925 resultados para NM LASER


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Abstract Background Recent reviews have indicated that low level level laser therapy (LLLT) is ineffective in lateral elbow tendinopathy (LET) without assessing validity of treatment procedures and doses or the influence of prior steroid injections. Methods Systematic review with meta-analysis, with primary outcome measures of pain relief and/or global improvement and subgroup analyses of methodological quality, wavelengths and treatment procedures. Results 18 randomised placebo-controlled trials (RCTs) were identified with 13 RCTs (730 patients) meeting the criteria for meta-analysis. 12 RCTs satisfied half or more of the methodological criteria. Publication bias was detected by Egger's graphical test, which showed a negative direction of bias. Ten of the trials included patients with poor prognosis caused by failed steroid injections or other treatment failures, or long symptom duration or severe baseline pain. The weighted mean difference (WMD) for pain relief was 10.2 mm [95% CI: 3.0 to 17.5] and the RR for global improvement was 1.36 [1.16 to 1.60]. Trials which targeted acupuncture points reported negative results, as did trials with wavelengths 820, 830 and 1064 nm. In a subgroup of five trials with 904 nm lasers and one trial with 632 nm wavelength where the lateral elbow tendon insertions were directly irradiated, WMD for pain relief was 17.2 mm [95% CI: 8.5 to 25.9] and 14.0 mm [95% CI: 7.4 to 20.6] respectively, while RR for global pain improvement was only reported for 904 nm at 1.53 [95% CI: 1.28 to 1.83]. LLLT doses in this subgroup ranged between 0.5 and 7.2 Joules. Secondary outcome measures of painfree grip strength, pain pressure threshold, sick leave and follow-up data from 3 to 8 weeks after the end of treatment, showed consistently significant results in favour of the same LLLT subgroup (p < 0.02). No serious side-effects were reported. Conclusion LLLT administered with optimal doses of 904 nm and possibly 632 nm wavelengths directly to the lateral elbow tendon insertions, seem to offer short-term pain relief and less disability in LET, both alone and in conjunction with an exercise regimen. This finding contradicts the conclusions of previous reviews which failed to assess treatment procedures, wavelengths and optimal doses.

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Nerve-related complications have been frequently reported in dental procedures, and a very frequent type of occurrence involves the inferior alveolar nerve (IAN). The nerve injury in humans often results in persistent pain accompanied by allodynia and hyperalgesia. In this investigation, we used an experimental IAN injury in rats, which was induced by a Crile hemostatic clamp, to evaluate the effects of laser therapy on nerve repair. We also studied the nociceptive behavior (von Frey hair test) before and after the injury and the behavioral effects of treatment with laser therapy (emitting a wavelength of 904 nm, output power of 70 Wpk, a spot area of *0.1 cm2, frequency of 9500 Hz, pulse time 60 ns and an energy density of 6 J/cm2). As neurotrophins are essential for the process of nerve regeneration, we used immunoblotting techniques to preliminarily examine the effects of laser therapy on the expression of nerve growth factor (NGF) and brainderived neurotrophic factor (BDNF). The injured animals treated with laser exhibited an improved nociceptive behavior. In irradiated animals, there was an enhanced expression of NGF (53%) and a decreased BDNF expression (40%) after laser therapy. These results indicate that BDNF plays a locally crucial role in pain-related behavior development after IAN injury, increasing after lesions (in parallel to the installation of pain behavior) and decreasing with laser therapy (in parallel to the improvement of pain behavior). On the other hand, NGF probably contributes to the repair of nerve tissue, in addition to improving the pain-related behavior.

