65 projection imaging technique, allows for larger FOVs to be 66 investigated in shorter times. However, in conventional XGI, 67 the directional sensitivity of the measurement depends on the 68 relative orientation of the linear gratings and local anisotropic 69 microstructure 16. To expand the directional sensitivity of this 70 technique, a set of measurements is typically required with the 71 sample rotated around an axis parallel to the beam direction. 72 Instead of a linear grating, a periodic array of multi-circular 73 gratings can be used to capture 2D-omnidirectional X-ray 74 scattering signals within a single projection shot, removing 75 the necessity of rotation of the sample relative to the grat-76 ing alignment 28. Including the additional measurements with 77 tilted rotation axes, the reduction in acquisition time achieved 78 with this single-shot method is significant. Recently, the num-79 ber of required detector pixels to resolve the fringes in each 80 unit cell has been considerably reduced. As a result, the sys-81 tem autocorrelation length, spatial resolution and FOV can 82 be more effectively decoupled 29. Although speckle-based 83 imaging 30 could in principle provide similar information, this 84 technique requires high resolution, thus limiting the actual 85 FOV obtained in a single shot. Additionally, for the speckle-86 based approach it is still not completely clear how to quanti-87 tatively interpret the scattering signal. Here, the X-ray tensor 88 tomography with circular gratings providing single-shot 2D-89 omnidirectional scattering sensitivity is presented. 90 The experimental setup is illustrated in Fig. 1(a). The sam-91 ple stage is capable of introducing a tilt (θ) of the rotation (ϕ) 92 axis. The circular unit cell grating has a global period P which 93 is half of the repetition period of the unit cell and a local period 94