Simon Zabler’s research while affiliated with Deggendorf Institute of Technology and other places

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Publications (72)


Determining the optimal choice of attenuation filters and propagation distance for polychromatic phase‐contrast micro‐computed tomography of a multi‐material electromotor using synchrotron radiation
  • Article
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April 2025

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13 Reads

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Simon Zabler

Optimizing phase‐contrast micro‐computed tomography (µCT) for a given object is not trivial if the radiation is polychromatic and the object multi‐material. This study demonstrates how an optimal combination of propagation distance and mean energy (set by attenuation filters) may be derived for such an object (an electromotor scanned on beamline BM18 at ESRF in Grenoble, France). In addition to appropriate image quality metrics, it is mandatory to define a task. In that respect, raising Emean from 100 keV to 164 keV mitigates beam hardening by metal parts, yet raising Emean further to 230 keV deteriorates CNR² (where CNR is contrast‐to‐noise ratio) due to higher image noise. Propagation distances between d = 2 m and 25.3 m are evaluated crosswise with energy. While longer propagation distances generally yield higher CNR², shorter distances appear favorable when discerning plastic near metal parts. SNR² (where SNR is signal‐to‐noise ratio) power spectra and modulation transfer (MTF) are evaluated independently from two‐dimensional projections supporting volume image analysis for which image sharpness depends strongly on the digital filters (Paganin and Wiener) which are applied along with filtered back‐projection. In summary, optimizing synchrotron µCT scans remains a very complex task which differs from object to object. A physically accurate model of the complete imaging process may not only allow for optimization by simulation but also ideally improve CT image reconstruction in the near future.

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Figure 1: Twin robot CT at the Deggendorf Institute of Technology (DIT)
Figure 2: The left image depicts a rendering of the calibration body used for the DLT based calibration. The center image shows a toy car mustang made from LEGO. The rightmost image shows a reconstructed slice of the sphere packing. The reconstruction was used here for visualization purposes because the object is made of opaque material.
Figure 5: Circular CT Trajectory. The plots illustrate the metrics Tenengrad variance and Shannon entropy along the respective x, y, and z directions of the volume of the calibration object.
Figure 6: Sinusoidal CT trajectory. Description comparable to figure 5.
Figure 7: SART reprojection error of the circular CT trajectory.

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Safeguarding accuracy for CT imaging with industrial robots: Efficient calibration methods for arbitrary trajectories

February 2025

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107 Reads

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1 Citation

e-Journal of Nondestructive Testing

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Conventional industrial computed tomography (CT) systems are constrained in their choice of acquisition trajectories due to their mechanical design. These systems are very precise instruments since they do only move on primarily highly accurate rotational stages. In order to be able to scan an arbitrary Region of Interest (ROI), regardless of the position, size and weight of the specimen, conventional industrial robots can be used as flexible 6 degrees of freedom (DOF) manipulators. For example in a twin robot computed tomography system, acquisition geometries with arbitrary tool poses can be realized. In scientific applications, the quality of the CT volume image is of primary interest, whereas in an industrial environment it is often a matter of balancing quality and acquisition time. Common industrial robots cannot achieve the required positional accuracy without calibration to generate an ideal reconstruction. In the presented study, methods for the geometric correction of CT scans are compared. Image based correction is compared to general machine calibration and full pose tracking by laser trackers. Image quality metrics such as the Modulation Transfer Function, Shannon entropy and Tenengrad variance are utilized to evaluate and compare the reconstruction quality of the various correction and calibration approaches. The assessment of the reconstruction quality revealed a comparable reconstruction quality between the approaches, with the machine calibration approach emerging as one of the best, while also reducing the time-intensive correction overhead.


