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91.
Turbulent flows in nature and technology possess a range of scales. The largest scales carry the memory of the physical system in which a flow is embedded. One challenge is to unravel the universal statistical properties that all turbulent flows share despite their different large-scale driving mechanisms or their particular flow geometries. In the present work, we study three turbulent flows of systematically increasing complexity. These are homogeneous and isotropic turbulence in a periodic box, turbulent shear flow between two parallel walls, and thermal convection in a closed cylindrical container. They are computed by highly resolved direct numerical simulations of the governing dynamical equations. We use these simulation data to establish two fundamental results: (i) at Reynolds numbers Re ∼ 102 the fluctuations of the velocity derivatives pass through a transition from nearly Gaussian (or slightly sub-Gaussian) to intermittent behavior that is characteristic of fully developed high Reynolds number turbulence, and (ii) beyond the transition point, the statistics of the rate of energy dissipation in all three flows obey the same Reynolds number power laws derived for homogeneous turbulence. These results allow us to claim universality of small scales even at low Reynolds numbers. Our results shed new light on the notion of when the turbulence is fully developed at the small scales without relying on the existence of an extended inertial range.An enduring notion in the phenomenology of turbulence is the universality of small scales. It has been taken for granted in theoretical approaches (e.g., refs. 18) and analyzed in numerical simulations (911) as well as various laboratory experiments (e.g., refs. 5 and 12). The standard paradigm is that whereas the large scales are nonuniversal, reflecting the circumstances of their generation, an increasingly weaker degree of nonuniversality is imparted to small scales with increasing separation between the large and small scales. This scale separation is thought to increase with the flow Reynolds number, so a proper test of universality has been thought to require very high Reynolds numbers. Consequently, many substantial efforts have been made to produce such high-Reynolds-number flows (e.g., ref. 12).Here, we show evidence for an alternative point of view: If one resolves small scales accurately, one observes, even at low Reynolds numbers, universal scaling of velocity gradients that manifest primarily at small scales. We stress that small-scale dynamics are strongly nonlinear even in low-Reynolds-number flows driven by large-scale forcing. There is thus considerable merit in measuring or simulating low-Reynolds-number flows much more accurately than has been the practice and exploring the evidence for universality (or lack thereof), instead of advancing as inevitable the notion that useful lessons about universality are possible only at very high Reynolds numbers. Indeed, another result of this paper is that there exists a threshold Reynolds number above which Gaussian-like fluctuations tend to assume intermittent characteristics of fully developed flows and that these features can be extracted by accessing increasingly smaller scales even if the Reynolds numbers are quite moderate. The latter result is especially important for purposes of identifying a fixed point in certain renormalization group expansion procedures (8).  相似文献   
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The general model of epitope‐type MDM2 inhibitor was developed based on the structural information on the complexes between MDM2 and various low molecular weight ligands found in the PDB database. Application of this model to our in‐house library has led us to a new scaffold capable of interrupting protein–protein interactions. A synthetic library based on this and related scaffolds resulted in new classes of compounds that possess biochemical and cellular activity and good pharmacokinetic properties. We assume that such general approach to PPI inhibitors design may be useful for the development of inhibitors of various PPI types, including Bcl/XL.  相似文献   
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Photocatalysts based on zinc hydroxide and a solid solution of CdS and ZnS were prepared via the precipitation method and used for photocatalytic hydrogen production from aqueous solutions of inorganic (Na2S/Na2SO3) and organic (ethanol) sacrificial agents. The photocatalysts were tested in cyclic experiments for hydrogen evolution and studied using X-ray diffraction (XRD), UV-Vis diffuse reflectance spectroscopy, high-resolution transmission electron microscopy (HRTEM), energy-dispersive X-ray spectroscopy (EDX), and X-ray photoelectron spectroscopy (XPS) techniques. Different transformations of the β-Zn(OH)2 co-catalyst were observed in the presence of inorganic and organic sacrificial agents; namely, ZnS was formed in Na2S/Na2SO3 solution, whereas the formation of ε-Zn(OH)2 was detected in solution with ethanol. The composite Zn(OH)2/Cd1−xZnxS photocatalysts have great potential in various photocatalysis processes (e.g., hydrogen production, CO2 reduction, and the oxidation of organic contaminants) under visible light.

