Related Experiment Video
Updated: Oct 29, 2025

09:49
An Experimental Protocol for Femtosecond NIR/UV - XUV Pump-Probe Experiments with Free-Electron Lasers
Published on: October 23, 2018
16.2K
Photon-electron coincidence experiments at synchrotron radiation facilities with arbitrary bunch modes
C Ozga1, C Honisch1, Ph Schmidt1
1Institut für Physik und CINSaT, Universität Kassel, Heinrich-Plett-Straße 40, 34132 Kassel, Germany.
The Review of Scientific Instruments
|July 10, 2021
Summary
We adapted electron-photon coincidence detection for synchrotron radiation
Area of Science:
- Atomic and Molecular Physics
- Synchrotron Radiation Science
- Quantum Optics
Background:
- Electron-photon coincidence detection is crucial for studying atomic and molecular processes.
- Adapting this technique to multibunch modes at synchrotron sources presents challenges due to continuous excitation.
Purpose of the Study:
- To adapt electron-photon coincidence detection for the multibunch hybrid mode at BESSY II.
- To enable high-resolution coincidence measurements in quasi-continuous excitation patterns.
Main Methods:
- Utilized single-event-based data acquisition and relative detection times.
- Modeled accidental coincidences using non-coincident electron and photon spectra.
- Applied the adapted scheme to study CO2 photoionization and subsequent photon emission.
Main Results:
- Successfully validated the method by reproducing prior single-bunch results.
- Obtained radiative lifetime and electron binding energy for CO2 ionization in good agreement with literature.
- Demonstrated the method's effectiveness in multibunch hybrid mode.
Conclusions:
- The adapted coincidence detection scheme is effective for multibunch synchrotron operation.
- This technique enhances the versatility of coincidence measurements at various light sources.
- No additional experimental adjustments are needed for broader applicability.
More Related Videos
Related Concept Videos
The de Broglie Wavelength
31.0K
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...
31.0K
π Electron Effects on Chemical Shift: Overview
1.3K
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,...
1.3K
¹³C NMR: ¹H–¹³C Decoupling
1.3K
The probability of having two carbon-13 atoms next to each other is negligible because of the low natural abundance of carbon-13. Consequently, peak splitting due to carbon-carbon spin-spin coupling is not observed in spectra. However, protons up to three sigma bonds away split the carbon signal according to the n+1 rule, resulting in complicated spectra.
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
A broadband decoupling technique is used to simplify these complex, sometimes overlapping, signals. Broadband decoupling relies on a...
1.3K
Interaction of EM Radiation with Matter: Spectroscopy
2.4K
Electromagnetic (EM) radiation can be considered an oscillating electric and magnetic field propagating through a medium that can interact with matter in its path. The electric field in the radiation can interact with electrical charges in the atoms or molecules in the matter. On the other hand, the magnetic field can interact with the magnetic field in the atomic nucleus. The study of the interaction between electromagnetic radiation and matter is termed spectroscopy. Spectroscopy is the study...
2.4K
NMR Spectrometers: Radiofrequency Pulses and Pulse Sequences
1.1K
A pulse is a short burst of radio waves distributed over a range of frequencies that simultaneously excites all the nuclei in the sample. Upon passing a radio frequency pulse along the x-axis, the nuclei absorb energy corresponding to their Larmor frequencies and achieve resonance. This shifts the net magnetization vector from the z-axis toward the transverse plane. This angle of rotation of the magnetization vector, or the flip angle, is proportional to the duration and intensity of the pulse.
1.1K
Atomic Emission Spectroscopy: Interference
340
In atomic emission spectroscopy (AES), high-temperature atomizers excite a broad range of elements and molecules that generate complex emissions from sources such as oxides, hydroxides, and flame combustion products in the flame or plasma. Several strategies can be employed to minimize spectral interferences caused by overlapping emission lines or bands. These include increasing instrument resolution, choosing alternative emission lines, optimally placing the detector in low-background regions,...
340

