室溫準(zhǔn)連續(xù)多量子阱二極管激光器調(diào)諧特性

第8卷第2期2010年3月納米技術(shù)與精密工程N(yùn)anoteclmologyandPrecisionEngineeringV01.8No.2Mar.2010TunabilityofMultipleQuantum-WellDiodeLaserinQuasi-ContinuousWaveatRoomTemperatureDUZhen-hui,ZHAIYa—qiong,HUBo,QIRu.bin(StateKeyLaboratoryofPrecisionMeasuringTechnologyandInstruments,T/觚jinUniversity,Tianjin300072,ChinaAbstract:Inordertoteststrain—compensatedmultiplequantumwell(SC—MQWlasersfordetectionofgasmolecules,basedontunable—diode—laserabsorptionspectroscopy(TDLAS,thetunabilityofSC—MQWdiodelaserwasinvestigatedonquasi—continuouswave(QCWoperationatroomtemperature.Ap—plyingtherateequationofsemiconductorlaser,theeffectsoftheinjectedcurrentandthetemperatureontheoutputwavelengthofSC-MQWlaserswereanalyzed.Moreover,thetuningcharacteristicsofSC—MQWlaserdiodeatvarioustemperaturesandcurrentsweremeasuredwith盯一IRspectrometer.ResultsshowthatitCallbetunedtoabout20amwitharateofabout0.03nm/mAbychangingtheinjectedcurrentofthelaserdiode,andthetuningrateofthelaserdiodewithtemperatureisabout0.25nm/。C.TheoveralltuningrangeCallcover50nmbycombiningthecurrentandtemperaturetuning.SC—MQWdiodelaserprovestohavegoodapplicationprospectsfordetectinggasesofvolatileorganiccompoundswithband—likeabsorptioncharacteristics.Keywords:tunablediodelaser;tunability;quasi■-continuouswave;multiplequantum--welldiodelaser室溫準(zhǔn)連續(xù)多量子阱二極管激光器調(diào)諧特性杜振輝，翟雅瓊，胡波，齊汝賓(天津大學(xué)精密測試技術(shù)及儀器國家重點(diǎn)實(shí)驗(yàn)室,天津300072摘要:為了將應(yīng)變補(bǔ)償多量子阱(SC.MQW激光器用于調(diào)諧激光吸收光譜(TDLAS技術(shù)進(jìn)行氣體分子檢測,研究了SC-MQW激光器在宣溫、準(zhǔn)連續(xù)工作模式下的調(diào)諧特性.從半導(dǎo)體激光器的速率方程出發(fā)，分析了SC-MQW激光器輸出波長與溫度和注入電流的關(guān)系;使用傅里葉變換紅外光譜儀(FT-IR測量了激光器分別在不同電流、溫度條件下的調(diào)諧特性，得到SC-MQW激光器在允許工作電流范圍內(nèi)的調(diào)諧范圍接近20am，電流調(diào)諧率約為0.03nm/mA;溫度調(diào)諧率約為0.25nm/oC;電流和溫度聯(lián)合調(diào)諧的波長覆蓋范圍達(dá)50BIn.結(jié)果表明,該激光器在帶狀吸收譜的揮發(fā)性有機(jī)物氣體檢測方面有很好的應(yīng)用前景.關(guān)鍵詞:可調(diào)諧二極管激光器;調(diào)諧特性;準(zhǔn)連續(xù)波;多量子阱二極管激光器中圖分類號:0433.1;TN248.4文獻(xiàn)標(biāo)志碼:A文章編號:1672-6030(2010-02-0126-06Thetechnologyoftunablediodelaserabsorptionspectroscopy(TDLASwithtunablediodelaser(TDLasit8coreelementCanbeusedinreal—timeon.1inemea8.urementandanalysisofgases.Duetoitshighsensitivity.excellentselectivity,smallvolumeandlowcost,ithasbeenwidelyappliedinfieldslikechemicalanalysis,en一vironmentaldetectionandscientiffcresearch【1.3].Atpresent,thetypesofTDLmainlyincludeleadsaltdiode收稿日期:2009—12-22.基金項(xiàng)目:國家高技術(shù)研究發(fā)展(863計(jì)劃資助項(xiàng)目(2006AA062410;天津市自然科學(xué)基金資助項(xiàng)目(06YFJMJC06700作者簡介:杜振輝(1967一，男，博士，副教授.通訊作者:杜振輝。duzhenhui@.ca.萬方數(shù)據(jù)2010年3月杜振輝等:室溫準(zhǔn)連續(xù)多量子阱二極管激光器調(diào)諧特性(英文?127■laser,distributedfeedback(DFBdiodelaser,verticalcavitysurfaceemittinglaser(VCSELandquantumca8-cadelaser(QCL,etc‘4弓|.TheradiationwavelengthsofleadsaltdiodelaserandQCLlieinmid—infraredfinger-printregion,butthenecessityoflowtemperaturefortheiroperationhaslimitedtheirwideapplication(4巧1:thenear.infraredDFBdiodelaserwhichoff,hatesfromopticalcommunicationtechnologyhasexcellentmonochromaticityandstability,butitsselectableoutputwavelengthrangeissmall(between1.2斗mand1。