Christian Grünzweig’s research while affiliated with Paul Scherrer Institute and other places

What is this page?


This page lists works of an author who doesn't have a ResearchGate profile or hasn't added the works to their profile yet. It is automatically generated from public (personal) data to further our legitimate goal of comprehensive and accurate scientific recordkeeping. If you are this author and want this page removed, please let us know.

Publications (95)


ANAXAM @ TOMCAT 2.0: easy access to cutting-edge tomographic microscopy for industry
  • Article

February 2025

·

13 Reads

e-Journal of Nondestructive Testing

·

Vladimir Novak

·

Christian Gruenzweig

·

[...]

·

TOMCAT is a tomographic microscopy beamline at the Swiss Light Source (SLS) of the Paul Scherrer Institut (PSI) [1]. For almost two decades, TOMCAT has been offering its cutting-edge tomographic microscopy capabilities to various industries in need of non-destructive, non-invasive, volumetric, and functional material characterization beyond what is currently possible with conventional X-ray tubes [2]. Five years ago, PSI (together with two Swiss institutes and the Canton of Aargau in Switzerland) has co-founded ANAXAM – a technology transfer center that facilitates the use of advanced analytical methods at large-scale facilities such as the SLS for industrial applications. A collaboration between TOMCAT and ANAXAM has leveled up the imaging capabilities that can be offered to industry. One of the main advantages is that ANAXAM has enabled speedy realizations of necessary sample environments that can be used during synchrotron X-ray tomographic microscopy experiments. In this paper, we show examples of successful investigations performed for several industries such as medical technology, pharmaceuticals, marine industry, automotive, and food [3, 4]. In September 2023, TOMCAT paused its operation to allow for the construction of the new SLS 2.0 storage ring [5] in combination with several beamline upgrades [6]. SLS 2.0 is expected to resume operation mid 2025 with a significantly improved machine performance such as smaller source size, improved beam collimation and higher intensity. TOMCAT 2.0 will leverage on the higher brilliance of SLS 2.0 by deploying its upgrade program on two beamlines: (1) I-TOMCAT will be a brand-new instrument based on an insertion device of the latest generation; and (2) S-TOMCAT, the original beamline, will be refurbished with a new high-field superconducting 5T bending magnet. Here we discuss overall possibilities of TOMCAT 2.0 and ANAXAM with respect to industrial applications.



(a) Climatic chamber for offline pre-conditioning of up to 16 syringes with controlled temperature and pressure cycles. The chamber is showed without the front cover to provide a view inside it. (b) Climatic chamber for in-line (in-situ) conditioning of up to 4 syringes with controlled temperature and pressure cycles, see Table I.
Examples of syringe needles imaged by neutron radiography without (left) and with (right) liquid presence in needle (indicated by yellow circle) in as-received samples. Top image shows acquired projection and the bottom one is after application of edge enhancement filter.
Impact of temperature and pressure cycling on the formation of liquid in the syringe needle observed by neutron radiography: before (left column) and after (right column) 5 °C to 25 °C cycling; before and after 5 °C to 40 °C cycling, and before and after 101 kPa to 55 kPa cycling. The liquid segments are indicated by yellow circles.
Air bubble movement at the entrance to syringe needle during (a) 5 °C to 40 °C temperature cycling and (b) 101 kPa to 55 kPa pressure cycling observed by in-situ neutron radiography. Videos showing evolution of air buble during cycling are available in SI.
Comparison of needle imaging by (a) neutron radiography (2D) and (b) synchrotron X-ray tomography (3D) for as-received PFS with liquid presence. Neutron radiography was done with pixel size 13.5 µm and FOV 27.5 × 27.5 mm². Synchrotron X-ray tomography was performed with pixel size 1.6 µm and FOV 4.2 × 4.2 x 3.0 mm².

