Giorgio Tortarolo

Evaluating image resolution in stimulated emission depletion microscopy

Precise knowledge of the effective spatial resolution in a stimulated emission depletion (STED) microscopy experiment is essential for reliable interpretation of the imaging results. STED microscopy theoretically provides molecular resolution, but practically different factors limit its resolution. Because these factors are related to both the sample and the system, a reliable estimation of the resolution is not straightforward. Here we show a method based on the Fourier ring correlation (FRC), which estimates an absolute resolution value directly from any STED and, more in general, point-scanning microscopy image. The FRC-based resolution metric shows terrific sensitivity to the image signal-to-noise ratio, as well as to all sample and system dependent factors. We validated the method both on commercial and on custom-made microscopes. Since the FRC-based metric can be computed in real time, without any prior information of the system/sample, it can become a fundamental tool for (i)xa0microscopy users to optimize the experimental conditions and (ii)xa0microscopy specialists to optimize the system conditions.

Gated‐sted microscopy with subnanosecond pulsed fiber laser for reducing photobleaching

The spatial resolution of a stimulated emission depletion (STED) microscope is theoretically unlimited and practically determined by the signal‐to‐noise ratio. Typically, an increase of the STED beams power leads to an improvement of the effective resolution. However, this improvement may vanish because an increased STED beams power is often accompanied by an increased photobleaching, which worsen the effective resolution by reducing the signal strength. A way to lower the photobleaching in pulsed STED (P‐STED) implementations is to reduce the peak intensity lengthening the pulses duration (for a given average STED beams power). This also leads to a reduction of the fluorophores quenching, thus a reduction of the effective resolution, but the time‐gated detection was proved to be successful in recovering these reductions. Here we demonstrated that a subnanosecond fiber laser beam (pulse width ∼600 ps) reduces the photobleaching with respect to a traditional stretched hundreds picosecond (∼200 ps) beam provided by a Ti:Sapphire laser, without any effective spatial resolution lost.

Removal of anti-Stokes emission background in STED microscopy by FPGA-based synchronous detection

In stimulated emission depletion (STED) microscopy, the role of the STED beam is to de-excite, via stimulated emission, the fluorophores that have been previously excited by the excitation beam. This condition, together with specific beam intensity distributions, allows obtaining true sub-diffraction spatial resolution images. However, if the STED beam has a non-negligible probability to excite the fluorophores, a strong fluorescent background signal (anti-Stokes emission) reduces the effective resolution. For STED scanning microscopy, different synchronous detection methods have been proposed to remove this anti-Stokes emission background and recover the resolution. However, every method works only for a specific STED microscopy implementation. Here we present a user-friendly synchronous detection method compatible with any STED scanning microscope. It exploits a data acquisition (DAQ) card based on a field-programmable gate array (FPGA), which is progressively used in STED microscopy. In essence, the FPGA-based DAQ card synchronizes the fluorescent signal registration, the beam deflection, and the excitation beam interruption, providing a fully automatic pixel-by-pixel synchronous detection method. We validate the proposed method in both continuous wave and pulsed STED microscope systems.

Image formation in image scanning microscopy, including the case of two-photon excitation

The effect of combining the image scanning microscopy (ISM) technique with two-photon fluorescence microscopy is analyzed. The effective spatial frequency cutoff can be doubled, as compared with conventional two-photon fluorescence microscopy, and the magnitude of the optical transfer function near the cutoff of conventional two-photon microscopy is increased by orders of magnitude. For the two-photon case, it is found that the optimum pixel reassignment factor in ISM is not equal to one half, as is often assumed in single-photon fluoresence image scanning microscopy, because the excitation and detection point spread functions are different. The optimum reassignment factor depends on the noise level, and in general the useful cutoff spatial frequency is about 1.8 times that for conventional two-photon microscopy. The effect of altering the reassignment factor in single-photon fluorescence ISM with a Stokes shift is also investigated. Illumination using pupil filters, such as by a Bessel beam, is considered. Using a ring detector array is found to result in good imaging behavior, exhibiting a sharpening of the point spread function by a factor of 1.7 compared with conventional fluorescence. Image formation in ISM can be considered in a four-dimensional spatial frequency space, giving new insight into the imaging properties. This approach is related to phase space representations such as the Wigner distribution function and the ambiguity function. A noniterative algorithm for image restoration is proposed.

Photon-separation to enhance the spatial resolution in pulsed STED microscopy

Stimulated emission depletion microscopy (STED) is one of the pivotal super-resolution techniques. It overcomes the spatial resolution limit imposed by the diffraction by using an additional laser beam, the STED beam, whose intensity is directly related to the achievable resolution. Despite achieving nanometer resolution, much effort in recent years has been devoted to reduce the STED beam intensity because it may lead to photo-damaging effects. Exploring the temporal dynamics of the detected fluorescence photons and accessing the encoded spatial information has proven to be a powerful strategy, and has contributed to the separation by lifetime tuning (SPLIT) technique. The SPLIT technique uses the phasor analysis to efficiently distinguish photons emitted from the center and the periphery of the excitation spot. It thus improves the resolution without increasing the STED beam intensity. This method was proposed for architectures based on STED beam running in continuous wave (CW-STED microscopy). Here, we extend it to architectures based on pulsed STED beam (pSTED microscopy). We show, through simulated and experimental data, that the SPLIT-pSTED method reduces the detection volume of the pSTED microscope without significantly reducing the signal-to-noise ratio of the final image, thus effectively improving the resolution without increasing the STED beam intensity.

