Surface Deposition Induced Reduction of the Ground State Spin in Cr10 Wheel

Abstract We report the deposition of monolayers and multilayers of {Cr10(OMe)20(O2CCMe3)10} wheels, hereafter {Cr10}, onto Au(111) and Cu(111) single‐crystal substrates, and their characterization combining scanning tunneling microscopy, X‐ray photoelectron spectroscopy, X‐ray absorption spectroscop...

Full description

Bibliographic Details
Main Authors: Elena Bartolomé, Ludovica Ferrari, Francesco Sedona, Ana Arauzo, Javier Rubín, Javier Luzón, Julia Herrero‐Albillos, Mirco Panighel, Aitor Mugarza, Marzio Rancan, Mauro Sambi, Lidia Armelao, Juan Bartolomé, Fernando Bartolomé
Format: Article
Language:English
Published: Wiley-VCH 2023-07-01
Series:Advanced Materials Interfaces
Subjects:
Online Access:https://doi.org/10.1002/admi.202300146
_version_ 1797676533371895808
author Elena Bartolomé
Ludovica Ferrari
Francesco Sedona
Ana Arauzo
Javier Rubín
Javier Luzón
Julia Herrero‐Albillos
Mirco Panighel
Aitor Mugarza
Marzio Rancan
Mauro Sambi
Lidia Armelao
Juan Bartolomé
Fernando Bartolomé
author_facet Elena Bartolomé
Ludovica Ferrari
Francesco Sedona
Ana Arauzo
Javier Rubín
Javier Luzón
Julia Herrero‐Albillos
Mirco Panighel
Aitor Mugarza
Marzio Rancan
Mauro Sambi
Lidia Armelao
Juan Bartolomé
Fernando Bartolomé
author_sort Elena Bartolomé
collection DOAJ
description Abstract We report the deposition of monolayers and multilayers of {Cr10(OMe)20(O2CCMe3)10} wheels, hereafter {Cr10}, onto Au(111) and Cu(111) single‐crystal substrates, and their characterization combining scanning tunneling microscopy, X‐ray photoelectron spectroscopy, X‐ray absorption spectroscopy, X‐ray natural linear dichroism, and X‐ray magnetic circular dichroism (XMCD). {Cr10} in bulk shows axial magnetic anisotropy and a cluster total spin S  =  9 ground state, stemming from an interaction scheme of two semi‐crowns containing four Cr3+ ions interacting ferromagnetically, separated by two Cr3+ antiferromagnetically coupled. The one‐monolayer (1ML) samples of {Cr10} sublimated on Ag(111) and Cu(111) show slightly different applied magnetic field dependence of XMCD signal. The field‐dependence of the magnetization evolves from a lower curve for the 1ML {Cr10} samples to a curve resembling the bulk one as the number of layers is increased, as shown in a 14ML sample. Monte Carlo simulations allow rationalizing the magnetization curves of the 1ML samples in terms of a reduction of the cluster ground‐state total spin, S  =  3 or S  =  6, as a consequence of variations in the intra‐wheel coupling interactions induced by the on‐surface deposition. The sensitivity of the magnetic configuration of {Cr10} to minor distortions of the intramolecular conformation might be exploited to control magnetism by external stimuli for applications.
first_indexed 2024-03-11T22:29:33Z
format Article
id doaj.art-1a5a08b03d754e58bb32893e4f1a3a98
institution Directory Open Access Journal
issn 2196-7350
language English
last_indexed 2024-03-11T22:29:33Z
publishDate 2023-07-01
publisher Wiley-VCH
record_format Article
series Advanced Materials Interfaces
spelling doaj.art-1a5a08b03d754e58bb32893e4f1a3a982023-09-23T06:52:43ZengWiley-VCHAdvanced Materials Interfaces2196-73502023-07-011020n/an/a10.1002/admi.202300146Surface Deposition Induced Reduction of the Ground State Spin in Cr10 WheelElena Bartolomé0Ludovica Ferrari1Francesco Sedona2Ana Arauzo3Javier Rubín4Javier Luzón5Julia Herrero‐Albillos6Mirco Panighel7Aitor Mugarza8Marzio Rancan9Mauro Sambi10Lidia Armelao11Juan Bartolomé12Fernando Bartolomé13Escola Universitària Salesiana de Sarrià (EUSS) Passeig Sant Joan Bosco 74 Barcelona 08017 SpainDipartimento di Scienze Chimiche Università di Padova Via Marzolo 1 Padova 35131 ItalyDipartimento di Scienze Chimiche Università di Padova Via Marzolo 1 Padova 35131 ItalyInstituto de Nanociencia y Materiales de Aragón (INMA) Universidad de Zaragoza – CSIC Pedro Cerbuna 12 Zaragoza 50009 SpainInstituto de Nanociencia y Materiales de Aragón (INMA) Universidad de Zaragoza – CSIC Pedro Cerbuna 12 Zaragoza 50009 SpainCentro Universitario de la Defensa Academia General Militar Zaragoza SpainInstituto de Nanociencia y Materiales de Aragón (INMA) Universidad de Zaragoza – CSIC Pedro Cerbuna 12 Zaragoza 50009 SpainCNR‐IOM Laboratorio TASC Basovizza Trieste 34149 ItalyCatalan Institute of Nanoscience and Nanotechnology (ICN2) CSIC and BIST Campus UAB Barcelona 08193 SpainInstitute of Condensed Matter Chemistry