Above a characteristic temperature, some insulating materials, typically metal oxides, undergo a reversible transition into a low resistivity phase. Such metal-insulator transition (MIT) materials are being studied for possible applications in electronic devices, as this transition can be triggered locally via Joule-heating. Among the known MIT materials, niobium dioxide (NbO2) is of particular interest because it has a transition temperature (1081 K) that is above typical operating temperatures for semiconductor electronics applications.In bulk NbO2 the MIT occurs due to a crystallographic transformation between rutile and distorted rutile structure above and below the transition temperature, respectively [1]. In an NbO2 thin film device under voltage bias, this transition produces a volatile and reversible low resistance state above a threshold voltage. Because of this property, NbO2 has been suggested as a possible selector material in crossbar arrays of resistive memory elements as a method for preventing "sneak current" switching. Though several bulk heating and biasing studies have been performed, the MIT in nanoscale devices under local Joule heating is not well understood. Here we report on imaging the MIT in situ in nanoscale, horizontally-aligned Pt/NbO2/Pt devices with multi-detector scanning transmission electron microscope (STEM) imaging.Our horizontal devices (Figure 1, left inset) allow TEM imaging of an MIT material between biasing electrodes. Ti/Pt (5/25 nm) electrodes (50 nm wide with 30 nm between electrodes) were fabricated on an electron transparent Si3N4 membrane using electron beam lithography. 50 nm of NbO2 was deposited over the electrodes via pulsed laser deposition at 700 o C substrate temperature in 2 mTorr Ar+O2 growth atmosphere with 1% O2 content using an NbO2 ceramic target (AJA International.). Film quality and thickness were assessed with x-ray photoelectron spectroscopy, x-ray diffraction, and x-ray reflectometry, confirming the major NbO2 phase, which forms with an additional top Nb2O5 layer of 2 nm due to air exposure [2]. STEM video was obtained simultaneously from 3 different detectors, collecting electrons at low (bright field or BF), intermediate (dark field or DF), and higher scattering angles (high-angle dark field or HDF). Each detector is sensitive to different contrast mechanisms; diffraction contrast is more apparent at low and intermediate scattering angles while thickness and atomic number Z contrast dominate at higher angles.Current-voltage (IV) data acquired in situ show an electroforming step and two subsequent transition cycles (Figure 1, left). The bias voltage was ramped slowly (~50 mV/s) and the current was limited to 40 µA. After an initial electroforming step, the device exhibited reversible, polarity-independent threshold switching at ~1V. Such switching repeated over multiple cycles. We observed similar behavior in several devices biased in situ. Despite our non-standard geometry, the devices switched with an electric field of ~3x10 7 V/m and ~1 nW/nm ...