Instrument Information
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| IDENTIFIER |
urn:nasa:pds:context:instrument:issna.co::1.1
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| NAME |
IMAGING SCIENCE SUBSYSTEM - NARROW ANGLE
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| TYPE |
IMAGER
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| DESCRIPTION |
Introduction to the Cassini Imaging Science Subsystem: Narrow Angle Camera Instrument Overview=================== The Cassini ISS consists of two fixed focal length telescopes, anarrow angle camera (NAC) and a wide angle camera (WAC). The NAC is95 cm long and 40 cm x 33 cm wide, and has a focal length of 2002.70+/- 0.07 mm in the clear filter. The two cameras together have a massof 57.83 kg, and sit on the Remote Sensing Palette (RSP), fixed tothe body of the Cassini Orbiter, between the Visual and InfraredMapping Spectrometer (VIMS) and the Composite Infrared Spectrometer(CIRS), and above the Ultraviolet Imaging Spectrometer (UVIS). Theapertures and radiators of both telescopes are parallel to each other. The NAC has its own set of optics, mechanical mountings, CCD, shutter,filter wheel assembly, temperature sensors, heaters, and electronics,the latter of which consists of two parts: the sensor head subassemblyand the main electronics subassembly. The Sensor Head electronicssupports the operation of the CCD detector and the preprocessing ofthe pixel data. The Main Electronics provide the power and performall other ISS control functions, including generating and maintaininginternal timing which is synchronized to the Command Data System(CDS) timing of 8 Hz, control of heaters, and the two hardware datacompressors. The Cassini Engineering Flight Computer (EFC) is aradiation-hardened processor that controls the timing, internalsequencing, mechanism control, engineering and status dataacquisition, and data packetization. The NAC is an f/10.5 reflecting telescope with an image scale of ~6microrad/pixel, a 0.35 deg x 0.35 deg field of view (FOV), and aspectral range from 200 nm - 1100 nm. Its filter wheel subassemblycarries 24 spectral filters: 12 filters on each of two wheels. Thisallows for in-line combinations of filters for greater flexibility.Each wheel is designed to move independently, in either the forwardor reverse direction, at a rate of 3 positions per second. A homingsensor on each wheel defines a home wheel position, and wheelpositioning can be commanded absolutely or relatively. Unlike the WAC, the NAC is thermally isolated from the RSP in order tominimize the effects of RSP thermal transients on the NAC imagequality. The temperature of the CCD is controlled by a passive radiator,directly connected to the focal plane, along with an active'performance' heater on the CCD to adjust the temperature. Thetemperature of the optical elements is controlled by active heaterspositioned along the optical path. These optical elements are kept towithin 1 degree Celsius to maintain camera focus without an activefocusing mechanism. Low expansion invar spacers are also used. Theradiator subassembly also includes two sets of spacecraft-controlleddecontamination heaters which are used to minimize deposition ofvolatile contaminants on either the detector or radiator and tominimize radiation damage to the CCD. All heaters are commandable (ONor OFF) during flight. Optics------ The narrow angle camera optics were specially designed to improve onthe quality and resolution of images of the bodies in the Saturnsystem returned by Voyager. It is based on a Ritchey-Chretienreflector design. The focal plane field of view is limited by thesize of the CCD. The NAC point spread function (PSF) was designed tobe approximately the same physical size as a pixel in the near-IR.The full width at half maximum (FWHM) of the PSFs of the NAC throughthe clear filters is 1.3 pixels. The nominal pixel scale is 5.9907microradians/pixel. All the reflective optical elements within the NAC (the primary andsecondary mirrors) are manufactured of fused silica; all refractiveNAC elements (such as the field correctors and the window on thesealed CCD package) are made of either fused silica or single-crystalvacuum-UV-grade calcium fluoride. Antireflection coatings consistingof single layer MgFl2 were deposited on the field correctors and CCDwindow; a multi-layer MgFl2 coating was applied to the primary andsecondary aluminum-coated mirrors to enhance reflectivity. A fusedsilica quartz plug is placed immediately in front of the CCD packageto protect the detector against