Upload
eugene-stewart
View
218
Download
0
Embed Size (px)
DESCRIPTION
Vibrational Autoionization of MX Rydberg States Formation of MX + Ions in Selected Rovibronic States?
Citation preview
Autoionization Branching Ratios for Metal Halide Molecules
Jeffrey J. KayLawrence Livermore National Laboratory
OSU Molecular Spectroscopy SymposiumSession RD (Spectroscopic Perturbations)
23 June 2011
Robert W. FieldMassachusetts Institute of Technology
Cold MoleculesCurrently there is great interest in producing dense
samples of cold molecules and ions
Low velocities, long interaction times allow investigation of unexplored areas of molecular physics:
Cold Chemistry
Control UsingExternal Fields
Precision Spectroscopic Measurements
Time Variation of mp/me, Ammonia
New States of Matter
Quantum Degeneracy
Vibrational Autoionization of MX Rydberg States
Formation of MX+ Ions in Selected Rovibronic States?
Producing MX+ by Autoionization
Most ionization methods non-state-selective
Electron bombardmentNonresonant photoionization
What about autoionization?Specific rovibronic MX Rydberg levels can be selected by laser and spontaneously eject an electron, leaving behind MX+ ion.
What is the MX+ rovibrational state distribution? MX X 2S+1ΛΩ
MXIntermediate
State
MX Rydberg State
|n,L,Λ,v,J>
MX+ + e-
IonizationContinua
J+=0 J+=1J+=2
J+=3
Production of state-selected metal halide ions?
Autoionization Branching RatiosProduct state distributions following autoionization difficult to calculate.
MX n, l ,λ,v, J → e− e,λ + MX + v+, J+
MX+ rovibronic state distribution depends sensitively on electron-ion electrostatic interactions, especially their dependence on R
The only molecule with accurate and complete predictions of autoionization rovibronic branching ratios:
H2
One state 60+ decay channels!
Quantum Defect Model for CaFRecently, we developed a complete quantum defect theory (QDT) model for CaF
Summarizes electron-ion interactions in terms of an R-, E-dependent quantum defect matrix, μ(R, E)
75 parameter model = Infinite # of Rydberg statesVibronic perturbations
Vibrational autoionizationRotational autoionization
Quantum Defect Model for CaF
A molecule summarized in 75 parametersAll spectra. All dynamics.
Electronic Structure of CaFCaF is a prototypical MX molecule
F-
Any MX molecule can be built-up from CaF by adding core-excited states and spin-orbit effects
“Sodium Atom” of diatomics:One unpaired electron outside closed shells
Ca2+
e-
Quantum Defect Theory
1ion CoulombH H H H + +
ψλN+v+
fλ E λ,m N+ ,v+ δλN+v+ ;λ'N+ 'v+ '
− KλN+v+ ;λ'N+ 'v+ '
gλ'N+ 'v+ '
E λ,m N+ 'v+ 'λ'N+ 'v+ '∑
Electron radial wave functions
Ion corewavefunctions
Reaction matrix elements
Scattering Theory: Physics Embodied in Reaction Matrix
3. Form superposition of channel functions
4. Determine: At which energies do wavefunctions satisfy boundary conditions?
2. Define “channel functions” for all energies:
1. Separate H into e-, ion, interaction terms:
The Reaction Matrix
el vib rot
Rψδ ion∑ Rψδ eλion vibion rotion∑
Short Range: Born-Oppenheimer products
Long Range:Electron-ion products
rr = rc
Division of space
r = rvr
Reaction Matrix is the Heart of a QDT Model“Frame Transformation” allows expression in terms of quantum defects
Core Short Range Long Range
Frame TransformationAt large electron-ion separation, both forms of wavefunction must be equal:
vrr r i j ion ion ioni j
A el vib rot B Ryd el vib rot
By explicitly matching wavefunctions, can express LARGE number of reaction matrix elements in terms of SMALL number of quantum defects.
