An introduction to CCD operation.docx

上传人:b****1 文档编号:938150 上传时间:2023-04-30 格式:DOCX 页数:9 大小:80.28KB
下载 相关 举报
An introduction to CCD operation.docx_第1页
第1页 / 共9页
An introduction to CCD operation.docx_第2页
第2页 / 共9页
An introduction to CCD operation.docx_第3页
第3页 / 共9页
An introduction to CCD operation.docx_第4页
第4页 / 共9页
An introduction to CCD operation.docx_第5页
第5页 / 共9页
An introduction to CCD operation.docx_第6页
第6页 / 共9页
An introduction to CCD operation.docx_第7页
第7页 / 共9页
An introduction to CCD operation.docx_第8页
第8页 / 共9页
An introduction to CCD operation.docx_第9页
第9页 / 共9页
亲,该文档总共9页,全部预览完了,如果喜欢就下载吧!
下载资源
资源描述

An introduction to CCD operation.docx

《An introduction to CCD operation.docx》由会员分享,可在线阅读,更多相关《An introduction to CCD operation.docx(9页珍藏版)》请在冰点文库上搜索。

An introduction to CCD operation.docx

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

展开阅读全文
相关资源
猜你喜欢
相关搜索

当前位置:首页 > 初中教育 > 中考

copyright@ 2008-2023 冰点文库 网站版权所有

经营许可证编号:鄂ICP备19020893号-2