“…These are core−shell NPs with a citrate shell from NanoMaterials Technology Pte Ltd. (known as JHU NPs) and matrix-based NPs constituted by superparamagnetic iron oxide NPs dispersed in a dextran matrix, from micromod Partikeltechnologie GmbH (known as nanomag-D-spio). 58 Their heating properties, also tested through in silico simulations of magnetic hyperthermia applied to murine models, 59 are available from the literature in terms of SLP versus H ̂a and f. 35 In particular, for JHU NPs, when f = 150 kHz, the SLP varies between 150 and 480 W/g in the range of H ̂a 10−40 kA/m, while, when f = 300 kHz, the SLP varies between 50 and 780 W/g in the range of H ̂a 5−20 kA/ m. For nanomag-D-spio NPs, when f = 150 kHz, the SLP varies between 15 and 45 W/g in the range of H ̂a 10−40 kA/ m, while, when f = 300 kHz, the SLP varies between 15 and 70 W/g in the range of H ̂a 5−20 kA/m. As a result of the different heating properties, MNP concentrations on the order of 5 mg/ mL are potentially sufficient for reaching 60 °C and activating the polymerization in 2 min when using JHU NPs and AC magnetic fields with f = 150 kHz and H ̂aa = 40 kA/m (Figure 3D).…”