π–π Stacking, spin density and magnetic coupling strength

2013 ◽  
Vol 42 (44) ◽  
pp. 15559 ◽  
Author(s):  
Yan-Hui Chi ◽  
Jing-Min Shi ◽  
Hong-Nan Li ◽  
Wei Wei ◽  
Ethan Cottrill ◽  
...  
2005 ◽  
Vol 19 (15n17) ◽  
pp. 2538-2543 ◽  
Author(s):  
YI QUAN ZHANG ◽  
CHENG LIN LUO ◽  
ZHI YU

Magnetic coupling constants J for the complete structures of [ Gd(capro) 2( H 2 O )4 Cr(CN) 6]• H 2 O (capro represents caprolactam) (a) and trans-[ Fe(CN) 4(μ- CN )2 Gd ( H 2 O )4 (bpy) ]•4 H 2 O •1.5 bpy (b) have been calculated using hybrid density functional theory (DFT) B3LYP combined with a modified broken symmetry approach (BS). The calculated J value of -0.24 cm-1 for a is very close to the experimental -0.33 cm-1. They both show the antiferromagnetic interaction between Gd(III) and Cr(III) . For b, although the sign of the calculated J value of 4.24 cm-1 is different from that of the experimental -0.38 cm-1, the two values both show the weak magnetic coupling interaction between Gd(III) and Fe(III) . The spin density distributions are discussed on the basis of Mulliken population analysis. For complexes a and b, both transition metal ( Fe(III) or Cr(III) ) and rare earth Gd(III) display a spin polarization effect on the surrounding atoms, where a counteraction of the opposite polarization effects leads to a low spin density on the bridging ligand C1N1 . For the compounds Gd(III) - Cr(III) (a) and Gd(III) - Fe(III) (b) in the HS states, Cr(III) has stronger spin polarization influence on the bridging atoms than Fe(III) even causing the positive spin population on the bridging atom N1 .


2017 ◽  
Vol 19 (45) ◽  
pp. 30814-30821 ◽  
Author(s):  
Yeonsig Nam ◽  
Daeheum Cho ◽  
Jin Yong Lee

Reversible spin control of zigzag MoS2 nanoribbons by applying an electric field with enhancement of magnetic coupling strength.


2007 ◽  
Vol 76 (21) ◽  
Author(s):  
M. Bernien ◽  
X. Xu ◽  
J. Miguel ◽  
M. Piantek ◽  
Ph. Eckhold ◽  
...  

2015 ◽  
Vol 44 (16) ◽  
pp. 7437-7448 ◽  
Author(s):  
Yong Wang ◽  
Chensheng Lin ◽  
Xiao Ma ◽  
Zhenzhen Xue ◽  
Xiaoquan Zhu ◽  
...  

This work shows that for the investigated FeIII–NC–MII–CN–FeIII complexes the magnetic coupling strength between the distant FeIII ions increases with the diamagnetic cyanidometal bridge in the order of Fe < Ru < Os.


2008 ◽  
Vol 8 (12) ◽  
pp. 6593-6597
Author(s):  
J. M. Montejano-Carrizales ◽  
P. G. Alvarado-Leyva ◽  
E. M. Sosa-Hernandez

The magnetic properties of a pair V4 atomic clusters embedded in bulk Fe are determined by using a realistic spd-band Hubbard-like model. The spin density distribution is calculated self-consistenly in the unrestricted Hartree-Fock approximation. The local magnetic moments μ(i) are obtained at various atoms i of the cluster and of the surrounding Fe matrix. We consider two different geometrical arrangements for V clusters, collinear (C) and non-collinear (NC). In all the cases studied the magnetic coupling in the interface cluster-matrix is antiferromagnetic, and the ferromagnetic order of the matrix is not broken by the presence of the V atoms, although the local magnetic moments of Fe atoms at the interface cluster-matrix, are reduced respect to Fe bulk magnetization (2.22 μB) about 8%–20%. We compare the results with those of just one V4 atomic cluster embedded in bulk Fe.


2011 ◽  
Vol 987 (1-3) ◽  
pp. 138-143 ◽  
Author(s):  
Li Yu ◽  
Jing-Min Shi ◽  
Yi-Quan Zhang ◽  
Yu-Qing Wang ◽  
Ya-Nan Fan ◽  
...  

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