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Crystal Field Theory - Octahedral Complexes02:58

Crystal Field Theory - Octahedral Complexes

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Crystal Field Theory
To explain the observed behavior of transition metal complexes (such as colors), a model involving electrostatic interactions between the electrons from the ligands and the electrons in the unhybridized d orbitals of the central metal atom has been developed. This electrostatic model is crystal field theory (CFT). It helps to understand, interpret, and predict the colors, magnetic behavior, and some structures of coordination compounds of transition metals.
CFT focuses on...
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Potential Due to a Polarized Object01:29

Potential Due to a Polarized Object

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A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
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Crystal Field Theory - Tetrahedral and Square Planar Complexes02:46

Crystal Field Theory - Tetrahedral and Square Planar Complexes

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Tetrahedral Complexes
Crystal field theory (CFT) is applicable to molecules in geometries other than octahedral. In octahedral complexes, the lobes of the dx2−y2 and dz2 orbitals point directly at the ligands. For tetrahedral complexes, the d orbitals remain in place, but with only four ligands located between the axes. None of the orbitals points directly at the tetrahedral ligands. However, the dx2−y2 and dz2 orbitals (along the Cartesian axes) overlap with the ligands less than the dxy,...
41.7K
Aromatic Hydrocarbon Anions: Structural Overview01:18

Aromatic Hydrocarbon Anions: Structural Overview

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Neutral hydrocarbons like cyclopentadiene with an odd number of carbon atoms and one intervening CH2 group in the ring are not aromatic. Cyclopentadiene with 4 π electrons does not satisfy the 4n + 2 π electron rule. Additionally, the intervening CH2 group is sp3 hybridized and lacks a vacant p orbital, thereby interrupting the overlap of p orbitals in a continuous manner and preventing the delocalization of π electrons throughout the ring.
Due to the absence of continuous...
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IR Absorption Frequency: Delocalization01:04

IR Absorption Frequency: Delocalization

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Electron delocalization refers to the distribution of electrons across multiple atoms within a molecule rather than being confined to a single atom or bond. This phenomenon is common in systems with conjugated bonds—structures where alternating single and double bonds allow π-electrons to move freely across the network. The movement of electrons stabilizes the molecule and can affect various chemical properties, including vibrational frequencies observed in IR spectroscopy.
In IR...
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π Molecular Orbitals of the Allyl Cation and Anion01:18

π Molecular Orbitals of the Allyl Cation and Anion

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An allyl group is a three-carbon conjugated system where the sp³-hybridized allylic carbon is bonded to a CH=CH2 group via a single bond. Allyl anions can be obtained by treating propene with a strong base that can deprotonate methyl groups. Allyl cations are formed as intermediates during substitution reactions involving allylic halides. In both cases, the hybridization of the allylic carbon changes from sp3 to sp2, giving rise to a carbon chain with three sp2-hybridized carbons, each with...
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Updated: Jun 13, 2025

Excitonic Hamiltonians for Calculating Optical Absorption Spectra and Optoelectronic Properties of Molecular Aggregates and Solids
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Localized and Delocalized Charge Distribution in a Diamine Cation and Rydberg Excited State: A Challenging Test for

Benedikt O Birgisson1, Marta Gałyńska1,2, Hemanadhan Myneni1

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Density functional theory calculations reveal how electron distribution in N,N'-dimethylpiperazine (DMP) depends on Fock exchange and self-interaction correction. Stronger Fock exchange or full self-interaction correction favors localized electrons, crucial for accurate excited state and ionized molecule modeling.

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Measurement of Ultrafast Vibrational Coherences in Polyatomic Radical Cations with Strong-Field Adiabatic Ionization
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Area of Science:

  • Computational Chemistry
  • Quantum Chemistry
  • Materials Science

Background:

  • Accurate modeling of electron distribution is vital for understanding molecular properties.
  • Density functional theory (DFT) is a powerful tool, but its accuracy depends on functional choice.
  • The behavior of N,N -dimethylpiperazine (DMP) in excited and ionized states presents a challenge for DFT.

Purpose of the Study:

  • To test the performance of various density functionals in describing electron localization/delocalization.
  • To investigate the impact of Fock exchange (FE) weight in hybrid functionals.
  • To evaluate the effectiveness of self-interaction correction (SIC) in DFT calculations for DMP.

Main Methods:

  • Calculations employed density functionals across Jacob's ladder, including LDA, hybrids, and double hybrids.
  • Investigated DMP in its 3s Rydberg excited state and fully ionized DMP+ cation.
  • Analyzed the effects of varying FE weights in PBE0 and applied full and scaled SIC to PBE.

Main Results:

  • Common hybrid functionals (e.g., PBE0 with 0.25 FE) yield delocalized charge for DMP+.
  • Functionals with higher FE weights (e.g., PBE0(0.50), BHLYP) and full SIC produce localized charge minima.
  • For the Rydberg state, PBE0(0.32) shows both localized and delocalized holes, while PBE shows only delocalized.

Conclusions:

  • The balance of localized vs. delocalized electrons in DMP is sensitive to DFT functional parameters.
  • Higher Fock exchange or full SIC is necessary to capture charge localization in ionized DMP.
  • Reducing self-interaction error is critical for accurate DFT predictions of DMP's Rydberg excited state.