2016
DOI: 10.1103/physrevb.94.224426
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Magnetic anisotropy in surface-supported single-ion lanthanide complexes

Abstract: Single-ion lanthanide-organic complexes can provide stable magnetic moments with well-defined orientation for spintronic applications on the atomic level. Here, we show by a combined experimental approach of scanning tunneling microscopy and X-ray absorption spectroscopy that dysprosium--tris(1,1,1-trifluoro-4-(2-thienyl)-2,4butanedionate) (Dy(tta)3) complexes deposited on a Au(111) surface undergo a molecular distortion, resulting in distinct crystal field symmetry imposed on the Dy ion. This leads to an easy… Show more

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Cited by 11 publications
(13 citation statements)
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“…The inverted orientation indicates that for Dy‐TDA networks the effective CF acting on the Dy atoms does not follow the coordination symmetry axis. A further comparison with Dy 3+ ions in the dysprosium‐tris(1,1,1‐trifluoro‐4‐(2‐thienyl)‐2,4‐butanedionate) (Dy(tta) 3 ) complex on Au(111) [ 10 ] also confirms that the alignment of the Dy 4f orbitals in the Dy‐TDA network is close to the surface plane (see the Experimental Section for more details).…”
Section: Resultsmentioning
confidence: 79%
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“…The inverted orientation indicates that for Dy‐TDA networks the effective CF acting on the Dy atoms does not follow the coordination symmetry axis. A further comparison with Dy 3+ ions in the dysprosium‐tris(1,1,1‐trifluoro‐4‐(2‐thienyl)‐2,4‐butanedionate) (Dy(tta) 3 ) complex on Au(111) [ 10 ] also confirms that the alignment of the Dy 4f orbitals in the Dy‐TDA network is close to the surface plane (see the Experimental Section for more details).…”
Section: Resultsmentioning
confidence: 79%
“…On the other side, in the work of Stoll et al. [ 10 ] it is defined as (μ25°μ90°); considering that μ θ = [cos (θ)] 2 ·μ V + [sin (θ)] 2 ·μ H (see supplementary note 6 of ref. [ 44 ] ), this implies that (μ25°μ90°)= 0.18 · (μHμV).…”
Section: Methodsmentioning
confidence: 99%
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“…In magnetic systems with easy-axis magnetic anisotropy, two magnetic states with opposite magnetic moments are separated by an energy barrier and may have long magnetic relaxation times. , For the ultimate goal to realize high-density data storage and quantum computation using single atoms or molecules, there is an ongoing pursuit of single magnetic atoms and molecules with large easy-axis magnetic anisotropy. For most magnetic atoms adsorbed on metal substrates, their magnetic moments are easily screened or even quenched by itinerant electrons, , while only rare cases show magnetic anisotropy energy of no more than 10 meV on Pt(111) surface. To achieve large magnetic anisotropy, an insulating layer was used to decouple the magnetic atoms from metal substrates, whereas this strategy requires the system to be prepared and kept at low temperature. , In organometallic complexes, the molecular ligands provide an alternative way to decouple magnetic atoms from metal substrates. , Moreover, the ligand field surrounding the magnetic atom can determine its spin and orbital degrees of freedom and thus dictates its magnetic anisotropy by spin-orbit coupling. , In this scenario, a ligand field that can keep the magnetic atom in high-spin state and preserve its orbital angular momentum is highly desired . Until now, although various surface-adsorbed organometallic complexes were reported to show magnetic anisotropy energy in the order of several millielectronvolts, organometallic complexes with easy-axis magnetic anisotropy have been rarely addressed. , It still remains a challenge to realize large easy-axis magnetic anisotropy in organometallic complexes.…”
mentioning
confidence: 99%