The low-temperature (LT) gas atmosphere carburization processing, invented by Swagelok Co. for the surface hardness improvement of 316L austenitic stainless steel (SS), was applied to other SSs, corrosion resistant steels and superalloys [1] including [2]. The model of colossal supersaturation with interstitial carbon atoms [3,4] of the surface grains crystal lattice, currently accepted as explanation of the SSs surface carburization effects, was automatically extended to the LT surface carburized IN-718 -the subject of this report. The predicted dilatation of matrix lattice that would normally happen in LT carburized IN-718, is denied by the anomaly [2] reported for the IN-718 carburized at 843K, i.e. an apparent contraction instead of dilatation of the crystalline lattice, occurring inside the topmost layer ≈ 2µm thick. What motivated our study was this anomaly, together with the huge modification of peaks shapes in the X-ray diffractograms (XRD) observed when we scanned the carburized alloy surface. We intended to check the model validity of the colossal lattice supersaturation with C atoms of the grains from inside the carburized case, tens of µm-s thick and the grains microstructure, in order to understand the anomaly by use of the JEM-ARM200F microscope. The ion milling procedure of thinning was adapted with the aim of accessing the microstructure of the topmost layer, a few µm-s thick, of the carburized at 843K free surface of IN-718. This layer contains a highly stressed and fragile material. The adaptation consisted in: (a) a two stage thinning operation, with TEM examination at the end of each stage, the 2 nd stage ion milling being applied to the already perforated samples after the 1 st stage milling; (b) the dimpling and ion milling of only the uncarburized side of the TEM disk at the 1 st stage and the further ion milling of both sides of the already thinned area at the 2 nd thinning stage; (c) the use of Cu contamination of the carburized side during the 1st stage ion milling as a protection and marker of the free carburized surface. The procedure offers the certitude of accessing the microstructure (nanostructure in our case) of the topmost layer, roughly ≈5µm thick. We also used a method of rough estimation of depth of the TEM observed nanostructure features. The nanostructure features identified in the topmost layer about 5µm thick do not resemble the grains microstructure predicted by the carbon supersaturation model. Our findings are the following: (a) the fragmentation into nanocrystals of the initial matrix rough grains, together with the formation of an amorphous phase that contains either much carbon or no carbon at all, but always contains oxygen and the main alloy elements. We identified low amounts of carbide nanocrystals of type Cr23-xFexC6, M23C6 and MC, with FCC structure and lattice parameters of 10.62 Å -11.12 Å and 4.48Å. (Figure- The LT carburization treatment triggers a more complex transformation than the bare carbon paraequilibrium diffusion through the matrix interstitial ...