CCSD3ZF0000100000001NJPL3IF0PDS200000001 = SFDU_LABEL RECORD_TYPE = STREAM SPACECRAFT_NAME = GALILEO_ORBITER INSTRUMENT_NAME = "NEAR INFRARED MAPPING SPECTROMETER" INSTRUMENT_ID = NIMS OBJECT = TEXT NOTE = "Description of special processing applied to 'garbled' NIMS EDRs from the G1 encounter, pointed to from label of 'ungarbled' EDRs." PUBLICATION_DATE = 1998-05-01 END_OBJECT = TEXT END At least two NIMS anomalies occurred during the G1 encounter. Beginning with the G1JNHOTMAP01 observation, near Galileo's closest approach to Jupiter, NIMS data appeared 'garbled', though in a systematic way which gave hopes of recovery. Sometime after the G1INNSPEC_01 observation, the data were still garbled, but no longer in a systematic way. Subsequent analysis concluded that the phase 2 NIMS RAM software had halted at that point, presumably due to radiation, but that CDS was still picking up garbage out of the NIMS buffer. (A later reload of the RAM software restored functionality.) The data acquired between the first and second anomalies was mostly reconstructed, based on an analysis of the RAM processing and the systematic appearance of the data. It was concluded that radiation most likely altered a variable in the RAM so that the formatter (*) lost sync with the code. An algorithm was developed involving bit shifts and byte order re-arrangements, based on the assumption that the formatter was one step ahead of the code (in a cycle of 4 steps, one for each mirror position in an RTI). Since the 'ungarbled' data appeared plausible to NIMS scientists (especially off-limb data which could be assumed to be dark) and since there was a reasonable scenario for the behavior of the RAM software, the NIMS team feels justified in distributing the ungarbled data with a high probability that it is correct. The algorithm mentioned above assumes that all wavelengths were selected, as in the G1INNSPEC_01 observation. In such cases, the original data could be completely reconstructed, except for a couple of bits at one end of the observation. But when wavelength editing in the instrument was selected, as in G1JNHOTMAP01 and most of the other garbled observations, this was not entirely true. Due to the interaction of the garbling mechanism and the wavelength editing code, and depending on the edit pattern selected, data from some wavelengths lost two bits of significance, and data from some others were entirely lost. (*) See the NIMS instrument paper and VOLINFO.TXT for background to this discussion, and see SPECPROC.TXT on the G1 Cube CD-ROM (forthcoming) for further details of the algorithm and a complete description of limitations on data accuracy for each of the 11 ungarbled observations. [Prepared by R. Mehlman, 01 May 1998]