Image Scanning Microscopy with Single-Photon Detector Array

Image scanning microscopy (ISM) improves the spatial resolution of conventional confocal laser-scanning microscopy (CLSM), but current implementations reduce versatility and restrict its combination with fluorescence spectroscopy techniques, such as fluorescence lifetime. Here, we describe a natural design of ISM based on a fast single-photon detector array, which allows straightforward upgrade of an existing confocal microscope, without compromising any of its functionalities. In contrast to all-optical ISM implementations, our approach provides access to the raw scanned images, opening the way to adaptive reconstruction methods, capable of considering different imaging conditions and distortions. We demonstrate its utility in the context of fluorescence lifetime, deep, multicolor and live-cell imaging. This implementation will pave the way for a transparent and massive transition from conventional CLSM to ISM. confocal microscopy | time-resolved spectroscopy | image scanning microscopy | single-photon detector array

Image scanning microscopy (ISM) with a single photon avalanche diode (SPAD) array detector

If a scanning illumination spot is combined with a detector array, we acquire a 4 dimensional signal. Unlike confocal microscopy with a small pinhole, we detect all the light from the object, which is particularly important for fluorescence microscopy, when the signal is weak. The image signal is basically a cross-correlation, and is highly redundant. It has more than sufficient information to reconstruct an improved resolution image. A 2D image can be generated from the measured signal by pixel reassignment. The result is improved resolution and signal strength, the system being called image scanning microscopy. A variety of different signal processing techniques can be used to predict the reassignment and deconvolve the partial images. We use an innovative single-photon avalanche diode (SPAD) array detector of 25 detectors (arranged into a 5× 5 matrix). We can simultaneously acquire 25 partial images and process to calculate the final reconstruction online.

Improving multiphoton STED nanoscopy with separation of photons by LIfetime Tuning (SPLIT)

Stimulated emission depletion (STED) microscopy is a powerful bio-imaging technique since it provides molecular spatial resolution whilst preserving the most important assets of fluorescence microscopy. When combined with twophoton excitation (2PE) microscopy (2PE-STED), the sub-diffraction imaging ability of STED microscopy can be achieved also on thick biological samples. The most straightforward implementation of 2PE-STED microscopy is obtained by introducing a STED beam operating in continuous wave (CW) into a conventional Ti:Sapphire based 2PE microscope (2PE-CW-STED). In this implementation, an effective resolution enhancement is mainly obtained implementing a time-gated detection scheme, which however can drastically reduce the signal-to-noise/background ratio of the final image. Herein, we combine the lifetime tuning (SPLIT) approach with 2PE-CW-STED to overcome this limitation. The SPLIT approach is employed to discard fluorescence photons lacking super-resolution information, by means of a pixel-by-pixel phasor approach. Combining the SPLIT approach with image deconvolution further optimizes the signal-to-noise/background ratio.

Image scanning microscopy using a SPAD detector array (Conference Presentation)

The use of an array of detectors can help overcoming the traditional limitation of confocal microscopy: the compromise between signal and theoretical resolution. Each element independently records a view of the sample and the final image can be reconstructed by pixel reassignment or by inverse filtering (e.g. deconvolution). In this work, we used a SPAD array of 25 detectors specifically designed for this goal and our scanning microscopy control system (Carma) to acquire the partial images and to perform online image processing. Further work will be devoted to optimize the image reconstruction step and to improve the fill-factor of the detector.

A novel pulsed STED microscopy method using FastFLIM and the phasor plots

Stimulated emission depletion (STED) microscopy is a powerful super-resolution microscopy technique that enables observation of macromolecular complexes and sub-cellular structures with spatial resolution below the diffraction limit. The spatial resolution of STED is limited by power of the depletion laser at the specimen plane. Higher depletion laser power will improve resolution, but at the cost of increased photo-bleaching, photo-toxicity, and anti-stoke emission background. This degrades the signal-to-noise ratio, and can significantly limit STED applications in living specimens. Here, we present an efficient multi-color STED microscopy method based on the digital frequency domain fluorescence lifetime imaging (FastFLIM) and the phasor plots. Our approach utilizes a combination of pulsed excitation and pulsed depletion lasers to record the time-resolved photons by FastFLIM. We demonstrate that the resolution is improved without increasing the depletion laser power by digital separation of the depleted species from the partially depleted species based on their different decay kinetics. We show the utility of this novel STED method applied in both fixed and live cellular samples, and also show its application to fluorescence lifetime correlation spectroscopy (FLCS) measurements. By combining fluorophores with different fluorescence lifetimes, we simultaneously record two-color STED images of cells labeled with Atto655 and Alexa647 in a single scan by using a single pair of excitation and depletion lasers. This novel approach shortens the data acquisition time while minimizing the photo-toxicity caused when using two separate depletion lasers.