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By numerically solving the time-dependent Schr?dinger equation, we observe a remarkable strong-field interference patte in the photoelectron momentum distribution of a hydrogen atom ionized by a few-cycles laser pulse. This inter-ference patte is joined together with the familiar near-forward strong-field photoelectron holographic interference. By applying the strong-field approximation theory, we investigate the formation of this interference patte, which arises from the interference between the backward rescattered part and the direct part of the tunneling ionized electron wave packet. We demonstrate that this backward rescattered photoelectron holographic interference can also be observed in a more realistic parallel two-color laser field. These results pave a new way to look into the atomic and molecular structure with ultrafast timescale.