962 resultados para Microscopia confocal
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The add protection effect promoted by traces of PdCl2 in [Ni(dmgH)(2)] spot tests was elucidated from confocal Raman microscopy imaging, which revealed the formation of protecting layers of [Pd(dmgH)(2)] closing the extremities of the [Ni(dmgH)(2)] filaments.
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The aim of this study was to evaluate the penetration of endodontic sealer into the dentin tubules, the integrity of the sealer layer perimeter, and the sealer area at the apical third after different filling techniques by confocal laser scanning microscopy (CLSM). Forty-five mandibular premolars were mechanically prepared with ProTaper files, until F5 file. Thereafter, they were filled with an epoxy-resin sealer (AH Plus) mixed with Rhodamine B dye (0.1% proportion) and allocated in three groups: Group 1, single master cone; Group 2, cold lateral compaction; and Group 3, Thermafil. For confocal laser scanning microscopy analysis, the specimens were transversely sectioned at 4 mm from the apex. The images at x10 and x40 were analyzed by Imagetool 3.0 software. Significant differences were not found among the three experimental groups according the dentin-impregnate area by the sealer (P = 0.68) and between the sealer and root canal perimeter (P = 0.18). However, root canal filling techniques were significantly different when apical sealer areas were compared (P = 0.001). Thermafil group showed smaller sealer areas (8.09%) while cold lateral compaction and gutta-percha master cone showed similar areas (17.37 and 21.18%, respectively). The dentin-impregnated area was not dependent on the root canal filling technique. Single master cone, cold lateral condensation and Thermafil techniques presented integrity of the sealer perimeter close to 100% and Thermafil resulted in a significantly thinner sealer layer. Microsc. Res. Tech. 75:12771280, 2012. (C) 2012 Wiley Periodicals, Inc.
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Abstract Background Delignification pretreatments of biomass and methods to assess their efficacy are crucial for biomass-to-biofuels research and technology. Here, we applied confocal and fluorescence lifetime imaging microscopy (FLIM) using one- and two-photon excitation to map the lignin distribution within bagasse fibers pretreated with acid and alkali. The evaluated spectra and decay times are correlated with previously calculated lignin fractions. We have also investigated the influence of the pretreatment on the lignin distribution in the cell wall by analyzing the changes in the fluorescence characteristics using two-photon excitation. Eucalyptus fibers were also analyzed for comparison. Results Fluorescence spectra and variations of the decay time correlate well with the delignification yield and the lignin distribution. The decay dependences are considered two-exponential, one with a rapid (τ1) and the other with a slow (τ2) decay time. The fastest decay is associated to concentrated lignin in the bagasse and has a low sensitivity to the treatment. The fluorescence decay time became longer with the increase of the alkali concentration used in the treatment, which corresponds to lignin emission in a less concentrated environment. In addition, the two-photon fluorescence spectrum is very sensitive to lignin content and accumulation in the cell wall, broadening with the acid pretreatment and narrowing with the alkali one. Heterogeneity of the pretreated cell wall was observed. Conclusions Our results reveal lignin domains with different concentration levels. The acid pretreatment caused a disorder in the arrangement of lignin and its accumulation in the external border of the cell wall. The alkali pretreatment efficiently removed lignin from the middle of the bagasse fibers, but was less effective in its removal from their surfaces. Our results evidenced a strong correlation between the decay times of the lignin fluorescence and its distribution within the cell wall. A new variety of lignin fluorescence states were accessed by two-photon excitation, which allowed an even broader, but complementary, optical characterization of lignocellulosic materials. These results suggest that the lignin arrangement in untreated bagasse fiber is based on a well-organized nanoenvironment that favors a very low level of interaction between the molecules.