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Intestinal ischemia and reperfusion (i-I/R) is an insult associated with acute respiratory distress syndrome (ARDS). It is not known if pro- and anti-inflammatory mediators in ARDS induced by i-I/R can be controlled by low-level laser therapy (LLLT). This study was designed to evaluate the effect of LLLT on tracheal cholinergic reactivity dysfunction and the release of inflammatory mediators from the lung after i-I/R. Anesthetized rats were subjected to superior mesenteric artery occlusion (45 min) and killed after clamp release and preestablished periods of intestinal reperfusion (30 min, 2 or 4 h). The LLLT (660 nm, 7.5 J/cm(2)) was carried out by irradiating the rats on the skin over the right upper bronchus for 15 and 30 min after initiating reperfusion and then euthanizing them 30 min, 2, or 4 h later. Lung edema was measured by the Evans blue extravasation technique, and pulmonary neutrophils were determined by myeloperoxidase (MPO) activity. Pulmonary tumor necrosis factor-α (TNF-α), interleukin-10 (IL-10), intercellular adhesion molecule-1 (ICAM-1), and isoform of NO synthase (iNOS) mRNA expression were analyzed by real-time PCR. TNF-α, IL-10, and iNOS proteins in the lung were measured by the enzyme-linked immunoassay technique. LLLT (660 nm, 7.5 J/cm(2)) restored the tracheal hyperresponsiveness and hyporesponsiveness in all the periods after intestinal reperfusion. Although LLLT reduced edema and MPO activity, it did not do so in all the postreperfusion periods. It was also observed with the ICAM-1 expression. In addition to reducing both TNF-α and iNOS, LLLT increased IL-10 in the lungs of animals subjected to i-I/R. The results indicate that LLLT can control the lung's inflammatory response and the airway reactivity dysfunction by simultaneously reducing both TNF-α and iNOS.

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Low level laser therapy is used as a treatment of several conditions, including inflammatory processes and wound healing. Possible changes in mechanical properties of cells, caused by illumination, are investigated with optical magnetic twisting cytometry (OMTC), which is a technique used to evaluate mechanical properties in cell culture. Ferromagnetic micro beads are bound to cell cytoskeleton, the beads are magnetized vertically and a horizontal twisting magnetic field is applied causing a torque that moves the beads and deforms the cell, the beads rotate and displace. Based on the lateral displacement of the beads, elastic shear and loss moduli are obtained. Samples of human bronchial epithelial cell culture were divided in two groups: one was illuminated with a 660 nm red laser, 30 mW power, 0.75 W/cm2 irradiance, during different time intervals, and the other one, the control group, was not illuminated. The values of the mechanical constants of the cells of the control group showed a tendency of increasing with the time out of the incubator. On the other hand, the illuminated group showed constancy on the behavior of both moduli, keeping the normal conditions of the cell culture. Those results indicate that illumination can induce cells to homeostasis, and OMTC is sensitive to observe departures from the steady conditions. Hence, OMTC is an important technique which can be used to aggregate knowledge on the light effect in cell cytoskeleton and even on the low level laser therapy mechanisms in inflammatory processes and/or wound healing.

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Low level laser therapy is used as a treatment of several conditions, including inflammatory processes and wound healing. Possible changes in mechanical properties of cells, caused by illumination, are investigated with optical magnetic twisting cytometry (OMTC), which is a technique used to evaluate mechanical properties in cell culture. Ferromagnetic micro beads are bound to cell cytoskeleton, the beads are magnetized vertically and a horizontal twisting magnetic field is applied causing a torque that moves the beads and deforms the cell, the beads rotate and displace. Based on the lateral displacement of the beads, elastic shear and loss moduli are obtained. Samples of human bronchial epithelial cell culture were divided in two groups: one was illuminated with a 660 nm red laser, 30 mW power, 0.75 W/cm2 irradiance, during different time intervals, and the other one, the control group, was not illuminated. The values of the mechanical constants of the cells of the control group showed a tendency of increasing with the time out of the incubator. On the other hand, the illuminated group showed constancy on the behavior of both moduli, keeping the normal conditions of the cell culture. Those results indicate that illumination can induce cells to homeostasis, and OMTC is sensitive to observe departures from the steady conditions. Hence, OMTC is an important technique which can be used to aggregate knowledge on the light effect in cell cytoskeleton and even on the low level laser therapy mechanisms in inflammatory processes and/or wound healing.

