Abstract:liquid-nitrogen temperature [3] or single atoms exhibiting extremely long magnetic relaxation times. [4][5][6] In particular, systems based on late lanthanide family elements, like Dy and Tb, have been largely in focus, including single-molecule, [2,3] singleatom, [4,5] or single-chain magnets. [7,8] Adsorption of SMMs on surfaces allows to study individual molecular units, as well as to realize transport schemes essential for the implementation of SMMs in molecular-scale spintronics or quantum computing devic… Show more
“…S16 in ESI†). This proves that the X-ray irradiation considerably accelerates magnetic relaxation in Tb 2 @C 79 N. Such X-ray induced demagnetization was reported earlier in monolayers of metallofullerenes 61,62,96 and TbPc 2 , 46 but the effect in Tb 2 @C 79 N is more pronounced. Further measurements of (sub)monolayer films demonstrate that not only the demagnetization rate but also the population of valence orbitals may be affected by X-ray irradiation through secondary processes.…”
Section: Computational Modelingsupporting
confidence: 85%
“…[56][57][58][59][60][61][62] The nitride clusterfullerenes Dy 2 ScN@C 80 and DySc 2 N@C 80 were shown to maintain their SMM properties in monolayers on metallic substrates. [56][57][58][59][60] _ENREF_71_ENREF_73 Even more promising are recent studies of Dy 2 @C 80 (CH 2 Ph) deposited onto graphene 61 and Tb 2 @C 80 (CH 2 Ph) on graphene and HOPG, 62 which demonstrated that dimetallofullerenes with single-electron lanthanidelanthanide bonds can also sustain their superb SMM performance in monolayers. Magnetic hysteresis in these monolayers was observed at considerably higher temperatures than in all other surface-supported SMMs, reaching 28 K for a self-assembled monolayer of Tb 2 @C 80 (CH 2 Ph) derivative.…”
Section: Introductionmentioning
confidence: 99%
“…However, a realization of hysteretic behaviour in monolayers is not straightforward and was demonstrated only for a handful of SMMs, 35–55 including some metallofullerene-SMMs. 56–62 The nitride clusterfullerenes Dy 2 ScN@C 80 and DySc 2 N@C 80 were shown to maintain their SMM properties in monolayers on metallic substrates. 56–60 Even more promising are recent studies of Dy 2 @C 80 (CH 2 Ph) deposited onto graphene 61 and Tb 2 @C 80 (CH 2 Ph) on graphene and HOPG, 62 which demonstrated that dimetallofullerenes with single-electron lanthanide–lanthanide bonds can also sustain their superb SMM performance in monolayers.…”
Realization of stable spin states in surface-supported magnetic molecules is crucial for their applications in molecular spintronic, memory storage or quantum information processing. In this work, we studied the surface...
“…S16 in ESI†). This proves that the X-ray irradiation considerably accelerates magnetic relaxation in Tb 2 @C 79 N. Such X-ray induced demagnetization was reported earlier in monolayers of metallofullerenes 61,62,96 and TbPc 2 , 46 but the effect in Tb 2 @C 79 N is more pronounced. Further measurements of (sub)monolayer films demonstrate that not only the demagnetization rate but also the population of valence orbitals may be affected by X-ray irradiation through secondary processes.…”
Section: Computational Modelingsupporting
confidence: 85%
“…[56][57][58][59][60][61][62] The nitride clusterfullerenes Dy 2 ScN@C 80 and DySc 2 N@C 80 were shown to maintain their SMM properties in monolayers on metallic substrates. [56][57][58][59][60] _ENREF_71_ENREF_73 Even more promising are recent studies of Dy 2 @C 80 (CH 2 Ph) deposited onto graphene 61 and Tb 2 @C 80 (CH 2 Ph) on graphene and HOPG, 62 which demonstrated that dimetallofullerenes with single-electron lanthanidelanthanide bonds can also sustain their superb SMM performance in monolayers. Magnetic hysteresis in these monolayers was observed at considerably higher temperatures than in all other surface-supported SMMs, reaching 28 K for a self-assembled monolayer of Tb 2 @C 80 (CH 2 Ph) derivative.…”
Section: Introductionmentioning
confidence: 99%
“…However, a realization of hysteretic behaviour in monolayers is not straightforward and was demonstrated only for a handful of SMMs, 35–55 including some metallofullerene-SMMs. 56–62 The nitride clusterfullerenes Dy 2 ScN@C 80 and DySc 2 N@C 80 were shown to maintain their SMM properties in monolayers on metallic substrates. 56–60 Even more promising are recent studies of Dy 2 @C 80 (CH 2 Ph) deposited onto graphene 61 and Tb 2 @C 80 (CH 2 Ph) on graphene and HOPG, 62 which demonstrated that dimetallofullerenes with single-electron lanthanide–lanthanide bonds can also sustain their superb SMM performance in monolayers.…”
Realization of stable spin states in surface-supported magnetic molecules is crucial for their applications in molecular spintronic, memory storage or quantum information processing. In this work, we studied the surface...