Figure 1: Simulation of a capillary filled with spheres, projected thickness (left), X-ray projection with noise (middle), Xray projection with phase contrast, noise and scintillator spots (right).
Figure 2: slice through the 3D reconstructed volume of the capillary in Figure 1, no artifacts (left), noise present (middle), noise and ring artifact stemming from scintillator spots (right).
Figure 3: Evaluation of the synthetic displacement field based on the measured volume and the synthetically deformed volume. The specimen consists of a magnesium-5%-gadolinium alloy and surrounding bone. The field component in the direction of the screw's symmetry axis is shown. Adapted from [10].
Figure 8: Slice through a volume of a battery scanned on the synchrotron at the Helmholtz-Zentrum Berlin, (a) original, (b) compressed by a factor of 10, (c) profile line through (a) and (b), (d) magnified detail of (c).
A Framework for the AI-based visualization and analysis of massive amounts of 4D tomography data for end users of beamlines

February 2025

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116 Reads

e-Journal of Nondestructive Testing

The size of 4D tomography datasets acquired at synchrotron or neutron imaging facilities can reach several terabytes, which presents a significant challenge for their evaluation. This paper presents a framework that allows a compressed dataset to be kept in memory and makes it possible to evaluate and manipulate the dataset without requiring enough memory to decompress the entire dataset. The framework enables the compensation of imaging artifacts, including the compression artifacts of the 4D dataset, through the integration of neural networks. The reduction of imaging artifacts can be performed at the imaging facility or at the user's home institution. This framework reduces the computational burden on the computing infrastructure of large synchrotron and neutron facilities by allowing end users to process datasets on their institution's computers. This is made possible by compressing TBs of data to less than 128 GB, allowing powerful PCs to process TBs of 4D tomography data.


Denoising and deconvolving CT images of unknown origin: comparing linear Wiener-deconvolution with deep convolutional neural network Noise2Inverse

February 2025

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8 Reads

e-Journal of Nondestructive Testing

Low-dose CT scans are very fast, but they feature strong pixel noise which, in turn, invites for efficient denoising the same way that strong image blur invites for sharpening the images. Wiener-deconvolution serves as a starting point, combining these two operations in a linear Fourier filter. It may apply in 2D or 3D and requires merely estimates of the Signal-to-Noise Ratio SNR2 as well as the system Modulation Transfer Function (MTF). Meanwhile, any linear filter is unable to adapt to local contrast variations in the images. Therefore, convolutional neural networks (CNN) such as MSDnet or UNet can significantly improve reconstructions from low-dose CT scans thanks to their non-linear nature. The Noise2Inverse framework allows for training these CNN using a split-and-merge of two subsets generated from one raw CT dataset. This study investigates denoising by N2I with respect to the input data quality, the CNN network architecture and the fidelity of the features in the resulting denoised volume images. Unlike Wiener filtering, N2I is far more effective in removing pixel noise. Yet, these models give the vague impression that they might generate ghosts of small features (pores or spots) in the object. Image quality metrics like Fourier Shell Correlation and SNR2 power spectra show clear improvement. In particular, Noise2Inverse preserves the signal power spectrum of all scans reliably. Nevertheless, locally inspecting image features must remain a core technique when the CNN models are applied, i.e. for industrial inspection.



