An introduction to CCD operation.docx
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AnintroductiontoCCDoperation
AnintroductiontoCCDoperation
Thebasics
AChargeCoupledDevice(CCD)isahighlysensitivephotondetector.TheCCDisdividedupintoalargenumberoflight-sensitivesmallareas(knownaspixels)whichcanbeusedtobuildupanimageofthesceneofinterest.Aphotonoflightwhichfallswithintheareadefinedbyoneofthepixelswillbeconvertedintoone(ormore)electronsandthenumberofelectronscollectedwillbedirectlyproportionaltotheintensityofthesceneateachpixel.WhentheCCDisclockedout,thenumberofelectronsineachpixelaremeasuredandthescenecanbereconstructed.
Thepicturehereshowsa"typical"CCD.TheCCDitselfisprimarilymadeofsiliconandthestructurehasbeenalteredsothatsomeofthesiliconatomshavebeenreplacedwithimpurityatoms.
ThefigurebelowshowsaverysimplifiedcrosssectionthroughaCCD.ItcanbeseenthattheSiliconitselfisnotarrangedtoformindividualpixels. Infact,thepixelsaredefinedbythepositionofelectrodesabovetheCCDitself.Ifapositivevoltageisappliedtotheelectrode,thenthispositivepotentialwillattractallofthenegativelychargedelectronsclosetotheareaundertheelectrode.Inaddition,anypositivelychargedholeswillberepulsedfromtheareaaroundtheelectrode.Consequentlya"potentialwell"willforminwhichalltheelectronsproducedbyincomingphotonswillbestored.
AsmoreandmorelightfallsontotheCCD,thenthepotentialwellsurroundingthiselectrodewillattractmoreandmoreelectronsuntilthepotentialwellisfull(theamountofelectronsthatcanbestoredunderapixelisknownasthefullwellcapacity).TopreventthishappeningthelightmustbepreventedfromfallingontotheCCDforexample,byusingashutterasinacamera.Thus,animagecanbemadeofanobjectbyopeningtheshutter,"integrating"foralengthoftimetofillupmostoftheelectronsinthepotentialwell,andthenclosingtheshuttertoensurethatthefullwellcapacityisnotexceeded.
AnactualCCDwillconsistofalargenumberofpixels(i.e,potentialwells),arrangedhorizontallyinrowsandverticallyincolumns.ThenumberofrowsandcolumnsdefinestheCCDsize,typicalsizesare1024pixelshighby1024pixelswide.TheresolutionoftheCCDisdefinedbythesizeofthepixels,alsobytheirseparation(thepixelpitch).InmostastronomicalCCDsthepixelsaretouchingeachotherandsotheCCDresolutionwillbedefinedbythepixelsize,typically10-20µm.Thus,a1024x1024sizedCCDwouldhaveaphysicalareaimagesizeofabout10mmx10mm.
HowisaCCDclockedout?
ThefigurebelowshowsacrosssectionthrougharowofaCCD.EachpixelactuallyconsistsofthreeelectrodesIØ1,IØ2,andIØ3.Onlyoneoftheseelectrodesisrequiredtocreatethepotentialwell,butotherelectrodesarerequiredtotransferthechargeoutoftheCCD.Theuppersectionofthefigure(section1)showschargebeingcollectedunderoneoftheelectrodes.TotransferthechargeoutoftheCCD,anewpotentialwellcanbecreatedbyholdingIØ3high,thechargeisnowsharedbetweenIØ2andIØ3(section2).IfIØ2isnowtakenlow,thechargewillbefullytransferredunderelectrodeIØ3(section3).TocontinueclockingouttheCCD,takingIØ1highandthentakingIØ3lowwillensurethatthechargecloudnowdriftsacrossundertheIØ1electrodes.Asthisprocessiscontinued,thechargecloudwillprogresseitherdownthecolumn,oracrosstherow,dependingupontheorientationoftheelectrodes.
Thefigurebelow(calledaclockingdiagram)showstheprogressionunderwhicheachelectrodeisheldhighandlowtoensurethatchargeistransferredthroughtheCCD.
Initially,IØ2ishigh-usuallytoaround12V,andthechargeisheldunderthatelectrodeasin
(1)previously.WhenIØ3isheldhigh,andIØ2istakenlow(usually0V),thechargemigratesundertheIØ3electrode(asin
(2)).Finally,takingIØ1highandIØ3lowtransfersthechargeunderIØ1(asin(3)).Thisprocessisrepeatedintransfer2andtransfer3,thechargehasnowbeenmovedthreepixelsalong.Thisprocessisknownaschargecoupling(henceCCD).
FormostoftheCCD,theelectrodesineachpixelarearrangedsothatthechargeistransferreddownwardsalongthecolumns.Hence,duringtheCCDclockingoperation,rowsaretransferreddownwardstothefinalrow(thereadoutregister)whichisusedtotransferthechargeineachpixeloutoftheCCDsoitcanbemeasured.
Inthereadoutregister,theelectrodesarearrangedsothatthechargeistransferredinthehorizontaldirection,alongthereadoutregister.
