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An SN2 reaction of an alkyl halide is a single-step process in which bond formation between the nucleophile and the substrate and bond breaking between the substrate and the halide occurs simultaneously through a transition state without forming an intermediate.
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An atomic orbital represents the three-dimensional regions in an atom where an electron has the highest probability to reside. The radial distribution function indicates the total probability of finding an electron within the thin shell at a distance r from the nucleus. The atomic orbitals have distinct shapes which are determined by l, the angular momentum quantum number. The orbitals are often drawn with a boundary surface, enclosing densest regions of the cloud.
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The mathematical expression known as the wave function, ψ, contains information about each orbital and the wavelike properties of electrons in an isolated atom. When atoms are bound together in a molecule, the wave functions combine to produce new mathematical descriptions that have different shapes. This process of combining the wave functions for atomic orbitals is called hybridization and is mathematically accomplished by the linear combination of atomic orbitals. The new orbitals that...
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Low scaling EOM-CCSD and EOM-MBPT(2) method with natural transition orbitals.

Young Choon Park1, Ajith Perera1, Rodney J Bartlett1

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A new low-scaling method for equation-of-motion coupled-cluster (EOM-CCSD) calculations significantly reduces computational cost by focusing on dominant excitations. This approach enables accurate excited-state calculations with improved efficiency.

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Area of Science:

  • Computational Chemistry
  • Quantum Chemistry
  • Theoretical Chemistry

Background:

  • Equation-of-motion coupled-cluster (EOM-CCSD) theory is a powerful method for calculating excited states.
  • Traditional EOM-CCSD methods suffer from high computational scaling, limiting their application to larger systems.
  • Natural Transition Orbitals (NTOs) provide a compact representation of excited states.

Purpose of the Study:

  • To develop a low-scaling computational method for EOM-CCSD and its approximations.
  • To reduce the computational cost associated with the double excitation vector (R2) in EOM calculations.
  • To enable accurate excited-state calculations for larger molecular systems.

Main Methods:

  • Selection of dominant occupied and virtual orbitals from NTOs based on transition density matrix eigenvalues.
  • Modification of the R2 vector to retain only the most significant excitation contributions.
  • Implementation of a low-scaling approach with an overall computational complexity of ~M^5.

Main Results:

  • The modified R2 vector effectively captures dominant excitations within reduced subspaces.
  • The developed method achieves a computational scaling of ~M^5 for the EOM part.
  • Energy deviations due to R2 truncation are minimal (average ~0.03 eV) compared to untruncated EOM-CCSD.

Conclusions:

  • The proposed low-scaling method provides an accurate and efficient approach for excited-state calculations.
  • This method is compatible with various NTO generation techniques, including time-dependent density functional theory.
  • The ~M^5 scaling opens possibilities for applying EOM-CCSD and MBPT(2) to larger and more complex systems.