magnon. Let us now discuss the character of the state of GdNi$_{2}$B$_{2}$C below 3.5 K. A recent magnetoelastic study [@Massalami-GdNi2B2C-singlecrystal-1] on single crystal GdNi$_{2}$B$_{2}$C demonstrated the presence of substantial magnetoelastic and anisotropic exchange interactions, in particular below $T<T_{R}$. The magnitude of the $\epsilon^{\gamma}$ strain mode (which leads to symmetry lowering from four-fold tetragonal to two-fold orthorhombic) is very large and increases with decreasing temperature leading progressively to an orthorhombic-distorted magnetic state wherein the moments, due to entropy arguments, approach equal amplitudes. Based on the suggestion of Detlefs et al [@Detlefs-GdNi2B2C-XRES], the magnetic structure below $T_{R}$  is either a  transverse modulated state with moment orientation away from the b-axis in the bc-plane or a modified spiral-like structure which, due to the low symmetry (2mm) of the \[100\] direction, is likely to suffer fanning or bunching (becoming more stronger as the temperature is decreased). Tomala et al [@Tomala-GdNi2B2C-MES], on exploring these two structural possibilities, argued that the $^{155}$Gd Mossbauer spectra at 4.2K $<$$T<T_{R}$ were better fitted with a bunched spiral-like state. In this Mossbauer analysis, the c-component was found to be almost equal ( $\sim$75% at 4.2 K) to the b-component, a result that does not reflect the 2mm-symmetry of the \[100\] 