Bragg waveguides are fundamental components in photonic integrated circuits and are particularly interesting for mid-IR applications in high index, highly nonlinear materials. In this work, we present Bragg waveguides fabricated in bulk chalcogenide glass using an ultrafast laser. Waveguides with near circularly symmetric cross sections and low propagation loss are obtained through spatial and temporal beam shaping. Using a single-pass technique, the waveguide and Bragg structure are formed at the same time. First through sixth order gratings with strengths of up to 25 dB are realized, and performance is evaluated based on the modulation duty cycle of the writing beam. Chalcogenide (ChG) glasses are known for their excellent mid-IR transparency and large nonlinear refractive indices of up to 1000 times that of fused silica [1,2]. These unique traits make them attractive in a wide range of applications. In particular, ChG glasses are suitable substrate materials for fabricating photonic integrated circuits (PICs), due to inherently large χ 3 nonlinearities with ultrafast response times and low two-photon absorption at telecom wavelengths. These properties become especially important in applications such as high-data-rate signal processing [3][4][5]. In such PIC devices, Bragg waveguides are often employed as basic building blocks, enabling operations such as 2R regeneration [6,7], and all-optical switching [8]. Fabrication of these structures generally relies on thin film deposition and various photolithography schemes. However, thin-film processes incur restrictions when building multilayer structures for complex optical interconnects by limiting devices to a planar geometry. Ultrafast laser writing offers great design flexibility with its capability for making three-dimensional structures [9,10] and is a proven technique to form high-quality waveguides in bulk optical substrates. Extensions of this technology have also been applied to the fabrication of Bragg waveguides in fused silica using several approaches, such as the point-by-point technique [11][12][13], and the multiscan technique [14]. Applying these methods to ChG glasses, however, presents a unique design challenge. The high refractive index of these materials induces spherical aberrations at the focus of the writing beam, which are further compounded by nonlinear effects brought about by high-intensity laser pulses. These interactions often lead to self-focusing and filamentation, producing highly asymmetrical waveguides with an elongated cross section and multiple guiding regions [15]. Mitigation of these effects is essential for fabricating high-quality waveguides in ChG glasses.Recently, it has been demonstrated that temporal [16] and spatial beam shaping [17] may be used to control the size and shape of the cross section of a laser-written waveguide. These techniques, combined with adjustment of other processing parameters such as writing speed, pulse energy, and repetition rate, have produced nearly symmetric waveguides with propagation losses ...