Recent developments in the integration of microwave sources in an ASIC have allowed to develop so-called electron paramagnetic resonance on a chip (EPRoC), allowing for extremely compact and low-cost EPR instrumentation.[1] Recently, this method has showcased its potential for electrical detection of magnetic resonance (EDMR) in a thin a-Si:H solar cell, detecting EDMR through a change in conductivity in the photoactive layer.[2] Here, we extend EDMRoC spectroscopy to measurements of EDMR in lateral SiC MOSFETs, combining it with the powerful charge pumping (CP) characterization technique. In CP, the gate voltage is periodically changed between inversion and accumulation so that a rectified current can be extracted from the transistor channel region originating from a recombination of charges at defect trapping sites.[3] CP-EDMR has demonstrated the capability of identifying and quantifying charge traps within the transistor channel of SiC MOSFETs [4], but requires advanced instrumentation and is therefore not generally applicable in both fundamental and applied research as well as in industrial environments. In this paper we demonstrate for the first time CP-EDMRoC as a versatile, fast and sensitive method to detect EDMR in SiC MOSFET devices. Figure 1 shows a photograph of the EDMRoC printed integrated circuit board. The microwaves are integrated using an array of voltage-controlled oscillators (VCO) (indicated by the red rectangle) with overall dimensions of 6cm x 12 cm, which can be mounted between two permanent magnets (Figure 2). The sample is positioned above the microwave antenna using a customized holder PCB (Figure 3) providing the electrical connections for the CP experiments. In conventional EDMR the device is inserted inside a microwave cavity at a fixed microwave frequency to create a standing wave with maximal magnetic and minimal electrical component of the microwaves at the position of the device for highest magnetic resonance signal and lowest losses. A spectrum is then obtained by scanning the applied magnetic field. In contrast, in EDMRoC the microwave frequency is not fixed, allowing for scanning of either the magnetic-field or the microwave frequency. Moreover, for sensitive detection, conventional EDMR uses magnetic field modulation, which causes induction currents in the device circuitry that yield a background signal, while in EDMRoC this can be avoided using frequency modulation. Hence intrinsically, EDMRoC is expected to result in lower background signal and better signal intensity, though in the previous solar cell work [2] signal-to-noise ratios worse by at least a factor 10 were reported for EDMRoC. In this work, by the clever design of the device and device holder, matching the dimensions of the microwave antenna, we demonstrate signal-to-noise ratios that are very similar in state-of-the-art cavity-based EDMR and in EDMRoC (Figure 4). Moreover, the large sweepable magnet used in conventional EDMR was found to result in additional noise, such that EDMRoC using a permanent magnet as in Figure 2 demonstrates an even better signal-to-noise ratio (Figure 5). A detailed comparison will be presented to compare representative microwave powers, demonstrating EDMRoC as a versatile, compact, and low-cost alternative to conventional EDMR.