77 resultados para Làsers


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Els stents són unes pròtesis endovasculars. L’objectiu del projecte és el disseny i desenvolupament d’un utillatge que permeti la seva fabricació per tall làser. S’utilitzarà el làser del GREP (Grup de Recerca en Enginyeria de Producte, Procés i Producció) de la Universitat de Girona, el qual està instal•lat sobre el capçal d’un centre de mecanitzat convencional

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El láser de Nd:YAG está compuesto por un granate de itrio y aluminio, contaminado por neodimio. Emite a una longitud de onda de 1064 nm, en el infrarrojo cercano. A diferencia de otros láseres, el láser de Nd:YAG, puede transmitirse a través de fibra óptica, lo cual permite una fácil aplicación de este tipo de energía en espacios anatómicos bucodentarios de difícil acceso. Este hecho, asociado al potente efecto bactericida que produce esta longitud de onda, lo convierten en una herramienta ideal en los tratamientos endodóncicos y periodontales, en los que puede mejorar los resultados obtenidos con las técnicas convencionales. También se utiliza en ciertos tratamientos de Cirugía Bucal, principalmente para las exéresis de lesiones de tejidos blandos.

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By exciting at 788 nm, we have characterized the near infrared emissions of trivalent thulium ions in monoclinic KGd(WO4)2 single crystals at 1.48 and 1.84 mm as a function of dopant concentration from 0.1% to 10% and temperature from 10 K to room temperature. We used the reciprocity method to calculate the maximum emission cross-section of 3.0310220 cm2 at 1.838 mm for the polarization parallel to the Nm principal optical direction. These results agrees well with the experimental data. Experimental decay times of the 3H4!3F4 and 3F4!3H6 transitions have been measured as a function of thulium concentration.

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Objective: The aim of this in vitro experimental study was to perform histological evaluation of the thermal effect produced on soft tissue irradiated with CO2, Er,Cr:YSGG or diode lasers. Study design: Porcine oral mucosa samples were irradiated with Er,Cr:YSGG laser at 1 W with and without water / air spray, at 2 W with and without water / air spray, and at 4 W with water / air spray, with CO2 laser at 1 W, 2 W, 10 W, 20 W continuous mode and 20 W pulsed mode and diode laser at 2W, 5W, and 10W pulsed mode. The thermal effect was evaluated measuring the width of damaged tissue adjacent to the incision, stained positively for hyalinized tissue with Hematoxylin-Eosin and Masson Trichrome stains. Besides, histological changes in the irradiated tissue were described using subjective grading scales. Results: The evaluated lasers developed a wide range of thermal damage with significant differences between groups. The samples with lowest thermal effect were those irradiated with Er,Cr:YSGG laser using water / air spray, followed by CO2 and diode lasers. Conclusions: Emission parameters of each laser system may influence the thermal damage inflicted on the soft tissue, however, the wave length of each laser determines the absorption rate characteristics of every tissue and the thermal effect

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Laser diffraction (LD) and static image analysis (SIA) of rectangular particles [United States Pharmacopeia, USP30-NF25, General Chapter <776>, Optical Miroscopy.] have been systematically studied. To rule out sample dispersion and particle orientation as the root cause of differences in size distribution profiles, we immobilize powder samples on a glass plate by means of a dry disperser. For a defined region of the glass plate, we measure the diffraction pattern as induced by the dispersed particles, and the 2D dimensions of the individual particles using LD and optical microscopy, respectively. We demonstrate a correlation between LD and SIA, with the scattering intensity of the individual particles as the dominant factor. In theory, the scattering intensity is related to the square of the projected area of both spherical and rectangular particles. In traditional LD the size distribution profile is dominated by the maximum projected area of the particles (A). The diffraction diameters of a rectangular particle with length L and breadth B as measured by the LD instrument approximately correspond to spheres of diameter ØL and ØB respectively. Differences in the scattering intensity between spherical and rectangular particles suggest that the contribution made to the overall LD volume probability distribution by each rectangular particle is proportional to A2/L and A2/B. Accordingly, for rectangular particles the scattering intensity weighted diffraction diameter (SIWDD) explains an overestimation of their shortest dimension and an underestimation of their longest dimension. This study analyzes various samples of particles whose length ranges from approximately 10 to 1000 μm. The correlation we demonstrate between LD and SIA can be used to improve validation of LD methods based on SIA data for a variety of pharmaceutical powders all with a different rectangular particle size and shape.

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Bi1.5Zn1Nb1.5O7 (BZN) epitaxial thin films were grown by pulsed laser deposition on Al2O3 with a double ZnO buffer layer through domain matching epitaxy (DME) mechanism. The pole figure analysis and reciprocal space mapping revealed the single crystalline nature of the thin film. The pole figure analysis also shows a 60º twinning for the (222) oriented crystals. Sharp intense spots in the SAED pattern also indicate the high crystalline nature of BZN thin film. The Fourier filtered HRTEM images of the BZN-ZnO interface confirms the domain matched epitaxy of BZN with ZnO buffer. An electric field dependent dielectric tunability of 68% was obtained for the BZN thin films with inter digital capacitors patterned over the film.

