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![Page 1: Oxidation State Ambiguity in f Element Organometallics - a Spectroscopic and Quantum Chemical Journey Nik Kaltsoyannis Department of Chemistry, University.](https://reader035.fdocuments.us/reader035/viewer/2022062422/56649e8b5503460f94b90ab4/html5/thumbnails/1.jpg)
Oxidation State Ambiguity in f Element Organometallics -
a Spectroscopic and Quantum Chemical Journey
Nik KaltsoyannisDepartment of Chemistry, University College London
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Outline of presentation
Story 1: X-ray absorption spectroscopy of Ce compounds
Story 2: Gas-phase photoelectron spectroscopy of CeCp3
Story 3: Multiconfigurational quantum chemical calculations of M(COT)2
(COT = 8-C8H8; M = Th, Pa, U, Pu, Cm and Ce)
Story 4: Multiconfigurational quantum chemical calculations of CeCp3 and CeCp3+ (Cp = 5-C5H5)
Ln(COT)2 the “lanthanocenes”An(COT)2 the “actinocenes”
Ce
CeCp3
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Story 1: X-ray absorption spectroscopy of Ce compounds
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Qualitative molecular orbital diagram for
M(COT)2 M = f element
COT(COT)2
0 (a2u)
1 (e1g)
2 (e2u)
3 (e3g)
4 (b1u)
a2u
a1g
e1u
e1g
e2g
e2u
e3u
e3g
b2g
b1u
f
d
f (e3u)
f (e1u)
f (e2u)
f (a2u)
d (a1g)
d (e1g)
d (e2g)
M(COT)2M
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The traditional view of Ce(COT)2 and Th(COT)2
2 (e2u)e2g
e2u
ff (e3u)
f (e1u)
f (e2u)
f (a2u)
Ground state is 1A1g with an electronic configuration e2u(p2)4f0
Þ M(IV) and 2 x COT2-
Correct description of Th(COT)2 BUT NOT Ce(COT)2
M. Dolg, P. Fulde, H. Stoll, H. Preuss, A. Chang and R. M. Pitzer J. Chem. Phys. 195 (1995) 71
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Dolg et al.’s view of Ce(COT)2
2 (e2u)e2g
e2u
ff (e3u)
f (e1u)
f (e2u)
f (a2u)
2 (e2u)e2g
e2u
ff (e3u)
f (e1u)
f (e2u)
f (a2u)
Ground state is 1A1g with two contributing electronic configurations e2u(p2)4f0 (20%) + e2u(p2)3f1 (80%)
Þ Ce(III) and 2 x COT1.5-
20%
80%
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Can we test this experimentally (how do we measure oxidation state)?
N. M. Edelstein, P. G. Allen, J. J. Bucher, D. K. Shuh, C. D. Sofield, A. Sella, M. Russo, N. Kaltsoyannis and G. Maunder J. Am. Chem. Soc. 118 (1996) 13115
X-ray Absorption Near Edge Spectroscopy (XANES)
Ce K edge (1s electrons)
Need a variable energy light source capable of delivering c. 40 keV photons (Stanford Synchrotron)
Representative K-edge spectra of Ce compounds
CeO2 (Ce(IV))
