Matias URDAMPILLETA - TEL
Matias URDAMPILLETA - TEL Matias URDAMPILLETA - TEL
tel-00770488, version 1 - 7 Jan 2013 Int. J. Mol. Sci. 2011, 12 6658 magnetic leads. Indeed, the spin-dependent transport through this supramolecular spin valve is completely determined by the magnetic properties of the molecular species magnetically coupled to the conducting channel of the CNT. Similar results were recently obtained using graphene nanoconstriction decorated with TbPc2 magnetic molecules [11]. In this case, a magnetoconductivity signal as high as 20% was found for the spin reversal. These results show the behavior of multiple-field-effect nanotransistors with sensitivity at the single-molecule level. The paper is structured as follows. In Section 2, we introduce different methods used to fabricate and measure the supramolecular based junctions. The results section (Section 3) describes the magnetic properties of the pyrene functionalized heteroleptic bis-phthalocyaninato-Terbium (III) SMMs (called TbPc2 in the following) used in this study. In Section 3.1, we briefly discuss the magnetization reversal mechanisms of the TbPc2 SMM, namely QTM and the direct relaxation process, using µ-SQUID measurements on diluted crystals of molecules. Section 3.2 exhibits the electronic transport features of the spin valve, being in the closed quantum dot regime. Then, in Section 3.3, we present the spin-valve behavior revealed by the magneto-conductance measurements under magnetic field sweeps. The anisotropic dependence of the hysteretic conductance jumps is also studied and in good agreement with the expected uniaxial anisotropy of TbPc2 SMMs. Finally, Section 4 discusses the spin valve mechanism in further detail and we conclude with a brief outlook. 2. Devices Fabrication In this project we studied about 150 samples of which 28 showed magnetic signals related to the TbPc2-SMMs and eight of them were studied in detail, manifesting similar behavior concerning their magneto-conductance. In contrast to our first publication [6], the sample presented in this paper was fabricated using CVD nanotubes. Catalyst islands were designed on SiO2 by creating holes by optical lithography in LOR3A resist, which were filled with Fe/Mo catalyst in nanoporous alumina. After liftoff of the resist, nanotubes were grown in a Firstnano CVD oven at 750 °C, whereby methane was used as a carbon source [12]. SWNTs were located by AFM or SEM with respect to lithographically patterned markers and then contacted with 50 nm Pd by standard electron-beam lithography, defining 200 nm long CNT junctions. A solution containing bis(phthalocyaninato)terbium (III) substituted with pyrene groups [13] with a 10 −6 molarity was dropped on the device and dried under nitrogen flow. Samples with large resistance (>100 kΩ) at room temperature were micro bounded and measurements were carried out in a dilution fridge with a base temperature of 40 mK. The electronic temperature was estimated to be around 150 mK. 3. Results 3.1. Magnetic Properties of the TbPc2 SMMs Among the existing SMMs families, single ion lanthanide complexes are among the most simple and robust systems [13]. Here we focus our attention on the TbPc2 SMM based on a single Tb 3+ ion coordinated to two phthalocyanine (Pc) ligands as depicted in Fdigure 1(a). The SMM behavior originates from the electronic multiplet substructure of the Tb 3+ ion in its (4f) 8 electronic configuration leading to a J = 6 magnetic moment. The TbPc2-SMM exhibits a significantly large axial magnetic
tel-00770488, version 1 - 7 Jan 2013 Int. J. Mol. Sci. 2011, 12 6659 anisotropy originating from the strong spin-orbit coupling in lanthanide ions and from the ligand field potential made by the two Pc ligands. It leads to a well-defined ground state configuration (J = 6, |Jz| = 6) separated from the first excited state (J = 6, Jz = 5) by an energy splitting ΔE ~ 600 K [14]. All our measurements were performed at very low temperatures, so that we only consider the lowest energy substates available with Jz = ± 6, the corresponding Zeeman diagram is plotted in Figure 1(b). Apart from the Terbium(III) ion, the molecule has a spin ½ delocalized over the two phtalocyanines groups [15]. This unpaired electron mediates a magnetic coupling between the Terbium 4f electrons and its environment. Figure 1. Magnetization reversal mechanisms in the TbPc2 SMM (alkyl and pyrene substituents are omitted for reasons of clarity). (a) Scheme of the TbPc2-SMM. The terbium ion has a J = 6 magnetic moment and an unpaired electron is delocalized over the organic part; (b) Zeeman diagram calculated for the TbPc2 SMM ground state (J = 6, |Jz| = 6). The interaction with the Tb nucleus spin I = 3/2 splits each electronic substate through the hyperfine coupling, providing a path for Quantum Tunneling of Magnetization (QTM) at the anti-crossing of two levels; (c) Hysteresis loops of the crystallized TbPc2-SMM (2% in the YPc2 matrix) measured at 40 mK for different sweeping rates ranging from 1 to 280 mT.s −1 . QTM reflects in staircase-like steps of the hysteresis loops at low magnetic fields, each step corresponding to a level anti-crossing. Molecules, which did not undergo QTM can relax their magnetization to a lower energy state by the direct transition (DT) occurring at larger magnetic fields.