Howthechargeismeasured
ThefinalprocessontheCCDisthereadingofeachpixelsothatthesizeoftheassociatedchargecloudcanbemeasured.Attheendofthereadoutregisterisanamplifierwhichmeasurethevalueofeachchargecloudandconvertsitintoavoltage,atypicalconversionfactorbeingaround5-10µVperelectronwith"typical"fullwellvaluesbeingabout100,000electronsorso.
ACCDcamerawillconsistoftheCCDchip,andassociatedelectronics,whichisusedatthispointtoamplifythesmallvoltageontheCCD,removenoisecomponents,digitisethepixelvaluesandoutputthevaluesofeachpixelforexample,toaPC,wheretheimagecanbeprocessedinsoftwareandtheimagedisplayed.TheCCDisananaloguedevice,andtheanaloguevoltagevaluesareconvertedintoadigitalformbythecameraelectronics.
SomeaspectsofCCDbehaviour
QuantumEfficiency
Noteveryphotonfallingontoadetectorwillactuallybedetectedandconvertedintoanelectricalimpulse.ThepercentageofphotonsthatareactuallydetectedisknownastheQuantumEfficiency(QE).Forexample,thehumaneyeonlyhasaQEofabout20%,photographicfilmhasaQEofaround10%,andthebestCCDscanachieveaQEofover80%.Quantumefficiencywillvarywithwavelength.
Wavelengthrange
CCDscanhaveawidewavelengthrangerangingfromabout400nm(blue)toabout1050nm(Infra-red)withapeaksensitivityataround700nm.However,usingaprocessknownasbackthinning,itispossibletoextendthewavelengthrangeofaCCDdownintoshorterwavelengthssuchastheExtremeUltravioletandX-ray.
DynamicRange
Theabilitytoviewbrightandfaintsourcescorrectlyinthesameimageisaveryusefulpropertyofadetector.Thedifferencebetweenabrightestpossiblesourceandthefaintestpossiblesourcethatthedetectorcanaccuratelyseeinthesameimageisknownasthedynamicrange.WhenlightfallsontoaCCDthephotonsareconvertedintoelectrons.Consequently,thedynamicrangeofaCCDisusuallydiscussedintermsoftheminimumandmaximumnumberofelectronsthatcanbeimaged.AsmorelightfallsontotheCCD,moreandmoreelectronsarecollectedinapotentialwell,andeventuallynomoreelectronscanbeaccommodatedwithinthepotentialwellandthepixelissaidtobesaturated.ForatypicalscientificCCDthismayoccurataround150,000electronsorso.Theminimumsignalthatcanbedetectedisnotnecessarilyoneelectron(correspondingtoonephotonatvisiblewavelengths).Infact,thereisaminimumamountofelectronicnoisewhichisassociatedwiththephysicalstructureoftheCCDandisusuallyaround2-4electronsforeachpixel.Thus,theminimumsignalthatcanbedetectedisdeterminedbythisreadoutnoise.
Intheexampleabove,theCCDwouldhaveadynamicrangeof150,000:
4(takingtheuppernoiselevel).But-thisdynamicrangeisalsodependentontheabilityoftheelectronicstobeablefullydigitiseallofthisdynamicrange(seethemoredetailedCCDinformationfordiscussionsonelectronicsresolution).
Linearity
Onthewhole,theeyeisnotalineardetector(exceptoververysmallvariationsinintensity)andhasalogarithmicresponse.Animportantconsiderationinadetectorisitsabilitytorespondlinearlytoanyimageitviews.Bythiswemeanthatifitdetects100photonsitwillconverttheseto100electrons(ifwehad100%QE)andifitdetects10000photons,itwillconverttheseto10000electrons.Insuchasituation,wesaythatthedetectorhasalinearresponse.Sucharesponseisobviouslyveryusefulasthereisnoneedforanyadditionalprocessingontheimagetodeterminethe'true'intensityofdifferentobjectsinanimage.
Noise
OneofthemostimportantaspectsofCCDperformanceisitsnoiseresponse.ThereareanumberofcontributionstothenoiseperformanceofaCCD,thesearebrieflylistedhere:
∙Darkcurrent-i.ethermallygeneratednoise.Atroomtemperature,thenoiseperformanceofaCCDcanbeasmuchasthousandsofelectronsperpixelpersecond.Consequently,thefullwellcapacityofeachpixelwillbereachedinafewsecondsandtheCCDwillbesaturated.Darkcurrentcanbemassivelyreducedbycooling.Forexample,thenoiseperformanceoftheCCDcouldbereducedfromthousandsofelectronsatroomtemperaturetoonlytensofelectronsperpixelpersecondat-40degreesC.Bycoolingdowntotemperaturesbelowabout-70degreesCdarkcurrentcanbevirtuallyeliminated(substantiallybelowoneelectronperpixelpersecond).AsecondwayofreducingnoiseistoslightlyaltertheCCDprocessingtechniquetoproduceaMulti-Pinned-Phase(MPP)CCD.Thistechniquecanreducethedarkcurrenttoverylowlevels(afewhundredelectronsperpixelpersecondatroomtemperature).
∙Readoutnoise -theultimatenoiselimitoftheCCDisthereadoutnoise.ThereadoutnoiseoriginatesfromtheconversionoftheelectronsineachpixeltoavoltageontheCCDoutputnode(atypicalvaluewouldbearound4µVperelectron