We use Rayleigh and Love wave Green's functions estimated from ambient seismic noise to study crustal structure and radial anisotropy in the tectonically complex and seismically active region west of the Sichuan Basin and around the Eastern Himalaya Syntaxis. In agreement with previous studies, low velocity zones are ubiquitous in the mid-lower crust, with substantial variations both laterally and vertically. Discrepancies between 3-D shear velocity from either Rayleigh (VSV) or Love (VSH) waves are examined both in view of non-uniqueness of tomographic solutions and radial anisotropy. Low shear wave speed and radial anisotropy with VSH > VSV are most prominent in mid-lower crust in area northwest to the Lijiang-Muli fault and around the Red River and Xiaojiang faults. This anisotropy could be caused by sub-horizontal mica fabric and its association with low velocity zones suggests mica alignment due to flow in deep crustal zones of relatively low mechanical strength.
 Despite decades of research, the mechanism of crustal deformation and eastward expansion of the Tibetan Plateau are still under debate. As the conjunction between the Tibetan Plateau and the Yangtze Indo-China blocks and the southern end of the trans-China seismicity belt, SE Tibet is of particular interest. GPS data [Zhang et al., 2004; Shen et al., 2005] and geological studies [Wang et al., 1999; Wang and Burchfiel, 2000] show that in this region the upper crust rotates clockwise around the Eastern Himalayan Syntaxis. But how this surface motion is related to deformation at larger depth is not yet known.
 Along with geological data, including constraints on shortening and uplift history, the topography of this region – in particular, the gentle slope from ∼5 km on the Plateau to less than 1 km in the southeast and the steep margin west of the Sichuan Basin – was used by Royden et al.  to argue for flow in the deep crust. The area is intersected, however, by major fault systems, such as the Red River, Lijiang-Muli, Xianshuihe-Xiaojiang, and Longmenshan faults (Figure 1), which seismicity and GPS measurements [Shen et al., 2005] indicate are active block boundaries. These observations mostly pertain to the (near) surface, and more direct information about the deeper crust is needed to understand the large scale deformation this region.
 Radial anisotropy, that is, the difference in propagation speed of horizontally and vertically polarized waves – inferred, respectively, from Love and Rayleigh wave data – has been used to diagnose specific styles of crustal deformation [Shapiro et al., 2004; Moschetti et al., 2010]. For example, crustal flow can produce a horizontal mica fabric, which, in turn, can produce significant radial anisotropy [e.g., Weiss et al., 1999; Shapiro et al., 2004]. Following our work on crustal heterogeneity and azimuthal anisotropy in the southeastern margin of Tibet [Yao et al., 2008, 2010], we determine radial anisotropy from ambient noise tomography [e.g., Shapiro et al., 2005; Yao et al., 2006] with empirical Green's functions (EGFs) for short- and intermediate period Rayleigh and Love wave propagation. A major objective of this study is to establish spatial correlations between LVZs and the type and strength of radial anisotropy.
2. Data and Method
 It is now well established that cross correlation of ambient noise recorded at two seismic stations can be used to measure the Green's function, hereinafter referred to as the empirical Green's function (EGF), of wave propagation between these stations (see auxiliary material, Section 1) [Lobkis and Weaver, 2001; Weaver and Lobkis, 2004; Roux et al., 2005]. For our study in SE Tibet we estimate Rayleigh wave EGFs from vertical component and Love wave EGFs (Figures S1a and S1b) from transverse component data recorded in 2003 and 2004 at a temporary array of 25 stations in SE Tibet and at KMI (Kunming, Yunnan), a permanent station of the global seismograph network (Figure 1).
 Following Yao et al. [2006, 2008] we use a 3-step procedure to invert for 3-D shear wave velocity variations. In the first step, we measure phase velocity dispersion curves for appropriate station pairs (Figures S1c and S1d). In the second step, we use these dispersion curves to construct phase velocity maps at different periods (7–40s); for each point on a 0.5°-by-0.5° grid, phase velocities are then calculated for a range of frequencies. As an example, dispersion curves of Rayleigh and Love waves at grid point (26°N, 102°E) are presented in Figure 2a. Finally, we use the neighborhood algorithm (NA) [Sambridge, 1999a, 1999b] to invert (for each grid-point) the dispersion data for variations of VSV and VSH with depth (Figure 2b); these 1-D profiles are combined into 3-D VSV and VSH models (Figure S2).
3. Shear Wave Velocity Structure and Radial Anisotropy
 The VSV model obtained here from ambient noise interferometry agrees with the results that Yao et al.  obtained from a combination of ambient noise interferometry and two-station analysis. In particular, LVZs are prominent in the middle and lower crust and some are bounded by faults, such as the Xianshuihe and Lijiang-Muli faults (Figure S2 of the auxiliary material).
