Related Experiment Video
Updated: Apr 25, 2026

10:12
Synchrotron X-ray Microdiffraction and Fluorescence Imaging of Mineral and Rock Samples
Published on: June 19, 2018
8.3K
Intensity interferometry of single x-ray pulses from a synchrotron storage ring
A Singer1, U Lorenz1, A Marras2
1Deutsches Elektronen-Synchrotron DESY, Notkestraße 85, D-22607 Hamburg, Germany.
Physical Review Letters
|August 23, 2014
Summary
We measured X-ray coherence using a new detector at PETRA III. Results match theoretical models, advancing synchrotron radiation analysis.
Area of Science:
- X-ray physics
- Synchrotron radiation science
- Detector technology
Background:
- High-brilliance synchrotron radiation sources enable advanced X-ray experiments.
- Accurate measurement of X-ray coherence is crucial for applications like coherent imaging.
- Novel detector technologies are needed to keep pace with source brilliance.
Purpose of the Study:
- To report on measurements of second-order intensity correlations using a novel detector.
- To determine the transverse coherence length of X-rays at 14.4 keV.
- To validate the performance of an adaptive gain integrating pixel detector prototype.
Main Methods:
- Utilized the high-brilliance storage ring PETRA III.
- Employed a prototype adaptive gain integrating pixel detector.
- Measured second-order intensity correlations at various spatial separations for individual synchrotron radiation pulses (14.4 keV, ~5 MHz).
Main Results:
- Successfully recorded individual synchrotron radiation pulses.
- Determined the transverse coherence length at 14.4 keV.
- Achieved good agreement between experimental measurements and Gaussian Schell model simulations.
Conclusions:
- The adaptive gain integrating pixel detector is suitable for high-brilliance synchrotron radiation measurements.
- The experimental method accurately determines transverse coherence length.
- Validated theoretical models for X-ray coherence at high energies.
Related Concept Videos
X-ray Imaging
7.7K
German physicist Wilhelm Röntgen (1845–1923) was experimenting with electrical current when he discovered that a mysterious and invisible "ray" would pass through his flesh but leave an outline of his bones on a screen coated with a metal compound. In 1895, Röntgen made the first durable record of the internal parts of a living human: an "X-ray" image (as it came to be called) of his wife’s hand. Scientists worldwide quickly began their own experiments with...
7.7K
X-ray Crystallography
21.5K
The size of the unit cell and the arrangement of atoms in a crystal may be determined from measurements of the diffraction of X-rays by the crystal, termed X-ray crystallography.
Diffraction
Diffraction is the change in the direction of travel experienced by an electromagnetic wave when it encounters a physical barrier whose dimensions are comparable to those of the wavelength of the light. X-rays are electromagnetic radiation with wavelengths about as long as the distance between neighboring...
Diffraction
Diffraction is the change in the direction of travel experienced by an electromagnetic wave when it encounters a physical barrier whose dimensions are comparable to those of the wavelength of the light. X-rays are electromagnetic radiation with wavelengths about as long as the distance between neighboring...
21.5K
X-ray Diffraction of Biological Samples
3.8K
X-ray diffraction or XRD is an analytical tool that utilizes X-rays to study ordered structures such as crystalline organic and inorganic samples, polycrystalline materials, proteins, carbohydrates, and drugs.
According to Bragg's law, when X-rays strike the sample positioned on a stage, the rays are scattered by the electron clouds around the sample atoms. The X-ray diffraction or scattering is caused by constructive interference of the X-ray waves that reflect off the internal...
According to Bragg's law, when X-rays strike the sample positioned on a stage, the rays are scattered by the electron clouds around the sample atoms. The X-ray diffraction or scattering is caused by constructive interference of the X-ray waves that reflect off the internal...
3.8K
Atomic Emission Spectroscopy: Interference
782
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,...
782
IR Spectrometers
3.1K
There are two main infrared (IR) spectrophotometers: dispersive IR spectrometers and Fourier transform infrared (FTIR) spectrometers. In a dispersive IR spectrometer, a beam of infrared radiation produced by a hot wire is divided into two parallel equal-intensity beams using mirrors. One beam passes through the sample, while another is a reference beam. The beams then move through the monochromator, which separates the radiations into a continuous spectrum of different frequencies. The...
3.1K

