Self-diffusion and Cooperative Diffusion in Semidilute Polymer Solutions as measured by Fluorescence Correlation Spectroscopy

We present a comprehensive investigation of polymer diffusion in the semidilute regime by fluorescence correlation spectroscopy (FCS) and dynamic light scattering (DLS). Using single-labeled polystyrene chains, FCS leads to the self-diffusion coefficient while DLS gives the cooperative diffusion coefficient for exactly the same molecular weights and concentrations. Using FCS we observe a new fast mode in the semidilute entangled concentration regime beyond the slower mode which is due to self-diffusion. Comparison of FCS data with data obtained by DLS on the same polymers shows that the second mode observed in FCS is identical to the cooperative diffusion coefficient measured with DLS. An in-depth analysis and a comparison with current theoretical models demonstrates that the new cooperative mode observed in FCS is due to the effective long-range interaction of the chains through the transient entanglement network

Large area SiPM and high throughput timing electronics: toward new generation time-domain instruments

We present here a novel time-domain diffuse optical detection chain consisting of a large area Silicon PhotoMultipliers (SiPM) coupled to a high count-rate timing electronics (TimeHarp 260 PICO) to achieve sustainable count-rates up to 10 Mcps without significant distortions to the distribution of time-of-flight (DTOF). Thanks to the large area of the detector (9 mm2) and the possibility to directly place it in contact with the sample (thus achieving a numerical aperture close to unity), the photon collection efficiency of the proposed detection chain is almost two orders of magnitude higher than traditional fiber-mounted PMT-based systems. This allows the detection also of the few late photons coming from deeper layers at short acquisition times, thus improving the robustness of the detection of localized inhomogeneities. We then demonstrate that, despite the high dark count rate of the detector, it is possible to reliably extract the optical properties of calibrated phantoms, with proper linearity and accuracy. We also explore the capability of the new detection chain for detecting brain activations. This work opens up the possibility of ultimate performance in terms of high signal and photon throughput, with compact, low cost, relatively simple front-end electronics detector coupled to innovative timing electronics, with exciting opportunities to expand it to tomographic applications

Analyzing blinking effects in super resolution localization microscopy with single-photon SPAD imagers

For many scientific applications, electron multiplying charge coupled devices (EMCCDs) have been the sensor of choice because of their high quantum efficiency and built-in electron amplification. Lately, many researchers introduced scientific complementary metal-oxide semiconductor (sCMOS) imagers in their instrumentation, so as to take advantage of faster readout and the absence of excess noise. Alternatively, single-photon avalanche diode (SPAD) imagers can provide even faster frame rates and zero readout noise. SwissSPAD is a 1-bit 512×128 SPAD imager, one of the largest of its kind, featuring a frame duration of 6.4 μs. Additionally, a gating mechanism enables photosensitive windows as short as 5 ns with a skew better than 150 ps across the entire array. The SwissSPAD photon detection efficiency (PDE) uniformity is very high, thanks on one side to a photon-to-digital conversion and on the other to a reduced fraction of "hot pixels" or "screamers", which would pollute the image with noise. A low native fill factor was recovered to a large extent using a microlens array, leading to a maximum PDE increase of 12×. This enabled us to detect single fluorophores, as required by ground state depletion followed by individual molecule return imaging microscopy (GSDIM). We show the first super resolution results obtained with a SPAD imager, with an estimated localization uncertainty of 30 nm and resolution of 100 nm. The high time resolution of 6.4 μs can be utilized to explore the dye's photophysics or for dye optimization. We also present the methodology for the blinking analysis on experimental data