A terahertz time-domain spectroscopy system based on a femtosecond Yb:KGW laser, photoconductive emitters made using a low-temperature-grown (LTG) GaAs layer annealed at different temperatures, and a photoconductive detector made using a Si-doped GaBiAs epitaxial layer, has been demonstrated. Useful spectral bandwidth of the system, that might be used in spectroscopy experiments, was up to 3 THz and its dynamical range exceeded 50 dB when the LTG GaAs emitter annealed at 4208C was used. It has been concluded that the breakdown field of as-grown layers is much larger than that of annealed layers; this process provides rather large optical-to-THz radiation conversion efficiencies for the emitters made from moderately annealed LTG GaAs.Introduction: Optoelectronic terahertz (THz) systems, in which femtosecond laser pulses are used both for the generation and for the detection of THz pulses either by the optical rectification effect or by employing photoconductive components made from semiconductors with subpicosecond electron lifetimes are finding an increasing number of applications in spectroscopy and imaging [1]. Typically, Ti:sapphire laser pulses with a central wavelength around 800 nm and photoconductors manufactured from low-temperature-grown (LTG) GaAs epitaxial layers are used for this purpose. Recently, more compact, efficient, and cost-effective than Ti:sapphire laser solid-state and fibre laser systems that are generating femtosecond pulses at near-infrared wavelengths from 1 to 1.5 mm have been developed [2,3]. GaAs is not sensitive at these wavelengths; therefore alternative semiconductor materials with narrower energy bandgaps have been examined [4]. Ion-implanted InGaAs was used for manufacturing ultrafast photoconductors sensitive at 1.5 mm wavelength [5], whereas optoelectronic THz components activated by a femtosecond 1 mm wavelength laser were manufactured from the GaBiAs alloy [6].In this Letter, we propose the manufacture of optoelectronic THz range components sensitive to near-infrared radiation from as-grown or annealed at moderate ( 4008C) temperatures LTG GaAs layers. It is known that as-grown LTG GaAs contains a large density (10 19 to 10 20 cm 23 ) As-antisite defects (As Ga ) that create an impurity band in the middle of the energy bandgap of GaAs. The optical absorption coefficient for the electron transitions from this band to the conduction band at room temperature is 10 4 cm 21 at 1 mm wavelength and 1.6 × 10 3 cm 21 at 1.55 mm [7].