6斗m,leadingtotheshorttuningrangeandweakabsorptionofthematerialtobedetected,therefore,itcanonlydetectfewkindsofga-sesoflowmolecularweightwithlineabsorption(CH4,HF,NH3,CO,C02,H20,etc..Thefundamentalos-cillatoryfrequencyoforganicmoleculesnormallyliesinthemid—infraredband(3斗m——20斗m,andtheabsorp-tionofnear—infraredspectramainlyincludesharmonicab-sorptionandsum—frequencyabsorption,whereasthesum—frequencyabsorptionusuallyliesinthewavelengthran99of2.0“m——2.5"mwhichistheidealwavebandforon—linemonitoringoforganicgasesinthesensethatthereisnoobstructionofwaterabsorptionandsum—frequencyab-sorptionishigherthanhigh—orderharmonicabsorptioninintensity.However.thesum—frequencyabsorptionofo卜ganicmoleculesusuallyshowsacharacteristicofband—likeabsorption,whichrequiresarelativelywiderangeofwavelengthforthespectrumanalyzer.AsthetuningrangeofpresentTDLisshort(1nm.2nmIs],itcanonlydetectcertainsegmentofband—likeabsorptionline,an—abletoimplementtheabsorption■-linediscerningtechnolo--gYwhichisadistinctivefeatureofTDLAS,whichmeanstIlatitisunabletodetectgaseswithband—likeabsorptioncharacteristics.Asaresult,itissignificanttoinvestigatethewide--rangetunabilityofLDatnear?-infraredbandof2.0pm—_2.5燦mfordetectingvolatileorganicgaseswithband-likeabsorptioncharacteristics.Thestrain—compensatedmulti-quantumwell(SC—MQWstructureofdiodelaserisabletoreducethresholdcurrentandimprovetemperaturecharacteristic,whichcanimproveitstunability.OnthetIleoreticalbasisoftherateequationofsemiconductorlasers,thepaper嘰alyzIestheeffectsoftemperatureandcurrentonthetunabilityofSC.MQWdiodelasers,andproposestocombinetempera—tureandcurrenttuningtoexpandthetuningrangeofla-sers,whichisverifiedthroughexperiments.1AnalysisofthetunabilityofSC-MQWdiodelasersTheactivelayerofSC-■MQWdiodelaserisastruc--tureofstrain-compensatedmulti—quantumwell.Thequantumwellstructureisdevelopedwiththetechnologyofmetallorganicschemicalvapordeposition[9-10],whilequantumwelllasersareoflowthresholdcurrent,highquantumefficiencyandhiShoscillationfrequency,andcandirectlyworkunderrelativelyhightemperature.Theintroductionofstrainreducesthefinitemassofholesandfurtherreducesthetransitionbetweenvalencebands,sothethresholdcurTentofQWlasersissharplyreduced[11-123.Simultaneouslythequantumefficiency,theoscillationfrequency,andfurthermore,thetemperaturecharacteris—ticsareimproved80thatnon—refrigerationoperationofla-ser8canberealized.Moreover。thestraincompensationhasenhancedtheworklifeoflasersthroughimprovementofmaterialqualitr.Inaddition,strain—compensatedquantumwelllasershaveahighermodulationrateandcanreachalargertuningrangeunderpermittedworkingconditionthanaveragelasers.TherateequationofSC—MQWlasersisexpressedasfoilows[13|:idN=iJ—7°W—GS(1面dS=(G—ys+R叩,(2警一等(s圳一％tOFAn(3。whereNdenotesthecarrierconcentration,Sdenotespho一tondensity,咖denotesthephaseposition,Jdenotesthedensityofinjectedcurrent,ddenotesthethicknessofae一tirearea,edenotestheelectroncharge,7edenotesthecarrierrecombinationrate,Gdenotesthenetstimulatedemissionrate,7denotestheattenuationrateofphotons,R卵denotestheratechangecausedbycompositionofspontaneouslyemittedphotonstophotons,nMstandsformoderefractiveindex,ngstandsforgrouprefractivein—dex,(I'standsforradiationmodefrequency,力standsforcavityresonantfrequency,J1standsforthelimitingfactorsofmodefield,andAnstandsforthevariationofrefrac.tireindex.Thereisalinearrelationshipbetweenthevariationof萬方數(shù)據(jù)-128-納米技術(shù)與精密工程第8卷第2期refractiveindexAnandthechargecarderconcentrationIV[131:An=bN(4AconclusioncanbedrawnfromEqs.