radiation damage and to minimizeradiation- induced noise in the images. Geometric fidelity in the NAC is very good: pre-flight analyticalcalculations indicate distortions of less than a pixel at the cornersof the field of view, and subsequent observations of the Pleiades andthe open cluster M35 set the value to 0.45 pixels. Filters------- The ISS filter assembly design -- consisting of two filter wheels anda filter changing mechanism -- is inherited from the Hubble SpaceTelescope WF/PC camera. Each wheel is designed to move independently,in either the forward or reverse direction, at a rate of 3 positionsper second in the NAC. A homing sensor on each wheel defines a homewheel position: wheel positioning can be commanded absolutely orrelatively. The Cassini Imaging Science Team has deliberately duplicated 63% ofthe filters in both the NAC and WAC. These include sevenmedium/broadband filters from the blue to the near-IR forspectrophotometry, 2 methane and 2 continuum band filters foratmospheric vertical sounding, 2 clear filters, and a narrow band Halpha filter for lightning observations. The clear filter is in the 'home' slot of each filter wheel, since itwas deemed that sticking of a filter wheel, should it occur, was mostlikely to occur in the home position. Typically a clear filter in onewheel is combined with a color filter in the other wheel, thoughtwo-filter combinations can also be used. Because of its reflecting optics and its unique ability to see in theUV, only the NAC carries filters for UV observations. The lumigencoating provides a unique spectral capability, unavailable on eitherthe Voyager or Galileo imaging systems, which Cassini carries to theouter solar system for the first time. It enables spectral responsedown to 200 nm. To take advantage of this capability, we have spannedthe range from 230 nm to 390 nm with three UV filters: UV1, UV2, andUV3. The NAC filter wheel also contains narrow-band filters for atmosphericstudies. Methane absorption bands and continuum wavelengths areavailable using the MT1/CB1, MT2/CB2 and MT3/CB3 filters. (CB1 is a2-lobed continuum filter, with lobes on each side of the methaneabsorption band.) A HAL filter is also included for observing H-alphaemissions from lightning. Finally, the NAC carries three polarization filters covering thevisible spectrum: P0, P60 and P120. As their names indicate, thesepolarizers have principle transmission axes separated by 60 degrees,in order to measure intensity and the degree and direction of linearpolarization regardless of camera orientation. The NAC also has asingle infrared polarizer, IRP0. The polarizers are, of course, to be used in combination with otherspectral filters, so filter placement was important. In the NAC, the 3visible polarizers and the one IR polarizer can all be used inconjunction with a suite of spectral filters on the opposite wheelcovering the UV to the near-IR. Table 1: ISS NAC Filter Characteristics Filter Lambda_cen Lambda_eff Science Justification----------------------------------------------------------------------UV1 258W 264 aerosolsUV2 298W 306 aerosols, broadband colorUV3 338W 343 aerosols, broadband color,polarizationBL2 440M 441 medium-band color, polarizationBL1 451W 455 broadband colorGRN 568W 569 broadband colorMT1 619N 619 methane band, vertical soundingCB1 619N 619 2-lobed continuum for MT1CB1a 635 635CB1b 603 603RED 650W 649 broadband colorHAL 656N 656 H-alpha/lightningMT2 727N 727 methane band, vertical soundingCB2 750N 750 continuum for MT2IR1 752W 750 broadband colorIR2 862W 861 broadband color; ring absorption bandMT3 889N 889 methane band, vertical soundingCB3 938N 938 continuum for MT3, see thru Titan hazeIR3 930W 928 broadband colorIR4 1002LP 1001 broadband colorCL1 611 651 wide open, combine w/wheel 2 filtersCL2 611 651 wide open, combine w/wheel 1 filtersP0 617 633 visible polarization, 0 degreesP60 617 633 visible polarization, 60 degreesP120 617 633 visible polarization, 120 degreesIRP0 746 738 IR polarization, see thru Titan haze Table 2: NAC Two-Filter Bandpasses Filters lambd_cen lambda_eff--------------------------------UV2-UV3 316 318RED-GRN 601 601RED-IR1 702 702IR2-IR1 827 827IR2-IR3 902 902IR4-IR3 996 996 (All wavelengths in nm. Central wavelengths (lambda_cen) are computedusing the full system transmission function. Effective wavelengths(lambda_eff) are computed using the full system transmission functionconvolved with a solar spectrum. Bandpass types: SP = short wavelengthcutoff; W = wide; N = narrow; LP = long wavelength cutoff.) With the exception of the