+2

Unraveling Pre-filled Syringe Needle Clogging: Exploring a Fresh Outlook Through Innovative Techniques
  • Article
  • Publisher preview available

February 2024

·

246 Reads

·

3 Citations

Pharmaceutical Research

Objective This study aimed to investigate the movement of liquid in the needle region of staked-in-needle pre-filled syringes using neutron imaging and synchrotron X-ray tomography. The objective was to gain insights into the dynamics of liquid presence and understand the factors contributing to needle clogging. Methods Staked-in-needle pre-filled syringes were examined using neutron radiography and synchrotron X-ray phase-contrast computed tomography. Neutron radiography provided a 2D visualization of liquid presence in the needle, while synchrotron X-ray tomography offered high-resolution 3D imaging to study detailed morphological features of the liquid. Results Neutron radiography revealed liquid presence in the needle region for as-received samples and after temperature and pressure cycling. Pressure cycling had a more pronounced effect on liquid formation. Synchrotron X-ray tomography confirmed the presence of liquid and revealed various morphologies, including droplets of different sizes, liquid segments blocking sections of the needle, and a thin layer covering the needle wall. Liquid presence was also observed between the steel needle and the glass barrel. Conclusions The combination of neutron imaging and synchrotron X-ray tomography provided valuable insights into the dynamics of liquid movement in staked-in-needle pre-filled syringes. Temperature and pressure cycling were found to contribute to additional liquid formation, with pressure changes playing a significant role. The detailed morphological analysis enhanced the understanding of microstructural arrangements within the needle. This research contributes to addressing the issue of needle clogging and can guide the development of strategies to improve pre-filled syringe performance.

View access options

Schematic of the symmetric Talbot–Lau polarized neutron grating interferometer setup including the optional polarization analyzer. The setup consists of an adiabatic fast passage spin flipper (AFP), a source grating (G0)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(\mathrm {G_0})$$\end{document}, a phase grating (G1)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(\mathrm {G_1})$$\end{document}, an analyzer grating (G2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$(\mathrm {G_2}$$\end{document}, a polarization analyzer, a neutron detector and a guide field system (shaded pink). The spin analyzer can be moved out of the beam to the side, i.e. along the y-direction (IN and OUT). The probed polarization direction is along the z-axis. The magnetic sample is placed between G1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathrm {G_1}$$\end{document} and G2\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathrm {G_2}$$\end{document} at a distance Ls\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\mathrm { L_s}$$\end{document} from the latter one and moved along the x-axis direction to perform a correlation length scan. The inter-grating distance in a symmetric setup are equal to L and all periods are same (p). In the sketch the spin-flip and non-spin-flip small-angle scattering events are highlighted symbolically.
Modulation visibility for polarization-analyzed DFI. (a) Visibility maps for the symmetric Talbot-Lau polarized neutron grating interferometer setup in four configurations: without the polarization analyzer in place and spin-up |↑〉\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\big | \uparrow \big \rangle$$\end{document} (top left), without the polarization analyzer in place and spin-down |↓〉\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\big | \downarrow \big \rangle$$\end{document} (top right), with the polarization analyzer in place and spin-up |↑〉\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\big | \uparrow \big \rangle$$\end{document} (bottom left) and with the polarization analyzer in place and spin-down |↓〉\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\big | \downarrow \big \rangle$$\end{document} (bottom rigth). (b) Intensity modulation for the 4 different color coded configurations reported in (a) and the corresponding fitted sinusoidal curves. The color coded boxes in (a) delimit the fitted area for the intensity modulation fitting.
Photographic image of the NdFeB sintered magnetic sheet. The sintered magnet is characterized by big and isotropic grains of few micrometer in size. The sample is 0.15 mm thick and coated with 0.5 nm tantalum. The blue arrow indicates the easy axis of the magnetization. The scale in the background is expressed in (cm).
Measured polarized DFI of the sintered NdFeB magnet. (a) TI and DFI images of the NdFeB with and without the external magnetic field at ξ≃0.7μm\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\xi \simeq 0.7 \upmu \hbox {m}$$\end{document} and without analyzer in place. The North and the South poles of the applied field are depicted in red and blue, respectively. (b) DFI experimental values and the fitted Vs(ξ)V0\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\frac {V_s(\xi )}{V_0}$$\end{document} curves based on model of correlation functions G(ξ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$G(\xi )$$\end{document} for the four configurations without the external magnetic field corresponding to the V++\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{++}$$\end{document}, V-+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{-+}$$\end{document}, V+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{+}$$\end{document} and V-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{-}$$\end{document}. (c) DFI experimental values and the fitted DFI curves with the extracted correlation functions G(ξ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$G(\xi )$$\end{document} for the four configurations with the external magnetic field corresponding to the VH++\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{++}_{H}$$\end{document}, VH-+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{-+}_{H}$$\end{document}, VH+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{+}_{H}$$\end{document} and VH-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{-}_{H}$$\end{document}. The modeled G(ξ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$G(\xi )$$\end{document} functions were based on the description of random two phase media. The magnetization easy axis of the sample is along the short side of the sample and along the applied external magnetic field.
(a) Retrieved V+-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{+-}$$\end{document} and V--\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{--}$$\end{document} from the measured V+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{+}$$\end{document}, V-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{-}$$\end{document} and V++\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{++}$$\end{document}, without the external magnetic field. (b) Retrieved VH+-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{+-}_{H}$$\end{document} and VH--\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{--}_{H}$$\end{document} from the measured VH+\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{+}_{H}$$\end{document}, VH-\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{-}_{H}$$\end{document} and VH++\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$V^{++}_{H}$$\end{document}, with the applied external magnetic field. The G(ξ)\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$G(\xi )$$\end{document} functions were extracted by fitting the model for random two phase media.
Towards spatially resolved magnetic small-angle scattering studies by polarized and polarization-analyzed neutron dark-field contrast imaging

