1996
DOI: 10.1103/physrevb.54.14121
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Magnetic dimers of transition-metal atoms on the Ag(001) surface

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Cited by 36 publications
(12 citation statements)
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“…These results are in good agreement with the calculations performed for the 4d dimers on the Ag͑001͒ surface. 38 In the case of the 4d dimers the energy difference between the AFM and the FM solutions is systematically larger than the difference ⌬Eϭ⌬E FM Ϫ⌬E AFM in Table I. For example, for a Mo dimer the AFM state is more stable than the FM one, with moments, respectively, of m AFM ϭ3.17 B and m FM ϭ2.12 B , 37 and an energy difference of about 50 mRy.…”
Section: B Antiferromagnetic Solutionsmentioning
confidence: 86%
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“…These results are in good agreement with the calculations performed for the 4d dimers on the Ag͑001͒ surface. 38 In the case of the 4d dimers the energy difference between the AFM and the FM solutions is systematically larger than the difference ⌬Eϭ⌬E FM Ϫ⌬E AFM in Table I. For example, for a Mo dimer the AFM state is more stable than the FM one, with moments, respectively, of m AFM ϭ3.17 B and m FM ϭ2.12 B , 37 and an energy difference of about 50 mRy.…”
Section: B Antiferromagnetic Solutionsmentioning
confidence: 86%
“…But it is well known from general theorems about tight-binding bands 34 that there is a tendency towards antiferromagnetism for elements in the middle of transition metal series. Indeed antiferromagnetic solutions were obtained for finite-length 4d chains 37,38 and by means of total energy calculations they were predicted to be the more stable solutions for Nb and Mo dimers on the Ag͑100͒ terrace.…”
Section: B Antiferromagnetic Solutionsmentioning
confidence: 97%
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“…As atoms merge, subtle changes in orbital overlap and symmetry cause charge to shift from one atomic state to another, leading to a variation in local magnetic moments and exchange interactions. 1,2 Although such microscopic properties are usually inferred from macroscopic observations, recent advances in scanning tunneling microscopy ͑STM͒ have opened the possibility of probing local interactions in magnetic structures assembled atom by atom at surfaces. [3][4][5] At a surface, however, atomic scale magnetic structures can interact with the electronic degrees of freedom of the substrate, leading to the Kondo effect.…”
mentioning
confidence: 99%
“…All these methods share the same approach, i.e., they solve the problem in a finite volume taking into account the infinite host via appropriate boundary conditions for the Green's function. The Dyson equation, 11,12 the Korringa-Kohn-Rostoker method, 13,14 and the embedding method 15,16 are well known examples. Once the single particle Green's function of the interacting system is available one could compute the total energy.…”
Section: Introductionmentioning
confidence: 99%