clear filters and the polarizers, thefilters are all interference filters manufactured using an ion-aideddeposition (IAD) process which has the effect of making the filterstemperature and moisture tolerant, and resistant to delamination.Conventional interference filters have passbands which shift withtemperature. The shift can be significant for narrowband filterstargeted to methane absorption bands or the H_alpha line. Temperatureshifts for IAD filters is typically an order of magnitude or moresmaller than for conventional filters and is insignificant over thetemperature range (room temperature to 0 degrees C) relevant tocalibration and operation of the Cassini cameras. The NAC visible polarizers consist of a thin film (less than 1 micronsthick) of a polarizing polymer deposited between two fused silicaplates. The infrared polarizer has a 1 mm-thick layer of Polarcor(trademark Corning) cemented between two slabs of BK7-G18 glass.Polarcor is a borosilicate glass impregnated with fine metallic wires.Ideal polarizers block only photons whose electric vector isorthogonal to the principal axis of the polarizer. The visiblepolarizers fall short of this ideal behavior in two ways. Theytransmit too little of either polarization in the ultraviolet, andtoo much of the light polarized orthogonal to the principal axis inthe near-infrared. Their performance is best between 450 nm and 650nm where the principal axis transmission is between 0.45 and 0.65,and the orthogonal transmission is less than 1%. The useable range ofthe visible polarizers extends from the UV3 filter near 350 nm to theCB2 filter at 750 nm. The infrared polarizer has much betterperformance over its range (700 nm - 1100 nm) where the principaltransmission is greater than 0.9 and the orthogonal transmission is0.001 or less. Shutter------- Between the filter wheel assembly and the CCD detector is the shutterassembly, a two blade, focal plane electromechanical system derivedfrom that used on Voyager, Galileo and WFPC. To reduce scatteredlight, the shutter assembly was put in the optical train `backwards ,with the unreflective side towards the focal plane. Each blade movesindependently, actuated by its own permanent magnet rotary solenoid,in the sample direction: i.e., keeping the blade edge parallel to thecolumns of the CCD. The shutter assembly is operated in 3-phases: open(one blade sweeps across the CCD), close (the other blade sweepsacross the CCD to join the first), and reset (both bladessimultaneously sweep across the CCD in the reverse direction to thestart position). There are 64 commandable exposure settings which can be updated duringflight if so desired. These correspond to 63 different exposure times,ranging from 5 milliseconds to 20 minutes, and one `No Operationsetting. The shortest nonzero exposure is 5 msec. In the ISS flightsoftware, the time tag on the image is the time of the close of theshutter. Because of mechanical imperfections in the shutter mechanism,there is a difference between the commanded exposure time and theactual exposure time, and a gradient in exposure time across the CCDcolumns. At an operating temperature of 0 degrees C, the meandifferences in the NAC for commanded exposure times of 5, 25 and 100ms were measured to be 0.98, 1.52 and 0.97 ms, respectively. In allcases the actual exposure times are less than the commanded times.There is also a small temperature dependence to these shutter offsets. The 1024th column is illuminated first in both cameras. In the NAC,this column is illuminated for ~ 0.3 msecs longer than the firstcolumn. This value is independent of exposure time and reasonablyindependent of temperature. The expected precision or repeatabilityof an exposure (equal to the standard deviation of actual exposuredurations measured at any one location on the CCD in ground tests) is= 0.03 msec for the NAC. Corrections for the mean and thespatially-dependent shutter offsets are incorporated into the CassiniISS calibration software (CISSCAL). The shutters were tested forlight leak. None was detectable in the NAC at a fluence level of12,000 times full well exposure on the closed shutter. Detector-------- The CCD detector used in the Cassini ISS was manufactured by Loral,packaged by JPL, and employs three phase, front-side-illuminatedarchitecture. The imaging area -- the region on which light is focused-- is a square array of 1024 x 1024 pixels, each 12 microns on a side.The CCDs on both cameras were packaged, hermetically sealed andfronted by a fused silica window. The CCD's response to light is determined