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The objectives of this study were to evaluate the effect of low-level laser irradiation (LLLI) on bovine oocyte and granulosa cells metabolism during in vitro maturation (IVM) and further embryo development. Cumulus-oocytes complexes (COCs) were subjected (experimental group) or not (control group) to irradiation with LLLI in a 633-nm wavelength and 1 J/cm2 fluency. The COCs were evaluated after 30 min, 8, 16, and 24 h of IVM. Cumulus cells were evaluated for cell cycle status, mitochondrial activity, and viability (flow cytometry). Oocytes were assessed for meiotic progression status (nuclear staining), cell cycle genes content [real-time polymerase chain reaction (PCR)], and signal transduction status (western blot). The COCs were also in vitro fertilized, and the cleavage and blastocyst rates were assessed. Comparisons among groups were statistically performed with 5% significance level. For cumulus cells, a significant increase in mitochondrial membrane potential and the number of cells progressing through the cycle could be observed. Significant increases on cyclin B and cyclin-dependent kinase (CDK4) levels were also observed. Concerning the oocytes, a significantly higher amount of total mitogen-activated protein kinase was found after 8 h of irradiation, followed by a decrease in all cell cycle genes transcripts, exception made for the CDK4. However, no differences were observed in meiotic progression or embryo production. In conclusion, LLLI is an efficient tool to modulate the granulosa cells and oocyte metabolism

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Introduction: Laser hair removal is becoming an increasingly popular alternative to traditional methods such as shaving, waxing, among other methods. Semiconductor diode lasers are considered the most efficient light sources available and are especially well suited for clinical applications including hair reduction. The effectiveness of laser hair reduction depends on many variables, including the skin type of the patient. Material and Methods: A patient with Fitzpatrick Skin Type IV was submitted to laser hair removal of the arms with a high-power diode laser system with long pulses with a wavelength of 800 nm, a fluence of 40 J/cm2 and a pulse width of 20 ms. A 12-month follow-up assessment was performed and included photography and questionnaire. Results: Hypopigmentation was observed after a single laser hair removal section. After 6 months with the area totally covered, a gradual suntan with a sun screen lotion with an SPF of 15 was prescribed by the dermatologist. After 12 months of the initial treatment, a complete recovery of the hypopigmentation was achieved. Conclusion: Although a safe procedure, lasers for hair removal may be associated with adverse side effects including undesired pigment alterations. Before starting a laser hair removal treatment, patients seeking the eradication of hair should be informed that temporary, and possibly permanent, pigmentary changes may occur.

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Objectives: The objective of this study was to apply low-level laser therapy (LLLT) to accelerate the recovery process of a child patient with Bell's palsy (BP). Design: This was a prospective study. Subject: The subject was a three-year-old boy with a sudden onset of facial asymmetry due to an unknown cause. Materials and methods: The low-level laser source used was a gallium aluminum arsenide semiconductor diode laser device (660nm and 780 nm). No steroids or other medications were given to the child. The laser beam with a 0.04-cm2 spot area, and an aperture with approximately 1-mm diameter, was applied in a continuous emission mode in direct contact with the facial area. The duration of a laser session was between 15 and 30 minutes, depending on the chosen points and the area being treated. Light was applied 10 seconds per point on a maximum number of 80 points, when the entire affected (right) side of the face was irradiated, based on the small laser beam spot size. According to the acupuncture literature, this treatment could also be carried out using 10-20 Chinese acupuncture points, located unilaterally on the face. In this case study, more points were used because the entire affected side of the face (a large area) was irradiated instead of using acupuncture points. Outcome measures: The House-Brackmann grading system was used to monitor the evolution of facial nerve motor function. Photographs were taken after every session, always using the same camera and the same magnitude. The three-year-old boy recovered completely from BP after 11 sessions of LLLT. There were 4 sessions a week for the first 2 weeks, and the total treatment time was 3 weeks. Results: The result of this study was the improvement of facial movement and facial symmetry, with complete reestablishment to normality. Conclusions: LLLT may be an alternative to speed up facial normality in pediatric BP.

