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Related Concept Videos

Metallic Solids02:37

Metallic Solids

18.4K
Metallic solids such as crystals of copper, aluminum, and iron are formed by metal atoms. The structure of metallic crystals is often described as a uniform distribution of atomic nuclei within a “sea” of delocalized electrons. The atoms within such a metallic solid are held together by a unique force known as metallic bonding that gives rise to many useful and varied bulk properties.
All metallic solids exhibit high thermal and electrical conductivity, metallic luster, and malleability....
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Standard Electrode Potentials03:02

Standard Electrode Potentials

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On comparing the reactivity of silver and lead, it is observed that the two ionic species, Ag+ (aq) and Pb2+ (aq), show a difference in their redox reactivity towards copper: the silver ion undergoes spontaneous reduction, while the lead ion does not. This relative redox activity can be easily quantified in electrochemical cells by a property called cell potential. This property is commonly known as cell voltage in electrochemistry, and it is a measure of the energy which accompanies the charge...
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Metal-Ligand Bonds02:51

Metal-Ligand Bonds

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The hemoglobin in the blood, the chlorophyll in green plants, vitamin B-12, and the catalyst used in the manufacture of polyethylene all contain coordination compounds. Ions of the metals, especially the transition metals, are likely to form complexes.
In these complexes, transition metals form coordinate covalent bonds, a kind of Lewis acid-base interaction in which both of the electrons in the bond are contributed by a donor (Lewis base) to an electron acceptor (Lewis acid). The Lewis acid in...
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Bonding in Metals02:32

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Metallic bonds are formed between two metal atoms. A simplified model to describe metallic bonding has been developed by Paul Drüde called the “Electron Sea Model”. 
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Crystal Field Theory - Octahedral Complexes02:58

Crystal Field Theory - Octahedral Complexes

26.4K
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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Metal-Semiconductor Junctions01:24

Metal-Semiconductor Junctions

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The contact of metal and semiconductor can lead to the formation of a junction with either Schottky or Ohmic behavior.
Schottky Barriers
Schottky barriers arise when a metal with a work function (Φm) contacts a semiconductor with a different work function (Φs). Initially, electrons transfer until the Fermi levels of the metal and semiconductor align at equilibrium. For instance, if Φm > Φs, the semiconductor Fermi level is higher than the metal's before contact. The...
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High-Quality Local Pseudopotentials for Metals.

Yu-Chieh Chi1, Chen Huang2

  • 1Information Technology Services, California NanoSystems Institute, Center for Scientific Computing, University of California, Santa Barbara, California 93106, United States.

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|April 10, 2024
PubMed
Summary
This summary is machine-generated.

Accurate local pseudopotentials (LPSs) for all metals are crucial for orbital-free density functional theory (OF-DFT). This study developed high-quality LPSs for simple and transition metals, enabling reliable large-scale OF-DFT simulations.

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Area of Science:

  • Computational materials science
  • Quantum chemistry
  • Condensed matter physics

Background:

  • Orbital-free density functional theory (OF-DFT) offers computational efficiency for materials simulations.
  • Accurate local pseudopotentials (LPSs) are essential for OF-DFT, but high-quality LPSs for all metals, particularly transition metals, are lacking.
  • Existing LPSs often struggle to accurately represent the electronic structure of transition metals.

Purpose of the Study:

  • To develop high-quality local pseudopotentials (LPSs) applicable to all simple and transition metals for orbital-free density functional theory (OF-DFT).
  • To address the challenge of fitting both semicore and outermost valence orbitals in transition metals within the constraints of local pseudopotentials.
  • To enhance the applicability of OF-DFT for magnetic materials and alloys by incorporating spin-polarization effects.

Main Methods:

  • Developed LPSs by fitting atomic eigenvalues and orbital norms beyond cutoff radii for simple and transition metals.
  • Overcame fitting challenges for transition metals by excluding semicore orbitals from optimization, focusing on outermost valence orbitals crucial for bonding.
  • Introduced atomic spin-polarization energy as a metric for constructing LPSs for magnetic systems.

Main Results:

  • Achieved excellent fittings of outermost valence orbitals, satisfying norm-conserving conditions for high-quality LPSs.
  • Successfully developed LPSs for all simple and transition metals.
  • Demonstrated that LPSs for magnetic systems reasonably reproduced properties of magnetic metals and alloys when incorporating spin-polarization energy.

Conclusions:

  • The developed high-quality LPSs significantly advance the application of OF-DFT to all metals and their alloys.
  • These LPSs pave the way for large-scale, reliable OF-DFT simulations, overcoming a major computational bottleneck.
  • The methodology provides a robust framework for generating accurate pseudopotentials for diverse metallic systems, including magnetic ones.