Using a first-principles density functional approach, we calculate the firs
t-order Raman intensities of alpha -quartz. The dynamical charge tensors, v
ibrational frequencies and eigenmodes, and polarizability tensors are obtai
ned within a perturbational approach. We calculate Raman intensities by eva
luating the variation of the polarizability tensors for finite displacement
s of the atoms. Calculated intensities agree well with experimental data, s
howing an average error of 13% for relative intensities. Using our first-pr
inciples results as reference, we critically examine simple models for the
Raman activity. We first consider a bond polarizability model, for which th
e parameters are derived from our first-principles results for alpha -quart
z. This model reproduces the first-principles intensities with an average e
rror of 15%. In the attempt of reducing this error, we then introduce a mod
el in which the symmetry of the first neighbor shell is accounted for in th
e most general way. For alpha -quartz, this model extends the bond polariza
bility model, which is recovered as a special case. The model, which fully
accounts for the local symmetry, describes the first-principles results wit
hin an average error of 12%, marginally improving upon the bond polarizabil
ity model (15%). However, when these models with parameters derived for alp
ha -quartz are applied to a cristobalite polymorph, only the bond polarizab
ility model shows good transferability properties. These results support th
e use of the bond polarizability model as a simple scheme for calculating R
aman intensities in tetrahedrally bonded SiO2 systems.