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In der vorliegenden Arbeit ist die Konstruktion und der Aufbau eines Systems zur gepulsten Laserablation von dünnen Schichten beschrieben. Die hohe Flexibilität der Anlage wird ermöglicht durch einen sechsfach-Targethalter und eine Heizerkonstruktion, die einfachen Substrateinbau, hohe Temperaturhomogenität und einen zugänglichen Temperaturbereich von bis zu 1000°C erlaubt. Durch eine komplexe Laser-Optik, die eine homogene Energiedichte auf dem Target sicherstellt, wird eine optimale Filmqualität erreicht.Durch die Entwicklung einer zweistufigen Prozeßführung für Y-stabilisiertes ZrO2 wird eine Wachstumsbasis hoher kristalliner Qualität für funktionale Oxidschichten auf Silizium zur Verfügung gestellt. Es zeigt sich, daß die dielektrischen Eigenschaften der YSZ Schicht stark vom Sauerstoffgehalt, der Grenzflächenmorphologie sowie der Dicke der ersten Schicht abhängig sind. Basierend auf dieser Schicht wurde BaZrO3 als zusätzliche Pufferschicht für den Hochtemperatursupraleiter (HTSL) YBa2Cu3O7 ? untersucht. Unter Verwendung von SrTiO3 Substraten konnte die dielektrische Konstante von BaZrO3 zu ? ? 65 bestimmt sowie das Dispersionsverhalten mittels modifizierter Debye-Gleichungen erklärt werden. Vergleichende Messungen auf einkristallinen SrTiO3 Substraten zeigen eine erhöhte Übergangstemperatur von 90.2 K und eine wesentliche Verbesserung der Oberflächenrauhigkeit des HTSL von 2 nm (rms) durch die Verwendung von BaZrO3 Schichten hoher Qualität. Eine nur wenige Monolagen dicke zusätzliche BaZrO3 Pufferschicht auf YSZ-gepufferten Silizium Substraten verhindert die Ausbildung von ?9° rotierten YBCO Körnern, die üblicherweise bei der direkten Deposition auf YSZ beobachtet werden. Resistive Messungen mit Übergangstemperaturen oberhalb 89 K sind vergleichbar zu Ergebnissen, die für CeO2/YSZ Pufferschichtkombinationen erreicht werden. Durch kontinuierliche Gitteranpassung wurde eine neue Schichtabfolge YBCO/CeO2/YSZ/BaZrO3 für die Erzeugung bi-epitaxialer Korngrenzen-Josephson Kontake gefunden und deren Epitaxiebeziehungen geklärt. Eine in-situ deponierte Schichtabfolge zeigt mit einer Übergangstemperatur von 91.7 K und einer Übergangsbreite von 0.15 K supraleitende Eigenschaften vergleichbar zu den besten bisher auf diesem Gebiet erreichten Ergebnissen. Voruntersuchungen zur Realisierung eines Josephsonkontaktes mit dieser Schichtabfolge zeigen jedoch, daß die erreichten Eigenschaften für die technologische Anwendung nicht ausreichend sind.Die Verwendung einer YSZ/CeO2 Pufferschichtkombination ermöglicht die Herstellung von c Achsen orientiertem ferroelektrischem SrBi2Ta2O9 auf Silizium. Im Gegensatz hierzu führt die direkte Deposition auf Silizium zu polykristallinem SrBi2Ta2O9 oder zur Ausbildung der Pyrochlor Phase, wenn nur YSZ als Pufferschicht verwendet wird. Obwohl die Polarisierung von SrBi2Ta2O9 in der ab-Ebene liegt, konnte in MFIS Strukturen ein Speicherfenster von maximal 0.87 V beobachtet werden, was eine Verbesserung um nahezu einen Faktor drei im Vergleich zu polykristallinem SrBi2Ta2O9 bedeutet. Messungen an ferroelektrischen Kondesatorstrukturen ergeben Hystereseschleifen mit einer remanenten Polarisierung von Pr = 6.5 µC/cm2 sowie einem Koerzitivfeld von Ec = 35 kV/cm. AFM Messungen im Piezo-Response Modus zeigen ferroelektrische Domänen, die durch Anlegen einer Gleichspannung reversibel umpolarisiert werden können. Im Nicht-Kontakt AFM Modus wurde die lokale Polarisierung der Schichten zu 3.4 µC/cm2 bestimmt. Weiterhin wurde eine alternative Pufferschichtkombination SrZrO3/YSZ zur Erzeugung von a-Achsen orientiertem SrBi2Ta2O9 untersucht. SrZrO3 zeigt a Achsen Orientierung in vier Wachstumsdomänen, die durch ein Model erklärt werden können. Die SrBi2Ta2O9 Schicht zeigt a Achsen sowie (116)-orientierte Körner mit derselben Domänenstruktur. Die dielektrische Konstanten von SrZrO3 und SrBi2Ta2O9 wurden zu ? ? 29 und ? ? 20 bestimmt. Die beobachteten Speicherfenster sind allerdings nicht ferroelektrischer Natur, sondern wahrscheinlich durch mobile Ionen und Ladungsfangstellen in den Pufferschichten verursacht. Die stark abgesenkte dielektrische Konstante von SrBi2Ta2O9 kann durch die im Vergleich zu polykristallinem verkleinerte Korngröße erklärt werden.

