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Ab initio study of the amino group twisting and wagging reaction paths in the intramolecular charge transfer of 4-(N,N-dimethylamino)benzonitrile

Identifieur interne : 000704 ( Main/Corpus ); précédent : 000703; suivant : 000705

Ab initio study of the amino group twisting and wagging reaction paths in the intramolecular charge transfer of 4-(N,N-dimethylamino)benzonitrile

Auteurs : Wibke Sudholt ; Andrzej L. Sobolewski ; Wolfgang Domcke

Source :

RBID : ISTEX:DC1FA6F5EDCAA94238E255344BDF6B768E44C01B

Abstract

The behaviour of 4-(N,N-dimethylamino)benzonitrile in its locally-excited and charge-transfer singlet states following the twisting and wagging displacements of the amino group has been investigated theoretically. These reaction paths are expected to play a decisive role in the intramolecular charge transfer observed for this compound in polar solvents. Minimum-energy paths for the lowest excited singlet states have been determined at the CIS level. The corresponding potential-energy profiles have been calculated with the CASSCF and CASPT2 methods. The potential-energy functions depend strongly on the amount of electron correlation included. It can be concluded that, except for large twist angles, wagging leads only to minor changes in the potential-energy curves and dipole moments. The results suggest that the wagging angle can be excluded as a reaction coordinate for the intramolecular charge-transfer process as well as a coupling coordinate of the two lowest excited singlet states. Twisting of the amino group appears to be the relevant reaction coordinate for the intramolecular charge transfer in 4-(N,N-dimethylamino)benzonitrile.

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DOI: 10.1016/S0301-0104(98)00368-1

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ISTEX:DC1FA6F5EDCAA94238E255344BDF6B768E44C01B

