The 11 July 1992 occultation of Uranus by U103 (m(K) = 10.1) was obser
ved using the 5-m Hale telescope on Palomar Mountain in California, th
e 4-m telescope at Cerro Tololo Inter-American Observatory (CTIO) in C
hile, and the nearby 2.2-m telescope at European Southern Observatory
(ESO). All observations were taken using InSb aperture photometers and
K (lambda similar to 2.2 mu m) filters and provided high-quality prof
iles of the uranian rings. The ESO and Palomar ring event times have b
een incorporated into a comprehensive orbit model for the elliptical r
ings using all available Earth-based and Voyager occultation data, The
kinematical model was used to determine the radius scale and geometry
of the U103 occultation, as well as to provide absolute timing calibr
ation for the CTIO light curve, which was reconstructed from two-dimen
sional digital scans of a high-speed strip chart, All nine classical r
ings were clearly observed during both ingress and egress. In addition
, a sharp feature appeared in the CTIO ingress light curve with an orb
ital radius of 50,026.89 +/- 0.39 km, very close to the mean radius of
the lambda ring of 50,026.3 +/- 0.6 km found by M. R, Showalter (Scie
nce 267, 490-493, 1995) from an analysis of Voyager 2 images. The CTIO
feature is well above the noise: its equivalent width of E = 0.32 +/-
0.14 km corresponds to a 5-sigma detection. It is the only such signa
ture in the entire CTIO lightcurve, other than the previously known ri
ngs. The characteristic ring-like shape of the profile, its high SNR,
and its radial location all support the identification of this feature
as an Earth-based detection of the lambda ring. At the same time, if
the ring were azimuthally homogeneous with E greater than or similar t
o 0.32 km, it would have been clearly visible in the CTIO egress and P
alomar light curves, but no such features were found, The A ring is th
us azimuthally clumpy, resembling to some degree Neptune's are-like Ad
ams ring. At the nearby ESO station, a suggestive ingress feature appe
ared with a radius of 50,023.01 +/- 0.28 km, but the data are too nois
y to permit a positive identification; The orbital characteristics of
the A ring and its azimuthal brightness profile cannot be uniquely ext
rapolated from the Voyager encounter epoch to the time of the U103 occ
ultation because the mean motion and orbital radius of the ring are to
o uncertain. However, additional detections in archival Earth-based oc
cultation data or from future observations could allow a much better d
etermination of the dynamics of this dusty and clumpy ring. (C) 1996 A
cademic Press, Inc.