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Ce K-edge XANES results
1 CeO2 (solid) 8 Ce2(SO4)3 (solid) 15 Ce(NO3)3 (1.2 M HCl solution)
2 Ce(NH4)4(SO4)4.2H2O (solid) 9 CeSi2 (solid)
3 Ce(NH4)4(SO4)4.2H2O (1.6 M HNO3 soln.) 10 CeI3.(THF)x (THF soln.) 16 Ce[1,4(TMS)2C8H6]2 (toluene soln.)
4 Ce(CH3C(O)CHC(O)CH3)4 (toluene soln.) 11 Ce[(Me3C)2C5H3]3 (toluene soln.) 17 Ce[1,3,6(TMS)3C8H5]2 (toluene soln.)
5 CeCl3.6H2O (solid) 12 Ce2(SO4)3 (1.6 M HNO3 soln.) 18 Li{Ce[1,4(TMS)2C8H6]2} (toluene soln.)
6 CeF3 (solid) 13 Ce2(SO4)3 (1.2 M HCl soln.) 19 K{Ce(C8H8)2} (toluene soln.)
7 Ce2O2S (solid) 14 Ce(NO3)3 (1.6 M HNO3 soln.)
▼ Ce(IV) compounds
■ Ce(III) compounds
0
5
10
Compound
Shi
ft fr
om C
eB6
Sta
ndar
d (e
V)
Ce3+compoundsQ
Ce4+compoundsWSubstituted cerocenesL
Substitued cerocenes
Ce(III) !!
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H He
Li Be B C N O F Ne
Na Mg Al Si P S Cl Ar
K Ca Sc Ti V Cr Mn Fe Co Ni Cu Zn Ga Ge As Se Br Kr
Rb Sr Y Zr Nb Mo Tc Ru Rh Pd Ag Cd In Sn Sb Te I Xe
Cs Ba La Hf Ta W Re Os Ir Pt Au Hg Tl Pb Bi Po At Rn
Fr Ra Ac Rf Db Sg Bh Hs Mt
Ce Pr Nd Pm Sm Eu Gd Tb Dy Ho Er Tm Yb Lu
Th Pa U Np Pu Am Cm Bk Cf Es Fm Md No Lr
Increasing tendency toward lanthanide-like chemistry (An(III) dominant)
Þ Are the ground states of the later actinocenes multiconfigurational? Need: high-level ab initio calculations (see story 3….)
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Story 2: Gas-phase photoelectron spectroscopy of CeCp3
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Gaseousmolecules
The experiment
UV or X-ray light e-
e-
e-
Measure kinetic energy of electrons and determine ionization energy as the difference between the energy of the incident light photons and the electrons’ kinetic energy
Direct probe of electronic energy levels
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Compared with d-block complexes, very few lanthanide complexes have been studied in the gas phase, because it is very hard to see f-based bands in spectra
Two main reasons
1. With Ln(III) compounds ionizations from 4f orbitals come at similar ionization energies to those from ligand orbitals
2. With photon energies given by discharge lamps 4f cross sections (ionization probabilities) are low
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Ionization cross sections (ionization probabilities)
0
2
4
6
8
10
0 50 100 150 200
Calculated photoionization cross sections for C 2p and Ce 4f electrons
(Lindau and Leh)
C 2pCe 4f
Cro
ss s
ect
ion
Photon energy / eV
Delayed maximum
At photon energies accessible with a
discharge lamp, 4f electrons have very low ionization cross sections
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The “Elettra” synchrotron, Trieste, Italy
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Photoelectron spectrum of CeCp3
At low incident photon energies only ionizations from the Cp rings are visible
1500
1000
500
0
counts
20181614121086
IE / eV
Cp š
hv = 25 eV
Cp p
Cp p
0
2
4
6
8
10
0 50 100 150 200
Calculated photoionization cross sections for C 2p and Ce 4f electrons
(Lindau and Leh)
C 2pCe 4f
Cro
ss s
ect
ion
Photon energy / eV
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Low ionization energy band (A) clearly visible BUT also a band just above 10 eV (D) showing f characteristics
250x106
200
150
100
50
0
Counts
181614121086
IE / eV
hv = 40 eV
A
B
C3
D
E F
C1
C2
Photoelectron spectrum of CeCp3 (again)
Cp p
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Resonance structure is observed for bands A and Di.e. ionization of the single 4f electron gives rise to two cation states with f character
Are there really two f bands?
If the incident photon energy is sufficient to excite a Ce 4d core electron to a 4f orbital, a resonance will occur. Ionization of a 4f electron can borrow intensity from this transition and the ionization cross section can show a dramatic increase tune hn to the 4d ionization energy…..
8x106
6
4
2
0
Norm
alize
d c
ounts
181614121086
IE / eV
hv = 122 eV
A (f)
B C
D (f)
Cp p
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What the…..?
