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Section5:TheHydrogenAtom
Intheseslideswewillcover:
• The3DSchrödingerequation
• Particleinaboxanddegeneratequantumstates
• Radialandangularsolutionsforcentralpotentials
• Identificationoftheangularpiecewiththeangularmomentumeigenfunctions (sphericalharmonics)
• Infinitesphericalwell
• SolutionoftheradialequationfortheCoulombpotential
• Eigenfunctions ofthehydrogenatom
• Quantumnumbersofthehydrogenatom
Particleinabox
The3DSchrödingerEquation
• Wenowmovefromparticlesin1Dspace,to3Dspace
• Thederivativein1dimension, !"
!#",isreplacedbyits3D
equivalent,the“Laplacian”operator𝛻% = '"
'#"+ '"
')"+ '"
'*"
• The3Dtime-independentSchrödingerequationfortheenergyeigenfunctions 𝜓(𝑥, 𝑦, 𝑧) andeigenvalues𝐸 ishence:
• Thenormalisation conditionforthe3Dwavefunction is∫ 𝑑𝑥565 ∫ 𝑑𝑦5
65 ∫ 𝑑𝑧565 𝜓(𝑥, 𝑦, 𝑧) % = 1
−ℏ%
2𝑚𝜕%𝜓𝜕𝑥% +
𝜕%𝜓𝜕𝑦% +
𝜕%𝜓𝜕𝑧% + 𝑉 𝑥, 𝑦, 𝑧 𝜓 𝑥, 𝑦, 𝑧 = 𝐸𝜓 𝑥, 𝑦, 𝑧
Particleinabox
Particleinabox
• Agoodexampleisa“particleinabox”withpotential
• Welookforaseparablesolution
• Wefind,bysubstitutingthistrialsolutioninthe3DSchrödingerequationandre-arranging,
𝑉 𝑥 = ?0, 𝑥 < 𝐿, 𝑦 < 𝐿, 𝑧 < 𝐿∞, outsidethebox
𝜓 𝑥, 𝑦, 𝑧 = 𝑓 𝑥 𝑔 𝑦 ℎ(𝑧)
−ℏ%
2𝑚1
𝑓 𝑥𝑑%𝑓𝑑𝑥% +
1𝑔 𝑦
𝑑%𝑔𝑑𝑦% +
1ℎ 𝑧
𝑑%ℎ𝑑𝑧% = 𝐸
Particleinabox
Particleinabox
• Thatlastequationagain:
• Wecansolvethisequationusinganicepieceoflogic:§ eachterminthesquaredbracketonlydependson1variable(𝑥,𝑦 or𝑧)
§ eachofthosevariablesisfreetovaryindependentlyfromtheothers
§ inthiscase,theonlywaytomakethetermsalwayssumtoaconstantisifeachindividualterminthesquaredbracketisseparatelyaconstant
• Wefindthateachseparatefunction𝑓, 𝑔, ℎ satisfiesthe1DSchrödingerequationfortheinfinitepotentialwell.Wemultiplythemtogetherforthetotalsolution,𝜓 = 𝑓 Q 𝑔 Q ℎ
−ℏ%
2𝑚1
𝑓 𝑥𝑑%𝑓𝑑𝑥% +
1𝑔 𝑦
𝑑%𝑔𝑑𝑦% +
1ℎ 𝑧
𝑑%ℎ𝑑𝑧% = 𝐸
Particleinabox
Particleinabox
• Summarising,theparticleinaboxhasenergyeigenfunctionslabelledbythreequantumnumbers(𝑛#, 𝑛), 𝑛*)
• 𝜓STU(𝑥) arethedifferentstates𝑛 whicharesolutionsofthe1Dinfinitepotentialwell
• Theenergyeigenvaluesarethenthesumofthecorrespondingeigenvaluesforthe1Dinfinitepotentialwell,
• Wenoticeherethatdistincteigenfunctions canhavethesameenergy(degeneratestates),e.g.(2,1,1),(1,2,1) and(1,1,2)
𝜓VU 𝑥, 𝑦, 𝑧 = 𝜓SWTU 𝑥 𝜓SX
TU 𝑦 𝜓SYTU(𝑧)
𝐸(𝑛#, 𝑛), 𝑛*) =𝜋%ℏ%
8𝑚𝐿% 𝑛#% + 𝑛)% + 𝑛*%
Centralpotentials
Radialandangularsolutionsforcentralpotentials
• Acentralpotentialdependsonlyonthedistancefromtheorigin,𝑉 𝑥, 𝑦, 𝑧 = 𝑉(𝑟).Animportantexampleis,thepotentialaroundahydrogennucleus(proton)attheorigin
𝑟
+𝑒
−𝑒(Sorryfortheillustration
withclassicalpointparticles.Theyareofcourse
probabilitycloudsinQM!)
