Ice crystals in cirrus frequently exhibit the shape of a bullet rosett
e composed of multiple bullets that radiate from a junction center. Th
e scattering phase function of these ice crystals, pertinent to the ra
diation budget of cirrus, may differ from the one obtained for ice cry
stals with a simple geometrical shape. In this paper, the authors stud
ied the sensitivity of the scattering phase function of a bullet roset
te to its geometrical characteristics: the shape, aspect ratio, and sp
atial orientation. In doing so, they defined first an idealized bullet
rosette according to the current knowledge of the crystalline structu
re and nucleation process of bullet rosettes. The scattering phase fun
ction was computed with a ray-tracing method. The scattering phase fun
ction of a bullet rosette varies with its shape, and the lateral and b
ackward scattering tends to increase with the number of bullets/bullet
rosettes. This is due to the interaction of light scattered by a bull
et with its adjacent bullets. This feature qualitatively agrees with t
he earlier experimental results reported for irregularly shaped partic
les. However, for a bullet rosette with 3D random orientation, the eff
ect of this interaction is much smaller than expected. The normalized
scattering phase function locally differs only by about 20% from one s
hape to another. Earlier studies were made for ice crystals randomly o
riented in a 3D space, and in this case, the scattering properties hav
e been represented by 1D phase functions (versus the scattering angle)
. For a bullet rosette with preferred orientation, the scattering patt
ern (which is not azimuthally symmetrical and so depends on scattering
angles in the 3D space) varies significantly with the shape of the bu
llet rosette and the direction of incident light. Although the shape o
f a bullet rosette with 3D random orientation does not greatly affect
the general feature of normalized scattering phase functions, its geom
etrical shape still remains an important factor for scattering and mic
rophysical properties of cirrus. This is due to the fact that the geom
etrical cross section of a bullet rosette, perpendicular to the incide
nt light, changes with its shape. Thus, optical properties such as the
extinction coefficient of cirrus with a given ice water content may c
hange significantly with the ice crystal shape.