Assume neutral CeCp3 has a ground state with the configuration Lf1, where L represents the ligand electrons and f1 is the single 4f electron
The matrix element governing the band intensity for f ionization is given by
1 ˆLf | | LεO where is the free electron (g) wave
Note that (a) Le represents a configuration with ligand electrons and no f electrons, i.e. Lf0 and(b) the ion states corresponding to bands A and D in the photoelectron spectrum must have Le (Lf0) as a contributing configuration
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Assume that ionization of the f electron leads to ligand to metal charge transfer, generating a cation configuration with a hole in the ligand orbitals and a single Ce 4f electron, i.e. L-1f1 (sound familiar….?)
If Lf0 and L-1f1 have the same symmetry, mixing of the two configurations can generate two states of CeCp3
+
gc1Lf0 + c2L-1f1) band A – ground state of CeCp3+
ec3Lf0 – c4L-1f1) band D – excited state of CeCp3+
Our suggestion was that the ground state of CeCp3+ (formally Ce(IV)) is
multiconfigurational, in a manner comparable with that of neutral Ce(COT)2
What the…..? (continued)
M. Coreno, M. DeSimone, J. C. Green, N. Kaltsoyannis, N. Narband and A. Sella, Chemical Physics Letters 432 (2006) 17
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Story 3: Ab initio quantum chemical calculations of M(COT)2 (M = Th, Pa, U, Pu, Cm and Ce)
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• CASSCF/CASPT2 method• MOLCAS code• D2h point group
• Basis sets: correlation consistent, all-electron, ANO (27s24p18d14f)/[10s9p7d5f] for An, (25s22p15d11f)/[9s8p5d4f] for Ce, VDZP for C and H
• Scalar relativistic effects incorporated via 2nd order Douglas-Kroll• Spin-orbit free and spin-orbit coupled calculations
Computational details
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COT(COT)2
1 (e1g)
2 (e2u)
e1g
e2g
e2u
5f
6d
f (e3u)
f (e1u)
f (e2u)
f (a2u)
d (a1g)
d (e1g)
d (e2g)
M(COT)2M
Active spaces
Partial ground state geometry optimisations performed with ((12+n),16) active spaces (n = 0 (Ce, Th), 1 (Pa) and 2 (U)….)
Ground and excited states calculated with ((8+n),14) active spaces (n = 0 (Ce, Th), 1 (Pa), 2 (U)….)
For the partial geometry optimisations of the ground state of Pa(COT)2 (13,16), 11,451,440 configurations were included
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Results – Th(COT)2
Ground state is the expected 1Ag (d0f0)
Metal-ring distance; 2.015 Å (calc), 2.004 Å (expt)
Two lowest energy singlet and triplet states of each D2h irrep calculated (32 states)
Lowest energy dipole-allowed transition is to 1B1u (dσ1f0); 2.47 eV (calc), 2.76 eV (expt –
UV/Vis)
Spin-orbit coupling makes essentially no difference to energy spectrum (<0.05 eV).
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First excited states (Th(Cp'')3)Ground
state
Th(COT)2 energy level diagram
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Results – Pa(COT)2
Ground state is a degenerate pair of spin-orbit free states 2B2u/2B3u (d0ff1)
Metal-ring distance; 1.969 Å (calc), 1.964 Å (“expt”, average of Th(COT)2 and U(COT)2)
Two lowest energy doublet and quartet states of each D2h irrep calculated
Spin-orbit coupling makes a significant difference
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Pa(COT)2 energy level diagram(no spin-orbit coupling)
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The effect of spin-orbit coupling on the ground and lowest excited states of Pa(COT)2
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A comparison of the spin-orbit coupled Pa(COT)2 energy levels (eV) with those from previous calculations
State Symmetry This work Chang et al. a Li & Bursten b
1 E5/2u 0 0 0
2 E1/2u 0.003 0.166 0.049
3 E3/2u 0.459 0.477 0.369
4 E7/2u 0.584 0.362 0.379
5 E1/2u 0.642 0.569 0.541
6 E1/2g 0.880 0.925 0.685
7 E3/2u 1.467 1.222 1.122
a SOCI calculations using the experimental uranocene geometry (1.924 Å)b DFT calculation using the PW91 exchange-correlation functional, using an optimised geometry with ring-metal separation of 1.975 Å
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Results – U(COT)2
Metal-ring distance; 1.944 Å (calc), 1.924 Å (expt)
Spin-orbit coupled ground state is E3g
Dominant configuration of
spin-orbit free state
Total spin of spin-orbit free
state
This work Chang et al.