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Time-of-flight photoemission spectromicroscopy was used to measure and compare the two-photon photoemission (2PPE) spectra of Cu and Ag nanoparticles with linear dimensions ranging between 40 nm and several 100 nm, with those of the corresponding homogeneous surfaces. 2PPE was induced employing femtosecond laser radiation from a frequency-doubled Ti:sapphire laser in the spectral range between 375 nm and 425 nm with a pulse width of 200 fs and a repetition rate of 80 MHz. The use of a pulsed radiation source allowed us to use a high-resolution photoemission electron microscope as imaging time-of-flight spectrometer, and thus to obtain spectroscopic information about the laterally resolved electron signal. Ag nanoparticle films have been deposited on Si(111) by electron-beam evaporation, a technique leading to hemispherically-shaped Ag clusters. Isolated Cu nanoparticles have been generated by prolonged heating of a polycrystalline Cu sample. If compared to the spectra of the corresponding homogeneous surfaces, the Cu and Ag nanoparticle spectra are characterized by a strongly enhanced total 2PPE yield (enhancement factor up to 70), by a shift (about 0.1 eV) of the Fermi level onset towards lower final state energies, by a reduction of the work function (typically by 0.2 eV) and by a much steeper increase of the 2PPE yield towards lower final state energies. The shift of the Fermi level onset in the nanoparticle spectra has been explained by a positive unit charge (localized photohole) residing on the particle during the time-scale relevant for the 2PPE process (few femtoseconds). The total 2PPE yield enhancement and the different overall shape of the spectra have been explained by considering that the laser frequency was close to the localized surface plasmon resonance of the Cu and Ag nanoparticles. The synchronous oscillations induced by the laser in the metal electrons enhance the near-zone (NZ) field, defined as the linear superposition of the laser field and the field produced in the vicinity of the particles by the forced charge oscillations. From the present measurements it is clear that the NZ field behavior is responsible for the 2PPE enhancement and affects the 2PPE spatial and energy distribution and its dynamics. In particular, its strong spatial dependence allows indirect transitions through real intermediate states to take place in the metal clusters. Such transitions are forbidden by momentum conservation arguments and are thus experimentally much less probable on homogeneous surfaces. Further, we investigated specially tailored moon-shaped small metal nanostructures, whose NZ field was theoretically predicted, and compared the calculation with the laterally resolved 2PPE signal. We could show that the 2PPE signal gives a clear fingerprint of the theoretically predicted spatial dependence of the NZ field. This potential of our method is highly attractive in the novel field of plasmonics.

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Recent developments in the theory of plasma-based collisionally excited x-ray lasers (XRL) have shown an optimization potential based on the dependence of the absorption region of the pumping laser on its angle of incidence on the plasma. For the experimental proof of this idea, a number of diagnostic schemes were developed, tested, qualified and applied. A high-resolution imaging system, yielding the keV emission profile perpendicular to the target surface, provided positions of the hottest plasma regions, interesting for the benchmarking of plasma simulation codes. The implementation of a highly efficient spectrometer for the plasma emission made it possible to gain information about the abundance of the ionization states necessary for the laser action in the plasma. The intensity distribution and deflection angle of the pump laser beam could be imaged for single XRL shots, giving access to its refraction process within the plasma. During a European collaboration campaign at the Lund Laser Center, Sweden, the optimization of the pumping laser incidence angle resulted in a reduction of the required pumping energy for a Ni-like Mo XRL, which enabled the operation at a repetition rate of 10 Hz. Using the experiences gained there, the XRL performance at the PHELIX facility, GSI Darmstadt with respect to achievable repetition rate and at wavelengths below 20 nm was significantly improved, and also important information for the development towards multi-100 eV plasma XRLs was acquired. Due to the setup improvements achieved during the work for this thesis, the PHELIX XRL system now has reached a degree of reproducibility and versatility which is sufficient for demanding applications like the XRL spectroscopy of heavy ions. In addition, a European research campaign, aiming towards plasma XRLs approaching the water-window (wavelengths below 5 nm) was initiated.

