Abstract. Strong-field control of acetylene fragmentation by fully determined fewcycle laser pulses is demonstrated. The control mechanism is shown to be based on electron recollision and inelastic ionization from inner-valence molecular orbitals.Chemistry is usually perceived as breaking and making molecular bonds. These processes that typically occur on the timescale of tens of femtoseconds (fs) to nanoseconds are preceded and ultimately governed by the much faster intra-molecular motion of electrons that proceeds on the sub-femtosecond timescale [1,2]. This timescale matches the light oscillations of laser pulses carried at frequencies in the visible and near-infrared. As the electric field of strong laser pulses is capable of exerting forces onto the electrons that are comparable to those of the binding forces, it becomes possible to drive the intra-molecular electron density by light. Deterministic steering, however, requires fully controlled laser electric fields, for example few-cycle pulses with a locked carrier-envelope (CE) offset frequency. Using such pulses it has been shown that the localization of an electron during dissociation of D + 2 [3, 4] and CO + [5], as well as the directionality of multiple dissociative channels of CO [6] can be controlled.In this submission we extend this scheme from simple diatomics studied so far to chemically more relevant polyatomic molecules. Particularly interesting for applications are hydrocarbon molecules. It has been shown previously that dissociation of these molecules is accompanied by extraordinarily rich internal electronic dynamics [7,8] that are still far from being understood.We study the fragmentation of acetylene, C 2 H 2 , subject to fully determined few-cycle laser electric fields. In our experiments we generate 4.5 fs laser pulses by spectral broadening of ≈ 25 fs laser pulses from a Titanium-Sapphire laser amplifier system in a 1 m long hollow-core glass capillary filled with argon and subsequent recompression by several bounces from chirped mirrors. The pulses, with a spectrum centered around 750 nm are directed into an ultrahigh vacuum chamber where they are focused onto a cold supersonic jet of randomly aligned acetylene molecules. The three-dimensional momenta of the resulting ionic fragments from a single molecule are recorded as described previously [9]. As at maximum only one molecule interacts with one laser pulse it becomes possible to measure the duration and the carrier-envelope (CE) phase of each of the few-cycle pulses delivered at the repetition rate of 5 kHz on a single-shot basis [10][11][12] instead of actively stabilizing it, leading to improved accuracy. The peak intensity of the laser pulses on target was 1.5×10 14 W/cm 2 , as determined from a separate calibration measurement using single ionization of argon atoms in circularly polarized light [13]. a