Ptychography is a powerful computational imaging technique that reconstructs both the complex object function and the illumination probe from overlapping diffraction patterns. While it provides high-resolution, aberration-corrected imaging, its reliance on stepwise mechanical scanning limits acquisition speed. In this work, we propose a fly-scan ptychographic approach that enables continuous sample translation along arbitrary trajectories, significantly reducing measurement time. To account for motion-induced decoherence, we incorporate an object mode decomposition model combined with automatic differentiation for accurate trajectory correction. This method enables diffraction-limited reconstructions without the need for high-speed tracking, allowing fast and precise measurements using standard ptychographic setups.

Extreme ultraviolet pulses as generated by high harmonic generation (HHG) are a powerful tool for both time-resolved spectroscopy and coherent diffractive imaging. However, the combination of these techniques to achieve spatio-spectro-temporal data remains hardly explored due to the challenging and time-consuming data acquisition. Here, we present Fourier-transform spectroscopic holography (FTSH), an interferometric approach to spectroscopic imaging that combines Fourier-transform spectroscopy with holography. By encoding spectral information in the measured diffraction pattern, FTSH dramatically reduces the sampling requirements by one order of magnitude. This enables us to record full spectroscopic imaging data in less than 2 minutes, and makes FTSH especially promising for femtosecond time-resolved nano-spectroscopy using table-top HHG sources.

Ultrafast optical pump-probe spectroscopy is a powerful tool to study dynamics in solid materials on femto- and picosecond timescales. In such experiments, a pump pulse induces dynamics inside a sample by impulsive light-matter interaction, which can be detected using a time-delayed probe pulse. In addition to the desired dynamics, the initial interaction may also lead to unwanted effects that can result in irreversible changes and even damage. Therefore, the achievable signal strength is often limited by the pumping conditions that a sample can sustain. Here we investigate the optimization of ultrafast photoacoustics in various solid thin films. We perform systematic experiments aimed at maximizing the achievable signal-to-noise ratio (SNR) in a given measurement time while limiting sample damage. By varying pump and probe pulse energies, average pump fluence, and repetition rate, we identify different paths towards optimal SNR depending on material properties. Our results provide a strategy for the design of pump-probe experiments, to optimize achievable SNR for samples in which different damage mechanisms may dominate.

Lensless imaging techniques have been developed to visualize objects with high robustness and unprecedented resolution. Lensless imaging is based on the numerical reconstruction of the transmission or reflection function of a sample from optical diffraction measurements. Specifically, coherent diffractive imaging (CDI) and ptychography involve an iterative process of numerical propagation of coherent light waves between the sample and detector plane. However, in the standard propagation models, the pixel size of the reconstructed object image is typically fixed and wavelength-dependent, which limits CDI and broadband ptychography. Here we investigate three propagation models for far-field propagation that allow user-defined pixel size at the object plane. These propagators are the two-step Fresnel, scaled angular spectrum, and chirp-Z transform. We derive their analytical expressions and observe that all three models are mathematically equivalent, although they have a different physical origin. Each propagator can be written in two distinct versions, which conceptually represent propagation via different intermediate planes. We perform propagation simulations and ptychographic reconstructions on experimental data to compare the performance of these two different versions. We also investigate how sampling bandwidth requirements can affect the model accuracy due to physical errors associated with cropping of high spatial frequencies. Our results show that the choice of the intermediate plane can affect the reconstruction quality due to different sampling bandwidth requirements, which enables a wider choice of pixel sizes in the object plane. Our analysis provides guidelines for selecting an optimized object pixel size when performing reconstructions on broadband CDI and ptychography data.

Microscopy with table-top high-harmonic generation (HHG) sources enable high-resolution imaging with excellent material contrast, due to the short wavelength and numerous element-specific absorption edges available in this spectral range. However, accurate characterization of dispersive samples in terms of composition and thickness remains challenging due to the limitations of lens-based optics in this spectral range. Here, we performed spectrally resolved lensless imaging using multiple high harmonics. The diffractive shearing interferometry reconstruction serves as a foundational step for element-sensitive metrology, while ptychographic reconstruction enabled the retrieval of high-precision spectral imaging and quantitative thickness mapping. Our non-destructive method offers a powerful tool to extract both the material composition and layer thicknesses of complex nanostructured samples.

We present a maximum-likelihood estimation (MLE) framework tailored to event-driven detectors to perform computational image reconstruction and phase retrieval. Using Poissonian photon statistics, we built an event-based loss function that maximizes the probability of having the set of events and non-events given the initial parameters. Our loss function can be utilized in both optical and electron ptychography. We demonstrate experimental reconstructions using data acquired with a Timepix3 detector.

Ptychography is a computational imaging technique that enables the reconstruction of the amplitude and phase of an object and an illumination field using a series of recorded diffraction patterns [1]. Compared to conventional imaging techniques, ptychographic measurements offer more comprehensive information about the reconstructed object without requiring high-quality lenses, while also accommodating correction of experimental imperfections such as distance inaccuracies, angular misalignments, and other experimental errors. However, as ptychography is not a single-shot measurement technique, it is time-consuming, with a significant part of the measurement time attributed to the scanning process. Such mechanical scanning is inherently slow due to the acceleration limitations of the sample stage and the time required for stabilization [2].

The chemical and structural properties of a specimen can often be inferred by determining its complex refractive index. Ellipsometry is the standard method to measure the complex refractive index [1]. In ellipsometry, the complex refractive index is retrieved by acquiring absolute reflectivity changes for different states of the incident light (varying polarization or angle of incidence). While ellipsometry works well for bulk and thin-film specimens without transverse structure, imaging an object with spatially varying refractive index is difficult. Scanning ellipsometry uses a tightly focussed beam which requires accurate knowledge of the beam properties and more complex analysis. Furthermore, the signal is averaged over the spot size, limiting spatial resolution. Other implementations like imaging ellipsometry require an imaging setup with high-NA optics, which lead to measurement errors caused by aberrations and other defects. This becomes especially problematic when decreasing the wavelength in the extreme ultraviolet (EUV) regime, to improve spatial resolution.