Research
Research in the Center for Molecular Spintronics focuses on switchable paramagnetic molecules in the active layer of spintronic devices. Center researchers have established theoretically and experimentally that magnetic bistability in molecules has important consequences for electrical transport. Bistability allows the possibility to externally control the spin state in a molecular system using temperature, pressure, light, or electric field using spin-crossover (SCO) complexes and valence tautomers (VTs). For VT complexes, the concerted impact of SCO and intramolecular electron transfer suggests large spin-dependent electronic structure effects that will give rise to rich spintronic behaviors. There is a clear possibility to develop direct electric control of the magnetic properties of molecules. Such control would lead to high speed, low power computing applications in spintronics including magnetoelectric gating necessary for an all-organic spin field-effect transistor.
Paramagnetic molecules are a new paradigm for molecular spintronics. They can be used as “spin filters,” (as outlined recently by Phase II PI Professor Mark Ratner), thus allowing spintronic effects without ferromagnetic electrodes. In this case, the α (“up”) and β (“down”) orbital conduction channels derive from the frontier molecular orbitals of the spin-filtering molecule, and a spin-polarized current results from preferential coupling of one of these spin-dependent orbitals with the band structure of the electrodes. When this effect is combined with switchable and bistable paramagnetic molecules the result is a unique methodology for enhancing, modulating, and controlling the propagation of spin-polarized electron currents.
Impact of Spin-crossover (SCO) Transition on Thin Film Charge Transport.

Figure 1. a) Schematic change in oribital filling for a typical Fe(II) SCO material; b) Scanning tunneling microscope imageshowing submolecular resolution of an bilayer SCO compound on Au(111); c) Experimental I/V curves for a thick SCO film across the transition; d)Theoretically predicted I/V curve for the same materials.
Tunneling spectroscopy and electronic transport in switchable valence tautomer films.

Figure 2. (a) Molecular structure and conceptual switching device geometry that exploits the CoIII(Cat)(SQ)(CN-py)2 <-> CoII(SQ)2(CN-py)2 VT transition; (b) Spin density (red isosurface) from DFT calculations that confirms the intramolecular charge transfer picture from the catecholate ligands to the cobalt ion in the low-to-high-spin magnetic transition a the polymeric variant of the VT compound.

Figure 3. (a) Temperature-dependent differential conductance (dI/dV) and (b) derivative of differential conductance (d2I/dV2) vs. bias voltage and with visible light exposure (coincident with LMCT band). The traces are shifted for clarity. The resonances are peaks/dips in d2I/dV2 (indicated by the blue arrows) and are switched-off by light (red traces in (a) and (b)), thus returning to the high temperature behavior (orange traces at 150K). (c) Theoretical density of states plot that confirms the difference in minority and majority spin density conducive to the measured spin-valve effect. (d) Spin valve effect in permalloy/VT molecule/Co trilayer structure (Fig. 2(a)) – tunneling magnetoresistance (TMR = (RAP-RP)/RP) at two temperatures.
Strong Coupling of Paramagnetic Molecules to Graphene.

Figure 4. (a) STM image of FePc on epitaxial graphene: large FePc-FePc distance suggests a strong FePc-graphene interaction; (b) The HOMO and LUMO for FePc on graphene indicate significant interfacial electronic interactions; (c) Differential conductance measurement where a mixed orbital state is observed at 0.5 eV (blue arrow); (d) theoretical density of states (DOS) and its projection into the individual contribution of the molecule and the Fe center. The existence of mixed FePc and graphene states is confirmed by these results.
Spin-polarized Scanning Tunneling Microscopy of Alq3.
Spin-polarized scanning tunneling microscopy (SPSTM) experiments has been developed by Dougherty as a crucial characterization tool to advance center research. Preliminary experiments using this technique have provided insight into the role of the metal-molecule interface in spin injection into Alq3 (tris(8-hydroxyquinoxolinato)Al(III)). This organic semiconductor has been one of the most intensively-investigated spintronic materials due to multiple reports of Giant Magnetoresistive effects. Fig. 5a shows the highly disordered interface that is created in the first monolayer of Alq3 on layered antiferromagnetic Cr(001) surfaces. Figure 5b shows a spin-polarized conductance map of the clean metal surface where high and low conductances alternate between adjacent (001) terraces as their local magnetizations vary from aligned to anti-aligned with the probe tip magnetization.

Figure 5. (a) STM image of disordered monolayer of Alq3 on Cr(001); (b) Spin-polarized conductance map of Cr(001) layered antiferromagnetic surface; (c) Spin-polarized conductance map of submonolayer Alq3/Cr(001). Circle indicates a single molecule.
Center Manuscripts
- "Scanning tunneling microscopy of a disordered Alq3–metal interface," Wang, Z.; Pronschinske, A.; and Dougherty, D. B.; Organic Electronics, 2011
- "Substrate-Mediated Intermolecular Hybridization in Binary Phthalocyanine Superstructures," Calzolari, Arrigo; Jin, Wei; Reutt-Robey, Janice E.; and Buongiorno Nardelli, Marco; J. Phys. Chem. C, 2009
- "Laterally patterned magnetic nanoparticles," Jie, Yanni; Niskala, Jeremy R.; Johnston-Peck, Aaron C.; Krommenhoek, Peter J.; Tracy, Joseph B.; Fan, Huiqing; and You, Wei; J. Mater. Chem., 2012
- "Size-Dependent Nanoscale Kirkendall Effect During the Oxidation of Nickel Nanoparticles," Railsback, Justin. G.; Johnston-Peck, Aaron C.; Wang, Junwei; and Tracy, Joseph B.; ACS Nano, 2010
- "Synthesis of Au(Core)/Ag(Shell) Nanoparticles and their Conversion to AuAg Alloy Nanoparticles," Shore, Matthew S.; Wang, Junwei; Johnston-Peck, Aaron C.; Oldenburg, Amy L.; and Tracy, Joseph B.; Small, 2010








