A nonlinear propagation known as filamentation is produced when intense femtosecond laser pulses propagate in air. The dynamic equilibrium between the Kerr self-focusing and plasma-defocusing effects leads to filamentation[1–3]. Due to its potential applications in supercontinuum emission[4–6], extreme ultraviolet (EUV) emission[7,8], air lasing[9,10], THz radiation[11,12], remote sensing[13], guiding of corona discharges[14], machining[15] and weather control[16], filamentation of femtosecond laser pulses in optically transparent media has attracted a great deal of attention in recent years. One of the most profound effects during femtosecond filamentation is intensity clamping phenomena. It was observed in 1995 by Braun et al.[17] that the pulse energy inside a filament is generally constant within long propagation distances. Kasparian et al.[18] firstly proposed intensity clamping in 2000. Intensity clamping has a significant impact on the diameter and length of the filament[19]. The gas density effect on filamentation has been investigated[20,21]. The simulation by Geints et al.[20] shows that lowering the air pressure in the focusing zone can improve the highest attainable laser pulse intensity by an order of magnitude. The molecular number density of a gas varies with pressure, changing medium properties and affecting the filamentation process. However, Couairon et al.[21] numerically investigated filamentation at various air pressures by varying the parameters of the pulse in the propagation model. They found that the clamping intensity is insensitive to pressure. The pulse cumulative effect by high-repetition-rate lasers can also influence the local gas density in the filamentation region. After filamentation, the plasma will recombine rapidly, accompanied by the generation of shock waves and heat. Finally a ‘low-density hole’ is formed in the filament zone[22,23]. The low-density region will evolve at the rate of air molecule thermal diffusion, that is, up to milliseconds[24]. The low-density hole can be accumulated by pulses. As high-energy, ultrashort, high-repetition-rate laser systems become commercially available, research on the cumulative effects at repetition rates up to the kHz range can be experimentally achieved. The cumulative effects on filament-related applications of THz generation[25], wake dynamics[26] and the fluorescence[27] have been recently reported. However, the cumulative effect of the laser repetition rate on the intensity inside the filament, which is important to understand and control filament-related applications, is still unclear.