2016
DOI: 10.1039/c6cc03847f
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Electron–phonon coupling in engineered magnetic molecules

Abstract: We probe the electron-phonon coupling for in situ engineered porphyrin-based magnetic molecular layers supported on weakly reactive surfaces. Using high-resolution scanning tunneling microscopy and spectroscopy at 4.5 K we show that the electronic and magnetic properties of the engineered molecules are the result of interplay between many-body spin-flip excitations and electron-phonon interactions.

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Cited by 15 publications
(18 citation statements)
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“…In this framework, the Kondo effect 1,10,11 is the most frequently found. Since this phenomenon is an archetypal example of the formation of a many-body quantum state, it is central in the understanding of the electronic behavior of complex strongly correlated electrons systems such as heavy fermions 11,12 , Kondo insulators 13 , and nanoscale systems 2,3,5,[14][15][16][17][18][19][20][21][22][23][24][25][26][27] .…”
Section: Introductionmentioning
confidence: 99%
“…In this framework, the Kondo effect 1,10,11 is the most frequently found. Since this phenomenon is an archetypal example of the formation of a many-body quantum state, it is central in the understanding of the electronic behavior of complex strongly correlated electrons systems such as heavy fermions 11,12 , Kondo insulators 13 , and nanoscale systems 2,3,5,[14][15][16][17][18][19][20][21][22][23][24][25][26][27] .…”
Section: Introductionmentioning
confidence: 99%
“…Although T-shaped quantum dot systems discussed by us are only toy models, with the help of which we analyze the richness of emerging phenomena resulting from the interplay of three important factors, namely strong correlations, interference, and coupling with phonons, and discuss their impact on transport on a nanoscopic scale, the obtained results can be also qualitatively related to some experimental observations. Apart from many reports mentioned in the Introduction section, which demonstrate phonon-induced symmetric Kondo satellites, STM experiments presenting asymmetric satellite lines indicate the role of interference [ 51 ]. From the line widths of the central peaks or widths of satellite resonances one can infer about the Kondo temperature.…”
Section: Discussionmentioning
confidence: 99%
“…It has been shown that morphology manipulation of semiconductor QDs such as size, shape, strain distribution, or inhomogenities can influence the coupling strength of electron-phonon (e-ph) interactions [49]. The phononic effects appears not only in sequential tunneling, but also in the Kondo regime where vibrational sidebands have been also observed [45,[50][51][52][53][54]. The interplay of electron-phonon coupling and Kondo effect has been also studied theoretically [55][56][57][58][59][60].…”
Section: Introductionmentioning
confidence: 99%
“…This phenomenon is well known in condensed matter 16 and leads to a peak in the conductance, at zero bias which appears at low temperatures. Signatures of the Kondo effect have been observed in semiconducting 17,18 as well as in molecular [19][20][21][22][23][24][25][26] quantum dots. The conductance at zero bias reaches a maximum near the quantum of conductance G 0 , which in non-interacting systems can only be obtained by tuning the energy of one level near the Fermi energy.…”
Section: Introductionmentioning
confidence: 99%