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The cellular rheology has recently undergone a rapid development with particular attention to the cytoskeleton mechanical properties and its main components - actin filaments, intermediate filaments, microtubules and crosslinked proteins. However it is not clear what are the cellular structural changes that directly affect the cell mechanical properties. Thus, in this work, we aimed to quantify the structural rearrangement of these fibers that may emerge in changes in the cell mechanics. We created an image analysis platform to study smooth muscle cells from different arteries: aorta, mammary, renal, carotid and coronary and processed respectively 31, 29, 31, 30 and 35 cell image obtained by confocal microscopy. The platform was developed in Matlab (MathWorks) and it uses the Sobel operator to determine the actin fiber image orientation of the cell, labeled with phalloidin. The Sobel operator is used as a filter capable of calculating the pixel brightness gradient, point to point, in the image. The operator uses vertical and horizontal convolution kernels to calculate the magnitude and the angle of the pixel intensity gradient. The image analysis followed the sequence: (1) opens a given cells image set to be processed; (2) sets a fix threshold to eliminate noise, based on Otsu's method; (3) detect the fiber edges in the image using the Sobel operator; and (4) quantify the actin fiber orientation. Our first result is the probability distribution II(Δθ) to find a given fiber angle deviation (Δθ) from the main cell fiber orientation θ0. The II(Δθ) follows an exponential decay II(Δθ) = Aexp(-αΔθ) regarding to its θ0. We defined and determined a misalignment index α of the fibers of each artery kind: coronary αCo = (1.72 ‘+ or =’ 0.36)rad POT -1; renal αRe = (1.43 + or - 0.64)rad POT -1; aorta αAo = (1.42 + or - 0.43)rad POT -1; mammary αMa = (1.12 + or - 0.50)rad POT -1; and carotid αCa = (1.01 + or - 0.39)rad POT -1. The α of coronary and carotid are statistically different (p < 0.05) among all analyzed cells. We discussed our results correlating the misalignment index data with the experimental cell mechanical properties obtained by using Optical Magnetic Twisting Cytometry with the same group of cells.
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A causa della limitata estensione del campo di vista del sistema, con un microscopio ottico tradizionale non è possibile acquisire una singola immagine completamente a fuoco se l’oggetto è caratterizzato da una profondità non trascurabile. Fin dagli anni ’70, il problema dell’estensione della profondità di fuoco è stato ampiamente trattato in letteratura e molti metodi sono stati proposti per superare questo limite. Tuttavia, è molto difficile riuscire a decretare quale metodo risulti essere il migliore in una specifica applicazione, a causa della mancanza di una metrica validata e adatta ad essere utilizzata anche in casi reali, dove generalmente non si ha a disposizione un’immagine di riferimento da considerare come “la verità” (ground truth). L’Universal Quality Index (UQI) è ampiamente utilizzato in letteratura per valutare la qualità dei risultati in processi di elaborazione di immagini. Tuttavia, per poter calcolare questo indice è necessaria una ground truth. In effetti, sono state proposte in letteratura alcune estensioni dell’UQI per valutare il risultato dei metodi di fusione anche senza immagine di riferimento, ma nessuna analisi esaustiva è stata proposta per dimostrare la loro equivalenza con l’UQI standard nel valutare la qualità di un’immagine. In questo lavoro di Tesi, partendo dai limiti dei metodi attualmente utilizzati per l'estensione della profondità di campo di un microscopio, ed esposti in letteratura, per prima cosa è stato proposto un nuovo metodo, basato su approccio spaziale e fondato su analisi locale del segnale appositamente filtrato. Attraverso l’uso di sequenze di immagini sintetiche, delle quali si conosce la ground truth, è stato dimostrato, utilizzando metriche comuni in image processing, che il metodo proposto è in grado di superare le performance dei metodi allo stato dell'arte. In seguito, attraverso una serie di esperimenti dedicati, è stato provato che metriche proposte e ampiamente utilizzate in letteratura come estensione dell'UQI per valutare la qualità delle immagini prodotte da processi di fusione, sebbene dichiarate essere sue estensioni, non sono in grado di effettuare una valutazione quale quella che farebbe l'UQI standard. E’ quindi stato proposto e validato un nuovo approccio di valutazione che si è dimostrato in grado di classificare i metodi di fusione testati così come farebbe l’UQI standard, ma senza richiedere un’immagine di riferimento. Infine, utilizzando sequenze di immagini reali acquisite a differenti profondità di fuoco e l’approccio di valutazione validato, è stato dimostrato che il metodo proposto per l’estensione della profondità di campo risulta sempre migliore, o almeno equivalente, ai metodi allo stato dell’arte.
