In this note, we show that the latest spin grating measurement of spin helix by Koralek et al. [Nature 458, 610 (2009)] provides strong evidence of the infinite spin diffusion length of any spin polarization along the direction perpendicular to the effective magnetic field from the Dresselhaus and Rashba spin-orbit couplings with identical strengths in (001) GaAs quantum wells, predicted by Cheng et al. [Phys. Rev. B 75, 205328 (2007)]. PACS numbers: 72.25.Rb, 72.25.Dc, As one of the spintronic focuses, manipulations of electron spin in spin-orbit-coupled solid state systems have been extensively investigated due to the potential application in future quantum computation and quantum information processing.1 In confined semiconductors with zinc-blende structure, both the Dresselhaus spin-orbit coupling (SOC) 2 due to the bulk inversion asymmetry and the Rashba one 3 due to the structure inversion asymmetry are present, and the interplay of them gives rise to amazing effects as reported in the literature. 4,5,6,7,8,9,10,11,12,13 For example, an infinite spin relaxation time for spin-polarization along the (110) [or (110) depending on the sign of the Rashba term] direction was predicted by Averkiev and Golub 4 in (001) GaAs quantum wells (QWs) when the cubic term of the Dresselhaus SOC is excluded, and the two leading terms, i.e., the linear Dresselhaus term and the Rashba one, are of the same strengths. With the cubic term, the spin relaxation time along the (110) direction becomes finite, but still much longer than those in the other directions.
6Bernevig et al.8 predicted a persistent spin helix (PSH) by analyzing the symmetry with identical Dresselhaus and Rashba strengths, which was observed by Koralek et al.11 in the latest transient spin grating experiment.14 Moreover, Cheng et al. 12 studied the anisotropic spin diffusion/transport in (001) GaAs QWs with identical Dresselhaus and Rashba strengths and predicted that in the direction perpendicular to the effective magnetic field from the Dresselhaus and Rashba terms, i.e., (110) if the later is along the (110) direction, 15 the spin diffusion length is infinite regardless of the spin polarization direction. It seems rather strange that the spin diffusion length can be still infinite for the spin polarization direction other than the direction of the effective magnetic field. According to the well-known relation L s = √ D s τ s widely used in the transient spin grating works, 16 only a finite spin diffusion length L s can be obtained for a spin polarization other than the (110) direction, because the spin diffusion coefficient D s and the spin relaxation time due to the D'yakonov-Perel' (DP) mechanism 17 τ s are both finite. However, to determine the spin diffusion length via the transient spin grating signal, as pointed out by Weng et al., 13 the correct expression should beThis formula naturally gives an infinite spin diffusion length because φ = 0 for identical Dresselhaus and Rashba strengths. 13 In the following part, we will discuss the underlying physi...