Magnetization Process of Atacamite: A Case of Weakly Coupled S=1/2 Sawtooth Chains.


Journal

Physical review letters
ISSN: 1079-7114
Titre abrégé: Phys Rev Lett
Pays: United States
ID NLM: 0401141

Informations de publication

Date de publication:
21 May 2021
Historique:
received: 19 04 2019
revised: 25 03 2021
accepted: 30 03 2021
entrez: 10 6 2021
pubmed: 11 6 2021
medline: 11 6 2021
Statut: ppublish

Résumé

We present a combined experimental and theoretical study of the mineral atacamite Cu_{2}Cl(OH)_{3}. Density-functional theory yields a Hamiltonian describing anisotropic sawtooth chains with weak 3D connections. Experimentally, we fully characterize the antiferromagnetically ordered state. Magnetic order shows a complex evolution with the magnetic field, while, starting at 31.5 T, we observe a plateaulike magnetization at about M_{sat}/2. Based on complementary theoretical approaches, we show that the latter is unrelated to the known magnetization plateau of a sawtooth chain. Instead, we provide evidence that the magnetization process in atacamite is a field-driven canting of a 3D network of weakly coupled sawtooth chains that form giant moments.

Identifiants

pubmed: 34110224
doi: 10.1103/PhysRevLett.126.207201
doi:

Types de publication

Journal Article

Langues

eng

Sous-ensembles de citation

IM

Pagination

207201

Auteurs

L Heinze (L)

Institut für Physik der Kondensierten Materie, Technische Universität Braunschweig, D-38106 Braunschweig, Germany.

H O Jeschke (HO)

Research Institute for Interdisciplinary Science, Okayama University, Okayama 700-8530, Japan.

I I Mazin (II)

Department of Physics and Astronomy, George Mason University, Fairfax, Virginia 22030, USA.
Quantum Science and Engineering Center, George Mason University, Fairfax, Virginia 22030, USA.

A Metavitsiadis (A)

Institut für Theoretische Physik, Technische Universität Braunschweig, D-38106 Braunschweig, Germany.

M Reehuis (M)

Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, D-14109 Berlin, Germany.

R Feyerherm (R)

Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, D-14109 Berlin, Germany.

J-U Hoffmann (JU)

Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, D-14109 Berlin, Germany.

M Bartkowiak (M)

Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, D-14109 Berlin, Germany.

O Prokhnenko (O)

Helmholtz-Zentrum Berlin für Materialien und Energie GmbH, D-14109 Berlin, Germany.

A U B Wolter (AUB)

Institute for Solid State and Materials Research, Leibniz IFW Dresden, D-01069 Dresden, Germany.

X Ding (X)

National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.

V S Zapf (VS)

National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.

C Corvalán Moya (C)

National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.
National Atomic Energy Commission (CNEA), Tres de Febrero University (UNTREF), National Scientific and Technical Research Council (CONICET), Argentina.

F Weickert (F)

National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.

M Jaime (M)

National High Magnetic Field Laboratory, Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA.

K C Rule (KC)

Australian Nuclear Science and Technology Organisation, Lucas Heights, New South Wales 2234, Australia.

D Menzel (D)

Institut für Physik der Kondensierten Materie, Technische Universität Braunschweig, D-38106 Braunschweig, Germany.

R Valentí (R)

Institut für Theoretische Physik, Goethe-Universität Frankfurt, D-60438 Frankfurt am Main, Germany.

W Brenig (W)

Institut für Theoretische Physik, Technische Universität Braunschweig, D-38106 Braunschweig, Germany.

S Süllow (S)

Institut für Physik der Kondensierten Materie, Technische Universität Braunschweig, D-38106 Braunschweig, Germany.

Classifications MeSH