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Protocolli e metodologie di caratterizzazione di un sistema di misura di segnali fluorescenti in microscopia ottica
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A sample scanning confocal optical microscope (SCOM) was designed and constructed in order to perform local measurements of fluorescence, light scattering and Raman scattering. This instrument allows to measure time resolved fluorescence, Raman scattering and light scattering from the same diffraction limited spot. Fluorescence from single molecules and light scattering from metallic nanoparticles can be studied. First, the electric field distribution in the focus of the SCOM was modelled. This enables the design of illumination modes for different purposes, such as the determination of the three-dimensional orientation of single chromophores. Second, a method for the calculation of the de-excitation rates of a chromophore was presented. This permits to compare different detection schemes and experimental geometries in order to optimize the collection of fluorescence photons. Both methods were combined to calculate the SCOM fluorescence signal of a chromophore in a general layered system. The fluorescence excitation and emission of single molecules through a thin gold film was investigated experimentally and modelled. It was demonstrated that, due to the mediation of surface plasmons, single molecule fluorescence near a thin gold film can be excited and detected with an epi-illumination scheme through the film. Single molecule fluorescence as close as 15nm to the gold film was studied in this manner. The fluorescence dynamics (fluorescence blinking and excited state lifetime) of single molecules was studied in the presence and in the absence of a nearby gold film in order to investigate the influence of the metal on the electronic transition rates. The trace-histogram and the autocorrelation methods for the analysis of single molecule fluorescence blinking were presented and compared via the analysis of Monte-Carlo simulated data. The nearby gold influences the total decay rate in agreement to theory. The gold presence produced no influence on the ISC rate from the excited state to the triplet but increased by a factor of 2 the transition rate from the triplet to the singlet ground state. The photoluminescence blinking of Zn0.42Cd0.58Se QDs on glass and ITO substrates was investigated experimentally as a function of the excitation power (P) and modelled via Monte-Carlo simulations. At low P, it was observed that the probability of a certain on- or off-time follows a negative power-law with exponent near to 1.6. As P increased, the on-time fraction reduced on both substrates whereas the off-times did not change. A weak residual memory effect between consecutive on-times and consecutive off-times was observed but not between an on-time and the adjacent off-time. All of this suggests the presence of two independent mechanisms governing the lifetimes of the on- and off-states. The simulated data showed Poisson-distributed off- and on-intensities, demonstrating that the observed non-Poissonian on-intensity distribution of the QDs is not a product of the underlying power-law probability and that the blinking of QDs occurs between a non-emitting off-state and a distribution of emitting on-states with different intensities. All the experimentally observed photo-induced effects could be accounted for by introducing a characteristic lifetime tPI of the on-state in the simulations. The QDs on glass presented a tPI proportional to P-1 suggesting the presence of a one-photon process. Light scattering images and spectra of colloidal and C-shaped gold nano-particles were acquired. The minimum size of a metallic scatterer detectable with the SCOM lies around 20 nm.