April 2021

·

147 Reads

·

4 Citations

In the past decade neutron dark-field contrast imaging has developed from a qualitative tool depicting microstructural inhomogeneities in bulk samples on a macroscopic scale of tens to hundreds of micrometers to a quantitative spatial resolved small-angle scattering instrument. While the direct macroscopic image resolution around tens of micrometers remains untouched microscopic structures have become assessable quantitatively from the nanometer to the micrometer range. Although it was found that magnetic structures provide remarkable contrast we could only recently introduce polarized neutron grating interferometric imaging. Here we present a polarized and polarization analyzed dark-field contrast method for spatially resolved small-angle scattering studies of magnetic microstructures. It is demonstrated how a polarization analyzer added to a polarized neutron grating interferometer does not disturb the interferometric measurements but allows to separate and measure spin-flip and non-spin-flip small-angle scattering and thus also the potential for a distinction of nuclear and different magnetic contributions in the analyzed small-angle scattering.


Decomposing Magnetic Dark-Field Contrast in Spin Analyzed Talbot-Lau Interferometry: A Stern-Gerlach Experiment without Spatial Beam Splitting

February 2021

·

58 Reads

·

4 Citations

Physical Review Letters

We have recently shown how a polarized beam in Talbot-Lau interferometric imaging can be used to analyze strong magnetic fields through the spin dependent differential phase effect at field gradients. While in that case an adiabatic spin coupling with the sample field is required, here we investigate a nonadiabatic coupling causing a spatial splitting of the neutron spin states with respect to the external magnetic field. This subsequently leads to no phase contrast signal but a loss of interferometer visibility referred to as dark-field contrast. We demonstrate how the implementation of spin analysis to the Talbot-Lau interferometer setup enables one to recover the differential phase induced to a single spin state. Thus, we show that the dark-field contrast is a measure of the quantum mechanical spin split analogous to the Stern-Gerlach experiment without, however, spatial beam separation. In addition, the spin analyzed dark-field contrast imaging introduced here bears the potential to probe polarization dependent small-angle scattering and thus magnetic microstructures.


Initial development and testing of dysprosium-based scintillators for digital transfer method neutron imaging

January 2021

·

99 Reads

·

3 Citations

Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment

A new type of scintillator screen consisting of a ZnS scintillator with a dysprosium neutron converter is explored in a joint effort between Idaho National Laboratory (INL) and Paul Scherrer Institute (PSI). In contrast with a traditional prompt ⁶Li or Gd converters, a dysprosium converter generates a latent image as neutron activated dysprosium produces an isotope which decays with half-lives of 1.26 min and 2.3 h and the decay radiation excites the ZnS scintillator. The activated scintillator screen is physically transported out of the neutron beam and away from radioactive samples into the imaging apparatus and emits photons as the screen decays, which are read by a digital camera. This technology bridges the gap between traditional indirect transfer radiography and modern digital camera-based systems. This paper describes initial development of dysprosium-based scintillator screens and the results of initial tests performed at PSI. Some screen variants exhibit sufficient light output to produce good quality radiographs in a matter of minutes. The basic spatial resolution measured using a Siemens star is approximately 300μm. This work demonstrates for the first time that indirect digital transfer method neutron imaging is a plausible method of imaging highly radioactive sources such as irradiated nuclear fuel.