VSV and VSH are generally similar in the upper crust and upper mantle, but large differences occur in the middle and lower crust. A comparison of Love wave dispersion calculated from VSV profiles (obtained from vertical component data) with the observed dispersion shows that these differences (and, hence, the implied radial anisotropy) are required by our data. For example, Figure 2a shows that for (25°N, 102°E) Love wave dispersion calculated from VSV (cyan dashed line) is inconsistent with the observations (top red line with 1σ error bars), which are explained well by the VSH model (black line).
 We quantify radial anisotropy, ψ, as 2(VSH − VSV)/(VSH + VSV)*100%. In the upper crust ψ is less than 2% (Figure 3a), which we consider insignificant. In the middle and lower crust VSH is generally larger than VSV (Figures 3b, 3c, and 4), but strong anisotropy (ψ > 5%) is detected in Songpan-Ganze block and in the southern part of our study region, between the Red River and the Xiaojiang fault. In the center of the study area a zone of relatively high VSV (ψ < 0) is present in the middle and lower crust (Figures 3b, 3c, and 4). We note that uncertainty in the Moho depth only has a small effect on the estimate of radial anisotropy discussed here (see auxiliary material, Section 3).
4. Discussion and Conclusions
 GPS data [Shen et al., 2005] suggest different surface velocities in areas bounded by the Xianshuihe-Xiaojiang, Litang, Lijiang-Muli, and Red River faults. Our current and previous studies reveal substantial crustal heterogeneity, and the tomographically observed contrasts across the Litang, Red River, and Xiaojiang faults at shallow depth (Figures S2a and S2d) and the Lijiang-Muli and Xianshuihe-Xiaojiang faults in the middle crust (Figures S2b and S2e) suggest that these faults are indeed major tectonic boundaries. Combined with other geophysical observables (e.g., heat flow, resistivity, Poisson's ratio) the anomalously low shear velocities indicate low (mechanical) rigidity [Yao et al., 2008, 2010]. The ubiquitous LVZs may thus represent loci of ductile deformation in the deep crust. By themselves, however, they do not provide unequivocal evidence for horizontal flow.
 Our analysis of short-to-intermediate period horizontal and vertical component data suggests that, in general, radial anisotropy is weak at shallow depth but strong in the deep crust (with VSH significantly larger than VSV, that is, ψ > 0) (Figures 3 and 4). Interestingly, strong radial anisotropy occurs near the LVZs (that is, low VSV) that were detected by Yao et al.  and which are confirmed here. Indeed, in the middle crust of the Songpan-Ganze block and the part of the Yangtze craton between the Red River and Xiaojiang faults, VSV is low and ψ is large (VSH > VSV). This is not always the case, however. Near the north end of the Luzhijiang fault, for instance, VSV is relatively high and larger than VSH (ψ < 0). We note that radial anisotropy here may not be significant since Love wave dispersion is, within error, consistent with the VSV model (Figures 2c and 2d). The contrast with surrounding areas suggests that the small region confined by the Xianshuihe and Muli fault is relatively stable sub-block in the westernmost part of the Yangtze craton.
 For a more quantitative analysis of the relationship between wavespeed and radial anisotropy we plot radial anisotropy (ψ) versus shear velocity (dlnVSV) for different tectonic regions and crust layers. In the upper crust (Figure 5a) radial anisotropy is small (less than 2%) and there is no correlation between VSV and ψ. However, in the middle and lower crust, Figures 5b and 5c reveal a strong (negative) correlation between wavespeed and radial anisotropy in the lower crust beneath the western part of the study area (the Songpan-Ganze block, the westernmost part of the Yangtze craton and the Lhasa block) with LVZs (that is, dlnVSV < 0) coinciding with areas where VSH > VSV (that is, ψ > 0). We also note that the LVZs themselves cannot simply be explained by radial anisotropy (see auxiliary material, Section 4, Figure S6).
 Radial anisotropy in the deep crust (with VSH > 0) can be produced by a preferred orientation of mica crystals [Weiss et al., 1999; Nishizawa and Yoshitno, 2001]. Shapiro et al.  invoked a sub-horizontal mica fabric to explain radial anisotropy inferred from Love and Rayleigh wave propagation and to argue for thinning and lateral (channel) flow in the deep crust of Central Tibet. The strong radial anisotropy in and near LVZs inferred here may thus suggest (flow-induced) sub-horizontal alignment of mica in the mechanically weak zones of the deep crust beneath SE Tibet and SW China. This is consistent with deep crustal channel flow [e.g., Royden et al., 1997], but lateral heterogeneity and the major faults in the region likely play an important role in controlling the pattern of such flow.
 We thank two anonymous reviewers for their constructive comments, which helped us improve the manuscript. We also thank the Editor Michael Wysession for his assistance. This work was supported by NSF grant EAR-0910618.