(3and(4:fordiodelasersbasedoninjectedcurrentpumping,thechangeincurrentcardercausedbychangeofinjectedcurrenthascausedthechangeofrefractiveindex,andfi—naUycausedthechangeofphasepositionofradiationmode.AsthephasepositioninrateEq.(3isselfcon—sistent,itprovesthatthechangeofrefractiveindexAncausedbycarderhasinfluencedtheradiationmodefre—quencyto.Inanotherword,thechangeofinjectedcur-rentwillchangetheradiationwavelengthoflasers,whichisatraditionalexplanationforthefundamentalprincipleofcurrenttuning.Asamatteroffact,theinfluenceofcurrent.inducedJouleheathasalsobeeninvolvedinthechangeoflasers’wavelengthcausedbyinjectedcurrent.Theformulaoftheradiationwavelengthofdiodela-8ersAisA=2nMI/M(5where,Zdenotesthelasercavitylength,andMisaposi—tiveinteger.Withtheincreaseofinjectedcurrent,thereisathermalexpansioninthelaserresonantcavity,andthentheradiationwavelengthwillmovetothedirectionoflongwavelength.Asaresult,thecurrenttuningoflasersisacombiningeffectofthecartierchangecausedbyin-jectedcurrentandthecavitylengthchangecausedbyJouleheat.Inaddition,thetemperatureofthelaserresonatorcanalsobechangedbyexternallyappliedheat,sothattheoutputwavelengthcanbechanged.Thechangeinra—diationwavelengthcausedbytemperaturechangeisalsoreflectedintwoaspects:firsty,thechangeoftemperaturecausesthechangeinrefractiveindexofsemi—conductormaterials;secondly,thechangeoftemperaturecausesthechangeinlasercavitylength.Temperaturetuningcanbeexpressedasfollows[141:而AA:塵f黑+砌1(6斫2il麗+叫(6’where,adenotesthecoeffleientofthermalexpansionofthematerialsinactivelayer.ThefirsttermintherightsideofEq.(6denotesthechangeofrefractiveindexcausedbyincreaseoftemperature,andthesecondde—notesthechangeofwavelengthcausedbythethermalex—pansionoflasercavity.Infact,theinfluenceofcurrentandtemperatureontheoutputwavelengthofdiodelaserliesnotonlyintherefractiveindexoftheactivelayerandthelasercavitylength,butalsointhetemperaturecharacteristicsofIlia—terialbandgap,whoseeffecthasnotbeentakenintocon—siderationhere.2ExperimentaldevicesThetestsystemforthetuningcharacteristicsofdiodelasersisshowninFig.1,whichadoptstheSC—MQWdi—odelasersproducedbyIBSGCompany.Thediodelaserworksinquasi—continuouswaveatroomtemperature,whoseradiationpoweris2.5mW,radiationwavelengthis2.2斗m,thresholdcurrentis21mA,themaximumworkingcurrentis120mAandtherangeofworkingtem-peratureis一5°C——20cC.Thelaserhasintegratedtwo—stagePeltierthermoelectriccoolerandthermistortempera-turesensor.LDC-3908(ILXLightwaveisusedtocontrolthecurrentandtemperatureofthelasers.TheFouriertransforminfrared(FrIRspectrometerSpectrumGX(PerkinElmerworksinthemodeofexternallightsourcetomeasuretheoutputmodespectrumofthelasers,andtheresolutionofthemeasurementis0.1cm~,therangeofscanningwavenumberis4500cm一1—300Cm-1.Fig.lBlockdiagramforthetestsystemofdiodelasertuningcharacteristics3ExperimentalresultsandanalysisThroughtheexperiment,thetuningrateandrangeofSC?