(a) A schematic structure of the detector with the coated scintillators. (b) The simulated detected spectra with a 5 mm Sapphire and 89.5 mm glassy Carbon at $2\,\mathrm {m}$ and $29.7\,\mathrm {m}$ ODD with air absorption [21]. The $2\,\mathrm {m}$ ODD had additional a 45 mm glassy Carbon filter.
Top: transmission images of the MTF phantom ( $2\,\mathrm {LP}/\mathrm {mm}$ bar pattern) at $2\,\mathrm {m}$ (a) and $29.7\,\mathrm {m}$ (b) ODD for reflective coating. (c): Line plots of the transmission images of the MTF phantom. (d): The Fourier transforms of the line plots of no coating, black and reflective coating multiplied by the frequency at $2\,\mathrm {m}$ ODD. The envelope was fitted to the expected MTF as Voigt profile.
Top: transmission images of the $\mathrm {SNR^2}$ phantom (a $4\,\mathrm {mm}$ pouch of copper flakes) at $2\,\mathrm {m}$ (a) and $29.7\,\mathrm {m}$ (b) object-detector distance and reflective coating. The red bar in the images corner measures $5\,\mathrm {mm}$ . (c) $\mathrm {SNR^2}$ power spectra of the three different coatings and two detector positions. The inset showing the ratio of power spectra amplitudes of black and reflective coatings with respect to the uncoated scintillator.
Axial slices of the CT measurements on an electric motor at $2\,\mathrm {m}$ and $29.7\,\mathrm {m}$ ODD for the three coatings. The columns are the different coatings and the rows are different ODD and their magnified image patches. The patch in the first frame indicates the position, where the zoom is performed. The images of the scans at $2\,\mathrm {m}$ distance were reconstructed with NABU and the $29.7\,\mathrm {m}$ was obtained from two-step Paganin-type with Pyxit. An additional set of zoom images shows the result of applying a two-step Paganin and Wiener-deconvolution to the attenuation contrasted scans taken at $2\,\mathrm {m}$ distance. Parameter for the two-step Paganin were scaled and for Wiener-deconvolution were the same as for the $29.7\,\mathrm {m}$ scans. In third left frame two small patches indicate $\mathrm {CNR^2}$ measures which were calculated for evaluating the contrast between plastic and air.
Shown are the Fourier transform of $2\,\mathrm {m}$ distance without Coating and $29.7\,\mathrm {m}$ distance from no coating, black and reflective coating. Even harmonics are only seen in phase contrasted spectra whereas the attenuation contrast only displays odd harmonics.
Benefits of front coating crystalline scintillator screens for phase-contrast synchrotron micro-tomography

October 2024

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29 Reads

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1 Citation

Transparent crystalline scintillators such as cerium-doped YAG or LuAG are widely used in X-ray imaging for the indirect detection of X-rays. The application of reflective coatings on the front side to improve the optical gain is common practice for flat panel detectors with CsI or Gd2O2S powder scintillators but still largely unknown for crystalline scintillators such as LuAG. This work shows experimentally and quantitatively how a black and reflective coating on the X-ray side of a 2 mm LuAG:Ce scintillator improves the image quality compared to a 2 mm LuAG:Ce scintillator without a coating. The measurements have been done for two different distances, with 2 m and 29.7 m on the BM18 beamline of the European Synchrotron. The Modulation Transfer Function (MTF) and the Signal-to-Noise-Ratio (SNR²) power spectrum as well as contrast-to-noise ratio are used for comparing image quality. Propagation-based phase contrast strongly enhances the SNR² amplitudes (gain ≈10 from 2 m to 29.7 m object-detector distance) of the raw images’ spectrum independent of the scintillator coating. For both detector positions, the reflective coating is able to raise SNR² by up to 80% through the improved optical gain, while black coating does the opposite (decrease SNR² by 20%) with respect to no coating. With the tested optical setups, changes in MTF /sharpness between the coatings are minor. Comparing CNR² in CT scans of a multi-material sample, in this case an electric motor, we observe the reflective coating yielding better material contrast for plastic and air. Application and effect of Wiener-deconvolution, along with Paganin-type phase retrieval, are also discussed in the context of CT image quality.



