Abstract:We propose an encryption–decryption framework for validating diffraction intensity volumes reconstructed using single-particle imaging (SPI) with X-ray free-electron lasers (XFELs) when the ground truth volume is absent. This conceptual framework exploits each reconstructed volumes’ ability to decipher latent variables (e.g. orientations) of unseen sentinel diffraction patterns. Using this framework, we quantify novel measures of orientation disconcurrence, inconsistency, and disagreement between the decryptio… Show more
“…The angular correlation map was obtained by calculating the cross-correlation between the orientation posterior probability distributions of 2D diffraction. The rotational cross-correlation ξ rot iswhere Ω, K , and W are the 3D rotation, 2D diffraction pattern, and 3D model, respectively, and Ω′ is the relative 3D rotation in the cross-correlation . The angular correlation ξ ang (θ| K , W ) is then obtained by summing the correlation values of 3D rotations with the same angle of rotation.…”
Section: Methods and Experimentalmentioning
confidence: 99%
“…where Ω, K, and W are the 3D rotation, 2D diffraction pattern, and 3D model, respectively, and Ω′ is the relative 3D rotation in the crosscorrelation. 54 The angular correlation ξ ang (θ|K, W) is then obtained by summing the correlation values of 3D rotations with the same angle of rotation. An n-fold rotational symmetry results in high crosscorrelation at rotation angles of 2π/n, and these peaks are prominent for the majority of patterns for each 3D volume (Figure S4).…”
The structures, as building-blocks for designing functional nanomaterials, have fueled the development of versatile nanoprobes to understand local structures of noncrystalline specimens. Progresses in analyzing structures of individual specimens with atomic scale accuracy have been notable recently. In 2 most cases, however, only a limited number of specimens are inspected lacking statistics to represent the systems with structural inhomogeneity. Here, by employing single-particle imaging with X-ray free electron lasers and new algorithm for multiple-model 3D imaging, we succeeded in investigating several thousand specimens in a couple of hours, and identified intrinsic heterogeneities with 3D structures. Quantitative analysis has unveiled 3D morphology, facet indices and elastic strains. The 3D elastic energy distribution is further corroborated by molecular dynamics simulations to gain mechanical insight at atomic level. This work establishes a new route to high-throughput characterization of individual specimens in large ensembles, hence overcoming statistical deficiency while providing quantitative information at the nanoscale.Materials' functions are contingent on their structural properties 1,2 . This contingency has spurred the research on functional nanomaterials by designing structures that accommodate desired functions 3 . In this capacity, high-resolution structural probes are critical for detecting emergent functional properties induced by local structural motifs [4][5][6] . Detecting these motifs requires local structural characterization to image large numbers of specimens or large regions. Examples include reaction kinetics from in situ characterization and catalytic function of nanocrystals from 3D mapping of elastic strains, where such local probes using electrons or X-rays allow us to discover and study structure-function relations [6][7][8][9][10][11][12][13][14] .However, most of these local 3D probes only operate in a low-sampling mode requiring days of measurement time for each specimen. As such, inspecting only a few specimens makes it difficult to understand the whole system with statistical confidence. Such limited measurements can be a critical shortcoming, as the intrinsic structural aerosol particles in flight. Nature 486, 513-517 (2012). Liu, W.-L. et al. The influence of shell thickness of Au@TiO2 core-shell nanoparticles on the plasmonic enhancement effect in dye-sensitized solar cells.