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Advances in metastability exchange optical pumping (MEOP) of 3He at high laser powers, with its various applications, but also at high gas pressures p3 and high magnetic field strengths B, have provided strong motivation for revisiting the understanding and for investigating the limitations of this powerful technique. For this purpose, we present systematic experimental and theoretical studies of efficiency and of relaxation mechanisms in B≤30 mT and p3=0.63−2.45 mbar. 3He nuclear polarisation is measured by light absorption in longitudinal configuration where weak light beams at 1083 nm parallel to magnetic field and cell axis with opposite circular polarisations are used to probe the distribution of populations in the metastable state. This method is systematically tested to evaluate potential systematic biases and is shown to be reliable for the study of OP dynamics despite the redistribution of populations by OP light. Nuclear polarisation loss associated to the emission of polarised light by the plasma discharge used for MEOP is found to decrease above 10 mT, as expected, due to hyperfine decoupling in highly excited states. However, this does not lead to improved MEOP efficiency at high laser power. We find clear evidence of additional laser-induced relaxation instead. The strong OP-enhanced polarisation losses, currently limiting MEOP performances, are quantitatively investigated using an angular momentum budget approach and a recently developed comprehensive model that describes the combined effects of OP, ME and relaxation, validated by comparison to experimental results.

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L’attività sperimentale presentata in questo elaborato riguarda lo studio di una particolare applicazione che impiega la tecnologia laser per la lavorazione di materiali compositi ed è stata interamente svolta, in particolar modo nella sua parte operativa, presso i laboratori della Facoltà di Ingegneria a Bologna. Il lavoro di tesi ha come obiettivo fondamentale la valutazione degli effetti che i parametri di processo possono avere sulla qualità risultante nel procedimento di ablazione per i materiali compositi. Per questa indagine sono stati utilizzati campioni piani (tutti identici tra loro) con rinforzo in fibra di carbonio e matrice in resina epossidica, i quali sono stati lavorati con un laser Nd:YAG (λ = 1064 nm) funzionante in regime continuo. L’idea alla base dell’intera attività sperimentale è stata quella di realizzare una ablazione ottimale, rimuovendo dai campioni esclusivamente la resina (in maniera locale) e tentando, allo stesso tempo, di ottenere il minimo danneggiamento possibile per le fibre. Le prove effettuate non costituiscono naturalmente un punto di arrivo, bensì rappresentano piuttosto un punto di partenza per acquisire informazioni preliminari che potranno consentire, nel prossimo futuro, di proseguire con il perfezionamento del processo e la messa a punto dei parametri, al fine di conseguire una lavorazione che dia risultati effettivamente ottimali ed interessanti per l’eventuale applicazione industriale.