by the spectral dependenceof each pixel's quantum efficiency: i.e., the number of electronsreleased in the silicon layer for each photon incident on it. Infront-side-illuminated CCDs (like that in the Cassini ISS), theoverlying polysilicon gate structures don t transmit UV light. Toachieve the required UV response, a UV-sensitive organic fluorescentmaterial called lumogen was vacuum-deposited onto the CCD at 80degrees C after it was bonded. In this 0.6 micron layer, UV photonsare converted into visible photons in the 540 to 580 nm range thatreadily penetrate the silicon below. Under vacuum conditions, thelumogen layer would tend to evaporate when CCD temperatures reached60 degrees C. For this reason, the CCD sealed packages wereback-filled with inert argon gas to a half atmosphere pressure. Allflight candidate CCDs were coated with lumogen before the two flightCCDs were chosen and assigned to each camera. The efficiency of a CCD in the near-IR depends on its thickness, ormore precisely on the thickness of the very thin, high purity siliconlayer which is epitaxially grown over a thicker (~500 micron)substrate. It is the photons absorbed in the epitaxial layer that areconverted into the signal electrons that are subsequently collectedand sampled. Nearly all of the near-IR photons actually penetratebeyond the epi layer and create charge in the substrate. However, thepurity contrast between the substrate and the epi layer preventssubstrate-generated charge from entering the epi layer and beingcollected. Thus, the 1100 nm quantum efficiency is essentially thefraction of incident flux which is absorbed in the thin layer of puresilicon: the thicker the epi layer, the higher the infraredsensitivity. However, the thicker this layer, the lower the spatialresolution. A compromise was made in the manufacture of the CCD toyield some response near 1100 nm while maintaining high spatialresolution. The epi layer is 10 - 12 microns thick on Cassini andresults in a quantum efficiency (QE) of ~1% at 1000 nm. A compromise involving the near-IR response was also made in choosingthe CCD operating temperature. At Saturn, this temperature is -90 +/-0.2 degrees C and is a compromise between yielding an acceptably lowdark current (= 0.3 e-/sec/pixel) and maintaining a reasonablenear-IR response (which is diminished at low temperatures). CCDthermal control is achieved by means of balance between passiveradiation to space, which alone would maintain the CCD below itsoperating temperature at Saturn, and active heater control. Theradiator of each camera also supports a decontamination heater (35watts in all) that can heat the CCD to +35 degrees C to reduce thedeposition of volatile contaminants on either the detector or theradiator. (Because damage to the CCD due to cosmic rays can beannealed at elevated temperatures, the CCD operating temperatureduring cruise, when data were not being collected, was maintained at0 degrees C to minimize such damage.) The detector system includes an unilluminated region 8 samples wide -the 'extended pixel' region - extending into the negative sampledirection in the serial register. These pixels get read out first.Moreover, once an entire row of 1024 pixels is read up into theserial register and out to the signal chain, the read-out continuesfor 8 more clock cycles, or 'overclocked pixels,' to provide ameasure of the offset bias, the DN value that corresponds to zerosignal level. The extended pixel region and the overclocked pixels inprinciple provide two independent measures of offset bias and asample of the horizontal banding pattern that may be used to removethe pattern in images lacking dark sky. (A discussion of thehorizontal banding problem can be found in [PORCOETAL2004].) In the NAC, the extended region of the readout register, and thefirst 13 columns into the serial register are corrupted by agrounding problem with the epoxy that bonds the pure silicon layer tothe substrate. This causes spurious swings in the voltage during theinitial 'clockings' of data out of the CCD into the signal chain.Consequently, these columns of CCD data are unreliable, and the NAC'sextended pixel region cannot be used to monitor the camera's bias ornoise state. Scientific Objectives===================== See [PORCOETAL2004] for an in-depth description of Cassini ISS scienceobjectives. Camera Operation================ Operational States------------------ The ISS has three operational power states: On, Sleep and Off. In theOn state, the cameras are Active or Idle. In this state, both thespacecraft replacement