Magnetic effects in the paraxial regime of elastic electron scattering

被引:14
作者
Edstrom, Alexander [1 ]
Lubk, Axel [2 ]
Rusz, Jan [1 ]
机构
[1] Uppsala Univ, Dept Phys & Astron, Box 516, S-75121 Uppsala, Sweden
[2] Tech Univ Dresden, Triebenberg Lab, Dresden, Germany
基金
瑞典研究理事会;
关键词
ORBITAL ANGULAR-MOMENTUM; RAY CIRCULAR-DICHROISM; VORTEX BEAMS; MICROSCOPE; CRYSTALS;
D O I
10.1103/PhysRevB.94.174414
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Motivated by a recent claim [Phys.Rev.Lett. 116, 127203 ( 2016)] that electron vortex beams can be used to image magnetism at the nanoscale in elastic scattering experiments, using transmission electron microscopy, a comprehensive computational study is performed to study magnetic effects in the paraxial regime of elastic electron scattering in magnetic solids. Magnetic interactions from electron vortex beams, spin polarized electron beams, and beams with phase aberrations are considered, as they pass through ferromagnetic FePt or antiferromagnetic LaMnAsO. The magnetic signals are obtained by comparing the intensity over a disk in the diffraction plane for beams with opposite angular momentum or aberrations. The strongest magnetic signals are obtained from vortex beams with large orbital angular momentum, where relative magnetic signals above 10(-3) are indicated for 10 (h) over bar orbital angular momentum, meaning that relative signals of one percent could be expected with the even larger orbital angular momenta, which have been produced in experimental setups. All results indicate that beams with low acceleration voltage and small convergence angles yield stronger magnetic signals, which is unfortunately problematic for the possibility of high spatial resolution imaging. Nevertheless, under atomic resolution conditions, relative magnetic signals in the order of 10(-4) are demonstrated, corresponding to an increase with one order of magnitude compared to previous work.
引用
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页数:17
相关论文
共 45 条
[1]  
[Anonymous], 2015, JAP, V115
[2]  
[Anonymous], 1999, CLASSICAL ELECTRODYN
[3]  
Beche A., ULTRAMICROSCOPY, DOI [10.1016/j.ultramic.2016.05.006, DOI 10.1016/J.ULTRAMIC.2016.05.006]
[4]  
Blaha P., 2001, Calculating Cryst. Prop., V60
[5]  
Brown E., 1969, SOLID STATE PHYS, V22, P313
[6]   Magnetic anisotropy of L10 FePt and Fe1-xMnxPt -: art. no. 134411 [J].
Burkert, T ;
Eriksson, O ;
Simak, SI ;
Ruban, AV ;
Sanyal, B ;
Nordström, L ;
Wills, JM .
PHYSICAL REVIEW B, 2005, 71 (13)
[7]   Computational comparison of the conventional multislice method and the real space multislice method for simulating exit wavefunctions [J].
Cai, Can Ying ;
Zeng, Song Jun ;
Liu, Hong Rong ;
Yang, Qi Bin .
MICRON, 2009, 40 (03) :313-319
[8]   X-RAY CIRCULAR-DICHROISM AND LOCAL MAGNETIC-FIELDS [J].
CARRA, P ;
THOLE, BT ;
ALTARELLI, M ;
WANG, XD .
PHYSICAL REVIEW LETTERS, 1993, 70 (05) :694-697
[9]   THE SCATTERING OF ELECTRONS BY ATOMS AND CRYSTALS .1. A NEW THEORETICAL APPROACH [J].
COWLEY, JM ;
MOODIE, AF .
ACTA CRYSTALLOGRAPHICA, 1957, 10 (10) :609-619
[10]  
Dyck D. V., 1980, J MICROSC-OXFORD, V119, P141