Karel Houfek
description
Transcript of Karel Houfek
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Uncertainties in calculations of low-energy resonant electron collisions with
diatomic molecules
Karel Houfek
in collaboration with J. Horáček, M. Čížek and M. Formánek from Prague
V. McKoy and C. Winstead from CalTech, USAJ. Gorfinkiel and Z. Mašín from Open University, UK
C.W. McCurdy and T. Rescigno, LBNL, USA
Institute of Theoretical PhysicsFaculty of Mathematics and PhysicsCharles University in Prague
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Resonant electron-molecule collisions at low energies
Vibrational (VE) and rotational excitation including elastic scattering
Electronic excitation
Dissociative electron attachment (DA)
three-body decays etc.
We study also inverse process of DA called associative detachment (AD)
),(ABe)(),(ABe ffii NABN
BA)()(ABe ABi
*ABe)(ABe AB
)(ABe)(BA fAB
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Theoretical description of electron-molecule collisions
First fixed-nuclei calculations provide
• potential energy curves (surfaces) of neutral molecule (standard)and molecular ion where electron is bound (more difficult)
• fixed-nuclei scattering data (eigenphase sums, cross sections) –several methods available
from which a model for nuclear dynamics is constructed within some approximation• local complex potential approximation – simplest to use, first choice• nonlocal, complex, and energy-dependent potential – universal, but difficult
• R-matrix approach of Schneider et al – applied only to N2 and CO
Complex Kohn variational principle (Berkeley, USA)
R-matrix (UCL and OU, UK)
Schwinger multichannel variational method (CalTech, USA)
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Motivation for this talk – results for e + COSMC method for electron scattering + LCP and NRM for nuclear dynamics
Fixed-nuclei eigenphase sums
Potential energy curves
Cross sections – vibrational excitation
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Cross sections – vibrational excitation
Motivation for this talk – results for e + COSMC method for electron scattering + LCP and NRM for nuclear dynamics
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e + CO – comparison with previous calculations
Morgan, J. Phys. B 24 (1991) 4649Laporta, Cassidy, Tennyson, Celiberto, PSST 21 (2012) 045005
What is the best theoretical result and what uncertainties are there?
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e + CO – comparison of potential energy curves
Morgan, J. Phys. B 24 (1991) 4649Laporta, Cassidy, Tennyson, Celiberto, PSST 21 (2012) 045005
This gives us a hint of the origin of discrepancies and uncertainties
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Another example of results – e + HCl
Allan, Čížek, Horáček, Domcke, J. Phys. B 33 (2000) L209
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Nonlocal resonance model by Fedor et al – Phys. Rev. A 81 (2010) 042702
HCl – structures in the VE and DA cross sections
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HCl – origin of structures in the cross sections
Uncertainties in position of structures – shape and relative position of PECUncertainties in absolute values of the cross sections – details of the model used
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Uncertainties in calculations of e-M collisions
1) Potential energy curves (surfaces)
2) Fixed-nuclei electron scattering
3) Model for nuclear dynamics
various methods (HF, CASSCF, CI, CC) absolute energies are not important relative shape and position of curves (surfaces) is crucial, problem
of size consistency (N and N+1 electrons) known difficulties to obtain correct electron affinities
various models (SE, SEP, CAS) problem of consistency of scattering data with accurate potential
energy curves
different levels of approximation (effective range, LCP, NRM etc.) possibility of testing using two-dimensional model
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Potential energy curves – e + CO systemDifferent methods with aug-cc-pVTZ basis
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Potential energy curves – e + CO systemMRCI based on CASSCF(10,9) for larger basis sets
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LCP model with improved potentials – e + CO systemMorse potential and adjusted width to get a good agreement with experiment
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R-matrix electron scattering calculationsSchwinger multichannel variational method cannot describe the target beyond the Hartree-Fock approximation –> impossible to have a better description of the target consistent with electron scattering calculations
Possible with UK R-matrix polyatomic codes – several different scattering models available
• SE – static exchange – target at HF level
• SEP – static exchange plus polarization – target at HF level
• CAS – close-coupling model (only a few excited target states included) based on complete active space (CASSCF) calculations of the target
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R-matrix electron scattering calculations – CAS modelCASSCF (10,8) model – 6-311G** basis, 9-12 virtual orbitals, 13 states at R = 2.1
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R-matrix electron scattering calculations – CAS modelCASSCF (10,8) model – 6-311G** basis, 10 virtual orbitals, 13 states
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R-matrix electron scattering calculations – CAS modelCASSCF (10,8) model – 6-311G** basis, 10 virtual orbitals (1 different), 13 states
