We investigate the quasiparticle relaxation and low-energy electronic structure in undoped SrFe 2 As 2 exhibiting spin-density wave ͑SDW͒ ordering using optical pump-probe femtosecond spectroscopy. A remarkable critical slowing down of the quasiparticle relaxation dynamics at the SDW transition temperature T SDW = 200 K is observed. From temperature dependence of the transient reflectivity amplitude we determine the SDW-state charge gap magnitude, 2⌬ SDW / k B T SDW = 7.2Ϯ 1. The second moment of the Eliashberg function, ͗͑ប͒ 2 ͘ = 110Ϯ 10 meV 2 , determined from the relaxation time above T SDW , is similar to SmFeAsO and BaFe 2 As 2 indicating a moderate electron phonon coupling.The discovery of high-temperature superconductivity in iron-based pnictides 1-3 has attracted a great deal of attention recently. The question of the relative importance of the lattice and spin degrees of freedom for the superconducting pairing interaction becomes immediately apparent since the superconductivity appears upon doping the parent materials 4 which show the spin-density wave ͑SDW͒ ground state. Understanding the parent SDW compounds also from the point of electron-phonon, and not only the spin-spin and spincharge interactions, is therefore beneficial for understanding the nature of the superconducting coupling in the doped compounds.Time-resolved spectroscopy has been very instrumental in elucidating the nature of the electronic excitations in superconductors, particularly cuprates 5-19 and recently also iron pnictides. 20-24 Moreover, the relaxation kinetics can give us valuable information on the electronic structure 6 and electron-phonon coupling. 25 In this work we present a time-resolved femtosecond spectroscopy study of SrFe 2 As 2 in the normal and the SDW state. From the photoexcited carrier relaxation dynamics we determine the electron-phonon coupling parameters and the charge gap magnitude. We compare the results with recent data 24 in SmFeAsO and find that they are similar both in the SDW and normal state with some minor differences in the magnitude of the response at high temperatures.Optical experiments were performed using the standard pump-probe technique, with 50 fs optical pulses from a 250-kHz Ti: Al 2 O 3 regenerative amplifier seeded with an Ti: Al 2 O 3 oscillator. We used the pump photons with doubled ͑ប P = 3.1 eV͒ photon energy and the probe photons with 1.55 eV photon energy. The pump and probe polarizations were perpendicular to each other and oriented with respect to the crystals to obtain the maximum amplitude of the response at low temperatures. The pump and probe beam diameters were determined by measuring the transmittance of calibrated pinholes mounted at the sample position. 26 Single crystals of SrFe 2 As 2 were prepared by the self-flux method. 27 For optical measurements the cleaved crystals were glued on a Cu plate mounted in an optical liquid-He flow cryostat.In Fig. 1 we plot the temperature dependence of ⌬R / R transients in SrFe 2 As 2 . Below T SDW the transients are dominated by the ...