“…The angular correlation map was obtained by calculating the cross-correlation between the orientation posterior probability distributions of 2D diffraction. The rotational cross-correlation ξ rot iswhere Ω, K , and W are the 3D rotation, 2D diffraction pattern, and 3D model, respectively, and Ω′ is the relative 3D rotation in the cross-correlation . The angular correlation ξ ang (θ| K , W ) is then obtained by summing the correlation values of 3D rotations with the same angle of rotation.…”
Section: Methods and Experimentalmentioning
confidence: 99%
“…where Ω, K, and W are the 3D rotation, 2D diffraction pattern, and 3D model, respectively, and Ω′ is the relative 3D rotation in the crosscorrelation. 54 The angular correlation ξ ang (θ|K, W) is then obtained by summing the correlation values of 3D rotations with the same angle of rotation. An n-fold rotational symmetry results in high crosscorrelation at rotation angles of 2π/n, and these peaks are prominent for the majority of patterns for each 3D volume (Figure S4).…”
The structures, as building-blocks for designing functional nanomaterials, have fueled the development of versatile nanoprobes to understand local structures of noncrystalline specimens. Progresses in analyzing structures of individual specimens with atomic scale accuracy have been notable recently. In 2 most cases, however, only a limited number of specimens are inspected lacking statistics to represent the systems with structural inhomogeneity. Here, by employing single-particle imaging with X-ray free electron lasers and new algorithm for multiple-model 3D imaging, we succeeded in investigating several thousand specimens in a couple of hours, and identified intrinsic heterogeneities with 3D structures. Quantitative analysis has unveiled 3D morphology, facet indices and elastic strains. The 3D elastic energy distribution is further corroborated by molecular dynamics simulations to gain mechanical insight at atomic level. This work establishes a new route to high-throughput characterization of individual specimens in large ensembles, hence overcoming statistical deficiency while providing quantitative information at the nanoscale.Materials' functions are contingent on their structural properties 1,2 . This contingency has spurred the research on functional nanomaterials by designing structures that accommodate desired functions 3 . In this capacity, high-resolution structural probes are critical for detecting emergent functional properties induced by local structural motifs [4][5][6] . Detecting these motifs requires local structural characterization to image large numbers of specimens or large regions. Examples include reaction kinetics from in situ characterization and catalytic function of nanocrystals from 3D mapping of elastic strains, where such local probes using electrons or X-rays allow us to discover and study structure-function relations [6][7][8][9][10][11][12][13][14] .However, most of these local 3D probes only operate in a low-sampling mode requiring days of measurement time for each specimen. As such, inspecting only a few specimens makes it difficult to understand the whole system with statistical confidence. Such limited measurements can be a critical shortcoming, as the intrinsic structural aerosol particles in flight. Nature 486, 513-517 (2012). Liu, W.-L. et al. The influence of shell thickness of Au@TiO2 core-shell nanoparticles on the plasmonic enhancement effect in dye-sensitized solar cells.
“…This and some other methods (Yoon et al, 2016;Liu et al, 2018) rely on dividing the measured dataset into two or more parts and compare the independently recovered intensity distributions. However, Shen et al (2021) have shown that these methods suffer from serious problems. Most notably, the correlation can grow with increasing orientation disorder when approaching the powder average.…”
Section: Figurementioning
confidence: 99%
“…We can investigate the loss off resolution by calculating the FSC between the 3D intensity volume W reconstructed by either method and the ideally reconstructed intensity W T or the noiseless 3D model intensity distribution W 0 . We noted earlier that FSC, calculated between volumes reconstructed from two independent sets of measured data, suffers serious problems when used for characterization of the resolution errors (Shen et al, 2021). However, when FSC is calculated between a measured intensity volume W and model intensities W 0 with no errors or W T with well known errors (Poisson noise and interpolation The maximums of Pearson correlation between intensity volumes W x and W y as rotated relative to each other, for lysozyme (right) and RNA polymerase II (left) at various incident XFEL fluence values.…”
In single-particle imaging (SPI) experiments, diffraction patterns of identical particles are recorded. The particles are injected into the X-ray free-electron laser (XFEL) beam in random orientations. The crucial step of the data processing of SPI is finding the orientations of the recorded diffraction patterns in reciprocal space and reconstructing the 3D intensity distribution. Here, two orientation methods are compared: the expansion maximization compression (EMC) algorithm and the correlation maximization (CM) algorithm. To investigate the efficiency, reliability and accuracy of the methods at various XFEL pulse fluences, simulated diffraction patterns of biological molecules are used.
“…There is obviously a need to develop secure image methods in order to assure the safety of image transmission [1][2][3][4][5]. As a result, a secure method for encryption and decryption of digital images, well-known as cryptography, is developed thanks to the development of digital communication [6,7].…”
As the demand for secure digital data continues to increase, image encryption and decryption have recently received tremendous attention. The rapid development of ultrathin metasurfaces has mainly been driven by the desire for the introduction of novel methods with which electromagnetic waves can be manipulated. As a promising application of metasurfaces, metalenses have shown great potential to replace bulky traditional optical devices. In this work, we present that the images produced by a commercially available projector are encrypted by using the color superposition principle, and the fabricated metalens is subsequently utilized to perform image decryption with an incidence made of white light-emitting diodes (LEDs). The correct positions for image decryption are carefully found by three distinct diode lasers as incident light sources. Recent investigations show that high-performance metalenses can be successfully developed once the suitable dielectric material is chosen. As a consequence, our metalens of high performance is composed of hexagon-resonated elements (HREs) made of gallium nitride (GaN) and is capable of resolving line width as small as 870 nm. The metalens with a smaller diameter of 8 μm is numerically simulated with a diffraction-limited focusing efficiency as high as 92%. This work once again shows that GaN metalenses, as future optics, have great prospects in expanding widespread applications in the near future.
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.