The nature of the sacrificial agent affects the transformations of a Zn(OH)2 co-catalyst during photocatalytic hydrogen production.  相似文献   
98.
The incorporation into rigid silica host structures leads successfully to a significant luminescence enhancement of two zinc(ii) dipyrrins, known to be weak emitters in solution. One of these complexes shows a fluorescence efficiency of 55% and prolonged photo-stability once entrapped in silica, demonstrating high potential for applications in energy conversion.

Through incorporation into host–guest silica structures, typically poorly emissive zinc(ii) dipyrrins exhibit up to 100-fold fluorescence enhancement and prolonged photostability.

The search for ever more efficient and sustainable energetic solutions requires the development of new materials that are capable of high conversion rates with the least possible energy losses. Such a target is desirable, and currently tackled, for different types of conversion processes, e.g. light-to-electricity and electricity-to-light, and the primary step typically undertaken is the design of molecular dyes with controlled light absorption and emission bandwidths, alongside high transition efficiencies.1 Among the various classes of dyes studied so far, dipyrromethenes, often called dipyrrins, present particularly attractive advantages over others, such as simple, high-yielding and cheap synthetic routes, wide coordinative versatility towards semi-metals like boron and several metal ions, and finely tuneable optical activity through structural modification on the pyrrole rings by introduction of specific substituents.2–4 Alongside boron dipyrrins, the most extensively studied dipyrrin-based dyes so far, metal dipyrrins have recently gained attention and have been the subject of a growing number of studies on the application of their optical properties for energy conversion.5–8 One of the main drives for studies on metal dipyrrins is the possibility of (i) exploiting the presence of two or three dipyrrin-based chromophores in a complex, as opposed to bodipy dyes bearing only one, thus enhancing the light absorbing capability, and (ii) making use of specific central metal ions to further manipulate the optical properties and the coordination geometries.1,4 Zinc(ii) dipyrrins, among other metal complexes, are particularly attractive because of the presence of an earth-abundant central ion and the ability to form supramolecular structures and coordination polymers,9–12 commonly exhibiting a linear geometry, due to the easy functionalization on the meso-position of the dipyrrin. Despite their strong absorption in the blue-green region, though, with molar extinction coefficients up to above 300 000 M−1 cm−1, they are typically weak emitters because of the strongly competitive non-radiative deactivation pathways, introduced by the distorted tetrahedral coordination and a certain structural flexibility.5One of the possible solutions that has been recently adopted to improve the emission quantum yields of zinc complexes is the use of bulky coordinating ligands that are able to impose a high structural rigidity to the whole complexes. This strategy involves the design of suitable multi-steps synthetic routes, with the aim of expanding the dipyrrin core from the α- or the β-positions, so to introduce sterically hindering groups.7,13 An alternative solution, which we are presenting in this communication, for increasing the luminescence efficiency without having to introduce lengthy synthetic modifications is to impart the desired rigidity by encapsulation of the complexes into a spatially constraining host structure. This may, in principle, also help circumventing another strict limitation to fluorescence efficiencies that homoleptic bis(dipyrrinato) zinc complexes suffer from: the presence of symmetry-breaking charge transfer excited states, which become the lowest-lying states in polar solvents and, being prone to non-radiative decay, lead to fluorescence quenching.6Therefore, we chose two among the weakest bis(dipyrrinato) Zn(ii) emitters to build host–guest materials, where the role of the host is played by mesoporous silica of COK-12 type.14 The structures and the optical absorption of the two homoleptic complexes, 1 and 2, are shown in Fig. 1. They were first reported, respectively, by Nishihara''s and Thompson''s groups,6,7 and showed fluorescence quantum yields below 1% in mildly polar solvents, such as chloroform and dichloromethane, and of 2% (complex 1)13 and 16% (complex 2) in cyclohexane, the least polar solvents used in the above studies (see also Open in a separate windowFig. 1Chemical structures of the complexes 1 and 2, and absorption spectra recorded from 10−6 M dichloromethane solutions.Photophysical properties of the zinc complexes
Sample Φ F τ F c/ns k R/s−1 k NR/s−1