and Technologies for Energy (ICMATE) National Research Council (CNR) c/o Department of Chemical Sciences University of Padova via F. Marzolo 1 Padova 35131 ItalyDipartimento di Scienze Chimiche Università di Padova Via Marzolo 1 Padova 35131 ItalyDipartimento di Scienze Chimiche Università di Padova Via Marzolo 1 Padova 35131 ItalyInstituto de Nanociencia y Materiales de Aragón (INMA) Universidad de Zaragoza – CSIC Pedro Cerbuna 12 Zaragoza 50009 SpainInstituto de Nanociencia y Materiales de Aragón (INMA) Universidad de Zaragoza – CSIC Pedro Cerbuna 12 Zaragoza 50009 SpainAbstract We report the deposition of monolayers and multilayers of {Cr10(OMe)20(O2CCMe3)10} wheels, hereafter {Cr10}, onto Au(111) and Cu(111) single‐crystal substrates, and their characterization combining scanning tunneling microscopy, X‐ray photoelectron spectroscopy, X‐ray absorption spectroscopy, X‐ray natural linear dichroism, and X‐ray magnetic circular dichroism (XMCD). {Cr10} in bulk shows axial magnetic anisotropy and a cluster total spin S  =  9 ground state, stemming from an interaction scheme of two semi‐crowns containing four Cr3+ ions interacting ferromagnetically, separated by two Cr3+ antiferromagnetically coupled. The one‐monolayer (1ML) samples of {Cr10} sublimated on Ag(111) and Cu(111) show slightly different applied magnetic field dependence of XMCD signal. The field‐dependence of the magnetization evolves from a lower curve for the 1ML {Cr10} samples to a curve resembling the bulk one as the number of layers is increased, as shown in a 14ML sample. Monte Carlo simulations allow rationalizing the magnetization curves of the 1ML samples in terms of a reduction of the cluster ground‐state total spin, S  =  3 or S  =  6, as a consequence of variations in the intra‐wheel coupling interactions induced by the on‐surface deposition. The sensitivity of the magnetic configuration of {Cr10} to minor distortions of the intramolecular conformation might be exploited to control magnetism by external stimuli for applications.https://doi.org/10.1002/admi.202300146chromium wheelsscanning tunneling microscopysingle‐molecule magnetssublimated clusterssurface molecular magnetismX‐ray magnetic circular dichroism
spellingShingle Elena Bartolomé
Ludovica Ferrari
Francesco Sedona
Ana Arauzo
Javier Rubín
Javier Luzón
Julia Herrero‐Albillos
Mirco Panighel
Aitor Mugarza
Marzio Rancan
Mauro Sambi
Lidia Armelao
Juan Bartolomé
Fernando Bartolomé
Surface Deposition Induced Reduction of the Ground State Spin in Cr10 Wheel
Advanced Materials Interfaces
chromium wheels
scanning tunneling microscopy
single‐molecule magnets
sublimated clusters
surface molecular magnetism
X‐ray magnetic circular dichroism
title Surface Deposition Induced Reduction of the Ground State Spin in Cr10 Wheel
title_full Surface Deposition Induced Reduction of the Ground State Spin in Cr10 Wheel
title_fullStr Surface Deposition Induced Reduction of the Ground State Spin in Cr10 Wheel
title_full_unstemmed Surface Deposition Induced Reduction of the Ground State Spin in Cr10 Wheel
title_short Surface Deposition Induced Reduction of the Ground State Spin in Cr10 Wheel
title_sort surface deposition induced reduction of the ground state spin in cr10 wheel
topic chromium wheels
scanning tunneling microscopy
single‐molecule magnets
sublimated clusters
surface molecular magnetism
X‐ray magnetic circular dichroism
url https://doi.org/10.1002/admi.202300146
work_keys_str_mv AT elenabartolome surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT ludovicaferrari surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT francescosedona surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT anaarauzo surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT javierrubin surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT javierluzon surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT juliaherreroalbillos surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT mircopanighel surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT aitormugarza surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT marziorancan surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT maurosambi surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT lidiaarmelao surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT juanbartolome surfacedepositioninducedreductionofthegroundstatespinincr10wheel
AT fernandobartolome surfacedepositioninducedreductionofthegroundstatespinincr10wheel