𝑥 𝑦
𝑧
Centralpotentials
Radialandangularsolutionsforcentralpotentials
• Acentralpotentialdependsonlyonthedistancefromtheorigin,𝑉 𝑥, 𝑦, 𝑧 = 𝑉(𝑟).Animportantexampleis,thepotentialaroundahydrogennucleus(proton)attheorigin
• Theseproblemsarebesttreatedusingsphericalpolarco-ordinates,(𝑟, 𝜃, 𝜙)
• Non-examinable:weneedtheexpressionfortheLaplacianinsphericalpolarco-ordinates(ouch!):
𝛻% =1𝑟%
𝜕𝜕𝑟 𝑟%
𝜕𝜕𝑟 +
1𝑟% sin 𝜃
𝜕𝜕𝜃 sin 𝜃
𝜕𝜕𝜃 +
1𝑟%sin%𝜃
𝜕%
𝜕𝜙%
Centralpotentials
Radialandangularsolutionsforcentralpotentials
• Non-examinable:Weagainlookforaseparablesolutionfortheenergyeigenfunctions,
• Substitutingthisinthe3DSchrödingerequationandre-arranging,wefind:
• Byasimilarlogictothecubicalboxsolution… theleft-handsideofthisequationisafunctionof(𝜃, 𝜙) onlyandtheright-handsideisafunctionof𝑟 only.Buttheymustremainequalas(𝑟, 𝜃, 𝜙) varyindependently.Sotheymustbothbeequaltothesameconstant,let’scallit𝜆
𝜓 𝑟, 𝜃, 𝜙 = 𝑅 𝑟 𝑌(𝜃, 𝜙)
−ℏ%
𝑌1
sin 𝜃𝜕𝜕𝜃 sin 𝜃
𝜕𝑌𝜕𝜃 +
1sin%𝜃
𝜕%𝑌𝜕𝜙% =
ℏ%
𝑅𝜕𝜕𝑟 𝑟%
𝜕𝑅𝜕𝑟 + 2𝜇 𝐸 − 𝑉 𝑟 𝑟%
Switchingtousing𝜇 formass,since𝑚 isabouttomeansomethingelse
Centralpotentials
Radialandangularsolutionsforcentralpotentials
• Theleft-handsideofthisequationbecomes,
• Aha!Theleft-handsideisjusttheoperatorforthetotalangularmomentum,𝐿e%,fromthepreviousSection:
• Hence,theangularpieceoftheenergyeigenfunctions foracentralpotentialisjustthesphericalharmonicfunctions𝑌fg(𝜃, 𝜙) where𝜆 = 𝑙 𝑙 + 1 ℏ% – that’sconvenient
−ℏ%1
sin 𝜃𝜕𝜕𝜃 sin 𝜃
𝜕𝜕𝜃 +
1sin%𝜃
𝜕%
𝜕𝜙% 𝑌 𝜃, 𝜙 = 𝜆𝑌 𝜃, 𝜙
𝐿e%𝑌 = 𝑙 𝑙 + 1 ℏ%𝑌
Centralpotentials
Radialandangularsolutionsforcentralpotentials
• Substituting𝜆 = 𝑙 𝑙 + 1 ℏ% intheradialpiece,wefind
• Ausefulchangeofvariablesistosubstitute𝑢 𝑟 = 𝑟 Q 𝑅(𝑟)[i.e.𝑅 = 𝑢/𝑟].Inthiscase,
• Wenotethatthislooksjustlikea1DSchrödingerequation,excepttheusualpotentialhasbeenreplacedbyan“effective
potential” 𝑉 𝑟 + f fkT ℏ"
%lm"
−ℏ%
2𝜇1𝑟%
𝑑𝑑𝑟 𝑟%
𝑑𝑅𝑑𝑟 + 𝑉 𝑟 +
𝑙 𝑙 + 1 ℏ%
2𝜇𝑟% 𝑅 = 𝐸𝑅
−ℏ%
2𝜇𝑑%𝑢𝑑𝑟% + 𝑉 𝑟 +
𝑙 𝑙 + 1 ℏ%
2𝜇𝑟% 𝑢 = 𝐸𝑢
[Again,𝜇 =mass]
Note:thisequationdependsontheangularmomentumstate,through𝑙
Centralpotentials
Infinitesphericalwell
• Agoodexampleofthisisa“particleinasphere”,where
• Inthiscase,theenergyeigenfunctions 𝑢S(𝑟) at𝑟 < 𝑎 satisfy
• Boundaryconditionis𝑢 = 0 at𝑟 = 𝑎.Thefirsteigenfunctionsare𝑢 ∝ sin 𝑘𝑟 for𝑙 = 0 and𝑢 ∝ qrs tm
tm− cos 𝑘𝑟 for𝑙 = 1