Quantum Defect Matrix Elements(FEW)
Reaction Matrix Elements(MANY)
K
l v+N+ ,λ'v+ 'N+ ' Λ N+ N
Λ∑ χ
v+N+
R tanπmλλ'Λ R χv+ '
N+ ' R δR∫⎡⎣ ⎤⎦ N+ 'Λ
N
R
Rydberg States of CaF
CaF+ (1Σ+, v=0) + e-v+=0
v+=1Rydberg statesHund’s Case (b)
Ion core 1Σ+
Hund’s Case (b)
n*, l ,λ,N,M
Ionization Continuum
Hund’s Case (d) e, l N + ,v+ ,Λ+ = 0
1Σ+
1Σ+
Autoionization Branching Ratios
Γ
i→N +N ,±( ) ∝ α i , N , ±
dμdR
β j , N , ± β j , N , ± l ", N + ", N , ±,v = 0j , l∑
2
a i , N , ± = α i , N , ± l , N + , N , ±,v = 1 l , N + , N , ±,v = 1
l ,N +∑
b j , N, ± = l ', N + ', N ,v = 0 l ', N + ', N ,v = 0 β j , N , ±
l ',N + '∑
Rydberg StateHund’s Case (b)
ContinuumHund’s Case (b)
Eigenvector Decomposition(From MQDT Calculation)
Case (b) -> Case (d)
Quantum Defect Derivatives
Branching ratios can be calculated from quantum defect derivatives
Autoionization Branching Ratios: CaF
s Σ
p Σ
d Σ
f Σ
0% 10%
20%
30%
40%
50%
60%
70%
80%
90%
100%
N+ = 0N+ = 1 N+ = 2 N+ = 3
Branching Ratios for N = 0
‘d’ Σ Rydberg series produces primarily N+ = 0 ionsAutoionization produces mostly N+ = 0, 1
MostlyN+ = 0, 1
s Σ
p Σ
d Σ
f Σ
p Π
d Π
f Π
0% 10% 20% 30% 40% 50% 60% 70% 80% 90% 100%
N+ = 0N+ = 1 N+ = 2 N+ = 3N+ = 4
Autoionization Branching Ratios: CaFBranching Ratios for N = 1
Branching ratios broaden, shift to higher N+ (=1, 2)
MostlyN+ = 0,1,2
s Σ
p Σ
d Σ
f Σ
p Π
d Π
f Π
d Δ
f Δ
0% 10% 20% 30% 40% 50% 60% 70% 80% 90%100%
N+ = 0N+ = 1 N+ = 2 N+ = 3N+ = 4N+ = 5
Autoionization Branching Ratios: CaFBranching Ratios for N = 2
Branching ratios broaden, shift to higher N+ at higher N
MostlyN+ = 1,2,3
s Σ
p Σd Σf Σ
p Πd Πf Π
d Δf Δf Φ
0% 10% 20% 30% 40% 50% 60% 70% 80% 90% 100%
N+ = 0N+ = 1 N+ = 2 N+ = 3N+ = 4
Autoionization Branching Ratios: CaFBranching Ratios for N = 3
Branching ratios broaden, shift to higher N+ at higher N
MostlyN+ = 2,3,4
Branching Ratios: TrendsOverall trends we observe:
1. Best rotational selectivity at low N
2. Less selectivity at high N (more open channels)
3. <N+> = N
4. Propensity rule: N+ = N, N ± 1 (due to ΔL = ±1 L-mixing)
Autoionization Branching Ratios: General MX
Rydberg statesHund’s Case (a) n*, l , s, J, M
ContinuumHund’s Case (e) e, l , s, j J + ,S+ ,v+ ,Λ+
Expect similar trends for other MX molecules.(Greatest N+-selectivity at low N; Shift to high N+ at high N)
Methodology developed here applicable to any MX
Light molecules (MgF+, TiF+): Very similar trendsHeavy molecules (BaF+, HfF+): Coupling cases change due to spin-orbit
Rydberg statesHund’s Case (b) n*, l , N , M
ContinuumHund’s Case (d) e, l N + ,v+ ,Λ+
Low Z High Z
Acknowledgments
Funding: National Science Foundation
We thank Eric Cornell and the Cornell Group (JILA/Colorado) for their interest in vibrational
autoionization.
