Related Experiment Video
Updated: Jan 24, 2026

Light-driven Enzymatic Decarboxylation
Published on: May 22, 2016
Strong Light-Field Driven Nanolasers
Richard Hollinger1,2,3, Pavel Malevich4, Valentina Shumakova4
1Institute of Optics and Quantum Electronics , Friedrich-Schiller University Jena , Max-Wien-Platz 1 , 07743 Jena , Germany.
Researchers achieved population inversion and lasing in semiconductor nanowires using low-energy light. This novel method relies on the wave nature of electrons, not photon energy, for excitation.
Area of Science:
- Quantum physics
- Laser physics
- Semiconductor science
Background:
- Einstein's quantum theory of radiation underpins modern laser physics.
- Multiphoton pumping using intense, ultrashort lasers is understood via the particle picture of light.
- Excitation and population inversion in nonlinear regimes depend on photon energy and light intensity.
Purpose of the Study:
- To demonstrate population inversion and lasing in semiconductor nanowires at significantly lower pump photon energies.
- To explore excitation mechanisms beyond the traditional particle picture of light.
- To investigate the role of light's wave nature in achieving population inversion.
Main Methods:
- Utilizing semiconductor nanowires as the active gain medium.
- Employing intense laser pumping with significantly reduced photon energy.
- Analyzing the nonlinear interaction regime and electron behavior.
Main Results:
- Population inversion and lasing were achieved in semiconductor nanowires with low pump photon energy.
- The extremely high electric field of the pump induced band bending and electron tunneling.
- Excitation became independent of frequency, relying solely on incident light intensity, indicating a wave-based mechanism.
Conclusions:
- Population inversion and lasing can be achieved through mechanisms dominated by the wave nature of electrons.
- Light's classical Coulomb force plays a crucial role in this low-frequency excitation regime.
- This finding expands the understanding of light-matter interactions in semiconductor nanostructures.
Related Concept Videos
Titration Calculations: Strong Acid - Strong Base
A titration is carried out for 25.00 mL of 0.100 M HCl (strong acid) with 0.100 M of a strong base NaOH. The pH at different volumes of added base solution can be calculated as follows:
(a) Titrant volume = 0 mL. The solution pH is due to the acid ionization of HCl. Because this is a strong acid, the ionization is complete and the hydronium ion molarity is 0.100 M. The pH of the solution is then:
Strong Acid and Base Solutions
Titration of a Strong Acid with a Strong Base
Titration Calculations: Weak Acid - Strong Base
For the titration of 25.00 mL of 0.100 M CH3CO2H with 0.100 M NaOH, the reaction can be represented as:
Titration of a Weak Acid with a Strong Base
Titration of Polyprotic Acids with a Strong Base