Operando Visualization of Water Distribution in Gas Diffusion Media of PEFCs with an Optimized Neutron Grating Interferometer

April 2020

·

170 Reads

·

5 Citations

We demonstrated the use of a neutron grating interferometer setup (nGI) with a significantly improved contrast-to-noise ratio of the operando dark-field (DF) contrast visualization of water in gas diffusion media (GDM). The nGI parameters were optimized in such a way that we could perform DF imaging of a fully operational fuel cell including two GDM layers (anode and cathode side). The DF contrast is sensitive to the size and shape of microstructures and is in principle not influenced by large water clusters present in flow field channels. Thus, DF imaging can be applied to analyze water present in GDM overlapping with channels, which is not possible by attenuation contrast imaging when the cell is placed perpendicular to the beam direction. In GDM regions overlapping with ribs the distinction of hydrophilic and hydrophobic areas is facilitated as well compared to attenuation contrast imaging. Finally, we show that disturbing artefacts introduced by moving water clusters in the channels are considerably reduced by applying a golden ratio phase stepping scan strategy.


Figure 1. (a) Diffraction peak area cropped from the Laue data. (b) The same peak adjusted to be used as projection for tomography reconstruction. The size of the frame in which the peak is centred is decided based on the widest peak of the dataset, and the threshold value to bring the background to zero is calculated using the Otsu method 14 . (c-f) Position of the diffraction peaks from a single crystal grain in the sample reference system (SRS); (c,d) Isometric view of the diffraction peaks detected on the back-diffraction and forward diffraction detector, respectively, rotated into the SRS; (e,f) Top view of the diffraction peaks detected on the back-diffraction and forward diffraction detector rotated into the SRS. (g) A full grain volume (grain 1 from the Fe sample) as reconstructed with the SIRT-3D algorithm. The diffraction peak of (a,b) corresponds to this grain.
Figure 2. Three-dimensional orientation (top and bottom left) and morphology (top and bottom right) maps of the crystal grains of the Fe and Cu samples, respectively. The grains are colour-coded in accordance with their orientation based on the inverse pole figure colour map for a top view (positive z-direction) on the specimen. The shaded areas around the grains represent the shape of each sample. The small schematics given at the top and bottom of the figure show the volume area of each sample that was effectively illuminated by the neutron beam.
Figure 3. Validation of the Laue 3DNDT grain morphology reconstruction. (a,b) EBSD maps of the Cu sample taken at 1.6 mm and 3.2 mm from the surface of the sample, respectively. (c,d) Corresponding slices from the Laue 3DNDT morphology reconstruction. The grains for both the EBSD and Laue 3DNDT are numbered according to the Laue indexing order and are colour-coded in accordance with their orientation based on the inverse pole figure colour map for a top view (positive z-direction) on the specimen. In (a,b) the grain orientation is also schematically depicted as cubes. The black lines surrounding the grains indicate grain boundaries, while white and yellow lines show twin and double twin boundaries, respectively. Colour variation within one image (for the same grain) is attributed to the shift of the electron beam due to the large area scanned. Small colour variations for the same grains from different EBSD scans originate from slight misalignment of the sample after removing and reinserting it into the SEM sample chamber.
Grain morphology reconstruction of crystalline materials from Laue three-dimensional neutron diffraction tomography

February 2020

·

237 Reads

·

13 Citations

The macroscopic properties of advanced engineering and functional materials are highly dependent on their overall grain orientation distribution, size, and morphology. Here we present Laue 3D neutron diffraction tomography providing reconstructions of the grains constituting a coarse-grained polycrystalline material. Reconstructions of the grain morphology of a highly pure Fe cylinder and a Cu cube sample are presented. A total number of 23 and 9 grains from the Fe and Cu samples, respectively, were indexed and reconstructed. Validation of the grain morphological reconstruction is performed by post-mortem EBSD of the Cu specimen.


