polymer network, leading to novel actuation and morphing applications. [3][4][5][6] Moreover, nematic LCEs [1,7] exhibit unique mechanical properties, such as a higher viscoelasticity and a soft elasticity, by which the materials can deform under little increase in stress. The ability to reversibly switch them to a classic rubber elasticity, which is attained in an isotropic state by increasing the temperature (T), or light irradiation, [8][9][10][11] can further provide an LCE with a dynamic nature in terms of mechanical damping, [12][13][14] adhesion, [15,16] and friction. [17] Although their applicability as dynamic functional units has been well demonstrated in these systems, the changes to the underpinning mechanical properties, for example, stress-strain and viscoelastic responses associated with the phase transition, remain largely unexplored. Such a fundamental understanding will also help in material optimization for fine tuning of their functions. Thus, the present experimental study focuses on uncovering the correlation between the local nematic scaler order parameter Q and the basic mechanical properties by exploiting the non-glassy photoresponsive nematic LCE with azobenzene units [8][9][10]18] in the main chain.A polydomain nematic LCE was investigated as a simple system that has no macroscopic anisotropy as in an aligned monodomain system. [19] Polydomain LCEs are obtained by crosslinking monomer components in their isotropic state, and are often called "isotropic-genesis" LCEs. If they are crosslinked under a nematic state with a long-range nematic order, they are called "nematic-genesis." [20] The nematic-genesis LCE can show Schlieren textures [2,21] as in the low-M w nematic LC because they are simply frozen and memorized by crosslinking. By contrast, the isotropic-genesis polydomain LCE typically shows a mosaic of small randomly oriented birefringent nematic domains when the system enters the nematic phase. Although each nematic domain attempts to grow under the nematic mean field, the randomly frozen network topology, which operates as a random disorder, [22][23][24] disturbs the domain coarsening. As a result, each nematic domain typically shows a characteristic length of ≈1 µm with a unique relative orientational correlation, [25] which displays a Maltese cross pattern under depolarized light scattering (DPLS). [7,26] To the naked eye, polydomain LCEs appear to be opaque under visible light because of the size of the scattering centers, that is, nematic domains, which in an isotropic phase become Nematic liquid crystal elastomers (LCEs) generally show soft elasticity, masking entropic elasticity inherent in crosslinked networks. They macro scopically deform with little stress increase under straining because of the soft shear mode attained by nematic director rotations. Moreover, the nematic interaction in mainchain LCEs can arrest the ergodic response to cycling strain. It manifests hysteresis, slow relaxation, and increased vis cosity, which critically affect their mechanical applications...