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The aim of this work is to measure the stress inside a hard micro object under extreme compression. To measure the internal stress, we compressed ruby spheres (a-Al2O3: Cr3+, 150 µm diameter) between two sapphire plates. Ruby fluorescence spectrum shifts to longer wavelengths under compression and can be related to the internal stress by a conversion coefficient. A confocal laser scanning microscope was used to excite and collect fluorescence at desired local spots inside the ruby sphere with spatial resolution of about 1 µm3. Under static external loads, the stress distribution within the center plane of the ruby sphere was measured directly for the first time. The result agreed to Hertz’s law. The stress across the contact area showed a hemispherical profile. The measured contact radius was in accord with the calculation by Hertz’s equation. Stress-load curves showed spike-like decrease after entering non-elastic phase, indicating the formation and coalescence of microcracks, which led to relaxing of stress. In the vicinity of the contact area luminescence spectra with multiple peaks were observed. This indicated the presence of domains of different stress, which were mechanically decoupled. Repeated loading cycles were applied to study the fatigue of ruby at the contact region. Progressive fatigue was observed when the load exceeded 1 N. As long as the load did not exceed 2 N stress-load curves were still continuous and could be described by Hertz’s law with a reduced Young’s modulus. Once the load exceeded 2 N, periodical spike-like decreases of the stress could be observed, implying a “memory effect” under repeated loading cycles. Vibration loading with higher frequencies was applied by a piezo. Redistributions of intensity on the fluorescence spectra were observed and it was attributed to the repopulation of the micro domains of different elasticity. Two stages of under vibration loading were suggested. In the first stage continuous damage carried on until certain limit, by which the second stage, e.g. breakage, followed in a discontinuous manner.
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Introduzione L’efficacia dei chemio/radioterapici ha aumentato notevolmente l’aspettativa di vita delle pazienti oncologiche, tuttavia, questi trattamenti possono compromettere la funzionalità ovarica. La crioconservazione di tessuto ovarico, con il successivo reimpianto, ha lo scopo di preservare la fertilità delle pazienti a rischio di fallimento ovarico precoce. Scopo dello studio Definire la migliore procedura di crioconservazione e reimpianto in grado di ottenere la neovascolarizzazione del tessuto reimpiantato nel minor tempo possibile al fine di diminuire la perdita follicolare causata dall’ischemia durante la procedura. Materiali e metodi Per ciascuna paziente (3) le biopsie ovariche, sono state prelevate laparoscopicamente e crioconservate secondo il protocollo di congelamento lento/scongelamento rapido. Campioni di corticale ovarica sono stati processati per l’analisi istologica, ultrastrutturale, immuistochimica e confocale per valutare la preservazione morfologiaca del tessuto. Le fettine di corticale ovarica sono state scongelate e reimpiantate ortotopicamente (2), nelle ovaia e in due tasche peritoneali, o eterotopicamente (1), in due tasche create nel sottocute sovrapubico. Risultati Le analisi di microscopia hanno mostrato il mantenimento di una discreta morfologia dello stroma, e dei vasi criopreservati e un lieve ma non significativo danneggiamento dei follicoli scongelati. Tutte le pazienti hanno mostrato la ripresa della funzionalità endocrina rispettivamente dopo 2/4 mesi dal reimpianto. Il color-doppler, inoltre ha rivelato un significativo aumento della vascolarizzazione ovarica rispetto alla quasi totale assenza di vascolarizzazione prima del reimpianto, quando le pazienti mostravano una conclamata menopausa. Conclusioni Lo studio ha confermato la ripresa della vascolarizzazione dell’ovaio in seguito a reimpianto avascolare di fettine di corticale, senza l’impiego di fattori esogeni o meccanici aggiuntivi, in tempi concordanti con i dati della letteratura. I risultati sono incoraggianti e l’avanzare degli studi e della ricerca potranno contribuire allo sviluppo di nuove metodologie di reimpianto che possano avere un successo clinico ed una sicurezza superiori a quelle finora ottenute.