-MQWlaserswithcurrentandtemperaturearerespec■■tivelyinvestigated,andthecombiningtuningrangewithcurrentandtemperatureisalsoresearched.3.1CurrenttuningThelaseriskeptunderafixedtemperature,andtheinjectedcurrentincreasedstepbystep,thenthelongitu-dinalmodespectrumundereachcurrentismeasured,萬方數(shù)據(jù)2010年3月杜振輝等:室溫準(zhǔn)連續(xù)多量子阱二極管激光器調(diào)諧特性（英文?129■thatis,thecurrenttuningcharacteristicsareinvestigatedoFig.2showsthecurrenttuningcharacteristicsofthelaserunder15°C.Underacertaintemperature.withtheincreaseofinjectedcurrent,thewavelengthoftheradia—tionlasermovestothedirectionoflongwavelength.Whentheinjectedcurrentisatalowlevel,thelasershowsallexcellentcharacteristicofsinglelongitudinalmode.Andwhentheinjectedcurrentincreases,itturnsintomulti—longitudinalmodeoutput,withthedistancebetweenadjacentlongitudinalmodeas1.9nm(109GHz.Thecurrenttuningrateisabout0.03nm/mA.Inthepermittedrangeofworkingcurrent,thetuningrangeofabout20nmcanbeobtained.However,currenttuninginarelativelylargerangecallcausemodehoppingofthela-ser.Intherangeof30mA—100mAoftheinjectedcur-rent,twicemodehoppingtakesplaceintheoutputofthelaser.Inthenon—hoppingregion,thewavelengthofthelasershowsaquasi—linearchangewiththecurrentshowninFig.3.Theaveragecurrenttuningrateintherangeof30mA卅mAis0.0274nm/mA.intherangeof60mA——70mAis0.0296nm/mA.andintherangeof70mA一100mAis0.0355nm/mA.whichmeansthecur-renttuningrateriseswiththeincreaseofworkingcur-rent.BasedonEq.(5,theincreaseofcurrenttuningrateiscausedbytheJouleheateffectofthecurrent.Fig.2Energyspectraatdifferent螄幣ectedcurrentsAstheheateffectisproportionaltothesquareofcurrent,supposingthattherefractiveindexoftheactiveareaisinlinearrelationshipwiththeinjectedcurrent,themodelparameterofcurrenttuningaccordingtothequad—raticpolynomialstructureCallbeexpressedas五(i,r=u(Ti2+b(Ti+c(T(7where,a(T,b(Tandc(Trespectivelydenotesthemodelparametersofcurrenttuningatcertaintempera-Fig.3Modehoppingandtuningrateofcurrenttuningture.Whenthetemperatureofthelaseris15°C.thethreemodelparametersare3.7x10~.—2.6x10—4and2.1x10?.respectively.Themodelstructureandparameterwereverifiedbyexperimentsatdifferenttemperaturesandinjectedcur-rents,asshowninFig.4.Exceptthedeviationinthemeasurementresultofthreeparametersincluding(0oC,50mA,(10C,50mAand(5oC,85mA,otherdataallshowanexcellentconsistencywiththecurrenttuningmode.Inaddition,themodelparametersatdiffer-enttemperaturesarethesame,whichmeansthatthecur-renttuningrateisirrelativetotemperature.Fig.4Currenttuningrateatdifferenttemperatures3.2TemperaturetuningThelaserissettoworkatacertaininjectedcurrent.TheinteriortemperatureofthelaseriscontrolledwiththePehierpartsintegratedinthelaserdiodemoduletoin-creasebyacertainstep,andthenthelongitudinalmodespectrumateachtemperatureismeasured,thatis,thetemperaturetuningcharacteristicsareinvestigated.Fig.5showsthemodespectraoftemperaturetuning.Fig.6showstherelationshipbetweenthetemperatureandthedominantmodewavelengthofthelaser.Withtheriseoftemperature,theoutputwavelengthofthelaserincrea-眄阱旺s侶任似他2222222010年3月■y