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<div type="abstract" xml:lang="en">The behaviour of 4-(N,N-dimethylamino)benzonitrile in its locally-excited and charge-transfer singlet states following the twisting and wagging displacements of the amino group has been investigated theoretically. These reaction paths are expected to play a decisive role in the intramolecular charge transfer observed for this compound in polar solvents. Minimum-energy paths for the lowest excited singlet states have been determined at the CIS level. The corresponding potential-energy profiles have been calculated with the CASSCF and CASPT2 methods. The potential-energy functions depend strongly on the amount of electron correlation included. It can be concluded that, except for large twist angles, wagging leads only to minor changes in the potential-energy curves and dipole moments. The results suggest that the wagging angle can be excluded as a reaction coordinate for the intramolecular charge-transfer process as well as a coupling coordinate of the two lowest excited singlet states. Twisting of the amino group appears to be the relevant reaction coordinate for the intramolecular charge transfer in 4-(N,N-dimethylamino)benzonitrile.</div>
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<note type="content">Fig. 1: Projection of the CIS optimized geometries of DMABN along different reaction paths onto the plane spanned by the twisting and wagging coordinates. Crosses denote reaction paths where the Lb-like LE and La-like CT states can be distinguished by symmetry. Pluses denote the reaction path of C1 symmetry, where only the lowest excited singlet state can be optimized.</note>
<note type="content">Fig. 2: Potential-energy functions for the lowest excited singlet states calculated along the wagging reaction path for planar (a,c,e) and fully twisted (b,d,f) DMABN. Triangles denote the Lb-like LE state, squares the La-like CT state. (a,b): CIS energy for the optimized structures; (c,d): CASSCF energy calculated at CIS geometries; (e,f): CASPT2 energy calculated at CIS geometries. Energies are given relatively to the HF (a,b), CASSCF (c,d) and CASPT2 (e,f) ground-state energies calculated at the MP2 C2v minimum of the ground state.</note>
<note type="content">Fig. 3: CASSCF dipole moments for the lowest excited singlet states calculated along the wagging reaction path for planar (a) and fully twisted (b) DMABN. Triangles refer to the Lb-like LE state, squares to the La-like CT state, and circles to the ground state. Solid lines refer to a geometry optimized for the same state, dashed lines to a geometry optimized for the corresponding CT state.</note>
<note type="content">Fig. 4: Potential-energy functions for the lowest excited singlet states of DMABN calculated along the reaction paths for pure twisting (a,c,e) and combined twisting and wagging (b,d,f). The optimal values of δ are given in Fig. 1. Triangles denote the Lb-like LE state, squares the La-like CT state. Solid lines refer to a single-state optimized wavefunction at a geometry optimized for the same state, dashed lines refer to a single-state optimized wavefunction at a geometry optimized for the corresponding CT state, and dotted lines refer to a state-averaged wavefunction. (a,b): CIS energy for the optimized structures; (c,d): CASSCF energy calculated at CIS geometries; (e,f): CASPT2 energy calculated at CIS geometries. Energies are given relatively to the HF (a,b), CASSCF (c,d) and CASPT2 (e,f) ground-state energies calculated at the MP2 C2v minimum of the ground state. The point at θ=75° on the “S2” potential-energy curve in (f) is skipped due to its significant lower reference weight.</note>
<note type="content">Fig. 5: CASSCF dipole moments for the lowest excited singlet states of DMABN calculated along the reaction paths for pure twisting (a) and combined twisting and wagging (b). The optimal values of δ are given in Fig. 1. Triangles refer to the Lb-like LE state, squares to the La-like CT state, and circles to the ground state. Solid lines refer to a single-state optimized wavefunction at a geometry optimized for the same state, dashed lines refer to a single-state optimized wavefunction at a geometry optimized for the corresponding CT state, and dotted lines refer to a state-averaged wavefunction.</note>
<note type="content">Fig. 6: CASPT2 potential-energy functions for the lowest excited singlet states of DMABN calculated along the twisting coordinate (a) and the wagging coordinate (b) with all other coordinates frozen. Triangles denote the Lb-like LE state, squares the La-like CT state. Energies are given relatively to the CASPT2 ground-state energy calculated at the MP2 C2v minimum of the ground state.</note>
<note type="content">Table 1: Definition of active electrons and frozen, inactive and active orbitals in the CASSCF single-point calculations of DMABN following the different reaction paths along the twisting and wagging coordinates</note>
<note type="content">Table 2: Assignment of the lowest excited singlet states of DMABN in each point group to the Lb-like LE and La-like CT states following the different reaction paths along the twisting and wagging coordinates</note>
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<p>The behaviour of 4-(N,N-dimethylamino)benzonitrile in its locally-excited and charge-transfer singlet states following the twisting and wagging displacements of the amino group has been investigated theoretically. These reaction paths are expected to play a decisive role in the intramolecular charge transfer observed for this compound in polar solvents. Minimum-energy paths for the lowest excited singlet states have been determined at the CIS level. The corresponding potential-energy profiles have been calculated with the CASSCF and CASPT2 methods. The potential-energy functions depend strongly on the amount of electron correlation included. It can be concluded that, except for large twist angles, wagging leads only to minor changes in the potential-energy curves and dipole moments. The results suggest that the wagging angle can be excluded as a reaction coordinate for the intramolecular charge-transfer process as well as a coupling coordinate of the two lowest excited singlet states. Twisting of the amino group appears to be the relevant reaction coordinate for the intramolecular charge transfer in 4-(N,N-dimethylamino)benzonitrile.</p>