heaters and ISS decontamination heaters areoff. The camera software has active control over the performanceheaters to set appropriate operating temperatures for the optics andCCD detector. The Active sub-state is entered to collect science dataas well as for calibration and maintenance activities. Commandexecution in the active state includes science data readout, filterwheel movement, shutter movement, activation of light flood andcalibration lamps, and other high power consuming activities. Idle isa background state in which no commands are executing. When thecamera is in Idle, uploads can be processed, real-time and 'trigger'commands can be accepted from the CDS, and macros can be stored. Theexecution of any command sends the camera into the Active state. Thecamera always returns to Idle state after completing a commandsequence. In the NAC, peak power consumption during active imaging is26.2 watts. The ISS Sleep state is a non-data taking low power state that is usedwhen no activity is planned for an extended period of time. Duringthis state, the sensor head and main ISS electronics are drawingpower, and the optics and CCD heaters are on to maintain operatingtemperature limits. Spacecraft controlled replacement heaters areoff. The decontamination heaters may be used, if necessary. In Sleep,the NAC consumes 22.3 watts. In OFF, no power is drawn by the ISS. The spacecraft controlledreplacement heaters and ISS decontamination heaters may be turned onwhen necessary. The replacement heaters keep the ISS within allowableflight nonoperating temperature limits and the decontamination heaterscan be used to provide for CCD protection from the radiationenvironment and from the condensation of volatiles. In this state,the NAC consumes 8.4 watts. Detector Modes-------------- The CCD has the capability of being commanded to operate in full mode(i.e., 1x1) or either 2x2 or 4x4 on-chip pixel summation modes. Thelatter two modes are used for either enhancing signal-to-noise and/ordecreasing the data volume and/or read-out time at the expense ofspatial resolution. The full well of the CCD is roughly 120,000e-/pixel. Four gain states are available: for imaging faint objects(high gain, Gain 3) and bright objects (normal gain, Gain 2), and tomatch the output of the 2x2 (Gain 1) and 4x4 (Gain 0) full wells. Thesummation well can hold only 1.6 x 10^6 electrons; this corresponds tofull well with 4X4 summing. However, the relation between number ofelectrons in the signal and the digital data numbers (DN) into whichthe signal is encoded starts to become nonlinear above 10^6 electronsbecause at this signal level, the on-chip amplifier becomesnon-linear. For this reason, in the lowest gain state (Gain 0), thefull scale signal is set to correspond to ~ 10^6 electrons at 4095 DN. Table 3: NAC Gain States Gain State e-/DN Notes----------------------------------------------------------------0 233 +/- 29 Designed for 4x4 summation mode1 99 +/- 13 Designed for 2x2 summation mode2 30 +/- 3 Normal gain; used in 1x1 summation mode3 13 +/- 2 Used in 1x1; chosen to match read noise The capability also exists within the ISS to reduce the effect ofblooming, the phenomenon whereby a highly overexposed pixel can spillelectrons along an entire column of pixels, and sometimes along a row,when the full well of the CCD is exceeded. The default camera setuphas anti-blooming on, with the option to turn it off. Anti-bloomingmode is achieved by applying an AC voltage to the chip, forcingexcess electrons into the silicon substrate. An undesirable sideeffect of this action is to pump electrons into traps in the siliconat the expense of electrons in adjacent pixels. For long exposuresthis produces bright/dark pixel pairs. These were initially presentin nearly all the NAC flat field files obtained during calibration inthe thermal vacuum chamber. Corrected flat field files with thesepixel pairs removed have since been created. Camera Commanding----------------- The acquisition of images can be accomplished in several ways.Individual NAC or frames may be acquired, or the NAC and WAC can beused in simultaneous mode, called BOTSIM (for 'both simultaneous').The entire event, which is called a framing event and requires atotal duration called a 'framing time', is broken down into twosteps: the prepare cycle and the readout cycle. The prepare cycle is used to alter the state of the ISS, step thefilter wheels, perform heater operations, light flooding, and otherfunctions required to prepare for an exposure. It also includes theexposure time. The prepare