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R-matrix electron scattering calculations – CAS modelCASSCF (10,8) model – 6-311G** basis, 11 virtual orbitals, 9 states
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Vibrational excitation cross sections – e + CO
Nuclear dynamics – local vs. nonlocal theory
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Nuclear dynamics – local vs. nonlocal theorysimple two-dimensional model as a testing toolModel Hamiltonian – one nuclear (R) and one electronic (r) degree of freedom
),(2
)1(
2
1)(
2
1int22
2
02
2
rRVr
ll
dr
dRV
dR
dH
- potential energy of the neutral molecule- Morse potential
)(0 RV
l - angular momentum of the electron- p-wave (l = 1) or d-wave (l = 2)
),(int rRV - interaction potential- bound state of the electron for large R- resonance for small R Barrier for incoming electron →
shape resonance for small R
Houfek, Rescigno, McCurdy, Phys. Rev. A 73 (2006) 032721Houfek, Rescigno, McCurdy, Phys. Rev. A 77 (2008) 012710
incoming electron
vibrational m
otion
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Fixed-nuclei calculations – N2-like model
22
2
2
)1()(
2
1)(
2
r
lleR
dr
dRH r
el
Electronic Hamiltonian used in fixed-nuclei calculations
Cross sections (or phase shifts) resonance position and width electron bounding energy
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Exact wave function at a given energy
with the initial state
where is initial molecular vibrational state
Solution of the full 2D model
),(),(1
),(),( 0int
0 rRrRViHE
rRrR
)(Riv
)()(),( 20 krrjRrR lk
vi
elv EEEi Numerical solution using
finite elements with DVR basisand exterior complex scaling
N2-like model incoming electron
vibrational motion
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NO-like model – scattered wave functions for v i = 0
Franck-Condon region
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Nuclear dynamics – LCP approximation
Simple extensions of local complex potential approximation
• barrier penetration factor, nonlocal imaginary part
Vibrational excitation cross section
Dissociative attachment cross section
Local complex potential approximation
Details can be found in Trevisan et al, Phys. Rev. A 71 (2005) 052714
)(2
)()()(
2)(
2
12/1
2
2
RR
RRi
REdR
dE
ivEres
22/1
2
3
)2/(4
)( Evi
VEvv ffi kE
2
2
2
)(lim2
)( Rk
KE d
Ri
DADAvi
NO-like model
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Test of LCP approximation and its extensions NO-like model
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Nonlocal theoryDirect derivation by choosing a proper diabatic basis for electronic part of the problem
• discrete state
• othogonal “background” continuum states
satisfying conditions
Into which we can expand the full wave function
Using matrix elements of the electronic Hamiltonian in this basis
we finally get effective equations for nuclear motion
);( Rrk
);( Rrd
0),(
,0),(
R
Rr
R
Rr kd )();(lim rRr bdR
)2/'2/()2/)(()()(
)()(,)()(
2220'' kkkRVRHRV
RHRVRHRV
kelkkk
kelddkdeldd
),()(),()(),( RrRkdkRrRrR kkdd
)()()()',,(')()( RRVRRREFdRRRVTEii vdkdddR
)'(2/)()(')',,(12
0 RVikRVTERkdkVdRRREF dkRdk
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Nonlocal theory – cross sectionsVibrational excitation and dissociative attachment cross sections
It can be shown that for a properly chosen discrete statethere is no background contribution to the DA cross section.
But the VE T-matrix consists of two terms
The resonance term is calculated within nonlocal resonance theory
The background is non-zero even for inelastic vibrational excitationand for the 2D model can calculated exactly
2
2
2
)(lim2
)( Rk
KE d
Ri
DADAvi
,)(4
)(2
2
3
ETk
E VEvv
i
VEvv fifi
)();(lim rRr bdR
)()()( ETETET bgvv
resvv
VEvv fififi
Rddkvresvv fffi
VET )(
Rvldkdkv
lkvkv
bgvv iiffiifffi
JVJVET int)(
)();()( * rJRrdrRJ lkd
ldk ii
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smooth coupling (width) – works in all channels, reasonably small background
Test of nonlocal theory – NO-like model
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Local vs. nonlocal theory – e + F2 modelNO-like model – works in all channels, reasonably small background
works in all channels, reasonably small background
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the whole information about the dynamics is “hidden”in coupling (non-local potential)
Minimizing background – e + F2 model
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ConclusionsUncertainties in fixed-nuclei calculations
Uncertainties in nuclear dynamics
shape of potential energy curves (surfaces), relative positions of potentials for neutral molecule and molecular negative ion – advanced quantum chemistry methods (MRCI, CCSD(T) etc) are necessary, basis sets limit, no fitting to Morse or similar analytical potential –> comparison with available experimental data (electron affinities, spectroscopic constants etc.)
problem of consistency of scattering data with accurate potential energy curves– it is necessary to go beyond HF description of the target, adjusting parameters of electron scattering calculations to get correct electronic energies where electron is bound –> estimating errors by comparison of several scattering models
nonlocal theory necessary in many cases, simple extensions of local complex potential approximation can sometimes improved the results, but it strongly depends on the system
unknown background contribution –> uncertainties estimates frommodel calculations