eEDM Measurements: Cold Metal Halide Ions
Large dipole moment enables measurements of electron electric dipole moment (eEDM)
HfF+ electric field ~1010 V/cm
Easily trappable using RF traps
Metastable 3Δ1 state ideal for eEDM measurements
http://jila.colorado.edu/bec/CornellGroup/
Metal halide ions (MX+) are candidates for ultra-high-precision spectroscopic measurements
Cornell Group (JILA) eEDM SchemeHfF+: eEDM Measurements
Autoionization Branching Ratios: General MX
Γ
i→J +N ,±( ) ∝ α i , J, ±
dμdR
β j , J, ± β j , J, ± l "J + "J, ±,v = 0j , l∑
2
Initial State (Hund’s Case (a))
Final States(Hund’s Case (a))
Final States(Hund’s Case (e))
Rydberg statesHund’s Case (a) n*, l , s, J, M Continuum
Hund’s Case (e) e, l , s, j J + ,S+ ,v+ ,Λ+
Branching Ratios for High-Z MX+ Ions
R
Rydberg States of HfF
Rydberg statesHund’s Case (a)
Ion core 3Δ1
Hund’s Case (a)
n*, l , s, J, M
Ionization Continuum
Hund’s Case (e) e, l , s, j J + ,S+ ,v+ ,Λ+ = 2
HfF+ (1Σ+) + e-v+=0
v+=1
1Σ+
3Δ1
v+=03Δ1
v+=03Δ2
v+=03Δ3
(To Be Added)
Branching Ratios for HfF (3D Bar Chart)(Several values of J)
HfF+ Ion: eEDM Measurements
HfF+ Ion: eEDM Measurements
HfF+ Ion: eEDM Measurements
HfF+ Ion: eEDM Measurements
Hund’s Case (b) to Hund’s Case (d) Transformation
Ch. Jungen and G. Raseev, Phys. Rev. A 57 2407 (1998)
N + Λλ,N,M,Λ+ , π
11+δΛ,0δΛ+ ,0
11+δ
Λ+ ,0
−1 N−Λ 2N+ +1 1/2
× 1+δΛ+ ,0
−1π−q+ −N+ +λ⎡⎣ ⎤⎦
N+ λ NΛ+ Λ−Λ+ −Λ
⎛⎝⎜
⎞⎠⎟
Case (b): Good quantum numbers Λ, l , N , M ,Λ+ , p
N+,λ,N,M,Λ+, πCase (d): Good quantum numbers
Hund’s Case (a) to Hund’s Case (e) Transformation
Ch. Jungen and G. Raseev, Phys. Rev. A 57 2407 (1998)
Case (a): Good quantum numbers Λ,S,Ω, l , s, Λ+ ,S+ , J, M , pCase (e): Good quantum numbers j, J +,Ω+ ,λ,s,Λ+,S+ , J,M, π
Ω+J + j SΛΩl ,s,Λ+ ,S+ ,J , M , p( ) = −1( )S+ −Ω+ +l +Λ+ J +Ω 2S + 1( ) 2 j + 1( ) 2J + +1( )
1+ Δ1( ) 1+ Δ2( ) 1 + Δ3( )
⎡
⎣⎢⎢
⎤
⎦⎥⎥
× s S+ SΩ − Λ + Λ+ − Ω+ Ω+ − Λ+ −Ω + Λ
⎛
⎝⎜
⎞
⎠⎟
l s j
Λ − Λ+ Ω − Λ + Λ+ − Ω+ −Ω + Ω+
⎛
⎝⎜
⎞
⎠⎟
J + j J
Ω+ Ω − Ω+ −Ω
⎛
⎝⎜
⎞
⎠⎟
⎡
⎣⎢⎢
+δ Λ+ ,0 −1( )p−q−S+ − J + +l
× s S+ SΩ − Λ + Λ+ + Ω+ −Ω+ − Λ+ −Ω + Λ
⎛
⎝⎜
⎞
⎠⎟
l s j
Λ − Λ+ Ω − Λ + Λ+ + Ω+ −Ω + Ω+
⎛
⎝⎜
⎞
⎠⎟
J + j J
−Ω+ Ω + Ω+ −Ω
⎛
⎝⎜
⎞
⎠⎟
+Δ3 −1( )p−q−S− J
× s S+ S−Ω − Λ + Λ+ − Ω+ Ω+ − Λ+ Ω + Λ
⎛
⎝⎜
⎞
⎠⎟
l s j
Λ − Λ+ −Ω − Λ + Λ+ − Ω+ Ω + Ω+
⎛
⎝⎜
⎞
⎠⎟
J + j J
Ω+ −Ω − Ω+ Ω
⎛
⎝⎜
⎞
⎠⎟
Autoionization Branching Ratios
Γ
i→N +N ,±( ) ∝ α i , N , ±
dμdR
β j , N , ± β j , N , ± l "N + "N , ±,v = 0j , l∑
2
Branching ratios are calculated directly from quantum defect matrix elements, using a simple formula:
Quantum Defects (Coupling acts at short range = Case (b))
Initial State (Hund’s Case (b))
Final States(Hund’s Case (b))
Final States(Hund’s Case (d))