics and quantum computation applications. Even
more interesting are systems that exhibit both symmetry breaking order
parameters and topologically nontrivial states, which can give rise to exotic
collective modes and states. One such family is represented by the cubic
half-Heusler materials on which we have been collaborating. The
antiferromagnetism breaks time reversal and translational symmetries but
preserves the combination, leading to a new type of
system, the antiferromagnetic topological insulator.
Topological RPdBi
half-Heusler semimetals:
a new family of non-centrosymmetric magnetic
superconductors, Y. Nakajima, R. Hu, K. Kirshenbaum, A. Hughes, P.
Syers, X. Wang, K. Wang, R. Wang, S. Saha, D. Pratt, J.W. Lynn, and J.
Paglione,
Science
Advances 1, e1500242 (2015).
Large Anomalous Hall Effect in a Half
Heusler Antiferromagnet, T.
Suzuki, R. Chisnell, A. Devarakonda, Y.-T. Liu, J. W. Lynn, and J. G.
Checkelsky,
Nature Physics 12, 1119 (2016).
Press
Release.
Carrier Density Control of Magnetism and
Berry Phases in Doped EuTiO3, Kaveh Ahadi, Zhigang Gui,
Zach Porter, Jeffrey W. Lynn, Zhijun Xu, Stephen D. Wilson, Anderson
Janotti, and Susanne Stemmer,,
APL Materials 6,
056105 (2018).
Amplitude Mode in a Classical,
Two-dimensional Triangular Antiferromagnet,
Rebecca L. Dally, Yang Zhao, Zhijun Xu, Robin Chisnell,
Matthew Stone, Jeffrey W. Lynn,
Leon Balents,
and
Stephen D. Wilson,
Nature Communications 9, 2188 (2018).
Singular Angular Magnetoresistance and
Spontaneous Symmetry Breaking in a Magnetic Nodal Semimetal, T.
Suzuki, L. Savary, J.-P. Liu, J. W. Lynn, L. Balents, and J. G. Checkelsky,
Science
(2019).
Press Release.
5d
sytems; Iridates
Discovery of Topological Singularity Induced Kohn Anomaly in Weyl
Semimetal, Thanh Nguyen, Fei Han, Nina Andrejevic, Ricardo Pablo-Pedro,
Anuj Apte, Zhiwei Ding, Kunyan Zhang, Ahmet Alatas, Ercan Alp, Songxue Chi,
Jaime Fernandez-Baca, Masaaki Matsuda, David A. Tennant, Yang Zhao, Zhijun Xu,
Jeffrey W. Lynn, Shengxi Huang, and Mingda Li, (submitted),
arXiv:1906.00539.
Influence of Electron-doping on the Ground State of (Sr1-xLax)2IrO4,
Xiang Chen, Tom Hogan, D. Walkup, Wenwen Zhou, M. Pokharel, Mengliang Yao,
Wei Tian, Thomas Z. Ward, Y. Zhao, D. Parshall, C. Opeil, J. W. Lynn, Vidya
Madhavan, and Stephen D. Wilson,
Phys. Rev.
B
92, 017125 (2015).
Carrier Localization and Electronic Phase Separation in a doped Spin-Orbit Driven Mott Phase
in Sr3(Ir1-xRux)2O7, Chetan
Dhital, Tom Hogan, Wenwen Zhou, Xiang Chen, Zhensong Ren, Mani Pokharel,
Yoshinori Okada, M. Heine, Wei
Tian, Z. Yamani, C. Opeil, J. S. Helton, J. W. Lynn, Ziqiang Wang, Vidya
Madhavan, and Stephen D. Wilson,
Nature Communications 5, 3377
(2014).
Cd-doping effects in Ce2MIn8 (M=Rh and Ir) Heavy
Fermion Compounds, C. Adriano, C. Giles, E. M. Bitter, L. N. Coelho, F.
de Bergevin, C. Mazzoll, L. Paolasini, W. Ratcliff, R. Bindel, J. W. Lynn,
Z. Fisk, and P. G. Pagliuso,
Phys. Rev. B
81, 245115 (2010).
