A DFT analysis of the ground and charge-transfer excited states of Sc3N@Ih-C80 fullerene coupled with metal-free and zinc-phthalocyanine
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Amerikheirabadi, Fatemeh
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Univ Texas El Paso, Computat Sci Program, El Paso, TX 79968 USA
Univ Texas El Paso, Dept Phys, El Paso, TX 79968 USAUniv Texas El Paso, Computat Sci Program, El Paso, TX 79968 USA
Amerikheirabadi, Fatemeh
[1
,2
]
Diaz, Carlos
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Univ Texas El Paso, Computat Sci Program, El Paso, TX 79968 USAUniv Texas El Paso, Computat Sci Program, El Paso, TX 79968 USA
Diaz, Carlos
[1
]
Mohan, Neetha
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Univ Texas El Paso, Dept Phys, El Paso, TX 79968 USAUniv Texas El Paso, Computat Sci Program, El Paso, TX 79968 USA
Mohan, Neetha
[2
]
Zope, Rajendra R.
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Univ Texas El Paso, Computat Sci Program, El Paso, TX 79968 USA
Univ Texas El Paso, Dept Phys, El Paso, TX 79968 USAUniv Texas El Paso, Computat Sci Program, El Paso, TX 79968 USA
Zope, Rajendra R.
[1
,2
]
Baruah, Tunna
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Univ Texas El Paso, Computat Sci Program, El Paso, TX 79968 USA
Univ Texas El Paso, Dept Phys, El Paso, TX 79968 USAUniv Texas El Paso, Computat Sci Program, El Paso, TX 79968 USA
Baruah, Tunna
[1
,2
]
机构:
[1] Univ Texas El Paso, Computat Sci Program, El Paso, TX 79968 USA
[2] Univ Texas El Paso, Dept Phys, El Paso, TX 79968 USA
Endohedral metallofullerenes and phthalocyanine derivatives are recognized as excellent active materials in organic photovoltaics (OPVs). The tri-metallic nitride endohedral C-80 fullerenes have greater absorption coefficients in the visible region and electron-accepting abilities similar to C-60, which can allow for higher efficiencies in OPV devices. In this work, we have investigated the ground and charge transfer excited states of two co-facial donor-acceptor (D-A) molecular conjugates formed by the non-covalent coupling of trimetallic nitride endohedral fullerene (Sc3N@I-h-C-80) with metal-free (H2Pc) and zinc-phthalocyanine (ZnPc) chromophores using DFT calculations. The charge transfer (CT) excitation energies are calculated using the perturbative delta-SCF method that enforces orthogonality between the ground and excited states. The binding energies calculated using the PBE and DFT-D3 methods indicate that the dispersion effects play an important role in the stabilization of these complexes. The ground state dipole moment of the Sc3N@C-80-H2Pc dyad is much larger than that of Sc3N@C-80-ZnPc, but this is reversed in the excited state where the dipole moment of Sc3N@C-80-ZnPc increases significantly. The lowest few excitation energies in the gas phase for the two complexes are very close, in the range of 1.51-2.66 eV for Sc3N@C-80-ZnPc and 1.51-2.71 eV for the Sc3N@C-80-H2Pc complex. However, the lower ionization potential and lower exciton binding energy make the Sc3N@C-80-ZnPc dyad a better candidate for OPVs as compared to the Sc3N@C-80-H2Pc dyad.