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tel-00770488, version 1 - 7 Jan 2013<br />
Int. J. Mol. Sci. 2011, 12 6658<br />
magnetic leads. Indeed, the spin-dependent transport through this supramolecular spin valve is<br />
completely determined by the magnetic properties of the molecular species magnetically coupled to the<br />
conducting channel of the CNT. Similar results were recently obtained using graphene nanoconstriction<br />
decorated with TbPc2 magnetic molecules [11]. In this case, a magnetoconductivity signal as high<br />
as 20% was found for the spin reversal. These results show the behavior of multiple-field-effect<br />
nanotransistors with sensitivity at the single-molecule level.<br />
The paper is structured as follows. In Section 2, we introduce different methods used to fabricate<br />
and measure the supramolecular based junctions. The results section (Section 3) describes the<br />
magnetic properties of the pyrene functionalized heteroleptic bis-phthalocyaninato-Terbium (III)<br />
SMMs (called TbPc2 in the following) used in this study. In Section 3.1, we briefly discuss the<br />
magnetization reversal mechanisms of the TbPc2 SMM, namely QTM and the direct relaxation<br />
process, using µ-SQUID measurements on diluted crystals of molecules. Section 3.2 exhibits the<br />
electronic transport features of the spin valve, being in the closed quantum dot regime. Then, in<br />
Section 3.3, we present the spin-valve behavior revealed by the magneto-conductance measurements<br />
under magnetic field sweeps. The anisotropic dependence of the hysteretic conductance jumps is also<br />
studied and in good agreement with the expected uniaxial anisotropy of TbPc2 SMMs. Finally, Section<br />
4 discusses the spin valve mechanism in further detail and we conclude with a brief outlook.<br />
2. Devices Fabrication<br />
In this project we studied about 150 samples of which 28 showed magnetic signals related to the<br />
TbPc2-SMMs and eight of them were studied in detail, manifesting similar behavior concerning their<br />
magneto-conductance. In contrast to our first publication [6], the sample presented in this paper was<br />
fabricated using CVD nanotubes. Catalyst islands were designed on SiO2 by creating holes by optical<br />
lithography in LOR3A resist, which were filled with Fe/Mo catalyst in nanoporous alumina. After<br />
liftoff of the resist, nanotubes were grown in a Firstnano CVD oven at 750 °C, whereby methane was<br />
used as a carbon source [12]. SWNTs were located by AFM or SEM with respect to lithographically<br />
patterned markers and then contacted with 50 nm Pd by standard electron-beam lithography, defining<br />
200 nm long CNT junctions. A solution containing bis(phthalocyaninato)terbium (III) substituted with<br />
pyrene groups [13] with a 10 −6 molarity was dropped on the device and dried under nitrogen flow.<br />
Samples with large resistance (>100 kΩ) at room temperature were micro bounded and measurements<br />
were carried out in a dilution fridge with a base temperature of 40 mK. The electronic temperature was<br />
estimated to be around 150 mK.<br />
3. Results<br />
3.1. Magnetic Properties of the TbPc2 SMMs<br />
Among the existing SMMs families, single ion lanthanide complexes are among the most simple<br />
and robust systems [13]. Here we focus our attention on the TbPc2 SMM based on a single Tb 3+ ion<br />
coordinated to two phthalocyanine (Pc) ligands as depicted in Fdigure 1(a). The SMM behavior<br />
originates from the electronic multiplet substructure of the Tb 3+ ion in its (4f) 8 electronic configuration<br />
leading to a J = 6 magnetic moment. The TbPc2-SMM exhibits a significantly large axial magnetic