cycle is constructed from a series ofquantized windows of time in which specific functions are assigned tooccur. During the prepare cycle, the shutter blades are reset from theprevious exposure and the filter wheels are moved into position.Because simultaneous motion of each filter wheel requires more powerthan the ISS was allocated for peak operation, all filter wheels NACand WAC -- are moved separately. Windows of quantized duration areset aside for the motion of each filter wheel. Next, the CCD isprepared for exposure to light. This preparation begins with a wait;the duration of the wait is chosen to ensure that the shutter willclose exactly at the end of the prepare cycle. After the wait, alight-flood fills the wells of the CCD to many (~ 50) timessaturation, followed immediate by a read out. The entirelight-flood/erase event takes 950 msec and has the effect of erasingany residual image of previous exposures from the CCD. Within 5 msecof the end of the light-flood/erase event, the shutter is opened forthe commanded duration. (For dark frames, this duration is set tozero.) The image is tagged with the time of shutter close. During a BOTSIM, the prepare cycle is lengthened to include time toprepare both NAC and WAC. The NAC is prepared first; then the WAC isprepared so as to avoid simultaneous movement of any of the 4 filterwheels. If the NAC and WAC exposure times are different, the exposuresbegin in a staggered fashion so that the NAC and WAC shutters areclosed simultaneously. There are 63 discrete commandable exposuretimes which are accommodated within 13 discrete prepare cycle windows. During the following readout window, the CCD is read out, the data areencoded and/or compressed, and the results are packetized. For any ofthe 6 individual CDS pickup rates, there are 4 discrete readoutwindows for each camera. The readout window is scaled by the CDSpickup rate giving 24 actual readout windows per camera and 96 actualBOTSIM readout windows. Prepare times and readout times are chosen before uplink. The preparecycle is completely determinate; the readout time required to fullyread out an image is not. The required readout time during the imageevent will depend on the amount of data being read out of the CCD,and the CDS pickup rate or on the line readout rate from the CCD,whichever is slowest. If the data volume in the image wasunderestimated and the required readout time exceeds the commandedreadout time, the camera will cease reading out part way through animage and lines will be lost. For this reason, a great deal of efforthas gone into the amount of data returned for different scenes andchoices of compression parameters. The ISS can collect pixel (image) data, engineering data and statusdata, and packetize them with appropriate header information as eitherscience telemetry packets (which include all types of data) orhousekeeping packets (which only include engineering and status data).The latter are returned alone when ISS is in an ON power state but notactively taking images. The frequency with which housekeeping packetsare collected is 1 packet/sec and is programmable in flight. Theamount of housekeeping data that gets sent to the ground isdetermined by the rate at which CDS picks up such packets and iscurrently 1 housekeeping packet every 64 seconds. Data paths---------- The analog to digital (A/D) conversion happens right as the analogsignal is read out from the chip, after it has passed through theon-chip amplifier. Data from the ADC are encoded to 12-bit datanumbers (DN), giving a dynamic range of 4096. However, they arestored as 16-bits: the upper 4-bits are all 1 s. The ISS flightsoftware masks the upper 4 bits when doing calculations. Compressionand conversion functions are performed after the electrons areconverted to DN. The next juncture is a choice of data conversion(from 12 to 8 bits) or no data conversion. Unconverted data can thenproceed to a lossless compressor or undergo no compression at all.Converted data can undergo no compression or lossless or lossycompression. From there, the data are placed on the Bus InterfaceUnit (BIU), where they are ultimately picked up by the Command DataSystem (CDS) and sent to the Solid State Recorder (SSR) where theyare stored as 16-bit data. Data Compression---------------- Serious constraints are imposed on imaging of the Saturn system by thelimited storage volume on the spacecraft's SSR, and by the limitedcommunication bandwidth back to Earth. In order to make the mosteffective use of these resources, the Cassini imaging system includesthe