The theories of Brownian motion, the Debye rotational diffusion model, and hydrodynamics together provide us with the Stokes–Einstein–Debye (SED) relation between the rotational relaxation time of the -th degree Legendre polynomials , and viscosity divided by temperature, . Experiments on supercooled liquids are frequently performed to measure the SED relations, and $D_{\rm t}\tau_{\ell}D_{\rm t}$ is the translational diffusion constant. However, the SED relations break down, and its molecular origin remains elusive. Here, we assess the validity of the SED relations in TIP4P/2005 supercooled water using molecular dynamics simulations. Specifically, we demonstrate that the higher-order values exhibit a temperature dependence similar to that of , whereas the lowest-order values are decoupled with , but are coupled with the translational diffusion constant. We reveal that the SED relations are so spurious that they significantly depend on the degree of Legendre polynomials.

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