Schematic figure of conical connection with a short mating zone (mating zone: orange circle) and butt-joint connection with a slightly angulated platform before (a) and after load application (b). The antirotational indices are encircled in green color. Red lines demonstrate lateral force transmission on the implant wall in conical connections and vertical distribution in butt-joint connections. Butt-joint connections with an adequate preload of the abutment screw distribute the force more vertically into the implant shoulder
Microgap formation assessed using synchrotron radiography and phase-contrast radioscopy at upper (UL) and lower left abutment edge (LL) for different static load applications applied from left to right. Mounting force and loading angle induce increased microgaps at upper left abutment edge. (left radiographic image displays a MS implant as an example; I: Implant; A: Abutment; AS: Abutment screw)
Microgap formation at upper (UR) and lower right abutment edge (LR) for different static load applications. All implant systems showed decreasing microgaps under incremental loading at upper right abutment edge (UR). (left radiographic image displays a MS implant as an example; I: Implant; A: Abutment; AS: Abutment screw)
Synchrotron-based microtomography of microgap formation in MA implant. (I: Implant; A: Abutment; AS: Abutment screw); a: Even after force release a large microgap remains on the application side of the IAC. The azimuthal extension of the gap can be observed from horizontal micro-tomography slices (level of the slice is indicated by horizontal white line in the left hand tile, the diagonal white line in the right hand tile indicates the direction of previous load application) The side of application displays a sickle-shaped microgap (box in the right hand tile); b: Additional observation from radiography: off-axis loading leads to tilting abutment movement inside IAC and slight lateral implant wall deformation visible at right white positioning line
Phase-contrast radiographies of BE butt-joint connection prior to loading (a) and at force application of 30 N at 90° (b), 100 N at 90° (c) and 200 N at 30° (d) from the left side. Abutment displacement leads to almost parallel gap formation. Despite large microgaps (up to 40.5 μm) no implant wall deformation is visible on the opposing side indicated by transparent vertical positioning lines
In vitro assessment of internal implant-abutment connections with different cone angles under static loading using synchrotron-based radiation

March 2024

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262 Reads

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1 Citation

BMC Oral Health

Background The stability of implant-abutment connection is crucial to minimize mechanical and biological complications. Therefore, an assessment of the microgap behavior and abutment displacement in different implant-abutment designs was performed. Methods Four implant systems were tested, three with a conical implant-abutment connection based on friction fit and a cone angle < 12 ° (Medentika, Medentis, NobelActive) and a system with an angulated connection (< 40°) (Semados). In different static loading conditions (30 N − 90º, 100 N − 90º, 200 N − 30º) the microgap and abutment displacement was evaluated using synchrotron-based microtomography and phase-contrast radioscopy with numerical forward simulation of the optical Fresnel propagation yielding an accuracy down to 0.1 μm. Results Microgaps were present in all implant systems prior to loading (0.15–9 μm). Values increased with mounting force and angle up to 40.5 μm at an off axis loading of 100 N in a 90° angle. Conclusions In contrast to the implant-abutment connection with a large cone angle (45°), the conical connections based on a friction fit (small cone angles with < 12°) demonstrated an abutment displacement which resulted in a deformation of the outer implant wall. The design of the implant-abutment connection seems to be crucial for the force distribution on the implant wall which might influence peri-implant bone stability.


Development of an Algorithm for Correct Placement of the Basal Electrode Contact in the Context of Anatomy-Based Cochlear Implantation: A Proof of Concept

March 2024

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34 Reads

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2 Citations

Audiology and Neurotology

Background: Correct individual tonotopic frequency stimulation of the cochlea plays an important role in the further development of anatomy based cochlear implantation. In this context frequency specific fitting of the basal electrode contact with a normal insertion depth can be difficult since it is often placed in a frequency range higher than 10 kHz and current audio processors only stimulate for frequencies up to 8.5 kHz due to microphone characteristics. This results in a mismatch of the high frequencies. Therefore, this study represents a proof of concept for a tonotopic correct insertion and aims to develop an algorithm for a placement of the basal electrode below 8.5 kHz in an experimental setting. Methods: Pre- and postoperative flat-panel volume CT scans with secondary reconstructions were performed in 10 human temporal bone specimens. The desired frequency location for the most basal electrode contact was set at 8.25 kHz. The distance from the round window to the position where the basal electrode contact was intended to be located was calculated preoperatively using 3D-curved multiplanar reconstruction and a newly developed mathematical approach. A specially designed cochlear implant electrode array with customized markers imprinted on the silicone of the electrode array was inserted in all specimens based on the individually calculated insertion depths. All postoperative measurements were additionally validated using an otological planning software. Results: Positioning of the basal electrode contact was reached with only a small mean deviation of 37 ± 399 Hz and 0.06 ± 0.37 mm from the planned frequency of 8.25 kHz. The mean rotation angle up to the basal electrode contact was 51 ± 5 °. In addition, the inserted electrode array adequately covered the apical regions of the cochleae. Conclusion: Using this algorithm, it was possible to position the basal electrode array contact in an area of the cochlea that could be correctly stimulated by the existing speech processors in the context of tonotopic correct fitting.


