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正交晶系电荷密度波存在于铕铝的四方晶格上。

Orthorhombic charge density wave on the tetragonal lattice of EuAl.

作者信息

Ramakrishnan Sitaram, Kotla Surya Rohith, Rekis Toms, Bao Jin-Ke, Eisele Claudio, Noohinejad Leila, Tolkiehn Martin, Paulmann Carsten, Singh Birender, Verma Rahul, Bag Biplab, Kulkarni Ruta, Thamizhavel Arumugam, Singh Bahadur, Ramakrishnan Srinivasan, van Smaalen Sander

机构信息

Laboratory of Crystallography, University of Bayreuth, 95447 Bayreuth, Germany.

Department of Quantum Matter, Hiroshima University, 739-8530, Higashi-Hiroshima, Japan.

出版信息

IUCrJ. 2022 Apr 29;9(Pt 3):378-385. doi: 10.1107/S2052252522003888. eCollection 2022 May 1.

DOI:10.1107/S2052252522003888
PMID:35546799
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC9067112/
Abstract

EuAl possesses the BaAl crystal structure type with tetragonal symmetry 4/. It undergoes a charge density wave (CDW) transition at  = 145 K and features four consecutive antiferromagnetic phase transitions below 16 K. Here we use single-crystal X-ray diffraction to determine the incommensurately modulated crystal structure of EuAl in its CDW state. The CDW is shown to be incommensurate with modulation wave vector  = (0,0,0.1781 (3)) at 70 K. The symmetry of the incommensurately modulated crystal structure is orthorhombic with superspace group (00σ)00, where is a subgroup of 4/ of index 2. Both the lattice and the atomic coordinates of the basic structure remain tetragonal. Symmetry breaking is entirely due to the modulation wave, where atoms Eu and Al1 have displacements exclusively along , while the fourfold rotation would require equal displacement amplitudes along and . The calculated band structure of the basic structure and interatomic distances in the modulated crystal structure both indicate the Al atoms as the location of the CDW. The tem-per-ature dependence of the specific heat reveals an anomaly at  = 145 K of a magnitude similar to canonical CDW systems. The present discovery of orthorhombic symmetry for the CDW state of EuAl leads to the suggestion of monoclinic instead of orthorhombic symmetry for the third AFM state.

摘要

铕铝具有四方对称4/的BaAl晶体结构类型。它在145 K时经历电荷密度波(CDW)转变,并在16 K以下呈现四个连续的反铁磁相变。在此,我们使用单晶X射线衍射来确定铕铝在其CDW状态下的非公度调制晶体结构。结果表明,在70 K时,CDW与调制波矢 = (0,0,0.1781 (3)) 非公度。非公度调制晶体结构的对称性为正交晶系,超空间群为(00σ)00,其中 是4/的指数为2的子群。基本结构的晶格和原子坐标均保持四方晶系。对称性破缺完全归因于调制波,其中铕原子和Al1原子仅沿 方向有位移,而四重旋转则需要沿 和 方向有相等的位移幅度。基本结构的计算能带结构和调制晶体结构中的原子间距离均表明Al原子是CDW的位置。比热的温度依赖性在145 K处显示出一个与典型CDW系统大小相似的异常。目前对铕铝CDW状态正交对称性的发现导致了对第三个反铁磁状态为单斜对称性而非正交对称性的推测。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/e0a18f2a4dc7/m-09-00378-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/af6aef2807af/m-09-00378-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/2fb664c14bd1/m-09-00378-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/59583c4199ae/m-09-00378-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/ed9008fbd800/m-09-00378-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/e0a18f2a4dc7/m-09-00378-fig5.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/af6aef2807af/m-09-00378-fig1.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/2fb664c14bd1/m-09-00378-fig2.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/59583c4199ae/m-09-00378-fig3.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/ed9008fbd800/m-09-00378-fig4.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/a512/9067112/e0a18f2a4dc7/m-09-00378-fig5.jpg

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