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Die kollineare Laserspektroskopie hat sich in den vergangenen drei Jahrzehnten zur Bestimmung der Kernladungsradien mittelschwerer und schwerer kurzlebiger Atomkerne in ausgezeichneter Weise bewährt. Auf die Isotope sehr leichter Elemente konnte sie allerdings erst kürzlich erweitert werden. Dieser Bereich der Nuklidkarte ist von besonderem Interesse, denn die ersten ab-initio Modelle der Kernphysik, die den Aufbau eines Atomkerns basierend auf individuellen Nukleonen und realistischenWechselwirkungspotentialen beschreiben, sind gegenwärtig nur für die leichtesten Elemente anwendbar. Außerdem existiertrnin dieser Region eine besonders exotische Form von Atomkernen, die sogenanntenrnHalokerne. Die Isotopenkette der Berylliumisotope zeichnet sich durch das Auftreten des Ein-Neutronen Halokerns 11Be und des Zwei- oder Vier-Neutronen-Halos 14Be aus. Dem Isotop 12Be kommt durch seine Position zwischen diesen beiden Exoten und den im Schalenmodell erwarteten magischen Schalenabschluss N = 8 eine besondere Bedeutung zu.rnIm Rahmen dieser Arbeit wurden mehrere frequenzstabilisierte Lasersysteme für die kollineare Laserspektroskopie aufgebaut. An TRIGA-SPEC stehen nun unter anderem ein frequenzverdoppeltes Diodenlasersystem mit Trapezverstärker und frequenzkammstabilisierter Titan-Saphirlaser mit Frequenzverdopplungsstufe für die Spektroskopie an refraktären Elementen oberhalb von Molybdän zur Verfügung, die für erste Testexperimente eingesetzt wurden. Außerdem wurde die effiziente Frequenzvervierfachung eines Titan-Saphirlasers demonstriert. An ISOLDE/CERN wurde ein frequenzkammstabilisierter und ein jodstabilisierter Farbstofflaser installiert und für die Laserspektroskopie an 9,10,11,12Be eingesetzt. Durch das verbesserte Lasersystem und den Einsatz eines verzögerten Koinzidenznachweises für Photonen und Ionen gelang es die Empfindlichkeitrnder Berylliumspektroskopie um mehr als zwei Größenordnungen zu steigern und damit die früheren Messungen an 7−11Be erstmals auf das Isotop 12Be auszuweiten. Außerdem wurde die Genauigkeit der absoluten Übergangsfrequenzen und der Isotopieverschiebungen der Isotope 9,10,11Be signifikant verbessert.rnDurch den Vergleich mit Ergebnissen des Fermionic Molecular Dynamics Modells kann der Trend der Ladungsradien der leichteren Isotope durch die ausgeprägte Clusterstruktur der Berylliumkerne erklärt werden. Für 12Be wird ersichtlich, dass der Grundzustand durch eine (sd)2 Konfiguration statt der vom Schalenmodell erwarteten p2 Konfiguration dominiert wird. Dies ist ein klares Indiz für das bereits zuvor beobachtete Verschwinden des N = 8 Schalenabschlusses bei 12Be.

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In questo lavoro di Tesi viene studiata la realizzazione di un sistema per la generazione di seconda armonica di una luce laser infrarossa. Il lavoro è stato svolto presso l'Univerità di Firenze nell'ambito di un esperimento di fisica atomica, nel quale viene studiato il comportamento di una miscela di atomi freddi di Potassio-Rubidio. Per la realizzazione sperimentale è richiesto l'utilizzo di un fascio laser con luce verde a 532 nm. Per ottenere questo fascio si è ricorso alla generazione di seconda armonica di un laser con luce infrarossa a 1064 nm, sfruttando le proprietà dei cristalli non lineari. Il cristallo utilizzato è un cristallo periodically poled di Tantalato di Litio, che sfrutta la tecnica del Quasi-Phasematching per generare seconda armonica. L'obiettivo principale di questo lavoro è stato quello di caratterizzare il sistema di duplicazione per poter ottimizzare la produzione del fascio verde. Infatti la produzione di seconda armonica dipende da diversi fattori sperimentali, quali la temperatura alla quale si trova il cristallo e la posizione del fuoco del fascio incidente rispetto al cristallo. Per prima cosa si sono ottimizzati i parametri del fascio infrarosso, cercando quelli per i quali la produzione di seconda armonica è maggiormente efficiente. Questo è stato effettuato caratterizzando il fascio per trovarne la posizione del fuoco e la sua larghezza. Nella seconda parte si è studiata l'efficienza di produzione di seconda armonica. La temperatura del cristallo influenza notevolmente la produzione di seconda armonica, quindi si è cercata la temperatura ottimale a cui l'efficienza di duplicazione è massima. Inoltre si è anche calcolata l'ampiezza massima delle oscillazioni di temperatura a cui è possibile sottoporre il cristallo senza uscire dalla zona in cui la duplicazione è efficiente. Per trovare la temperatura ottimale si è studiato l'andamento dell'efficienza in funzione della temperatura del cristallo. Analizzando questo andamento si sono anche verificati i coefficienti non lineari del cristallo dichiarati dal produttore.