Broadband ultrashort terahertz (THz) pulses can be produced using plasma generation in a noble gas ionized by femtosecond two-color pulses. Here we demonstrate that, by using multiple-frequency laser pulses, one can obtain a waveform which optimizes the free electron trajectories in such a way that they acquire the largest drift velocity. This allows us to increase the THz conversion efficiency to 2%, an unprecedented performance for THz generation in gases. In addition to the analytical study of THz generation using a local current model, we perform comprehensive 3D simulations accounting for propagation effects which confirm this prediction. Our results show that THz conversion via tunnel ionization can be greatly improved with well-designed multicolor pulses. DOI: 10.1103/PhysRevLett.114.183901 PACS numbers: 42.65.Re, 32.80.Fb, 52.50.Jm Ultrashort pulses in the terahertz (THz) range (from ∼0.1 to ∼30 THz) are extremely important for various timeresolved studies in molecular physics, chemistry, material sciences, and security applications [1][2][3][4][5][6][7][8]. One of the major challenges in this field is the development of THz emitters producing high peak intensities. So far, besides conventional devices such as antennas, photoconductive switches, etc., two main techniques have been explored for producing subps THz pulses with energies in the microjoule range. The first method is based on optical rectification in second-order nonlinear crystals [9]. Pumped by multi-mJ single color pulses, this technique requiring phase matching can generate THz pulses with 10 μJ energy, but the bandwidth is limited to a few THz. Recently, large-sized organic crystals were used to deliver THz pulses with GV=m electric field strength, and a conversion efficiency of about 1% was demonstrated [10]. The second method is based on focusing a femtosecond pulse together with its second harmonic into a gas cell and create a plasma [11][12][13][14][15][16][17][18][19][20][21][22][23][24]. In such two-color pump setup, free electrons produced by tunnel ionization acquire a nonzero drift velocity and generate a quasi-dc current which is responsible for THz emission [19]. The mechanism underlying THz generation in gases is intrinsically related to the optically induced stepwise increase of the free electron density near the extrema of the ionizing optical field [15,16,22]. An easy explanation is that the Fourier transform of a steplike function in time has its maximum near the zero frequency. Besides, critical for the generated THz energy is a pronounced asymmetry in time of the pump wave shape with respect to the field extrema, which dictates the electron drift velocity. This gas-based scheme for THz generation provides higher breakdown threshold and broader spectral ranges than the method involving crystals [11][12][13][17][18][19][20]. THz pulses in gases with high field strength > 1 GV=m were simulated in [16]; however, the highest reported THz energies (5 μJ) correspond to conversion efficiencies of about 10 −4 only.In this Let...