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Energy Bands in Solids01:01

Energy Bands in Solids

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Isolated atoms have discrete energy levels that are well described by the Bohr model. And, it quantifies the energy of an electron in a hydrogen atom as En. Higher quantum numbers 'n' yield less negative, closer electron energy levels.
 Band Formation:
When atoms are brought close together, as in a solid, these discrete energy levels begin to split due to the overlap of electron orbitals from adjacent atoms. This split occurs because of the Pauli exclusion principle, which states...
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Semiconductors01:22

Semiconductors

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There is variation in the electrical conductivity of materials - metals, semiconductors, and insulators that are showcased with the help of the energy band diagrams.
Metals such as copper (Cu), zinc (Zn), or lead (Pb) have low resistivity and feature conduction bands that are either not fully occupied or overlap with the valence band, making a bandgap non-existent. This allows electrons in the highest energy levels of the valence band to easily transition to the conduction band upon gaining...
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Biasing of P-N Junction01:16

Biasing of P-N Junction

1.7K
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
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Biasing of Metal-Semiconductor Junctions01:27

Biasing of Metal-Semiconductor Junctions

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Biasing metal-semiconductor junctions involves applying a voltage across the junction. Specifically, the metal is connected to a voltage source, while the semiconductor is grounded. This technique is essential for controlling the direction and magnitude of current flow in electronic devices, including diodes, transistors, and photovoltaic cells.
In Schottky junctions, where the semiconductor is n-type, applying a positive voltage to the metal relative to the semiconductor reduces its Fermi...
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Band Theory02:35

Band Theory

17.0K
When two or more atoms come together to form a molecule, their atomic orbitals combine and molecular orbitals of distinct energies result. In a solid, there are a large number of atoms, and therefore a large number of atomic orbitals that may be combined into molecular orbitals. These groups of molecular orbitals are so closely placed together to form continuous regions of energies, known as the bands.
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
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Molecular Orbital Theory II03:51

Molecular Orbital Theory II

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Molecular Orbital Energy Diagrams
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Updated: Jan 8, 2026

Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations
13:56

Probe Type II Band Alignment in One-Dimensional Van Der Waals Heterostructures Using First-Principles Calculations

Published on: October 12, 2019

8.0K

Interface-Dipole-Driven Type-II Band Offset Engineering in Perovskite Heterostructures.

Lili Xu1, Shengli Zhang2, Yee Sin Ang1

  • 1Science, Mathematics and Technology (SMT) Cluster, Singapore University of Technology and Design, Singapore 487372, Singapore.

Nano Letters
|December 17, 2025
PubMed
Summary

Janus monolayers improve perovskite solar cells by creating a Type-II band alignment. This interface engineering boosts charge separation and carrier lifetimes, enabling efficient, transport-layer-free devices.

Keywords:
band structureelectronic propertiesfirst-principles calculationsperovskites

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Influence of Hybrid Perovskite Fabrication Methods on Film Formation, Electronic Structure, and Solar Cell Performance
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Low Pressure Vapor-assisted Solution Process for Tunable Band Gap Pinhole-free Methylammonium Lead Halide Perovskite Films
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Low Pressure Vapor-assisted Solution Process for Tunable Band Gap Pinhole-free Methylammonium Lead Halide Perovskite Films
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Low Pressure Vapor-assisted Solution Process for Tunable Band Gap Pinhole-free Methylammonium Lead Halide Perovskite Films

Published on: September 8, 2017

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Area of Science:

  • Materials Science
  • Condensed Matter Physics
  • Renewable Energy

Background:

  • Perovskite solar cells (PSCs) show high efficiency but are limited by nonradiative recombination.
  • Interfacial energy mismatches between perovskite and transport layers cause performance loss.

Purpose of the Study:

  • To engineer band alignment in PSCs using Janus monolayers.
  • To enhance charge separation and suppress recombination for higher efficiency.

Main Methods:

  • First-principles calculations to confirm band alignment.
  • Nonadiabatic molecular dynamics to predict carrier lifetimes.
  • Integration of Janus monolayers into perovskite heterostructures (CsPbBr3/MSSe/CsPbBr3).

Main Results:

  • Achieved dipole-driven Type-II band alignment in perovskite/Janus monolayer/perovskite structures.
  • Demonstrated extended carrier lifetimes in CsPbBr3/WSSe/CsPbBr3 due to strong dipole moments.
  • Identified Janus monolayers as effective for interfacial design.

Conclusions:

  • Janus monolayers offer a versatile platform for optimizing PSCs.
  • This strategy enables simplified, transport-layer-free, high-efficiency perovskite optoelectronics.
  • Interface-dipole engineering is key to overcoming PSC performance limitations.