Novel Coexistence of Superconductivity with Two Distinct Magnetic Orders
in Heavy Fermion Ce(Rh,Ir)In5, A. D. Christianson, A. Llobet,
W. Bao, J. S. Gardner, I. P. Swainson, J. W. Lynn, J.-M. Mignot, K. Prokes,
P. G. Pagliuso, N. O. Moreno, J. L. Sarrao, and A. H. Lacerda,
Phys. Rev.
Lett. 95, 217002 (2005).
Covalency Effects in the Magnetic Form Factor of Ir in K2IrCl6,
J. W. Lynn, G. Shirane, and M. Blume,
Phys. Rev.
Lett. 37,
154 (1976).
4d
materials; Ruthenates
Phase Diagram of
a-RuCl3
in an in-plane Magnetic Field, J. A. Sears, Y. Zhao, Z. Xu, J. W.
Lynn, and Young-June Kim,
Phys. Rev.
B 95, 180411(R) (2017).
Spin Dynamics and Two-dimensional Correlations in an FCC
Antiferromagnetic Sr2YRuO6,
S. M. Disseler, J. W. Lynn, R. F. Jardim, M. S. Torikachvili, and E.
Granado,
Phys. Rev.
B 93, 140407(R) (2016).
Two-Dimensional Magnetic Correlations and Partial Long-Range Order in Geometrically Frustrated Sr2YRuO6,
E. Granado, J. W. Lynn, R. F. Jardim, and M. Torikachvili,
Phys. Rev.
Lett. 110,
017202 (2013).
Spin-valve
Effect and Magnetoresistivity in Single Crystalline Ca3Ru2O7,
W. Bao, Z. Q. Mao, Z. Qu, and J. W. Lynn,
Phys. Rev. Lett. 100,
247203 (2008).
Unusual heavy-mass nearly ferromagnetic state with a surprisingly large
Wilson ratio in double layered ruthenates (Sr1-xCax)3Ru2O7,
Z. Qu, L. Spinu, H. Q. Yuan, V. Dobrosavljeviuc, W. Bao, J. W. Lynn, M. Nicklas, J. Peng, T. J. Liu, D. Fobes, E. Flesch, and Z. Q. Mao,
Phys. Rev. B
78,
180407(R) (2008).
Structure and Magnetism of Single Crystal Sr4Ru3O10:
A Ferromagnetic Triple-Layer Ruthenate, M. K. Crawford, R. L.
Harlow, W. Marshall, Z. Li, G. Cao, R. L. Lindstrom, Q. Huang, and J. W. Lynn,
Phys. Rev. B 65, 214412 (2002).
Synthesis
and crystal structure of La3RuO7, P. Khalifah, Q.
Huang, J. W. Lynn, R. W. Erwin, and R. J. Cava,
Materials Research Bulletin
35, 1 (2000).
Oxygen
Displacements and Search for Magnetic Order in Sr3Ru2O7,
Q. Huang, J. W. Lynn, R. W. Erwin, J. Jarupatrakorn, and R. J. Cava, Phys.
Rev. B 58, 8515 (1998).
5f
materials; Hidden order in URu2Si2
High temperature singlet-based magnetism from Hund's rule
correlations, Lin Miao,
Rourav Basak, Sheng Ran,
Yishuai Xu, Haowei He, Jonathan D. Denlinger, Yi-De Chuang,
Y. Zhao, Z. Xu, J. W. Lynn, J. R. Jeffries, S. R. Saha, Ioannis
Giannakis, Pegor Aynajian, Chang-Jong Kang, Yilin Wang, Gabriel Kotliar,
Nicholas P. Butch, L. Andrew Wray, (submitted).