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L'utilizzo dell'idrogeno come vettore energetico �è negli ultimi anni uno dei temi in maggior rilievo riguardo la sostenibilit�à energetica, questo per via della sua abbondanza in natura, della sua elevata energia chimica per unità di massa, e della non tossicità dei prodotti della sua combustione. Tuttavia non si conosce ancora una maniera e�fficiente di immagazzinarlo per poterlo utilizzare per applicazioni mobili. In questo lavoro di tesi sono state cresciute, e analizzate mediante microscopia elettronica, nanoparticelle di magnesio decorate con metalli di transizione (Pd e Ti), che si collocano tra i candidati più promettenti per lo stoccaggio di idrogeno a stato solido.
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Questo progetto di tesi ha come obiettivo lo sviluppo di un algoritmo per la correzione e la calibrazione delle immagini in microscopia a fluorescenza e della sua implementazione come programma. Infatti, senza tale calibrazione le immagini di microscopia a fluorescenza sarebbero intrinsecamente affette da molteplici tipi di distorsioni ottiche. Questo limita fortemente la possibilità di effettuare analisi quantitative del livello di fluorescenza osservato. Il difetto sul quale ci siamo soffermati è la disomogeneità di campo, ossia una non uniforme fluorescenza causata dalla forma irregolare del fascio di eccitazione. Per conseguire l'obiettivo da noi proposto è necessaria l'acquisizione, in parallelo al campione in esame, di immagini di calibrazione contenenti sfere nanometriche a fluorescenza nota. A partire da queste, tramite procedure di image processing da noi implementate, abbiamo stimato la funzione di correzione della fluorescenza, localmente per ogni punto dell'immagine. Per la creazione di tale algoritmo abbiamo ipotizzato una possibile distribuzione dell'intensità dovuta alla non omogeneità del fascio ed abbiamo quindi stimato i parametri tramite un'apposita procedura di maximum likelihood. Tale stima è stata eseguita tenendo conto di possibili effetti dovuti alla luminosità di background, alla sovrapposizione di più nanosfere e ad effetti di bordo nel corso dell'elaborazione. Questa procedura è stata ripetuta su quattro diverse immagini di calibrazione, per valutarne la consistenza e la validità. Inoltre, per poter verificare che il software di elaborazione abbia le desiderate proprietà di linearità tra segnale misurato ed intensità nota, ci siamo serviti di un'ulteriore immagine di calibrazione contenente una mistura di sfere nanometriche con intensità variabili su due ordini di grandezza. Il risultato di questo lavoro di tesi verrà incluso in un programma per la calibrazione delle immagini in fluorescenza acquisite al laboratorio di biofisica del Dipartimento di Fisica ed Astronomia di Bologna.
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Understanding and controlling the mechanism of the diffusion of small molecules, macromolecules and nanoparticles in heterogeneous environments is of paramount fundamental and technological importance. The aim of the thesis is to show, how by studying the tracer diffusion in complex systems, one can obtain information about the tracer itself, and the system where the tracer is diffusing. rnIn the first part of my thesis I will introduce the Fluorescence Correlation Spectroscopy (FCS) which is a powerful tool to investigate the diffusion of fluorescent species in various environments. By using the main advantage of FCS namely the very small probing volume (<1µm3) I was able to track the kinetics of phase separation in polymer blends at late stages by looking on the molecular tracer diffusion in individual domains of the heterogeneous structure of the blend. The phase separation process at intermediate stages was monitored with laser scanning confocal microscopy (LSCM) in real time providing images of droplet coalescence and growth. rnIn a further project described in my thesis I will show that even when the length scale of the heterogeneities becomes smaller than the FCS probing volume one can still obtain important microscopic information by studying small tracer diffusion. To do so, I will introduce a system of star shaped polymer solutions and will demonstrate that the mobility of small molecular tracers on microscopic level is nearly not affected by the transition of the polymer system to a “glassy” macroscopic state. rnIn the last part of the thesis I will introduce and describe a new stimuli responsive system which I have developed, that combines two levels of nanoporosity. The system is based on poly-N-isopropylacrylamide (PNIPAM) and silica inverse opals (iOpals), and allows controlling the diffusion of tracer molecules. rn