1a0.0031.751.71 × 1065.70 × 108
0.02d
1Sb0.0350.438.14 × 1072.24 × 109
2a0.0051.403.57 × 1067.11 × 108
0.16d2.4d7.5 × 107d3.41 × 108d
2Sb0.5501.344.10 × 1083.36 × 108
Open in a separate windowaFrom 10−6 M dichloromethane solutions.bFrom equimolar water suspensions and confirmed by solid state measurements using an integrated sphere.cLaser excitation at 475 nm, pulse width 62 ps, recorded at 530 nm.dIn cyclohexane (ref. 13).The experimental approach we used for improving the fluorescence yields further above the values obtained in non-polar solvents takes advantage of a well-established soft-template route: here, amphiphilic surfactants self-assemble in water to form rod-like micelles, around which a silica network grows from the hydrolysis and polycondensation of a suitable precursor.15 Due to the insolubility of the zinc dipyrrins in water, their addition during the self-assembly process leads to their spontaneous diffusion and encapsulation into the solvent-free, rigidified, hydrophobic core of the micelles, which are built using the gemini surfactant Pluronic-P123. In order to enable a homogeneous dispersion of the dyes, minimize intermolecular aggregation and prevent structural disruption of the micelles and, consequently, of the silica particles, we applied a recent strategy established in our group,16 using a low loading of complexes, at a 99 : 1 molar ratio of Pluronic-P123: complex for each of the host–guest systems, hereafter named 1S and 2S. The final samples were characterized by transition electron microscopy (TEM, Fig. 2) and small-angle X-ray scattering (SAXS, Fig. S7, see ESI), which confirm that the structural order and the morphology of the dye-doped silica particles are essentially preserved. The SAXS data reported in Fig. S7 show that the most intense peaks for the silica materials occur at q values of 0.64–0.66° and the q ratios of the main peak to the much weaker additional peaks at higher q conform within experimental error to the theoretical q ratios of 1 : √3 : 2 : √7 that correspond to the 2D hexagonal reflections of (10), (11), (20) and (21), respectively. The structures are, thus, consistent with literature values for COK-12 silica14 and prove that the dye-doped P-123 micelles maintain the same structural order of plain silica. This can be indeed visualised from the TEM micrographs in Fig. 2, where the silica particles show a highly ordered morphology with well visible parallel channels.Open in a separate windowFig. 2TEM micrographs of the host–guest systems 1S (top) and 2S (bottom).Therefore, as the pore channels do not undergo a detectable distortion (i.e. expansion), following encapsulation of the complexes, we can infer that the latter must experience considerably strong spatial constraints once entrapped into the hydrophobic core of the cylindrical micelles. UV-visible spectroscopy studies were then carried out on the samples, to evaluate the effects that such a structural rigidity exerts on the optical properties of the complexes. Because of the strong scattering effects caused by the silica suspensions, no absorption spectra could be recorded. Photoluminescence excitation spectra were measured in dichloromethane (DCM), which has a dielectric constant of 8.93. No changes were observed in the energy of the excitation transitions in comparison to that of the free complexes in solution (Fig. S8, see ESI). The emission energies of the complexes within the silica particles also remain unaltered, but two striking differences are noted. First, the fluorescence intensities are impressively enhanced, as it can be seen in Fig. 3.Open in a separate windowFig. 3Emission spectra of the complexes 1 (top) and 2 (bottom) from 4 × 10−6 M dichloromethane solutions (black lines), compared with equimolar suspensions of the host–guest silica systems in water. All spectra were recorded at λexc = 450 nm, with both excitation and emission slits set at 5 nm.Second, the emission bandwidth becomes much narrower in silica than in solution for both complexes, with the full width at half-maxima (FWHM) reducing from values that exceed 4300 cm−1, which are hardly measurable with absolute precision in solution due to the extremely weak and broad emission, to values in silica of ∼2300 cm−1 for 1 and ∼1200 cm−1 for 2. Such an effect is indicative of a restricted vibrational freedom of the complexes within the constrained micellar environment; moreover, considering that the FWHM in the emission band of 2 becomes close to the value in excitation, ∼1100 cm−1, it suggests that the structural rigidification forces the geometries of the ground and the excited state to be more similar to one another.The fluorescence quantum yields of all samples were recorded and allowed us to make some important observations: a 10-fold increase in the emission of 1 occurs upon