Distinct magnetic spectra in the hidden order and antiferromagnetic
phases in URu2-xFexSi2,
Nicholas P. Butch, Sheng Ran,
Inho Jeon, Noravee Kanchanavatee, Kevin Huang,
Alexander Breindel, M. Brian Maple, Ryan L. Stillwell, Yang Zhao, Leland
Harriger, and Jeffrey W. Lynn,
Phys. Rev.
B 94, 201102 (2016).
Chemical Pressure Tuning of URu2Si2
via Isoelectronic Substitution of Ru with Fe, Pinaki Das, N.
Kanchanavatee, J. S. Helton, K. Huang, R. E. Baumbach, E. D. Bauer, B. D.
White, V. W. Burnett, M. B. Maple, J.W. Lynn, and M. Janoschek,
Phys. Rev.
B
91, 085122 (2015).
Symmetry and Correlations Underlying Hidden Order in URu2Si2,
Nicholas P.
Butch, Michael E. Manley, Jason R. Jeffries, Marc Janoschek, Kevin Huang, M.
Brian Maple, Ayman H. Said, Bogdan M. Leu, and Jeffrey W. Lynn,
Phys. Rev.
B
91, 035128 (2015).
Absence of a static in-plane magnetic moment in the "hidden-order"
phase of URu2Si2,
P. Das, R. E. Baumbach, E. D. Bauer, K. Huang, M. B. Maple, Y. Zhao, J.
Helton, J. W. Lynn, and M. Janoschek,
New J. Phys.
15, 053031(2013).
Antiferromagnetic Critical Pressure in URu2Si2 under Hydrostatic Conditions,
N. P. Butch, J. R. Jeffries, S. X. Chi, J. B. Leão, and J. W. Lynn, and M.
B. Maple, Phys. Rev. B
82, 060408(R) (2010).
Non-Fermi
Liquid Behavior and Quantum Criticality in Sc1-xUxPd3
and URu2-xRexSi2, M. B.
Maple, N. P. Butch, E. D. Bauer, V. S. Zapf, P.-C. Ho, S. D. Wilson , P.
Dai, D. T. Adroja, S.-H. Lee, J.-H. Chung, J. W. Lynn,
Physica B
378-380, 911 (2006).
Spin Ice, Magnetic Monopoles, and Spin Liquids
Magnetic Monopoles are spin excitaitons in spin-ice, and as there is
no long range order these are also topoloigcal excitations of a kind:
Observation of Magnetic Monopoles in Spin Ice, Hiroaki Kadowaki,
Naohiro Doi, Yuji Aoki, Yoshikazu Tabata, Taku J. Sato, J. W. Lynn, K.
Matsuhira, and Z. Hiroi,
J. Phys. Soc. Japan 78,
103706 (2009).
Quantum Spin Fluctuations in the Spin Liquid State of Tb2Ti2O7,
Hiroshi Takatsu, Hiroaki Kadowaki, Taku J. Sato,
Jeffrey W. Lynn,
Yoshikazu Tabata,
Terno Yamakaki, and Kazuyuki Matsuhira,
J. Phys. Cond. Matr.
24, 052201 (2012).
Quadrupole Order in
the Frustrated Pyrochlore Tb2+xTi2−xO7+y,
H. Takatsu,
S. Onoda,
S. Kittaka, A. Kasahara, Y. Kono, T. Sakakibara, Y. Kato, B. Fåk, J. Ollivier, J. W. Lynn, T.
Taniguchi, M. Wakita, and H. Kadowaki,
Phys. Rev.
Lett. 116,
217201 (2016).
Spin correlations of quantum-spin-liquid and quadrupole-ordered
states of Tb2+xTi2-xO7+y,
Hiroaki Kadowaki, Mika Wakita, Björn Fåk, Jacques Ollivier, Seiko
Ohira-Kawamura, Kenji M Kofu-Nakajima, and Jeffrey W. Lynn,
Phys. Rev.
B
99, 014406 (2019).
See
Monopoles and
Related Systems
Recent Publications
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