A novel and universal interference structure is found in the photoelectron momentum distribution of atoms in intense infrared laser field. Theoretical analysis shows that this structure can be attributed to a new form of Coulomb-field-driven backward-scattering of photoelectrons in the direction perpendicular to the laser field, in contrast to the conventional rescattering along the laser polarization direction. This transverse backward-scattering process is closely related to a family of photoelectrons initially ionized within a time interval of less than 200 attosecond around the crest of the laser electric field. Those electrons, acquiring near-zero return energy in the laser field, will be pulled back solely by the ionic Coulomb field and backscattered in the transverse direction. Moreover, this rescattering process mainly occurs at the first or the second return times, giving rise to different phases of the photoelectrons. The interference between these photoelectrons leads to unique curved interference fringes which are observable for most current intense field experiments, opening a new way to record the electron dynamics in atoms and molecules on a time scale much shorter than an optical cycle.PACS numbers: 32.80. Wr, 33.60.+q, 61.05.jp In the ionization process of atoms in intense laser field, the electron wave packet (EWP) may follow different paths from its bound state to the continuum in the combined laser and Coulomb fields. The interference between the EWPs might create richly structured patterns in the final photoelectron distribution, which inherently encode the temporal and spatial information of the ions and electrons. For example, a holographic interference structure was recently observed in the photoelectron momentum distribution (PMD) of metastable xenon atom ionized by a 7 µm free-electron laser pulse [1]. This interference structure was explained as interference between the direct and the laser-driven forward-scattered EWPs generated within the same quarter-cycle of the laser pulse, providing an efficient way in exploring the structure and the dynamics of the atoms and molecules with attosecond temporal and angstrom spatial resolution. Thereafter, the photoelectron interference structure has been extensively investigated for a broad range of laser parameters covering tunneling to multiphoton ionization regimes, however, a full understanding of its underlying physics has not yet been achieved [2][3][4][5][6][7][8].Note that for the formation of this specific holographic interference structure, the reference wave, i.e., the direct electron, upon ionization, was assumed to be very weakly affected by the ionic Coulomb field, while the rescattered one, experienced strong Coulomb focusing and passed close to the ion, was considered as the signal wave. Moreover, previous studies have suggested that the Coulomb field plays a negligible role in the holographic interference patterns [1,2,4]. On the other hand, it has been generally accepted that the ionic Coulomb field plays a pivotal role in the ...