Characterization of oriented microstructures through anisotropic small-angle scattering by 2D neutron dark-field imaging

February 2020

·

439 Reads

·

20 Citations

Within neutron imaging, different methods have been developed with the aim to go beyond the conventional contrast modalities, such as grating interferometry. Existing grating interferometers are sensitive to scattering in a single direction only, and thus investigations of anisotropic scattering structures imply the need for a circular scan of either the sample or the gratings. Here we propose an approach that allows assessment of anisotropic scattering in a single acquisition mode and to broaden the range of the investigation with respect to the probed correlation lengths. This is achieved by a far-field grating interferometer with a tailored 2D-design. The combination of a directional neutron dark-field imaging approach with a scan of the sample to detector distance yields to the characterization of the local 2D real-space correlation functions of a strongly oriented sample analogous to conventional small-angle scattering. Our results usher in quantitative and spatially resolved investigations of anisotropic and strongly oriented systems beyond current capabilities. Acquiring orientation-resolved neutron images currently requires the sample or system to be rotated, precluding single-shot measurement. Here, the authors achieve small-angle scattering information with spatial resolution in a single shot through the inclusion of a circular diffraction grating.


Figure 2. The integrated light output of scintillator screens measured in counts per pixel during the 5-minute decay phase.
Figure 3. The light output per pixel of the seven screens that exhibited the highest light output. Individual images were taken every 2 s during 5-minute exposure and 5-minute decay phases. The light output builds up as the screens are exposed to the neutron beam for a longer amount of time. The beam is shut off after 300 seconds and the screens' light output decays away with time.
Gamma Discriminating Scintillation Screens for Digital Transfer Method Neutron Imaging

February 2020

·

72 Reads

·

4 Citations

Materials Research

A collaborative project between Idaho National Laboratory (INL) and Paul-Scherrer Institute (PSI) is investigating a new type of scintillation screen that uses ZnS scintillator material with a dysprosium neutron converter instead of traditional prompt converters such as 6 Li. Such a screen exposed to a neutron beam creates a latent image by neutron activation of the dysprosium in the scintillator screen. The activated screen is transported into a camera box allowing the camera to read a digital image from the photons emitted by the activated scintillation screen. Such an imaging system combines modern camera-based system architecture with the approach of traditional indirect transfer method radiography. The results show for the first time that the combination of dysprosium with a scintillation material like ZnS can produce light which is measurable under common camera-based detection conditions and that neutron radiographic images of reasonable quality can be produced. The resolution was poorer than expected at ~ 300 μm, but is on the order of the desired resolution of 100 μm. Potential improvements and additional converter materials may be investigated in the future that could increase the light output and improve spatial resolution.


Citations (74)


... One of the main advantages is that ANAXAM has enabled speedy realizations of necessary sample environments that can be used during synchrotron X-ray tomographic microscopy experiments. In this paper, we show examples of successful investigations performed for several industries such as medical technology, pharmaceuticals, marine industry, automotive, and food [3,4]. In September 2023, TOMCAT paused its operation to allow for the construction of the new SLS 2.0 storage ring [5] in combination with several beamline upgrades [6]. ...

Reference:

ANAXAM @ TOMCAT 2.0: easy access to cutting-edge tomographic microscopy for industry
Unraveling Pre-filled Syringe Needle Clogging: Exploring a Fresh Outlook Through Innovative Techniques

Pharmaceutical Research

... In this configuration, the interferometer is sensitive only to scattering in the direction of modulation of the moiré pattern [x axis in Fig. 1(a)]. Although not currently implemented in the tool that we introduce here, the development of multidirectional gratings and the inclusion of polarization analysis also broaden the sensitivity of the technique to anisotropic structure and magnetic properties of materials (Valsecchi et al., , 2021Busi et al., 2023). The autocorrelation length �, which is the microstructural length scale being probed, depends on the parameters of the interferometer (Strobl, 2015;Wen et al., 2008): ...

Towards spatially resolved magnetic small-angle scattering studies by polarized and polarization-analyzed neutron dark-field contrast imaging

... The Talbot-Lau structure was proposed for inertial detection for particle beams [53]. The Talbot-Lau interferometer was used with a neutron beam and exploited for investigation of the inner frameworks of electrical steel sheets [54], magnetic field spatial distribution [55], and the splitting of the spin states [56]. ...

Decomposing Magnetic Dark-Field Contrast in Spin Analyzed Talbot-Lau Interferometry: A Stern-Gerlach Experiment without Spatial Beam Splitting
  • Citing Article
  • February 2021

Physical Review Letters

... Screens 2, 4, and 7 exhibit high light output, confirming previous results that showed that thicker ZnS:Cu produced more light output. 17 These results demonstrate that thicker scintillator layers provide more light output because there is more scintillator material to interact with the radiation produced by the activated dysprosium. The resulting integrated decay-phase radiographs of the brightest screens have a grayscale range of ~40 000 gray levels in a 16-bit image (maximum 65 535 gray levels), which represents ~60% of saturation and demonstrates that this imaging method can produce images with comparable brightness as standard prompt imaging methods. ...