Identification of timbers in charcoal and substitutes based on NTFPs (Non-Timber-Forest-Products) and residues

March 2024

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46 Reads

For about a decade, the Thünen Institute of Wood Research has been analyzing wood species in charcoal and briquettes. The anatomical analyses can be used to check whether the species declarations of the product samples are correct. In addition, the origin information on the distribution areas of the specific taxa can be scrutinized (e.g., tropical vs. non-tropical). The investigations make an important contribution to quality assurance for the producers and traders of the products, and also serve to protect consumers. In the context of the studies, it has been observed that more raw and residual materials, such as non-timber forest products (NTFPs), are becoming established on the charcoal substitutes market. Anatomical studies are currently being carried out to characterize the structure of important NTFPs, such as coconut shells, olive or mango kernels, in order to describe them and reliably identify them using 3D-Refelcted-Light- Microscopy (3D-RLM) and nano-CT in practical applications for market analyses


Citations (44)


... To adjust the sample grating magnification while preserving the projected beamlet positions, a sample grating which retains the projected aperture period over a continuous range of magnifications is required, which is non-existent to our knowledge. Furthermore, while multi-resolution imaging is being thoroughly researched in various XPC techniques (edge illumination, grating based interferometry, propagation-based imaging,. . . ) [26][27][28][29], there is no laboratory XPC setup that allows to change the resolution over a continuous range of resolutions. Fig. 2. The misaligned gratings and detector that occurs when the sample grating and the object are positioned closer to the source. ...

Reference:

Gratings for multi-resolution edge illumination X-ray phase contrast imaging: concept and simulation
Multiresolution Phase-Contrast Tomography on BM18, a New Beamline at the European Synchrotron Radiation Facility
  • Citing Article
  • November 2024

Synchrotron Radiation News

... The screen's front facing the X-rays is covered by 100-150 nm aluminium (reflective coating) applied with physical vapour deposition (PVD), topped by 80-100 nm SiO 2 (protective research papers layer) applied by EB-PVD. Aluminium shows a reflectance >90% at 535 nm wavelength; we recently reported a significant benefit in terms of SNR with respect to uncoated screens (Diez et al., 2024). The lens projects the X-ray images from the screen onto an IRIS-15 sCMOS camera by Photometrics (Crytur, https://www.photometrics.com/products/iris-family/ ...

Benefits of front coating crystalline scintillator screens for phase-contrast synchrotron micro-tomography

... spatial resolution, thus offering information about features that are otherwise undetectable in attenuation or phase images. Numerous studies highlight the broad applicability of these three contrast channels across different fields [2,3,4,5,6,7,8,9]. Several multimodal experimental techniques have been developed to recover attenuation, phase, and dark-field images, each offering specific advantages and limitations. ...

A comparison of X-ray attenuation, differential phase, and dark-field contrast imaging for the detection of porosity in carbon fiber reinforced cyanate ester

NDT & E International

... The microgap behavior and abutment displacement were assessed with a MicroTC analysis (Figure 1, 2). [14][15][16] Dental implants were placed only in later-posterior sectors, and the dimensions used are shown in Table 1. ...

