Michael Henrichsen’s research while affiliated with Fraunhofer Institute of Optronics, System Technologies and Image Exploitation and other places

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Publications (18)


Laser Protection via Jointly Learned Defocus and Image Reconstruction
  • Preprint

January 2025

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3 Reads

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Michael Henrichsen

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Christian Kludt






Schematic presentation of the side view of a bistatic configuration of a laser source $L$ L and an observer $B$ B . The laser source generates at height ( ${h_L}$ h L ) a laser beam with declination angle ( ${\theta _L}$ θ L ), zenith angle ( ${\theta _s}$ θ s ), and azimuth angle ( ${\phi _s} = {0}$ ϕ s = 0 ), respectively, and distance ( ${R_{\textit{LZ}}}$ R LZ ) between the source and the water surface. This produces an elliptical laser spot along the optical axis on the mean surface plane. Point $Z$ Z describes the center of the laser spot. The reflected laser power is collected by an observer aperture, which has a distance ( ${R_{\textit{ZB}}}$ R ZB ) to the laser spot center, zenith angle ( ${\theta _r}$ θ r ), and azimuth angle ( ${\phi _r}$ ϕ r ).
Schematic presentation of the side view of a bistatic configuration of laser source $L$ L and observer $B$ B . The laser intensity incident on the water surface is characterized by the ratio ( ${P_i}/{A_L}$ P i / A L ) of emitted laser power ${P_i}$ P i to the area ${A_L}$ A L , which is illuminated by the incident laser beam.
Schematic presentation of the side view of a bistatic configuration of laser source $L$ L and observer $B$ B . Laser light is reflected into the solid angle ${\Omega _D}$ Ω D of the observer.
True-to-scale representation of the time-averaged received intensities ${I_r}$ I r displayed on the observer hemisphere for an air-incident laser beam focused on a circular spot with a diameter of about 5 cm before being projected onto the water surface. The laser spot center on the water surface is located at the coordinate origin. The laser source has the position (0 m, ${-}{500}\;{\rm m}$ − 500 m , 16 m). It is located in a “dark” (radiation-free) sky. The unit of the right scale is in ${\rm W}/{{\rm m}^2}$ W / m 2 . On the left is shown the enlarged portion of the intensity distribution with the pattern of the quads.
True-to-scale representation of the time-averaged received intensity ${I_r}$ I r with hazard area ( ${I_r}\; \gt \;{I_{\rm{MPE}}}$ I r > I M P E ) displayed on the observer hemisphere having the same position of the laser source (0 m, ${-}{500}\;{\rm m}$ − 500 m , 16 m) as in Fig. 4.

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Simulation of the reflection of a high energy laser beam at the sea surface for hazard and risk analyses
  • Article
  • Publisher preview available

May 2024

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42 Reads

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1 Citation

The application of a high energy laser beam in a maritime scenario necessitates a laser safety concept to prevent injury to personnel or uninvolved third parties from uncontrolled reflections of laser light from the sea surface. Therefore, it is crucial to have knowledge of the amount and direction of reflected laser energy, which varies statistically and depends largely on the dynamics of the wavy sea surface. These dynamics are primarily influenced by wind speed, wind direction, and fetch. An analytical model is presented for calculating the time-averaged spatial intensity distribution of the laser beam reflected at the dynamic sea surface. The model also identifies the hazard areas inside which laser intensities exceed a fixed exposure limit. Furthermore, as far as we know, our model is unique in its ability to calculate the probabilities of potentially eye-damaging glints for arbitrary observer positions, taking into account the slope statistics of gravity waves. This is a critical first step toward an extensive risk analysis. The simulation results are presented on a hemisphere of observer positions with fixed radii from the laser spot center. The advantage of the analytical model over our numeric (dynamic) model is its fast computation time. A comparison of the results of our new analytical model with those of the previous numerical model is presented.