Initial development and testing of dysprosium-based scintillators for digital transfer method neutron imaging

Nuclear Instruments and Methods in Physics Research Section A Accelerators Spectrometers Detectors and Associated Equipment

... One of the basic problems is a reliable determination of flux trapping. We use a complementary method, polarized neutron imaging, which enables us to determine the trapped field directly and which provides spatially resolved in-depth information from the entire volume of the investigated sample [17,[19][20][21][22][23][24][25]. In order to understand our investigations, some basics of polarized neutron imaging are given. ...

Visualization of compensating currents in type-II/1 superconductor via high field cooling
  • Citing Article
  • February 2020

... In addition to simulation studies, several experimental methods have also been employed to observe and study water transport and distribution, such as fluorescence microscopy (Bazylak et al., 2007;Litster et al., 2006), X-ray tomography (Atkinson et al., 2017;Cetinbas et al., 2019;Zenyuk et al., 2016), and neutron radiography (Cooper et al., 2017;Nasu et al., 2022;Pang et al., 2022;Pekula et al., 2005;Siegwart et al., 2020;Wu et al., 2021). Muirhead et al. experimentally investigated the liquid water accumulation in a GDL by a synchrotron X-ray radiography visualization tool and found that liquid water pools in open area with higher local porosity (Muirhead et al., 2018). ...

Operando Visualization of Water Distribution in Gas Diffusion Media of PEFCs with an Optimized Neutron Grating Interferometer

... While X-ray photons interact with electrons, neutrons interact with the atomic nucleus. Neutron tomography can be carried out by characterizing the neutron absorption [74], scattering cross-section [75,76], local diffraction [77] as well as by the phase change [78]. Neutrons are highly sensitive to light elements such as H, N, C, O and are attenuated very efficiently by proton-rich compounds such as water [79], and can be suitable to characterize in situ dissolution/disintegration of tablets. ...

Grain morphology reconstruction of crystalline materials from Laue three-dimensional neutron diffraction tomography

... An x-ray dark-field signal can be useful in various fields, including biomedical imaging, materials science and security screening. Safety or industrial applications include detecting and/or identifying goods that come in powder forms, such as drugs or explosives [29], [30], and imaging industrial parts made from carbon fibres [31]. Some possible biomedical imaging applications include imaging kidney stones of different compositions and microscopic morphology for classification [32], [33], imaging breast tissues with microcalcifications for early detection of cancer [34]- [37], and imaging bones to diagnose osteoporosis or undisplaced fractures [38], [39]. ...

Characterization of oriented microstructures through anisotropic small-angle scattering by 2D neutron dark-field imaging

... 10 The digital transfer method radiography explored in this work combines the advantages of digital neutron radiography, namely, quick acquisition times and high detection efficiency, with the transfer method's complete insensitivity to gamma radiation. 11 Figure 1 describes the digital transfer method radiography process in which a scintillator screen is first placed in the neutron beam and becomes activated in the pattern of the beam after passing through the imaging object. The converter material becomes activated when it absorbs neutrons and subsequently releases ionizing radiation as it decays. ...

Gamma Discriminating Scintillation Screens for Digital Transfer Method Neutron Imaging

Materials Research

... Advanced quantitative neutron dark-field imaging offers not only qualitative insights regarding structural inhomogeneities within sample volumes but also quantitative information on the respective local microstructures by providing real-space correlation functions, which are measured e.g. through sample-detector distance scans 5 . Therefore, this technique not only provides new understandings of the microstructural properties of materials but also offers a promising avenue for non-destructively investigating complex structures in bulk materials and assemblies subjected to external and internal stimuli, both in radiographic mode providing 2D thickness-average maps, and in tomographic mode, offering volumetric bulk insights of the studied materials 6 . Prominent examples of applications include the visualization of magnetic domains in electrical steels [7][8][9] , including time-resolved studies allowing to quantify the movement of domain walls in grain oriented electrical steels 10 . ...

3D sub-pixel correlation length imaging