Semiconductor quantum dots (QDs) coupled to high quality optical microcavities provide essential components for solid state cavity quantum electrodynamics systems. Indium Arsenide (InAs) QDs are one of the most promising candidates for quantum emitters due to their discrete density of states and high oscillator strength. When they are combined with small mode volume and high quality microcavities, strong light-matter interaction can be observed. Application of a magnetic field to QDs is necessary for several quantum information applications which require multi-level emitter structures [1][2]. Magnetic field lifts the degeneracy of QD exciton spin states due to the Zeeman effect, providing access to the individual QD spin states. In addition, a magnetic field can be useful as a method to tune QD emission frequency, which can be used to control the interaction between quantum emitters and an optical cavity [3][4][5]. We apply a magnetic field to photonic crystal cavity devices with embedded InAs QDs, and demonstrate strong coupling between individual QD exciton spin states and a photonic crystal cavity.The sample consists of a 160 nm thick Gallium Arsenide (GaAs) membrane with a single layer of InAs QDs in the middle of the GaAs layer. By using electron beam lithography and dry etching, high quality factor (> 8,000) photonic crystal cavities are fabricated. The sample is mounted in a cryostat and cooled down to a temperature of 4-50 K. We apply magnetic fields in parallel to the sample growth direction (Faraday configuration) up to 7 T by using a superconducting magnet and measure photoluminescence (PL) of the coupled QD-cavity devices.Under the magnetic field, each QD exciton splits into two energy branches based on electron/hole spin status. The energy shift of the two exciton states is caused by both the Zeeman energy splitting and diamagnetic shifting. At 7 T, the σ + exciton spin state red-shifts by about 0.2 nm and the σ -exciton spin state blue-shifts by about 0.6 nm. By using these tuning ranges, we can selectively bring only one of the excitonic states into resonance with the cavity. In Fig. 1, we demonstrate strong coupling between a QD spin state and a photonic crystal cavity by using the magnetic field as a tuning method of a QD emission frequency. The sample temperature is initially set to 34 K, where the QD emission wavelength is about 0.12 nm blue shifted from the cavity mode. When the magnetic field is applied, the σ + exciton spin state red shifts and passes through the cavity mode frequency. At around 2.1 T, the σ + state becomes resonant with the cavity and we observe clear anti-crossing between an exciton state and a cavity mode as shown in Fig. 1(a). In a similar way, Fig. 1(b) shows a strong coupling between the σ -state and the cavity with a magnetic field tuning.Next, we investigate the effect of magnetic field on the coupling strength between QD emitters and a cavity. In Fig. 2(a), we show QD-cavity spectra with temperature scanning at fixed magnetic fields of 0 and 1 T. At 0 T, there is no...