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Related Concept Videos

π Electron Effects on Chemical Shift: Overview01:27

π Electron Effects on Chemical Shift: Overview

An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0, resulting in...
Resonance and Hybrid Structures02:16

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According to the theory of resonance, if two or more Lewis structures with the same arrangement of atoms can be written for a molecule, ion, or radical, the actual distribution of electrons is an average of that shown by the various Lewis structures.
Resonance Structures and Resonance Hybrids
The Lewis structure of a nitrite anion (NO2−) may actually be drawn in two different ways, distinguished by the locations of the N–O and N=O bonds.
Induced Electric Dipoles01:28

Induced Electric Dipoles

A permanent electric dipole orients itself along an external electric field. This rotation can be quantified by defining the potential energy because the external torque does work in rotating it. Then, the potential energy is minimum at the parallel configuration and maximum at the antiparallel configuration. While the former is a stable equilibrium, the latter is an unstable equilibrium.
Since the absolute value of potential energy holds no physical meaning, its zero value can be chosen as per...
Inductive Effects on Chemical Shift: Overview01:27

Inductive Effects on Chemical Shift: Overview

The protons in unsubstituted alkanes are strongly shielded with chemical shifts below 1.8 ppm. Methine, methylene, and methyl protons appear at approximately 1.7, 1.2 and 0.7 ppm, while the proton signal from methane appears at 0.23 ppm. An electronegative substituent, such as chlorine, withdraws the electron density from the protons, increasing their chemical shift. Progressive substitution of the hydrogens in methane by chlorine shifts the proton signals increasingly downfield, to 3.05 ppm in...
Molecular Shape and Polarity03:37

Molecular Shape and Polarity

Dipole Moment of a Molecule
Resonance02:52

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The Lewis structure of a nitrite anion (NO2−) may actually be drawn in two different ways, distinguished by the locations of the N-O and N=O bonds.

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Updated: May 28, 2026

Monolayer Contact Doping of Silicon Surfaces and Nanowires Using Organophosphorus Compounds
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Resonance and localization effects at a dipolar organic semiconductor interface.

Mary P Steele1, Leah L Kelly, Nahid Ilyas

  • 1Department of Chemistry, The University of Arizona, 1306 E. University Blvd., Tucson, Arizona 85721, USA.

The Journal of Chemical Physics
|October 7, 2011
PubMed
Summary
This summary is machine-generated.

Investigating vanadyl naphthalocyanine (VONc) on graphite reveals charge-transfer interactions. Molecular coverage influences electronic states, creating hybrid states and affecting charge localization at the interface.

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Area of Science:

  • Surface science
  • Organic electronics
  • Spectroscopy

Background:

  • Organic semiconductors like vanadyl naphthalocyanine (VONc) are crucial for electronic devices.
  • Understanding interfacial electronic states is key to controlling charge transport.

Purpose of the Study:

  • To investigate the electronic states of VONc on highly oriented pyrolytic graphite.
  • To elucidate the role of interfacial charge-transfer and molecular coverage on these states.

Main Methods:

  • Angle-resolved two-photon photoemission (AR-TPPE) spectroscopy was employed.
  • Studies were conducted across 0-1 monolayer coverages of VONc.

Main Results:

  • Interfacial charge-transfer populates a VONc anion level, exhibiting distinct momentum dispersion.
  • Depolarization by neighboring molecules stabilizes this anion level with increasing coverage.
  • A hybrid image potential/anion state emerges near one monolayer, localizing progressively.

Conclusions:

  • Different charge-transfer interactions govern the electronic states at the VONc/graphite interface.
  • Molecular coverage significantly modifies the electronic structure and charge localization.