■-二=^―=__—予三―thati&thecurrenttuningchted.Fig.2showsthecurrentti萬方數(shù)據(jù)-130-納米技術(shù)與精密工程第8卷第2期se￥,whichisexpressedasmulti—moderadiation.Withintherangeof0°C——20°C.atuningrangeof30amcanbeobtmned,andthetemperaturetuningrateisabout0.25nm/C.Inarelativelylargerangeoftemperature,therealeseveraltimesofmodehoppinginthelaser.Inthenon-hoppingregion,thewavelengthofthelasershowsaquasi-linearchangewiththetemperature.Thetempera—turetuningrateofthelaserinnon—-hoppingregionisre--spectively0.2nm/。C,0.26nm/。C,0.26nm/。C,0.25nm/%,0.26nm/。C,0.26nm/°C,0.24nm/°C,0.21nm/。Cand0.21nm/。C,andthemaximumtuningrangewithouthoppingis0.65am.Hereisthecombiningtuningwithtemperatureandcurrent.Thelaserissettoscanwithinthewholerangeofworkingtemperature,andatthesametimetheinjectedcurrentofthelaserisrapidlyscannedwithintherangeofworkingcurrent.Thismethodofsimultaneouslychangingthetemperatureandinjectedcurrentcanexpandthetun-ingrange.UndertheconditionsoftemperaturewithinO一20Candcurrentwithin30mA一100mA.atuningrangeofover50nInisobtainedbyusingthiskindofSC—MQWlaser.Tab.1showsthecurrenttuningrangewith-outmodehoppingatdifferenttemperatures.Fig.5Mode叩舊ctl噙ofia,鴕rdiodeatdifferenttempera-tures22902285毫:2”280,{2270區(qū)226522602255Range:2286.O睜一2286.30Range:2293.6I卜2283.90nI曠一Range:2279.2驢一2279.65面Range:2275.00_—2275.25.mm?；?72.45—2272.95nm廠廄最e:2268.10一2268.60Kill/"Range:2263.55—2264.20nmage:2259.30_—2259.70nm:2255.25—2255.45llm02468101214161820Temperamre/'Crig.6ModehoppingandtIlIIingratebytemper-aturettmi,,gTab.lCurrenttuningrangewithoutmodehoppingatvarioustemperaturesTempe—rature/°CMode—hopfreetuningrange/rim02243.05-2243.202246.90_2247.152250.90_2251.102254.90-2255.302259.10_2259.452265.25_2265.5552255.45—2255.852259.60—2259.952263.80—2264.102269.80—2270.202274.05—2274.40102260.30—-2260.502264.25—-2264.552268.35—-2268.602272.45—-2272.752274.70—-2274.952278.75—.2279.30152272.85—-2273.652279.40—-2279.652283.50—_2284.50202274.10_2274.202278.05q278.352284.20—2284.502288.35.2289.202293.10_2293.35Thepaperproposesthatsimultaneoustuningofcur-rentandtemperaturecanexpandthetuningrangeofSC■MQWlaserto50nm,sothereisanexcellentprospectforittobeappliedtodetectinggasmoleculeswithbroadbandabsorptionpeak.Moreover,thePeltierpartsembeddedinthelaserdiodemodulecanrealizerapidtemperaturescanning.Underadrivingcurrentof1A,thechangingrateoftemperaturecanexceed10。C/s.ActuallyweusedSC—MQWlasertodetectorganicgasessuchasmethyl■benzeneandpropane,andtillnowtheresolutionratioCallreachthemagnitudeof10-6.InadditionothisSC.MQWlasercallalsobeappliedtodetectingmoleculesoflineabsorption.Arita[15.16。proposedthetheoryandtech—nologyofmulti■modelaserstodetecttracegases.Inthemode—hopping—freetuningrangeofmuhimodelasers,eachmoderespectivelyscanstheadjacentgasabsorptionlineinproperorder,andthismethodcanalsobringabouthighresolutionratio.Therefore.theSC-MQWlaserwithawidetuningrangecanbeusedasthelightsourceinTDLASsystemtodetectthegasmoleculeswithlineab—sorptionandband.1ikeabsorptioncharacteristics.4ConclusionsSC—MQWdiodelasershaveanexcellenttunabilitybycurrenttuningandtemperaturetuningin*130*ses,whichisexpressedasmultitherangeof0—20P,atuiquasi■■contin■-萬方數(shù)據(jù)2010年3月杜振輝等：室溫準(zhǔn)連續(xù)多量子阱二極管激光器調(diào)諧特性（英文）-131-UOUSwaveatroomtemperature.Underthepermittedcurrentcon—[7]LsekiT.AportableremotemethanedetectorusingallIn—ditionofinjectedandtempe