“…Recently, Fonin and co-workers were able to preserve the reported magnetic remanence of Dy 2 @C 80 (CH 2 Ph) on the graphene/Ir(111) surface exhibiting T B of 17 K at the field sweep rate of 2 T min −1 . 53 The integrating of SMM with hybrid materials usually diminishes its magnetic performance due to the formation of buffer environment between the substrate and magnetic materials; however, in this report, they were able to preserve magnetic remanence comparable with the original bulk system. 103 In addition, the utilization of paramagnetic bridging radical ligands enabling the establishment of strong magnetic coupling between the lanthanide centers under constrained coordination environments is becoming another successful strategy.…”
Section: ■ Strategies For Designing Hp−dy−smmsmentioning
The
present prospect of single-molecule magnets (SMMs) research
is more appealing after the detection of magnetic remanence above
liquid-nitrogen temperatures. From the current state-of-the-art of
the well matured molecular magnetism perspective, in this Review,
we discuss the recent emerging trends on the key synthetic strategies
employed to achieve exotic magnetic properties by providing representative
seminal reports on high-performance Dy(III)–SMMs (HP-Dy–SMMs).
Special emphasis has been given to monomeric HP-Dy–SMMs realized
via crystal field (CF), predominant bond, and organometallic approaches.
In addition, recent stimulating reports on endometallofullerenes (EMFs)
and radical-bridged systems possessing strong magnetic coupling are
encompassed. Likewise, the role of spin-vibration coupling in the
magnetic relaxation of Dy(III) MMs is also highlighted. To this end,
we believe more demanding theoretical studies are still anticipated
to forecast the promising molecule with magnetization blocking at
a practical temperature.
“…Even slight overheating changes its mechanism from nucleophilic substitution to radical polyaddition, which produces intractable mixtures of EMF(CH 2 Ph) n multiadducts. As di-EMFs with single-electron lanthanide–lanthanide bond are very robust SMMs and qubit candidates, ,,,− development of a streamlined approach to their synthesis and separation would be very beneficial.…”
Lanthanide dimetallofullerenes with single-electron M−M bonds are an important class of single molecular magnets and qubit candidates, but stabilization of their unique electronic and spin structure in the form of a neutral molecule requires functionalization of the fullerene cage with a single radical group. The lack of selectivity of the currently available procedure results in a complicated and tedious separation process. Here we demonstrate that electrophilic trifluoromethylation of a mixture of metallofullerene anions with Umemoto reagent II is highly selective toward M 2 @C 80 − (M = Tb, Y) anions, yielding M 2 @C 80 (CF 3 ) monoadducts as the main reaction product. Single-crystal Xray diffraction study proved attachment of the CF 3 group to the pentagon/hexagon/hexagon junction and revealed that positions of metal atoms inside the fullerene cage in the cocrystal with NiOEP are strongly related to the position of the porphyrin moieties. Magnetic characterization of Tb 2 @C 80 (CF 3 ) showed that it is a robust single-molecule magnet with broad magnetic hysteresis, 100 s blocking temperature of 25 K, and the relaxation barrier of 801(4) K, corresponding to the flipping of the Tb magnetic moment in the strongly ferromagnetically coupled [Tb 3+ −e−Tb 3+ ] spin system.
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