capability to convert the data from 12 bits to 8 bits (called dataconversion), and also to perform either 'lossless' or 'lossy' imagecompression. Data conversion, and both lossless and lossy compression,are implemented in hardware. Conversion to 8 bits -------------------- Two sub-options are available for 8-bit conversion. One is a varianton conventional 'square root' encoding. In such encoding, a look-uptable (LUT) is used to convert the original data values to 8-bitvalues. The output 8-bit values are related to the input values in anon-linear fashion, typically scaling with the square root of the12-bit value. This non-linear scaling more closely matches thequantization level to the photon shot noise so that the informationcontent is spread more evenly among the 256 levels. (The Cassini12-to-8 bit conversion table is provided with the calibration datavolume.) It differs somewhat from pure square-root encoding, havingbeen designed for the known noise properties of the Cassini camerasto distribute quantization-induced errors uniformly across thedynamic range of the system. The look-up table is stored in ROMwithin the cameras' memory and cannot be altered in flight; choice ofON or OFF is commandable in flight. The other sub-option is conversion from 12 bits to theleast-significant 8 bits LS8B). This type of conversion is useful forreducing the data volume of images taken of very faint targets, suchas diffuse rings or the dark side of Iapetus, which generally do notyield large signal levels and can be encoded to the lowest 8 bits. Lossless Compression -------------------- Both converted (8-bit) and unconverted (12-bit) data can be losslesscompressed. The ISS lossless hardware compressor is based on Huffmanencoding, a high efficiency, numerical encoding scheme in which thelength of the bit sequence used to encode a given number is chosenbased on the frequency of occurrence of that number. In ISS losslesscompression, each compressed image can be reconstructed on the groundwith no loss to the information content of the image, provided theimage entropy does not exceed the threshold where 2:1 compression isachieved. Scenes with low entropy will have compression ratios higherthan 2:1; scenes with high entropy will never compress greater than2:1, but the ends of lines will be truncated so that the total amountof data returned in a pair of lines of the image never exceeds thetotal number of bits for a single uncompressed line. The truncationscheme has been designed so that the truncation alternates -- i.e.,every other line -- from one line to the next, on the right (largesample number) side of the image. If the data loss is great, it canin principle result in the complete loss of every other line. Ineither case, with this scheme, information (though reduced in spatialresolution) can be retained across the image. Lossy Compression ----------------- Imaging sequences requiring larger compression ratios than can beachieved with the lossless compressor may instead be more stronglycompressed using the camera's lossy compression circuitry. Thiscapability requires that the data have been converted to the 8-bitform. Consequently, data conversion must be employed first before thedata are sent to the lossy compressor. Compression is implemented bya pair of specialized signal processing chips which perform avariation on the familiar JPEG (Joint Photographic Experts Group)compression algorithm used in many image transfer and storageapplications. The JPEG algorithm operates by selectively removinginformation from an image, particularly at high spatial frequencies.Lossy-compressed images thus tend to have reduced detail on finescales. For More Information==================== More information regarding the camera design, operation, imaging andcompression modes, and image calibration can be found in[PORCOETAL2004]. Additional discussion of calibration can also befound in the documentation for the calibration volume of this dataset.
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not applicable
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| REFERENCES |
Porco, C.C., R.A. West, S. Squyres, A. McEwen, P. Thomas, C.D. Murray, A. DelGenio, A.P. Ingersoll, T.V. Johnson, G. Neukum, J. Veverka, L. Dones, A. Brahic, J.A. Burns, V. Haemmerle, B. Knowles, D. Dawson, T. Roatsch, K. Beurle, and W. Owen, Cassini Imaging Science: Instrument Characteristics and Capabilities and Anticipated Scientific Investigations at Saturn, Space Science Reviews 115,363-497, 2004.
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