fp1ff1 1 70.7 68.0
fs1ff1 1 22.1 22.7
fs1ff1 0 7.0 5.3
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Results – U(COT)2
Comparison of experimental (UV/Vis) excitation energies (eV) with calculation
Expt This work
1.880
1.934 1.65
2.018 1.79
Both calculated transitions are principally f dσ in character
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Results – Ce(COT)2
Ground state is the expected 1Ag
Metal-ring distance; 1.964 Å (calc), 1.969 Å (expt)
Lowest energy dipole-allowed transitions are to 1B1u (d0fσ1) and 1B2u/1B3u (d0fp1); 2.47
eV (calc), 2.18 eV (expt – UV/Vis). Second dipole-allowed transition to 1B1u (d0fd1); 2.93 eV (calc), 2.63 eV (expt)
As with Th(COT)2, spin-orbit coupling makes essentially no difference to energy spectrum (<0.05 eV).
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Ce(COT)2 energy level diagram
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A look at the ground and first excited 1Ag states of Ce(COT)2
58.1% f0, 23.4% fd1, 8.7% fd2
84.6% fd1, 6.2% fd2
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How can we square this result with previous
theory and experiment for Ce(COT)2?
(number of states in state-average)
Cha
nge
in g
roun
d st
ate
ener
gy
Single state total energy = -257724.60 eV
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Experiment (XANES): 0.89 ± 0.03
C.H. Booth, M.D. Walter, M. Daniel, W.W. Lukens and R.A. Andersen Phys. Rev. Lett. 95 (2005) 267202
Ce(COT)2 f electron occupancy nf
Calculation: 0.90 ± 0.04
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Configurational admixture of Ce(COT)2 ground state as a function of ns
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Occupation (NOO) of the Ce(COT)2 ground state natural orbitals as a function of ns
A. Kerridge, R. Coates and N. Kaltsoyannis J. Phys. Chem. A 113 (2009) 2896
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Th Pa U Pu Cm0
0.05
0.1
0.15
0.2
0.25
0.3
0.35
What about the actinides?Occupation of the ground state e2u “f” natural orbitals in An(COT)2
Ce(COT)2 = 0.216
A. Kerridge and N. Kaltsoyannis J. Phys. Chem. A 113 (2009) 8737
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Story 4: Ab initio quantum chemical calculations of CeCp3 and CeCp3+
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8x10
6
6
4
2
0
Norm
alize
d c
ounts
181614121086
IE / eV
hv = 122 eV
A (f)
B C
D (f)
Cp p
Recall the PE spectrum of CeCp3…..