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<ce:simple-para>The behaviour of 4-(N,N-dimethylamino)benzonitrile in its locally-excited and charge-transfer singlet states following the twisting and wagging displacements of the amino group has been investigated theoretically. These reaction paths are expected to play a decisive role in the intramolecular charge transfer observed for this compound in polar solvents. Minimum-energy paths for the lowest excited singlet states have been determined at the CIS level. The corresponding potential-energy profiles have been calculated with the CASSCF and CASPT2 methods. The potential-energy functions depend strongly on the amount of electron correlation included. It can be concluded that, except for large twist angles, wagging leads only to minor changes in the potential-energy curves and dipole moments. The results suggest that the wagging angle can be excluded as a reaction coordinate for the intramolecular charge-transfer process as well as a coupling coordinate of the two lowest excited singlet states. Twisting of the amino group appears to be the relevant reaction coordinate for the intramolecular charge transfer in 4-(N,N-dimethylamino)benzonitrile.</ce:simple-para>
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<abstract lang="en">The behaviour of 4-(N,N-dimethylamino)benzonitrile in its locally-excited and charge-transfer singlet states following the twisting and wagging displacements of the amino group has been investigated theoretically. These reaction paths are expected to play a decisive role in the intramolecular charge transfer observed for this compound in polar solvents. Minimum-energy paths for the lowest excited singlet states have been determined at the CIS level. The corresponding potential-energy profiles have been calculated with the CASSCF and CASPT2 methods. The potential-energy functions depend strongly on the amount of electron correlation included. It can be concluded that, except for large twist angles, wagging leads only to minor changes in the potential-energy curves and dipole moments. The results suggest that the wagging angle can be excluded as a reaction coordinate for the intramolecular charge-transfer process as well as a coupling coordinate of the two lowest excited singlet states. Twisting of the amino group appears to be the relevant reaction coordinate for the intramolecular charge transfer in 4-(N,N-dimethylamino)benzonitrile.</abstract>
<note type="content">Fig. 1: Projection of the CIS optimized geometries of DMABN along different reaction paths onto the plane spanned by the twisting and wagging coordinates. Crosses denote reaction paths where the Lb-like LE and La-like CT states can be distinguished by symmetry. Pluses denote the reaction path of C1 symmetry, where only the lowest excited singlet state can be optimized.</note>
<note type="content">Fig. 2: Potential-energy functions for the lowest excited singlet states calculated along the wagging reaction path for planar (a,c,e) and fully twisted (b,d,f) DMABN. Triangles denote the Lb-like LE state, squares the La-like CT state. (a,b): CIS energy for the optimized structures; (c,d): CASSCF energy calculated at CIS geometries; (e,f): CASPT2 energy calculated at CIS geometries. Energies are given relatively to the HF (a,b), CASSCF (c,d) and CASPT2 (e,f) ground-state energies calculated at the MP2 C2v minimum of the ground state.</note>
<note type="content">Fig. 3: CASSCF dipole moments for the lowest excited singlet states calculated along the wagging reaction path for planar (a) and fully twisted (b) DMABN. Triangles refer to the Lb-like LE state, squares to the La-like CT state, and circles to the ground state. Solid lines refer to a geometry optimized for the same state, dashed lines to a geometry optimized for the corresponding CT state.</note>
<note type="content">Fig. 4: Potential-energy functions for the lowest excited singlet states of DMABN calculated along the reaction paths for pure twisting (a,c,e) and combined twisting and wagging (b,d,f). The optimal values of δ are given in Fig. 1. Triangles denote the Lb-like LE state, squares the La-like CT state. Solid lines refer to a single-state optimized wavefunction at a geometry optimized for the same state, dashed lines refer to a single-state optimized wavefunction at a geometry optimized for the corresponding CT state, and dotted lines refer to a state-averaged wavefunction. (a,b): CIS energy for the optimized structures; (c,d): CASSCF energy calculated at CIS geometries; (e,f): CASPT2 energy calculated at CIS geometries. Energies are given relatively to the HF (a,b), CASSCF (c,d) and CASPT2 (e,f) ground-state energies calculated at the MP2 C2v minimum of the ground state. The point at θ=75° on the “S2” potential-energy curve in (f) is skipped due to its significant lower reference weight.</note>
<note type="content">Fig. 5: CASSCF dipole moments for the lowest excited singlet states of DMABN calculated along the reaction paths for pure twisting (a) and combined twisting and wagging (b). The optimal values of δ are given in Fig. 1. Triangles refer to the Lb-like LE state, squares to the La-like CT state, and circles to the ground state. Solid lines refer to a single-state optimized wavefunction at a geometry optimized for the same state, dashed lines refer to a single-state optimized wavefunction at a geometry optimized for the corresponding CT state, and dotted lines refer to a state-averaged wavefunction.</note>
<note type="content">Fig. 6: CASPT2 potential-energy functions for the lowest excited singlet states of DMABN calculated along the twisting coordinate (a) and the wagging coordinate (b) with all other coordinates frozen. Triangles denote the Lb-like LE state, squares the La-like CT state. Energies are given relatively to the CASPT2 ground-state energy calculated at the MP2 C2v minimum of the ground state.</note>
<note type="content">Table 1: Definition of active electrons and frozen, inactive and active orbitals in the CASSCF single-point calculations of DMABN following the different reaction paths along the twisting and wagging coordinates</note>
<note type="content">Table 2: Assignment of the lowest excited singlet states of DMABN in each point group to the Lb-like LE and La-like CT states following the different reaction paths along the twisting and wagging coordinates</note>
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