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Fig. 5 Estimated marginal means of frontal asymmetry index (y scale) and frontal alpha power (x scale) collapsed over all fixed factors except the measurement moments, for all participants. Error bars stand for 95% confidence intervals. Symbols shown in the legend represent the measurement moments.
Fig. 6 Estimated marginal means of frontal asymmetry index (y scale) and frontal alpha power (x scale) at 11-deg dazzling angle and 25% target contrast for the three different ballistic goggles at the three measurement moments for all participants. Error bars stand for 95% confidence intervals. Symbols shown in the legend represent the measurement moments, and the colors stand for the different goggles.
Dazzling angles of the projected targets in chronological order during the 2021 campaign trials. The high-contrast target projection was used for all shots.
Dazzling angles and contrast levels of the projected targets during the preliminary 2022 trial, presented in chronological order for each set of goggles.
Investigating the impact of laser dazzling on shooting performance in a simulator environment: baseline scene

March 2024

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89 Reads

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1 Citation

Optical Engineering

Our study examines how laser dazzling affects human performance, specifically accuracy and reaction times, using a laser dazzling shooting simulator at the Royal Military Academy, Belgium. The research assesses the performance degradation under laser dazzling in a simple, baseline scene, including different target contrasts and the use of laser eye protection. Utilizing a 532 nm green laser for a safe yet effective dazzle, trained shooters’ performances were measured and analyzed. The results align strongly with a live shooting trial and correlate with Adrian/CIE visibility levels. Additionally, electrical brain activity data, acquired via electro-encephalography (EEG), provided insights into the shooters’ mental states. EEG-derived metrics, particularly frontal alpha asymmetry and frontal alpha power, revealed that participants experienced heightened negative and avoidance emotions, coupled with increased cognitive load prior to shooting. These responses returned to baseline levels postshooting. Moreover, distinct cognitive and emotional states were observed in relation to different types of laser eye protection goggles, potentially correlating with variations in shooting performance. These findings pave the way for future research with more advanced simulation scenes and deepen understanding of the effects of laser dazzle.


Fig. 1 Experimental setup for the investigation of the polymer perforation time
Fig. 3 Transmitted power over time for natural-colored PA 6.6
Investigation of the polymer material perforation time: comparison between two fiber laser wavelengths

February 2024

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57 Reads

Journal of Polymer Research

This study investigated the perforation time of polyamide 6.6 using fiber lasers at two different wavelengths: 1070 and 1943 nm. The novelty of this research lies in the comparison of perforation times at equivalent laser irradiances on the polymer sample with two different colors of polyamide 6.6: natural and black. The results revealed that, at comparable irradiance levels and beam diameters, the 1943 nm laser source perforated the polyamide 6.6 sample faster than the 1070 nm laser source. The difference in perforation time was found to be significantly higher for natural-colored polyamide 6.6 compared to black-colored polyamide 6.6. These findings suggest that, for material processing of polyamide 6.6, especially in terms of perforation, the use of 2 μm laser sources should be privileged over 1 μm laser sources.


Citations (4)


... Аpplication of LiDARs for detecting, recognizing, and tracking objects has recently expanded significantly. The most important characteristic for estimation of the target detection range is its laser radar cross section (LRCS) [1][2][3][4]. It depends on the geometric shape, reflective properties, and orientation of the object. ...

Reference:

Experimental Verification of Laser Radar Cross Section Model for Complex Targets with Gaussian Beam Irradiation
Investigations on the laser radar cross section of optical components
  • Citing Conference Paper
  • October 2023

... In the literature, these phenomena are discussed in terms of reflection caustics originating from dynamic surface processes on the molten metal [4]. A theoretical description of these phenomena and their significance for laser safety are already elaborated [4,27]. The reappearance of spikes in the present measurements is probably associated with molten edge regions on the sample that can contribute to a temporary increase in the scattering power (see Fig. 10). ...

Simulation of caustics caused by high-energy laser reflection from melting metallic targets adapted by a machine learning approach
  • Citing Conference Paper
  • November 2022

... In the military shooting training background, it was possible to find sixteen scientific publications ( [2], [8], [14], [15], [20], [24], [26], [30], [32], [38], [42], [43], [45], [47], [48], and [51]) in the last five years that address the application of virtual reality in this instructional activity (considering the Scopus and Web of Science (WoS) databases). Although there is this current discussion on the subject, the authors have not yet found any work that evaluates the application of a commercial Head-Mounted Display (HMD) in military pistol shooting training. ...

Simulating laser dazzling using augmented and virtual reality
  • Citing Conference Paper
  • September 2021

... Therefore, these possible health risks during free field usage must be quantified. The reflections from the target materials can evoke Nominal Ocular Hazard Distances (NOHD) amounting from meters up to several kilometers, depending on the material properties and laser parameters [13,33,34]. This can cause permanent eye and skin damage, as well as injury to operators [33]. ...

Laser safety assessments supported by analyses of reflections from metallic targets irradiated by high-power laser light