• Notethatthefullenergyeigenfunction alsoincludestheangularpiece,𝜓 𝑟, 𝜃, 𝜙 = [𝑢S 𝑟 /𝑟]𝑌fg(𝜃, 𝜙) – thestateoftheparticleischaracterisedby3quantumnumbers𝑛, 𝑙,𝑚
𝑉 𝑟 = ?0, 𝑟 < 𝑎∞, 𝑟 > 𝑎
−ℏ%
2𝜇𝑑%𝑢S𝑑𝑟% +
𝑙 𝑙 + 1 ℏ%
2𝜇𝑟% 𝑢S = 𝐸𝑢S
Centralpotentials
Infinitesphericalwell
• Herearethefirstfewradialeigenfunctions fortwovaluesof𝑙:
• Theprobabilityoffindingtheparticlebetween𝑟 and𝑟 + 𝑑𝑟 isgivenby𝑟% 𝜓 % ∝ 𝑟% 𝑅 % ∝ 𝑢 % – theextrafactorof𝑟% isappearingbecauseofthevolumeelementinsphericalpolars
𝑙 = 0 𝑙 = 1𝑢(𝑟) (unnormalised) 𝑢(𝑟) (unnormalised)
𝑟/𝑎 𝑟/𝑎
edgeedge
Eigenfunctions ofthehydrogenatom
SolutionofradialequationforCoulombpotential
• However,themostimportantexampleofacentralpotentialisanelectroninahydrogenatomorbitingaroundanucleus,whichfollowstheCoulomb
potentialenergy,𝑉 𝑟 = − y"
z{|}m
• Inthiscasetheradialequationbecomes(where𝑎 = 4𝜋𝜀�ℏ%/𝜇𝑒%),
−𝑑%𝑢S𝑑𝑟% + −
2𝑎𝑟 +
𝑙 𝑙 + 1𝑟% 𝑢S =
2𝜇𝐸ℏ% 𝑢S
𝑟
+𝑒
−𝑒
(Sorryfortheillustrationwithclassicalpointparticles.
TheyareofcourseprobabilitycloudsinQM!)
Eigenfunctions ofthehydrogenatom
SolutionofradialequationforCoulombpotential
• Wecansolvethisequationbyconsideringtwolimits…
• If𝑟 → ∞,wehave−!"�!m"
= %l�ℏ"𝑢.Werecognisethisequation
ashavingsolution𝑢(𝑟) ∝ 𝑒6m/�,where𝐸 = − ℏ"
%l�"
• If𝑟 → 0,wehave−!"�!m"
+ f(fkT)m"
𝑢 = 0.Thisequationhasasolution𝑢(𝑟) ∝ 𝑟fkT
• Thislogicmotivatesthatthecompletesolutionisapolynomialmultipliedbyanexponential,dependingonthevalueof𝑙
Eigenfunctions ofthehydrogenatom
• Thetextbookexplains[wewon’tgivethederivationheresinceit’sabitinvolved…] thattheenergyeigenvalues𝐸S canbecharacterisedbyasinglequantumnumber𝑛,andagivenenergyhas𝑛degenerateeigenfunctions 𝑢Sf(𝑟) givenby𝑙 = 0,1, … , 𝑛 − 1
• Herearesomesolutionsfor𝑅Sf 𝑟 = 𝑢Sf(𝑟)/𝑟 correspondingtothefirsttwovaluesof𝑛 = 1,2 andtheallowedvaluesof𝑙:
𝑅T� =2𝑎V/%
𝑒6m/�
𝑛 = 1 𝑛 = 2
𝑙 = 0
𝑙 = 1
𝑅%� =1
2� 𝑎V/%1 −
𝑟2𝑎 𝑒6m/%�
𝑅%T =1
2 6� 𝑎V/%𝑟𝑎 𝑒6m/%�(notallowed)
Eigenfunctions forhydrogenatom
Eigenfunctions ofthehydrogenatom
• Theradialextentoftheeigenfunctions arecharacterisedbythe
parameter𝑎 = z{|}ℏ"
ly"=
5.3×106TT𝑚 knownastheBohrradius
• Herearethefirstfewradialeigenfunctions,plottedasaprobabilitydensity 𝑢Sf % =𝑟% 𝑅Sf %
Eigenfunctions forhydrogenatom
Eigenfunctions ofthehydrogenatom
Energylevelsandquantumnumbersofhydrogenatom
• Thetextbookshowsthattheenergyeigenvaluesonlydepend
on𝑛,andaregivenby𝐸S = −𝐸T/𝑛%,where𝐸T =l%ℏ"
y"
z{|}
%.
