Small-scale Ring Structure Observed In Cassini UVIS Occultations Miodrag Sremčević LASP, CU Boulder UVIS team meeting, Boulder January 5, 2010 Cassini UVIS stellar occultations ● ● High Speed Photometer (HSP) 110 – 190nm >100 stellar occultations of the rings ● 1 - 8ms sampling rate (mostly 1ms used) ● Rings radial resolution from few to ~50m ● Signature of structure down to meter scale (1) A, B rings: self-gravity wakes (<50m) (2) A, B rings: overstable waves (100-200m) (3) B ring: irregular axisymmetric (~100m) (4) C ring: weak structure (<few 10m) Example occultation (β Cru Rev98) NOISE LEVEL F RiNG B RiNG C RiNG A RiNG Throughout main rings (C, B, Cassini, A rings) the noise by far exceeds expected (Poisson) values. β Persei occ. track “turnaround point” =tangent to rings = ∞ radial resolution Orbital motion ~20km/s For highest resolution: Match occultation track azimuthal motion to the orbital motion of the rings. Occultation moves as ring particles. Background: synthetic image from a UVIS occultation A ri ng Special occultation geometry β Persei Rev116 occultation At occultation turnaround (R=131,436km): ● ● Radial resolution (in 1ms) dR < 1cm Ring orbital motion = 17.0 km/s Occultation azimuthal speed = 16.2 km/s ==> Azimuthal resolution dL =~ 80cm ● Projected star diameter =~ 20cm ● Fresnel zone =~ 300cm β Persei Rev116 light curve Stellar level ~transparent gap ~opaque SG wake Optical depth histogram Size of the SG wakes and gaps Correlations: looking for particle signature Is it possible to observe individual particles? ● ● Limiting factor is Fresnel zone (2 – 3 m) VIMS γ Crucis occultations (R104 & R106) have Fresnel zone ~120m, and projected star ~200m, yet the overstable waves λ=~150m are observed Summary First time directly resolved A ring SG wakes ● Unique occultation with 80cm resolution (only diffraction limited) ● ~30% of the ring is transparent (τ<0.05) ~30% of the ring is opaque (τ>1.5) ~40% of the ring in intermittent state ● Opaque wakes are seen as large as 200m Purely transparent regions are bit shorter ● Only handful more opportunities until 2017: highest observation priority! Extra Slides (2) Overstable waves in inner A ring Wavelet transform Coadded wavelet Optical depth 9/12 Overstable waves time series ~150m 10/12 Overstable waves autocorrelation UVIS Local N-body simulation (H. Salo) 11/12 What is no structure signature? [p r r −〈p〉][pr −〈p〉] ∑ C r = 2 ∑ [p r −〈p〉] ● ● No structure == no correlations (stellar counts are independent and only the medium occulting the star can induce correlations) Anything different from 0 in the correlation plot indicates ring structure 4/14 Autocorrelation C(Δr) (1) Selfgravity wakes in A ring ΦV=32° ΦV=60° ΦV=73° ΦV=83° ΦV=99° ΦV=106° ΦV=112° ΦV=131° ΦV=148° Correlation lag Δr [km] ΦV=occultation track angle in the corrotating plane. Strong dependence on occultation geometry. 5/14 2D autocorrelation UVIS data N-body simulation (H. Salo) 6/14 Autocorrelation C(Δr) (3) Irregular B ring structure ΦV=41° ΦV=61° ΦV=74° ΦV=78° ΦV=100° ΦV=102° ΦV=105° ΦV=111° ΦV=116° Correlation lag Δr [km] Very weak dependence on occultation geometry! 10/14 Irregular B ring structure Structure has ~100m radial scale ● Axisymmetric (no angle dependence in occultations) ● Irregular in appearance (these are not waves) ● Very distinct from self-gravity wakes ● Viscous instability? - In 80-ies proposed as mechanism to produce irregular B ring structure - Fell out of favor since the needed theoretical criteria were not met (ring particles turned to be too inelastic) - Salo & Schmidt (2009) show that viscous instability is a valid mechanism, but still requires more elastic particles ● 11/14 Porco(2005) Double star occultations γ Lupi secondary No signature of the γ Lupi secondary Narrow ringlets (~few 100m) in inner A ring make ring self-similar ==> double star signature No structure here and thus no secondary star signature (SG wakes are much smaller than double star separations) 12/14 (4) Mysterious C ring structure γ Lupi secondary ● ● Secondary star signatures in many occultations indicate presence of structure in C ring. Possibly ~axisymmetric narrow ringlets or waves on tens of meters radial scale 13/14 Extra: UVIS occultation geometry (B,φ) determine line of sight (and were used to explain optical depth variation of A ring self-gravity wakes) ΦV= angle in the corrotating plane (describes occultation track motion) orbital motion towards star φ occultation track integration area ΦV radius Extra: Selfgravity wakes in A ring Strong correlations up to 100m both positive and negative FFT Autocorrelation Extra: SG wakes - UVIS vs local N-body Alp Vir Rev8 ingress UVIS HSP detector view (N-body simulations by H. Salo) simulation Sig Sgr Rev11 simulation Extra: Overstable waves tilt angle ~0 Extra slide: Pan wakes tilt angle (~1') Extra: overstable waves local N-body simulations (H. Salo) Extra slide: OS power spectrum UVIS Local Nbody simulation