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We develop a method for generating focused vector beams with circular polarization at any transverse plane. Based on the Richards-Wolf vector model, we derive analytical expressions to describe the propagation of these set of beams near the focal area. Since the polarization and the amplitude of the input beam are not uniform, an interferometric system capable of generating spatially-variant polarized beams has to be used. In particular, this wavefront is manipulated by means of spatial light modulators displaying computer generated holograms and subsequently focused using a high numerical aperture objective lens. Experimental results using a NA=0.85 system are provided: irradiance and Stokes images of the focused field at different planes near the focal plane are presented and compared with those obtained by numerical simulation.

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Objective: An evaluation and comparison is made of the thermal increment at different implant surfaces during irradiation with CO2 and ErCr:YSGG lasers. Study design: Five threaded and impacted implants with four types of surfaces were inserted in an adult pig rib: two implants with a hydroxyapatite surface (HA)(impacted and threaded, respectively), a machined titanium surface implant (TI mach), a titanium plasma spray surface implant (TPS), and a sandblasted, acid-etched surface implant (SBAE). A 0.5-mm diameter bone defect was made in the implant apical zone, and a type-K thermocouple (Termopar)® was placed in contact with the implant. The implants were irradiated in the coronal zone of each implant with a CO2 (4 W continuous mode) and an ErCr:YSGG laser (1.5 W, pulsed mode) first without and then with refrigeration. The temperature variations at the implant apical surface were recorded. Results: An apical temperature increase was recorded in all cases during CO2 and ErCr:YSGG laser irradiation without refrigeration. However, when the ErCr:YSGG was used with a water spray, a decrease in temperature was observed in all implants. The acid-etched and sandblasted surfaces were those most affected by the thermal changes. Conclusions: The ErCr:YSGG laser with a water spray applied to the sealing cap or coronal zone of the implants does not generate thermal increments in the apical surface capable of adversely affecting osseointegration and the integrity of the peri-implant bone tissue

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By exciting at 940 nm, we have characterized the 1.84 m near infrared emission of trivalent thulium ions in Yb3+, Tm3+:KGd WO4 2 single crystals as a function of the dopant concentration and temperature, from 10 K to room temperature. An overall 3H6 Stark splitting of 470 cm−1 for the Tm3+ ions in the Yb3+, Tm3+:KGd WO4 2 was obtained. We also studied the blue emission at 476 nm Tm3+ and the near infrared emissions at 1.48 m Tm3+ and 1 m Yb3+ as a function of the dopant concentration. Experimental decay times of the 1G4, 3H4, and 3F4 Tm3+ and 2F5/2 Yb3+ excited states have been measured as a function of Yb3+ and Tm3+ ion concentrations. For the 3F4 →3H6 transition of Tm3+ ions, we used the reciprocity method to calculate the maximum emission cross section of 3.07 10−20 cm2 at 1.84 m for the polarization parallel to the Nm principal optical direction.

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The analysis of paraxial Gaussian beams features in most undergraduate courses in laser physics, advanced optics and photonics. These beams provide a simple model of the field generated in the resonant cavities of lasers, thus constituting a basic element for understanding laser theory. Usually, uniformly polarized beams are considered in the analytical calculations, with the electric field vibrating at normal planes to the propagation direction. However, such paraxial fields do not verify the Maxwell equations. In this paper we discuss how to overcome this apparent contradiction and evaluate the longitudinal component that any paraxial Gaussian beam should exhibit. Despite the fact that the assumption of a purely transverse paraxial field is useful and accurate, the inclusion of the above issue in the program helps students to clarify the importance of the electromagnetic nature of light, thus providing a more complete understanding of the paraxial approach.

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A comparison is established between the contributions of transverse and longitudinal components of both the propagating and the evanescent waves associated to freely propagating radially polarized nonparaxial beams. Attention is focused on those fields that remain radially polarized upon propagation. In terms of the plane-wave angular spectrum of these fields, analytical expressions are given for determining both the spatial shape of the above components and their relative weight integrated over the whole transverse plane. The results are applied to two kinds of doughnut-like beams with radial polarization, and we compare the behavior of such fields at two transverse planes.

