Despite its promising therapeutic potential, nanoparticle-mediated magnetic hyperthermia is currently limited to treatment of localized and relatively accessible cancer tumors because the required therapeutic temperatures above 40 °C can only be achieved by direct intratumoral injection of conventional iron oxide nanoparticles. To realize the true potential of magnetic hyperthermia for cancer treatment, there is an unmet need for nanoparticles with high heating capacity that can efficiently accumulate at tumor sites following systemic administration and generate desirable intratumoral temperatures upon exposure to an alternating magnetic field (AMF). Although there have been many attempts to develop the desired nanoparticles, reported animal studies reveal the challenges associated with reaching therapeutically relevant intratumoral temperatures following systemic administration at clinically relevant doses. Therefore, we developed efficient magnetic nanoclusters with enhanced heating efficiency for systemically delivered magnetic hyperthermia that are composed of cobalt- and manganese-doped, hexagon-shaped iron oxide nanoparticles (CoMn-IONP) encapsulated in biocompatible PEG-PCL (poly(ethylene glycol)-b-poly(ɛ-caprolactone))-based nanocarriers. Animal studies validated that the developed nanoclusters are non-toxic, efficiently accumulate in ovarian cancer tumors following a single intravenous injection, and elevate intratumoral temperature up to 44 °C upon exposure to safe and tolerable AMF. Moreover, the obtained results confirmed the efficiency of the nanoclusters to generate the required intratumoral temperature after repeated injections and demonstrated that nanoclusters-mediated magnetic hyperthermia significantly inhibits cancer growth. In summary, this nanoplatform is a milestone in the development of systemically delivered magnetic hyperthermia for treatment of cancer tumors that are difficult to access for intratumoral injection.

Low-loss magnetization dynamics and strong magnetoelastic coupling are generally mutually exclusive properties due to opposing dependencies on spin-orbit interactions. So far, the lack of low-damping, magnetostrictive ferrite films has hindered the development of power-efficient magnetoelectric and acoustic spintronic devices. Here, magnetically soft epitaxial spinel NiZnAl-ferrite thin films with an unusually low Gilbert damping parameter (<3 × 10 ), as well as strong magnetoelastic coupling evidenced by a giant strain-induced anisotropy field (≈1 T) and a sizable magnetostriction coefficient (≈10 ppm), are reported. This exceptional combination of low intrinsic damping and substantial magnetostriction arises from the cation chemistry of NiZnAl-ferrite. At the same time, the coherently strained film structure suppresses extrinsic damping, enables soft magnetic behavior, and generates large easy-plane magnetoelastic anisotropy. These findings provide a foundation for a new class of low-loss, magnetoelastic thin film materials that are promising for spin-mechanical devices.

Domain structures in CoFeB-MgO thin films with a perpendicular easy magnetization axis were observed by magneto-optic Kerr-effect microscopy at various temperatures. The domain wall surface energy was obtained by analyzing the spatial period of the stripe domains and fitting established domain models to the period. In combination with SQUID measurements of magnetization and anisotropy energy, this leads to an estimate of the exchange stiffness and domain wall width in these films. These parameters are essential for determining whether domain walls will form in patterned structures and devices made of such materials.

Most studies on iron oxide nanocrystals (NCs) suggest that the magnetic properties depend strongly on size for diameters below 10 nm, but there is less agreement about how the structure of the NC surface influences magnetic properties. Because the magnetic properties of iron oxide NCs hold promise for applications from cancer detection and therapeutics to environmental remediation, it is imperative to understand how size influences those properties. In most cases, the effective magnetic size is significantly lower than the measured physical size, a finding attributed to spin canting or disorder at the NC surface. A complicating factor is that the reaction conditions used to produce samples influence their magnetic properties. Thus, we employed a continuous growth method involving layer-by-layer addition of precursor to produce single-crystalline, spherical cores with subnanometer precision over a range of sizes under the same reaction conditions. Analysis of the NCs by small-angle X-ray scattering, transmission electron microscopy, and powder X-ray diffraction showed that the NCs possess the spinel structure (primarily maghemite) and are crystalline, defect-free, and uniform in size. The saturation magnetization values for a series of eight distinct diameters between 4 and 10 nm increase smoothly with increasing size, from 55 to 78 Am 2 /kg. Magnetic sizes of the NCs determined by fitting magnetization curves to the Langevin function are nearly identical to the physical sizes, suggesting low levels of strain-producing defects and a very thin nonmagnetic surface layer on the NCs. The results suggest that syntheses that permit slower growth at reduced temperatures through a single reaction mechanism can enhance, and offer fine control over, magnetic properties.