Laser pulses with a duration of one femtosecond or shorter can be generated both in the IR-VIS and in the extreme UV, but the deep UV is a spectral region where such extremely short pulses have not yet been demonstrated. Here, a method for the synthesis of ultrashort pulses in the deep UV is demonstrated, which utilizes the temporal and spatial harmonics that are generated by two noncollinear IR-VIS pulses in a thin MgF2 plate. By controlling the groove-envelope phase of the IR-VIS pulses, spatial harmonics are concatenated to form deep UV waveforms with a duration of 1.5 fs.Waveforms with durations short enough to probe the electronic timescale can be generated both in the extreme UV and in the IR-VIS region of the electromagnetic spectrum. High-order harmonic generation can be used to generate isolated attosecond pulses and pulse trains in the extreme UV [1], and since very recently the coherent synthesis of optical pulses is used to generate subcycle optical waveforms in the IR-VIS region [2]. In the deep UV (DUV), where many basic aromatic molecules absorb radiation and undergo photochemical reactions [3], pulses with such extremely short durations have not yet been demonstrated [4]. Exploiting nondegenerate frequency mixing in a hollow waveguide [5], in filamentation [6] or in a thin transparent solid [7], it has been possible to generate pulses with a duration on the order of 10 fs [5]. A similar pulse duration has been achieved by achromatic frequency doubling of visible ultrashort pulses [8]. Also self-compression of DUV pulses by filamentation has been demonstrated, yielding comparatively short pulses of ∼ 15 fs [9]. The shortest pulse duration reported to date of 2.8 fs has been achieved by frequency conversion in a gas cell [10], which, however, requires extremely short (< 4 fs) fundamental pulses in the IR-VIS.Despite these engagements of several groups in the development of pulse generation methods, spectroscopy with sub-10-fs DUV pulses has not often been reported to date. A fundamental difficulty is rooted in the large group velocity dispersion of any optical component in the DUV, causing a DUV pulse to be readily broadened and distorted before it reaches the sample. As a rare exception, it was recently demonstrated that ∼ 10-fs-DUV pulses, generated by chirped-pulse four-wave mixing [11], can be used in pump-probe spectroscopy of an aqueous solution of thymine [3].For applications like transient absorption spectroscopy, DUV pulses with durations shorter than currently available would be very useful. For example, in order to observe the transient change of band structures in dielectrics and the related screenings in the presence of a strong field pulse, probe pulses are required that i) have a duration shorter than the optical period of the strong field pulse, ii) encompass the wavelength of the dielectric bandgap, and iii) are available at the sample position.Here, a scheme for the coherent synthesis of DUV waveforms is presented. The principle is the concatenation of spatial and temporal harmonic...