incorporation and the enhancement is even 100-fold in the case of 2 (see 6,7 homoleptic zinc bis-dipyrrins undergo photoinduced charge transfer from one ligand to the second one, which breaks the symmetry of the excited state. The latter is indeed defined as a symmetry-breaking charge-transfer (SBCT) state and becomes the lowest state even in mildly polar solvents such as dichloromethane. Since SBCT states are typically non-emissive in nature, this leads to a total emission quenching in dichloromethane, with fluorescence yields of 0.3% and 0.5% for 1 and 2, respectively, whereas in relatively apolar cyclohexane the above values increase up to 2% and 16%.13 Such trend reaches its extreme in the solvent-free and apolar environment of the micellar structures within the silica channels: therein, the absence of solvent stabilisation and the rigid environment further reduce the non-radiative deactivation pathways and lead to emission yields of 3.5% and 55%, respectively, for 1 and 2. The excited state lifetimes were also measured and show relatively milder effects from solution to solid state: a reduction by a factor of four for 1, whereas no significant change for 2 (see also the full decay profiles in ESI, Fig. S9).More insights on the photophysical dynamics can be gained from the comparison between the radiative and the non-radiative decay rates. For both complexes, the radiative rates increase dramatically, nearly 50-fold for 1 and over 100-fold for 2, and we consider this a further effect of the encapsulation of the complexes. Considering the restricted vibrational and rotational degrees of freedom within the silica host, significant geometrical distortions in the complexes from the ground to the excited state are energetically unfavoured; this may translate in an increased probability of radiative deactivation taking place from an excited state conformations near the initial Franck–Condon form. Such situation has also been demonstrated in previous examples of dipyrromethene complexes, where rigidification of the organic backbones with sterically hindered groups proved to increase the radiative rate.13,17On the other hand, the non-radiative rate almost quadruples for 1, whereas it halves for 2, showing that 1 is more affected by non-radiative quenching than 2 once it is encapsulated inside the silica template. We ascribe this behaviour to the effect that a partial intermolecular aggregation may have on 1, resulting from the tendency of the anthracene moieties to undergo π-stacking in a more constrained environment than in fluid solution. Such an effect could not be observed for 2, where the sterically hindered mesityl group prevents aggregation. Indeed, the reduced vibrational deactivation pathways in 2 contribute to a much larger increase in emission quantum yield than for 1.Considering the outstanding fluorescence efficiency of the 2S silica particles, we evaluated their possible exploitation for the design of new luminescent solar concentrators.18,19 For this purpose, thin films were prepared by dispersion of the luminescent silica particles in a transparent polymer, polymethyl methacrylate (PMMA), and the photostability of such films was tested against steady UV light irradiation over the course of twelve hours.For comparison, the tests were carried out also on polymeric films doped with the free complexes, using the same concentration of complexes present in the films containing the silica particles. The results are shown in Fig. 4, which reports the observed trend in photoluminescence intensity together with photographs of the polymeric films exposed to UV light before and after the stability tests. It is evident that the complex 2, once incorporated into the silica, retains its luminescence intensity throughout the test, whereas the emission from the free complex dispersed in PMMA halves its intensity in less than two hours of irradiation and photobleaches almost completely after twelve hours.Open in a separate windowFig. 4Top: photoluminescence stability tests performed on thin polymer films doped with the free complex 2 (black circles) and with silica particles embedding the complex (white circles); irradiation wavelength = 450 nm; detection wavelength = 520 nm. Bottom: photographs of the 2-doped (left) and the 2S-doped PMMA films (right), under UV light (365 nm), before (top pictures) and after (bottom pictures) the irradiation tests.It can then be concluded that the assembly strategy used in this study to improve the luminescence properties of notoriously weakly emissive zinc dipyrrins is impressively beneficial and it also serves as a mean to suppress photo-induced degradation of the complexes, demonstrating the potential of the systems presented in this communication for applications in sensitisation and light-emission technologies.  相似文献   
99.