ratureofthelasers,GaAsPDFBlaserratureofthelasers,GaAsPDFBlaser[J].EnvironmentalGeology,2004,46thecurrenttuningrangeisabout20amandthetempera—ture(8):1064.1069.tuningrangeisabout30andtemperaturenm.Thecombinationofcan[8]DongbleFengzhong,KanRuifeng,LiuWenqing,etal.Tuna—currentrangetotuningexpandthetuningisanexcellentbeappliedtodimelaserabsorptionspectroscopictechnologyanditsabout50砌.Therefore.therediodelaserstoapplicationsinairqualitymonitoring[J].ChineseJournalprospectforofQ拙口m聃zElectronics,2005,22(3)：315—325.[9]LiW,HerouxJB,ShaoH,etalSC—MQWStrain—compensatedIn—detectinggasmoleculeswithbroadbandabsorptionpeak.References：GaAsSb/AIGaAsSbmid—infraredquantum—wellAppl&dPhysicslasers[J].Letters,2004,S4(12)：2016—2018.Jingsong,ZhangYunmei,eta1.A[10]Chen[1]MartinPGaoting,Bai2岬A(chǔ).Near?infrareddimelaserspectroscopyinehem■wavebandInGaAsSb/MGaAsSbwidestripeMQWdimelasericalprocessandenvironmentalairSocmonitoring[J].Chem[J].ChineseJLasers,1998,25(12)：1069—1072.[11]ParkSeoung—Hwan,JeongWeon—Guk,ChoeByung—Doo.lagelt毫Rev,2002,31(4),201.210H,GurkC,et[2]KormannR,Fischermulti-lasermospherical.ApplicationofaSwain—compensatedInGaAs/InGaAsPquantumwelllatticetunabletracediodelaserabsorptionspectrometerforat—atmatchedtoGaAs[J].ApplPhysLeft,1995,66(2)：gasmeasurementsPartsub—ppbvlevels[J].20l—203.SpectrochimicaActaA：MolecularandBiomolecular[12]PengYuheng,AnHaiyan,ChenWeiyou,etal.Theoreticalmultiple—quan—Spectroscopy,2002,58(11)：2489—2498. [3]KanRuifeng,Liuanalysisturn—well293.Lasers,2005,f矗InGaAs(P)strain—compensatedWenqing,ZhangYujun,eta1.Tunablespectrometermonitorstheambientlasers[J].ChineseJLasers,1998,25(4)：289.dimelagerabsorptionmethanewithhighsensitivity[J].ChineseJ32(9)：1217—1220.[13]JeasB,Markas-ChristainA,BlumenthalDJ.TunableLaser[4]HvozdaraL,PenningtonN,KraftM,etcadelasersformid—infrareda1.QuantumDiodesandRelatedOpticaleas—Sources[M].2nded.Newspectroscopy[J].VibrationalJersey：JohnWiley&Sons,Inc,2005：85.Spectroscopy,2002,30(1)：53—58. [5]Thweatt[14]VicetA,YarekhaDA,OuvrardA,etal.Tunabilityofanti.andexperimentalWD,HarwardSrCN,ParrishME.Measurementinamonide—basedsemiconductorlasersdiodesofacroleinandl,3—butadienesmokeusingleadsaltsinglepuffofcigaretteevaluationofthethermalresistance[J].IEEProcOptoelec—tunabledimelaserinfraredspectrosco—Biomo—tron,2003.150(4):310—313.[l5]AritaY,Ewartpy[J].SpectrochimicaActa凡廳A：MolecularandlecularP.Multi—modeabsorptionspectroscopy[J].Spectroscopy,2007,67(1):16—24.al.VCSEL—basedstructuralanalysisofpharmaceuticalOpticsCommunications,2008,281(9):2561—2566. [6]SvenssonT,AnderssonM,RippeL,etoxygenspectroscopyfor[16]AritaY,StevensR,EwartP.Multi—modeabsorptionspec.troscopyofoxygenformeasurementofconcentration,temper—solids[J].ApplPhys345—354.B：LasersandOptws,2008,90(2)：atureandpressure[J].Appl詒dPhysics曰：LasersandOP—t/cs,2008,90(2)：205—211.萬方數(shù)據(jù)室溫準(zhǔn)連續(xù)多量子阱二極管激光器調(diào)諧特性作者：作者單位：刊名：英文刊名：年，卷(期：杜振輝，翟