Related Experiment Video
Updated: Apr 25, 2026

10:17
20 mJ, 1 ps Yb:YAG Thin-disk Regenerative Amplifier
Published on: July 12, 2017
12.3K
Theoretical analysis of high-harmonic generation in solids
G Vampa1, C R McDonald1, G Orlando1
1Department of Physics, University of Ottawa, Ottawa, Ontario K1N 6N5, Canada.
Physical Review Letters
|August 30, 2014
Summary
We theoretically investigate high-harmonic generation (HHG) in crystals using intense mid-infrared lasers. Our findings reveal that interband HHG, often overlooked, is the dominant mechanism, offering a new understanding of HHG in solids.
Area of Science:
- Solid-state physics
- Quantum optics
- Nonlinear optics
Background:
- High-harmonic generation (HHG) is a key process in nonlinear optics.
- Understanding HHG mechanisms in solids is crucial for advanced light source development.
- Previous studies have focused on intraband contributions to HHG in crystals.
Purpose of the Study:
- To theoretically investigate high-harmonic generation (HHG) in bulk crystals.
- To explore both interband and intraband HHG mechanisms.
- To identify the dominant HHG mechanism and its characteristics.
Main Methods:
- Theoretical investigation of HHG in bulk crystals.
- Analysis of intense mid-infrared laser interactions with photon energies below the band gap.
- Application of saddle point analysis in the Keldysh limit.
Main Results:
- Interband HHG is identified as the dominant mechanism, contrary to previous assumptions.
- Interband HHG in solids shares similarities with atomic HHG.
- Distinct wavelength dependencies were found for interband and intraband HHG.
Conclusions:
- Interband HHG is the primary driver of high-harmonic generation in bulk crystals under the studied conditions.
- The differing wavelength dependencies provide an experimental signature to differentiate between interband and intraband HHG.
- This research clarifies fundamental HHG mechanisms in solids and guides future experimental verification.
More Related Videos
Related Concept Videos
Generating Electromagnetic Radiations
8.6K
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in...
8.6K
Emission Spectra
65.0K
When solids, liquids, or condensed gases are heated sufficiently, they radiate some of the excess energy as light. Photons produced in this manner have a range of energies, and thereby produce a continuous spectrum in which an unbroken series of wavelengths is present.
65.0K
Standing Waves in a Cavity
1.7K
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.7K
The de Broglie Wavelength
25.6K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
25.6K
Band Theory
14.5K
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,...
The energy difference between these bands is known as the band gap.
Conductor, Semiconductor,...
14.5K
Energy Bands in Solids
2.4K
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...
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...
2.4K