In vitro assessment of internal implant-abutment connections with different cone angles under static loading using synchrotron-based radiation

BMC Oral Health

... This is also seen in the semitones evaluation: High frequencies should be perceived about 3 semitones higher, very low frequencies about 3 semitones lower in the postopABF. This is also in line with the results from a previous study, saying that frequency specific fitting of the basal electrode contact can be difficult with a normal insertion depth as it is often placed in a higher frequency range [10]. Regarding perioperative troubles like tinnitus and dizziness, we could not find a significant difference between preoperative and postoperative results. ...

Development of an Algorithm for Correct Placement of the Basal Electrode Contact in the Context of Anatomy-Based Cochlear Implantation: A Proof of Concept
  • Citing Article
  • March 2024

Audiology and Neurotology

... In principle, however, one major advantage of the semimanual 3P-technique is its generalizability since the three landmarks used in this study should be easily identifiable in high-resolution MR or CT sequences, independent of vendor or sequence characteristics. Future developments could include automatic landmark selection, for example, using deep learning 56 . ...

Towards fully automated inner ear analysis with deep-learning-based joint segmentation and landmark detection framework

... CT image contrast is based on the attenuation of X-rays, which depends on the X-ray energy as well as the chemical composition and density of scanned objects. In particular, CT is very suitable for correlative microscopy and imaging time-dependent processes thanks to its non-destructive nature [39][40][41]. Nowadays, CT has gained wide applications in many different fields, for example, as an advanced diagnosis method in medicine and an inspection method for material failure or damage [42][43][44][45]. Moreover, CT can be used for metrology or quality assurance in materials processing [46]. ...

Correlative microscopy using SEM based nano-CT
  • Citing Conference Paper
  • October 2023

... . In einer aktuellen Studie befassen sich Wissenschaftler des Thünen-Instituts für Holzforschung mit der Verwendung hochauflösender volumetrischer Bilder auf der Basis von sub-µCt. Das Potenzial der µ-CT-Technologie7,8 wird derzeit für eine Vielzahl von Anwendungen 5, 6 erforscht, und es wird untersucht, inwieweit dreidimensionale Darstellungen im Bereich der künstlichen Intelligenz verwendet werden können. Während die jüngsten Entwicklungen im Bereich der Holzanatomie sehr vielversprechend sind, wurde auf der Konferenz auch die Anwendung anderer wissenschaftlicher Techniken zur Identifizierung von Arten, geografischen Merkmalen und sogar von Individuen (stabile Isotope, Genomanalyse und Elementprofilierung) vorgestellt. ...

Applications in the scope of anatomical wood identification using sub-µCt based volumetric images IAWA-IUFRO Symposium -Session Title: 21 -Promoting Data-Driven Methods for Species and Origin Identification of Forest Products.

... CT image contrast is based on the attenuation of X-rays, which depends on the X-ray energy as well as the chemical composition and density of scanned objects. In particular, CT is very suitable for correlative microscopy and imaging time-dependent processes thanks to its non-destructive nature [39][40][41]. Nowadays, CT has gained wide applications in many different fields, for example, as an advanced diagnosis method in medicine and an inspection method for material failure or damage [42][43][44][45]. Moreover, CT can be used for metrology or quality assurance in materials processing [46]. ...

Three-dimensional imaging of microstructural evolution in SEM-based nano-CT
  • Citing Article
  • June 2023

Tomography of Materials and Structures

... Elastic gaps can be described as an intermittent passageway between the contacting surfaces, provoking the exchange of biological content between the IAC and the surrounding tissues. 11,63 Masticatory loads are influenced by different factors. [64][65][66][67][68][69][70][71] Occlusal forces vary depending on age, sex, the measurement method and devices, dentition characteristics, cranioencephalic morphology, zone of the dental arch, and buccal aperture. ...

Evaluation of Implant Body Diameter, Platform Diameter, and the Use of a Transepithelial Component on Implant-Abutment Connection Microgap: An In Vitro Study with In Situ Hard X-Ray Radiography
  • Citing Article
  • May 2023

The International journal of oral & maxillofacial implants