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Active spaces for CeCp3 and CeCp3+
2,3 (e1'')e
CpCp3CeCp3
e
a1
a2
1e
1a1
1a2
2e
2a1 + 3a1 + 3e + 4e
4a1 (dz2)
2a2
4f
5d
Ce
Inclusion of all 14 MOs too costly (5,8) for CeCp3 and (4,8) for CeCp3+ (4 a, 4 a)
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Configurational admixture of CeCp3+ 1A ground state as a function of ns
0
10
20
30
40
50
60
70
80
1 2 3 4 5 6 7 8 9 10
Number of states in average
Con
trib
utio
n of
con
figur
atio
n (%
)
2000 2000
2000 u0d0
2000 0020
Use natural orbitals and their occupations
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NOOs of CeCp3 2A ground state
Active space orbital 48a' 49a' 50a' 51a' 33a'' 34a'' 35a'' 36a''
Occupation 1.967 0.001 0.027 0.005 1.966 0.029 0.005 1.000
Single configurational stateOne 4f-localised NO
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NOOs of CeCp3
+ 1A ground state
Active space orbital 48a' 49a' 50a' 51a' 33a'' 34a'' 35a'' 36a''
Occupation 1.961 0.000 0.000 0.038 1.445 0.000 0.555 0.000
Strongly multi-configurational stateNo 4f-localised NO (as expected following 4f ionisation)Energy relative to CeCp3: 7.07 eV (band A in PE spectrum 6.77 eV)
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NOOs of CeCp3
+ fifth excited 1A and 1A states
Active space orbital 48a' 49a' 50a' 51a' 33a'' 34a'' 35a'' 36a''
Occupation 1A 1.509 1.000 0.001 0.490 0.963 0.000 0.000 0.037
Occupation 1A 0.985 1.013 0.000 0.002 1.473 0.000 0.526 0.001
Strongly multi-configurational statesNo 4f-localised NO (as expected following 4f ionisation)Energy relative to CeCp3: 10.00 and 10.17 eV (band D in PE spectrum 9.97 eV)
R. Coates, M. Coreno, M. DiSimone, J.C. Green, N. Kaltsoyannis, A. Kerridge, N. Narband and A. Sella Dalton Trans. (2009) 5943
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Conclusions - 1
Calculations (Dolg et al.) suggest that Ce(COT)2 has a multiconfigurational ground state, with a dominant f1 (Ce(III)) configuration. XANES results (us and Booth et al.) appear to support this.
Variable energy photoelectron spectroscopy of CeCp3 reveals not one but two f bands during resonance; is the ground state of CeCp3
+ multiconfigurational?
CAS calculations on An(COT)2 (An = Th, Pa, U) yield results consistent with experiment and previous computational studies.
CAS calculations on Ce(COT)2 produce excellent agreement with experiment for metal-ring separation, electronic excitation energies and f electron occupancy (nf).
Total energy of Ce(COT)2 ground state, nf, the natural orbitals and their occupations are essentially invariant to the number of states included in the state-average.
Description of ground state in terms of configurational admixture varies wildly as a function of state average configurational admixture not a reliable tool to describe the electronic structure of Ce(COT)2.
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Conclusions - 2
Ce(COT)2 is best described as Ce(IV) system in which transfer of electron density from ligand to metal through occupation of bonding orbitals allows measures of the effective oxidation state to be lower than the formal +4 value, and indeed closer to +3 in certain cases.
Occupation of the ground state e2u “f” natural orbitals increases markedly across the actinide series, indicating that the ground states of the later actinocenes are strongly multiconfigurational.
The ion states which give rise to bands A and D in the photoelectron spectrum of CeCp3
+ are strongly multiconfigurational, and do not possess a Ce 4f-localised natural orbital (i.e. they have the characteristics of f ionization).
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And finally……
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“The effective oxidation state of Ce in cerocene is intermediate between the formal Ce(IV) and Ce(III) situations. When interpreted as a Ce(IV) system the effective oxidation number is lowered toward III by strong orbital mixing, whereas when interpreted as a Ce(III) system a strong configurational mixing increases the effective oxidation number toward IV. The latter choice however is more compact since only two configurations…..are needed for building a sufficiently accurate zeroth-order wavefunction: the cerocene 1A1g ground state can be described as a…..mixture of about 70% 4f1p3 and 30% 4f0p4.”
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The without whom department
National Service for Computational Chemistry Software
BerkeleyNorm EdelsteinPat AllenJerry BucherDave ShuhChad Sofield
UCLAndy KerridgeRosie CoatesAndrea SellaMaria-Rosa RussoGraham MaunderNaima Narband
OxfordJenny Green
Trieste (Elettra)Monica DiSimoneMarcello Coreno
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