ThisisthefamousBohrformulaforthehydrogenenergylevels
Imagecredit:Hyperphysics
Eigenfunctions ofthehydrogenatom
Energylevelsandquantumnumbersofhydrogenatom
• Let’srecapthefullargument:
1. TheSchrödingerequationforacentralpotentialalwayshasseparablesolutions𝜓(𝑟, 𝜃, 𝜙) = 𝑅Sf 𝑟 𝑌fg(𝜃, 𝜙),where𝑌fg arethesphericalharmonicsand𝑅Sf satisfiesaradialequation
2. Hence,theseareautomaticallyeigenfunctions ofangularmomentum,with𝐿% = 𝑙(𝑙 + 1)ℏ% and𝐿* = 𝑚ℏ (−𝑙 ≤ 𝑚 ≤ +𝑙)
3. ForaCoulombpotentialinparticular,theenergyeigenvaluesdonotdependon𝑙,butonlyonasinglequantumnumber𝑛,𝐸S =− 𝐸T/𝑛%,withtherestriction0 ≤ 𝑙 ≤ 𝑛 − 1
4. Therearehence3quantumnumberswhichcharacterise thehydrogenatom:totalenergy(𝑛),totalangularmomentum(𝑙)andthe𝑧-componentofangularmomentum(𝑚)
Eigenfunctions ofthehydrogenatom
Energylevelsandquantumnumbersofhydrogenatom
• Thefulleigenfunctions 𝜓(𝑟, 𝜃, 𝜙) areacombinationoftheradialeigenfunction andsphericalharmonics:
Eigenfunctions ofthehydrogenatom
Energylevelsandquantumnumbersofhydrogenatom
• Countingthenumberofdistincteigenstatesassociatedwithaspecificenergy𝑛 …
• Thereare𝑛 possiblevaluesof𝑙
• Foreach𝑙,thereare(2𝑙 + 1) allowedvaluesof𝑚
• Combiningallthose,wefind𝑛% distinctstates
Eigenfunctions ofthehydrogenatom
Summary
• Thehydrogenatomhasdiscreteenergylevels𝐸S = −𝐸T/𝑛%,
where𝐸T =l%ℏ"
y"
z{|}
%and𝒏 istheenergyquantumnumber
• Foreachstate𝑛,thereare𝑛 differentvaluesof𝑙 =(0,1, … , 𝑛 − 1),where𝒍 isthequantumnumberfortotalangularmomentum and𝐿% = 𝑙(𝑙 + 1)ℏ%
• Foreachstate𝑙,thereare(2𝑙 + 1) differentvaluesof𝑚 =(−𝑙, −𝑙 + 1,… , 𝑙 − 1, 𝑙),where𝒎 isthequantumnumberforthe𝒛-componentofangularmomentum and𝐿* = 𝑚ℏ
• Theenergyeigenfunctions arethen𝜓Sfg 𝑟, 𝜃, 𝜙 =𝑅Sf 𝑟 𝑌fg 𝜃, 𝜙 = ���(m)
m𝑌fg 𝜃, 𝜙
Summary
Eigenfunctions ofthehydrogen
atom
Centralpotentials
• ForaCoulombpotential,theradialpiecetakestheformofapolynomialmultipliedbyanexponential
• Thehydrogenatomischaracterisedbyquantumnumbers(𝑛, 𝑙, 𝑚) for(𝐸, 𝐿%, 𝐿*) where0 ≤ 𝑙 ≤ 𝑛 − 1and−𝑙 ≤ 𝑚 ≤ 𝑙
• Ifthepotentialdependsonlyontheradius𝑟,thentheangularpieceof𝜓 istheangularmomentumeigenfunctions,thesphericalharmonics𝑌fg(𝜃, 𝜙)
• Theradialpieceof𝜓 satisfiesthe1DSchrödingerequationforaneffectivepotential,dependingon𝑙
• The3Dtime-independentSchrödingerequationis
− ℏ"
%g𝛻%𝜓 + 𝑉𝜓 = 𝐸𝜓,where𝛻% = '"
'#"+ '"
')"+ '"
'*"
• Aconvenientmethodofsolvingistosearchforawavefunction separableinthesystemco-ordinates
• Differenteigenfunctions whichhavethesameenergyarecalleddegeneratestates
Particleinabox