A coherent superposition of rotational states in D2 has been excited by nonresonant ultrafast (12 femtosecond) intense (2 × 10 14 Wcm −2 ) 800 nm laser pulses leading to impulsive dynamic alignment. Field-free evolution of this rotational wavepacket has been mapped to high temporal resolution by a time-delayed pulse, initiating rapid double ionization, which is highly sensitive to the angle of orientation of the molecular axis with respect to the polarization direction, θ. The detailed fractional revivals of the neutral D2 wavepacket as a function of θ and evolution time have been observed and modelled theoretically.PACS numbers: 42.50. Hz, 33.80.Gj, 33.80.Wz The importance of being able to enforce spatial order on an initially random ensemble of molecules has been recognized since the discovery of steric effects in chemical reactions [1]. Traditional 'brute force' techniques employing strong DC fields [2,3] have recently yielded to new, more subtle and yet more powerful and versatile techniques using intense laser systems [4,5]. In particular intense femtosecond pulses have been successfully used to align molecules along an axis for application in areas such as the study of fragmentation dynamics [6,7], high harmonic generation [8,9] and the creation of single cycle laser pulses [10]. In this case the alignment of a molecule (or spatial ordering of an ensemble of molecules) evolves temporally following the creation of a rotational wavepacket by a linearly polarized laser pulse of far shorter duration than the natural period of rotation.In this Letter, we report on a detailed ultrafast study of the temporal evolution of such a rotational wavepacket in the neutral deuterium molecule D 2 . The wavepacket is created impulsively by a 12 femtosecond laser pulse, with temporal and angular ordering probed at some later time with a similar pulse that initiates sequential double. Such high resolution measurements represent the state-of-theart in ultrafast molecular physics in the high rotational frequency limit as dictated by this most fundamental and theoretically tractable of molecules.It is known that an intense linearly polarized laser pulse interacting with an ensemble of molecules generates a degree of spatial alignment from a random ensemble [4,5]. The only condition for this phenomenon is that the molecular polarizability is anisotropic. Thus, the induced dipole moment created in the interaction with the electric field of the laser generates a torque that causes the axis of maximum polarizability to librate around the polarization vector of the laser field. Quantum mechanically, the process is described as a sequence of Rabi-type cycles accompanied by the exchange of two quanta of angular momentum between the molecule and the laser field. If the aligning pulse duration is much greater than the rotational period, the system evolves adiabatically to the the so-called pendular states, which dissipate as soon as the laser pulse passes [12]. However, when the pulse duration is much shorter than the rotational perio...