2017
DOI: 10.1063/1.4977598
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Magnetic gaps in organic tri-radicals: From a simple model to accurate estimates

Abstract: The calculation of the energy gap between the magnetic states of organic poly-radicals still represents a challenging playground for quantum chemistry, and high-level techniques are required to obtain accurate estimates. On these grounds, the aim of the present study is twofold. From the one side, it shows that, thanks to recent algorithmic and technical improvements, we are able to compute reliable quantum mechanical results for the systems of current fundamental and technological interest. From the other sid… Show more

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Cited by 6 publications
(7 citation statements)
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“…Here, the three NBOs are almost degenerate and most of the low-lying states have heavily multiconfigurational wave functions. Accurate theoretical studies are available for the energy gap between the ground state and the energetically lowest doublet state. ,, The doublet state is accessible with just a single SF operation on the high spin quartet state ( ); see the sketch in Figure a.…”
Section: Resultsmentioning
confidence: 99%
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“…Here, the three NBOs are almost degenerate and most of the low-lying states have heavily multiconfigurational wave functions. Accurate theoretical studies are available for the energy gap between the ground state and the energetically lowest doublet state. ,, The doublet state is accessible with just a single SF operation on the high spin quartet state ( ); see the sketch in Figure a.…”
Section: Resultsmentioning
confidence: 99%
“… a Optimized geometry with UB3LYP/cc-pVDZ. b Geometry from ref , with UB3LYP/6-311G­(d,p). c The energy gap for TMB – was obtained using 1SF-EA operation. All results with aug-cc-pVDZ basis set and natural orbitals truncated with a threshold of 0.0001. d CAS­(3,3) for TMB, CAS­(4,3) for TMB – , and CAS­(2,2) for MX. e CASSCF­(9,9)/6-31G­(d,p) from ref . f DDCI/6-31G­(d) using localized orbitals and complete virtual orbitals (fully variational) from ref . g CASPT2/6-31G­(d,p) with CASSCF­(9,9) orbitals from ref . h CASSCF­(10,9)/ANO-L and CASPT2/ANO-L using the same CASSCF orbitals from ref . i State-averaged MS-CASPT2/ANO-L from ref . j CASSCF/6-31G­(d) with CAS­(8,8) from ref . k CASPT2/6-31G­(d) with CASSCF orbitals with CAS­(8,8) from ref . l EOM-SF-CCSD/6-31G­(d) from ref . m Multireference second-order Møller–Plesset/aug-cc-pVTZ from ref . n LCCQMC/6-311++g­(d,p) from ref . …”
Section: Resultsmentioning
confidence: 99%
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“…1,3,5,-Trimethylenebenzene ( TriMB on Figure ) is the basis of many high-spin polyradicals described in the literature and has a quartet ground state. , With few experiments available, it was only recently studied using matrix isolation spectrocopy . Theoretical computations based on CASSCF and CASPT2N found an adiabatic doublet-quartet energy splitting of 0.6–0.7 eV , that has been corroborated in a recent work based on the DDCI CAS­(3,3) methodology …”
mentioning
confidence: 86%
“…Here, the three NBOs are nearly degenerate and most of the low-lying states have heavily multiconfigurational wavefunctions. Accurate theoretical studies are available for the energy gap between the ground state and the energetically lowest doublet state [83][84][85][86][87][88] . The doublet state is accesible with just a single spin-flip operation on the high spin quartet state (m s = 3 2 ), see the sketch in Figure 2(a).…”
Section: A All π-Polyradicalsmentioning
confidence: 99%