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Objetivos: Este trabajo pretende, en base a nuestra experiencia, valorar y discutir las indicaciones, ventajas e inconvenientes de la exéresis de los épulis de la cavidad bucal con el láser de dióxido de carbono (CO2) respecto al láser de Erbio:YAG (Er:YAG), el láser de diodo y el bisturí frío. Material y método: Se ha realizado un estudio retrospectivo de un grupo de 120 pacientes en los que se extirparon 128 épulis con el láser de CO2, láser de Er:YAG, láser de diodo y bisturí frío. Se realizaron controles postoperatorios a los 7, 15 y 30 días para comprobar la cicatrización y la evolución de la herida y a los 3, 6 y 12 meses verificando si se había producido o no la recidiva de la lesión. Resultados: Según las características clínicas y etiopatogénicas de las lesiones extirpadas, se han formado dos grupos: las lesiones hiperplásicas gingivales (77 casos) y los épulis fisurados (51 casos). La localización más frecuente de las hiperplasias gingivales fue la mandíbula (51.9%). Se encontró que la hiperplasia fibrosa fue el diagnóstico histopatológico más frecuente con 49 casos (63.6%). El porcentaje de recidiva tras su extirpación fue del 9,1%, de los cuales 5 casos eran hiperplasias fibrosas. Sólo hubo un caso de lesión maligna que fue diagnosticada de carcinoma de células escamosas infiltrante. Por otro lado, de los 51 épulis fisurados tratados, el 58.8% se encontraban en el maxilar superior. Éstos fueron diagnosticados histológicamente como hiperplasias fibrosas, recidivando en el 19.6% de los casos. Conclusiones: Aunque las diferentes técnicas quirúrgicas utilizadas en la extirpación del épulis de la cavidad bucal son correctas, en nuestra opinión, el láser de CO2 es el tratamiento de elección, ya que ofrece ventajas tanto intra como postoperatorias. Por otro lado, es indispensable analizar histopatológicamente toda lesión de la cavidad bucal para establecer un diagnóstico de certeza

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Objetivos: Este trabajo pretende demostrar que se pueden realizar la mayoría de las intervenciones quirúrgicas de la cavidad bucal en la población pediátrica en un medio ambulatorio, así como valorar y mostrar la actividad realizada en el Máster de Cirugía e Implantología Bucal de la Facultad de Odontología de la Universidad de Barcelona durante el año 2000. Diseño del estudio: Para la realización de este trabajo se ha contabilizado la actividad quirúrgica de las unidades de cirugía bucal y cirugía con láser en la población pediátrica en el Máster de Cirugía e Implantología Bucal de la Universidad de Barcelona. Resultados: De las 3187 intervenciones quirúrgicas realizadas en nuestro servicio, 489 fueron en pacientes menores de 18 años. La exodoncia quirúrgica de terceros molares inferiores fue la más frecuente (55'6%), seguida de otras extracciones dentarias (33'6%), quirúrgicas o no, y del resto de intervenciones (10'6%) que incluyeron: fenestraciones de caninos u otros dientes incluidos, exéresis de frenillos, de mucoceles y reubicaciones dentarias. Se presentaron complicaciones tras la extracción quirúrgica de los terceros molares en un 15'93% de los casos, siendo las más frecuentes el dolor (4'35%) y la tumefacción (4'35%), signos propios de la inflamación postoperatoria. Conclusiones: Nuestra experiencia muestra que la cirugía bucal ambulatoria puede practicarse de forma segura en la población pediátrica siempre y cuando se disponga de los medios y del personal sanitario adecuados

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The possibility of printing two-dimensional micropatterns of biomolecule solutions is of great interest in many fields of research in biomedicine, from cell-growth and development studies to the investigation of the mechanisms of communication between cells. Although laser-induced forward transfer (LIFT) has been extensively used to print micrometric droplets of biological solutions, the fabrication of complex patterns depends on the feasibility of the technique to print micron-sized lines of aqueous solutions. In this study we investigate such a possibility through the analysis of the influence of droplet spacing of a water and glycerol solution on the morphology of the features printed by LIFT. We prove that it is indeed possible to print long and uniform continuous lines by controlling the overlap between adjacent droplets. We show how, depending on droplet spacing, several printed morphologies are generated, and we offer, in addition, a simple explanation of the observed behavior based on the jetting dynamics characteristic of the LIFT of liquids.

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The optical, mechanical, and microstructural properties of MgF2 single layers grown by ion beam sputtering have been investigated by spectrophotometric measurements, film stress characterization, x-ray photoelectron spectroscopy (XPS), x-ray diffraction, and transmission electron microscopy. The deposition conditions, using fluorine reactive gas or not, have been found to greatly influence the optical absorption and the stress of the films as well as their microstructure. The layers grown with fluorine compensation exhibit a regular columnar microstructure and an UV-optical absorption which can be very low, either as deposited or after thermal annealings at very low temperatures. On the contrary, layers grown without fluorine compensation exhibit a less regular microstructure and a high ultraviolet absorption which is particularly hard to cure. On the basis of calculations, it is shown that F centers are responsible for this absorption, whereas all the films were found to be stoichiometric, in the limit of the XPS sensitivity. On the basis of external data taken from literature, our experimental curves are analyzed, so we propose possible diffusion mechanisms which could explain the behaviors of the coatings.