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Granular matter, also known as bulk solids, consists of discrete particles with sizes between micrometers and meters. They are present in many industrial applications as well as daily life, like in food processing, pharmaceutics or in the oil and mining industry. When handling granular matter the bulk solids are stored, mixed, conveyed or filtered. These techniques are based on observations in macroscopic experiments, i.e. rheological examinations of the bulk properties. Despite the amply investigations of bulk mechanics, the relation between single particle motion and macroscopic behavior is still not well understood. For exploring the microscopic properties on a single particle level, 3D imaging techniques are required.rnThe objective of this work was the investigation of single particle motions in a bulk system in 3D under an external mechanical load, i.e. compression and shear. During the mechanical load the structural and dynamical properties of these systems were examined with confocal microscopy. Therefor new granular model systems in the wet and dry state were designed and prepared. As the particles are solid bodies, their motion is described by six degrees of freedom. To explore their entire motion with all degrees of freedom, a technique to visualize the rotation of spherical micrometer sized particles in 3D was developed. rnOne of the foci during this dissertation was a model system for dry cohesive granular matter. In such systems the particle motion during a compression of the granular matter was investigated. In general the rotation of single particles was the more sensitive parameter compared to the translation. In regions with large structural changes the rotation had an earlier onset than the translation. In granular systems under shear, shear dilatation and shear zone formation were observed. Globally the granular sediments showed a shear behavior, which was known already from classical shear experiments, for example with Jenike cells. Locally the shear zone formation was enhanced, when near the applied load a pre-diluted region existed. In regions with constant volume fraction a mixing between the different particle layers occurred. In particular an exchange of particles between the current flowing region and the non-flowing region was observed. rnThe second focus was on model systems for wet granular matter, where an additional binding liquid is added to the particle suspension. To examine the 3D structure of the binding liquid on the micrometer scale independently from the particles, a second illumination and detection beam path was implemented. In shear and compression experiments of wet clusters and bulk systems completely different dynamics compared to dry cohesive models systems occured. In a Pickering emulsion-like system large structural changes predominantly occurred in the local environment of binding liquid droplets. These large local structural changes were due to an energy interplay between the energy stored in the binding droplet during its deformation and the binding energy of particles at the droplet interface. rnConfocal microscopy in combination with nanoindentation gave new insights into the single particle motions and dynamics of granular systems under a mechanical load. These novel experimental results can help to improve the understanding of the relationship between bulk properties of granular matter, such as volume fraction or yield stress and the dynamics on a single particle level.rnrn
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Caratterizzazione di un biomateriale a base di fitocomplessi, contenente ossalato di potassio, progettato per il trattamento dell'ipersensibilità dentinale.
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L’obiettivo di questa tesi è esfoliare mediante tecnica LPE qualche layer di grafite ed analizzare il campione ottenuto mediante la tecnica AFM. Negli studi sperimentali svolti nell’ambito di questa tesi sono state condotte tre tipologie di esperimenti: 1) analisi della grafite minerale prima del trattamento di esfoliazione; 2) esfoliazione LPE di grafite fissata su substrato di muscovite, in bagno ultrasonico con acqua bidistillata; 3) esfoliazione LPE di grafite fissata su muscovite, in bagno ultrasonico con azoto liquido. L’ultrasonicazione ha portato al distacco ed isolamento di frammenti di grafite di forma tipicamente triangolare e di dimensioni laterali micrometriche, i quali si sono depositati sul substrato di muscovite e ridepositati sulla grafite stessa. Inoltre ho osservato la presenza di diversi DLG (double-layer graphene) e addirittura la presenza di SLG (single-layer graphene) estesi alcune centinaia di nm. L’analisi AFM ha mostrato la presenza di bordi cristallografici definiti, a volte con la presenza di angoli di 120° e ha mostrato il fenomeno del “folding”.