Abstract:An ab initio-based global double many-body expansion potential energy surface is reported for the first electronic state of the NO(2)((2)A") manifold. Up to 1700 ab initio energies have been employed to map the full configuration space of the title molecule, including stationary points and asymptotic channels. The calculated grid energies have been scaled to account for the incompleteness of the basis set and truncation of the MRCI expansion and fitted analytically with a total root-mean-squared-deviation smal… Show more
“…More recently, a double many body expansion fit to 1700 points at the MRCI/aug-cc-VQZ level of theory for the 2 A 00 state was carried out. 17 In addition, quasi classical trajectory (QCT) calculations 2,9,13,18 have been reported for the temperature dependent rate for the N( 4 S) + O 2 -NO + O and its reverse reaction using different PESs.…”
Section: Introductionmentioning
confidence: 99%
“…3 Quite recent QCT simulations using again the DIM-based PES 15 mentioned above reported a rate of k n=1-0 = 4.34 AE 0.7(10 À11 ) cm 3 s À1 at T = 298 K from QCT simulations 21 which used the empirical DIM PES for the 2 A 0 ground state 15 and a more recent, MRCI-based fitted PES for the 2 A 00 state. 17 Given the rather heterogeneous situation for the quality of the existing PESs for studying the N( 4 S) + O 2 (X 3 S À g ) reaction and the vibrational relaxation of NO, the present work determines fully dimensional PESs using a consistent methodology to represent the 3 lowest electronic states, 2,4 A 0 and 2 A 00 as well as to evaluate the cross sections for the (forward)…”
Cross sections, rates, equilibrium constants and vibrational relaxation times for the N(4S) + O2(X3Σ−g) ↔ O(3P) + NO(X2Π) reaction from simulations on new, RKHS-based surfaces for the three lowest electronic states.
“…More recently, a double many body expansion fit to 1700 points at the MRCI/aug-cc-VQZ level of theory for the 2 A 00 state was carried out. 17 In addition, quasi classical trajectory (QCT) calculations 2,9,13,18 have been reported for the temperature dependent rate for the N( 4 S) + O 2 -NO + O and its reverse reaction using different PESs.…”
Section: Introductionmentioning
confidence: 99%
“…3 Quite recent QCT simulations using again the DIM-based PES 15 mentioned above reported a rate of k n=1-0 = 4.34 AE 0.7(10 À11 ) cm 3 s À1 at T = 298 K from QCT simulations 21 which used the empirical DIM PES for the 2 A 0 ground state 15 and a more recent, MRCI-based fitted PES for the 2 A 00 state. 17 Given the rather heterogeneous situation for the quality of the existing PESs for studying the N( 4 S) + O 2 (X 3 S À g ) reaction and the vibrational relaxation of NO, the present work determines fully dimensional PESs using a consistent methodology to represent the 3 lowest electronic states, 2,4 A 0 and 2 A 00 as well as to evaluate the cross sections for the (forward)…”
Cross sections, rates, equilibrium constants and vibrational relaxation times for the N(4S) + O2(X3Σ−g) ↔ O(3P) + NO(X2Π) reaction from simulations on new, RKHS-based surfaces for the three lowest electronic states.
“…The first step consists of defining the parametric equation that locates the crossing seam. Because it occurs at geometries with C 2v symmetry, 23,24 …”
Section: ■ Alternative Approach To the Problemmentioning
confidence: 99%
“…For convenience, we focus here on the lowest adiabatic sheet for which accurate ab initio calculations are affordable and compare the results with previously reported fits. 24 The new global PES reported so obtained is compared with two distinct DMBE forms. 24 They are all based on …”
Section: ■ Alternative Approach To the Problemmentioning
confidence: 99%
“…24 The new global PES reported so obtained is compared with two distinct DMBE forms. 24 They are all based on …”
Section: ■ Alternative Approach To the Problemmentioning
A method for modeling cusps on adiabatic potential energy surfaces without the need for any adiabatic-to-diabatic transformation is presented and shown to be successfully applied to the (2)A″ state of NO2. The more complicated case of a system with permutationally equivalent crossing seams is also examined and illustrated by considering the two first (2)A' states of the nitrogen trimer.
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