Background: T and B cell-mediated immunity can be assessed using T cell receptor excision circle (TREC) and Kappa-deleting recombination excision circle (KREC) analysis, respectively, and successful implementation of this method requires evaluation of the correlation between the TREC frequencies and T cell subsets as well as KREC levels and B lymphocyte subsets. The aim of the present study was to evaluate the correlation between the TREC/KREC concentrations and T/B lymphocyte subsets at different stages of COVID-19. Methods: We examined 33 patients in the acute stage of COVID-19 (including 8 patients with poor outcomes) and 33 COVID-19 survivors. TREC/KREC concentrations were measured using quantitative real-time PCR. T/B lymphocyte subsets were determined using flow cytometry. Results: Blood TREC and KREC levels were found to be significantly lower in the acute stage of COVID-19 compared to control values. Moreover, a zero blood TREC level was a predictor of a poor disease outcome. Reductions in CD3+CD4+CD45ROCD62L and CD3+CD8+CD45ROCD62L T cell counts (as well as in the main fractions of B1 and B2 B cells) indicated a favorable outcome in COVID-19 patients in the acute stage of the disease. Decreased CD3+CD4+CD45ROCD62L+ and CD3+CD8+CD45ROCD62L+ T cell frequencies and increased CD3+CD8+CD45ROCD62L cell counts were found to indicate a poor outcome in patients with acute COVID-19. These patients were also found to have increased B1 cell counts while demonstrating no changes in B2 cell counts. The levels of effector T cell subsets an naïve B cells were normal in COVID-19 survivors. The most pronounced correlations between TREC/KREC levels and T/B cell subsets counts were observed in COVID-19 survivors: there were positive correlations with naïve T and B lymphocytes and negative correlations with central and effector memory T cell subsets. Conclusions: The assessment of correlations between TREC and T cell subsets as well as KREC levels and B cell subset counts in patients with acute COVID-19 and COVID-19 survivors has shown that blood concentrations of TREC and KREC are sensitive indicators of the stage of antigen-independent differentiation of adaptive immunity cells. The results of the TREC and KREC analysis correlated with the stages of COVID-19 and differed depending on the outcome of COVID-19.  相似文献   
100.
A reductive filter paper for selective nitro reduction has been prepared by modification of a pristine cellulose filter paper by Pd/C nanoparticles, as a portable catalyst. The reaction was performed in two different set-ups including (i) filtration and (ii) sealed systems, in the presence of ammonium formate and ex situ generated hydrogen gas reducing agents, respectively. In the sealed system in the presence of H2 gas, the halogenated nitroarenes were completely reduced, while in the filtration system, different derivatives of the nitroarenes were selectively reduced to aryl amines. In both systems, the reduction of nitroarenes to aryl amines was performed with high efficiency and selectivity, comparable to a heterogeneous system. Reaction parameters were comprehensively designed using Design Expert software and then studied. The properties of the catalytic filter paper were studied in detail from the points of view of swellability, shrinkage, reusability, and stability against acidic, alkaline, and oxidative reagents.

A novel and efficient catalytic filtration has been developed for the selective reduction of nitro compounds on a Pd/C-doped cellulose filter paper.  相似文献   
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