How low-level laser therapy can change mechanical properties of cells.

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.

Photobiological effect of low-level laser irradiation in bovine embryo production system

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

A 12-month follow-up of hypopigmentation after laser hair removal

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.

Low-level laser therapy in pediatric Bell's palsy: case report in a three-year-old child

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.

In-situ-Präparation von komplexen supraleitenden und ferroelektrischen Heterostrukturen mittels gepulster Laser-Deposition

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.

Time-of-flight two-photon photoemission spectromicroscopy with femtosecond laser radiation

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.

Characterization and optimization of an x-ray laser for the spectroscopy of Li-like heavy-ions

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.

Metastability exchange optical pumping in 3 He gas up to 30 mT: Efficiency measurements and evidence of laser-induced nuclear relaxation

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.

Valutazione degli effetti dei parametri operativi nel processo di laser ablation su materiali compositi CFRP a matrice epossidica

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.

Laser systems for collinear spectroscopy and the charge radius of 12 Be

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.

Studio di un sistema per la generazione di seconda armonica di un laser infrarosso

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.

Analyse der intrazellulären Freisetzung von Wirkstoffmodellen via konfokaler Laser-Raster-Mikroskopie

In der vorliegenden Arbeit wurde gezeigt, wie man das Potential nanopartikulärer Systeme, die vorwiegend via Miniemulsion hergestellt wurden, im Hinblick auf „Drug Delivery“ ausnutzen könnte, indem ein Wirkstoffmodell auf unterschiedliche Art und Weise intrazellulär freigesetzt wurde. Dies wurde hauptsächlich mittels konfokaler Laser-Raster-Mikrokopie (CLSM) in Kombination mit dem Bildbearbeitungsprogramm Volocity® analysiert.rnPBCA-Nanokapseln eigneten sich besonders, um hydrophile Substanzen wie etwa Oligonukleotide zu verkapseln und sie so auf ihrem Transportweg in die Zellen vor einem etwaigen Abbau zu schützen. Es konnte eine Freisetzung der Oligonukleotide in den Zellen aufgrund der elektrostatischen Anziehung des mitochondrialen Membranpotentials nachgewiesen werden. Dabei war die Kombination aus Oligonukleotid und angebundenem Cyanin-Farbstoff (Cy5) an der 5‘-Position der Oligonukleotid-Sequenz ausschlaggebend. Durch quantitative Analysen mittels Volocity® konnte die vollständige Kolokalisation der freigesetzten Oligonukleotide an Mitochondrien bewiesen werden, was anhand der Kolokalisationskoeffizienten „Manders‘ Coefficients“ M1 und M2 diskutiert wurde. Es konnte ebenfalls aufgrund von FRET-Studien doppelt markierter Oligos gezeigt werden, dass die Oligonukleotide weder beim Transport noch bei der Freisetzung abgebaut wurden. Außerdem wurde aufgeklärt, dass nur der Inhalt der Nanokapseln, d. h. die Oligonukleotide, an Mitochondrien akkumulierte, das Kapselmaterial selbst jedoch in anderen intrazellulären Bereichen aufzufinden war. Eine Kombination aus Cyanin-Farbstoffen wie Cy5 mit einer Nukleotidsequenz oder einem Wirkstoff könnte also die Basis für einen gezielten Wirkstofftransport zu Mitochondrien liefern bzw. die Grundlage schaffen, eine Freisetzung aus Kapseln ins Zytoplasma zu gewährleisten.rnDer vielseitige Einsatz der Miniemulsion gestattete es, nicht nur Kapseln sondern auch Nanopartikel herzustellen, in welchen hydrophobe Substanzen im Partikelkern eingeschlossen werden konnten. Diese auf hydrophobe Wechselwirkungen beruhende „Verkapselung“ eines Wirkstoffmodells, in diesem Fall PMI, wurde bei PDLLA- bzw. PS-Nanopartikeln ausgenutzt, welche durch ein HPMA-basiertes Block-Copolymer stabilisiert wurden. Dabei konnte gezeigt werden, dass das hydrophobe Wirkstoffmodell PMI innerhalb kürzester Zeit in die Zellen freigesetzt wurde und sich in sogenannte „Lipid Droplets“ einlagerte, ohne dass die Nanopartikel selbst aufgenommen werden mussten. Daneben war ein intrazelluläres Ablösen des stabilisierenden Block-Copolymers zu verzeichnen, welches rn8 h nach Partikelaufnahme erfolgte und ebenfalls durch Analysen mittels Volocity® untermauert wurde. Dies hatte jedoch keinen Einfluss auf die eigentliche Partikelaufnahme oder die Freisetzung des Wirkstoffmodells. Ein großer Vorteil in der Verwendung des HPMA-basierten Block-Copolymers liegt darin begründet, dass auf zeitaufwendige Waschschritte wie etwa Dialyse nach der Partikelherstellung verzichtet werden konnte, da P(HPMA) ein biokompatibles Polymer ist. Auf der anderen Seite hat man aufgrund der Syntheseroute dieses Block-Copolymers vielfältige Möglichkeiten, Funktionalitäten wie etwa Fluoreszenzmarker einzubringen. Eine kovalente Anbindung eines Wirkstoffs ist ebenfalls denkbar, welcher intrazellulär z. B. aufgrund von enzymatischen Abbauprozessen langsam freigesetzt werden könnte. Somit bietet sich die Möglichkeit mit Nanopartikeln, die durch HPMA-basierte Block-Copolymere stabilisiert wurden, gleichzeitig zwei unterschiedliche Wirkstoffe in die Zellen zu bringen, wobei der eine schnell und der zweite über einen längeren Zeitraum hinweg (kontrolliert) freigesetzt werden könnte.rnNeben Nanokapseln sowie –partikeln, die durch inverse bzw. direkte Miniemulsion dargestellt wurden, sind auch Nanohydrogelpartikel untersucht worden, die sich aufgrund von Selbstorganisation eines amphiphilen Bock-Copolymers bildeten. Diese Nanohydrogelpartikel dienten der Komplexierung von siRNA und wurden hinsichtlich ihrer Anreicherung in Lysosomen untersucht. Aufgrund der Knockdown-Studien von Lutz Nuhn konnte ein Unterschied in der Knockdown-Effizienz festgestellt werden, je nach dem, ob 100 nm oder 40 nm große Nanohydrogelpartikel verwendet wurden. Es sollte festgestellt werden, ob eine größenbedingte, unterschiedlich schnelle Anreicherung dieser beiden Partikel in Lysosomen erfolgte, was die unterschiedliche Knockdown-Effizienz erklären könnte. CLSM-Studien und quantitative Kolokalisationsstudien gaben einen ersten Hinweis auf diese Größenabhängigkeit. rnBei allen verwendeten nanopartikulären Systemen konnte eine Freisetzung ihres Inhalts gezeigt werden. Somit bieten sie ein großes Potential als Wirkstoffträger für biomedizinische Anwendungen.rn

Laser-assisted lipolysis in the treatment of gynecomastia: a prospective study in 28 patients

Gynecomastia is the most common breast pathology. Numerous excisions and liposuction techniques have been described to correct bilateral male breast enlargement. Recently, there has been a shift from the open approach to minimally invasive techniques. This article reports a 5-year experience using laser-assisted lipolysis (LAL) to treat gynecomastia, and describes the surgical technique. Between January 2006 and December 2010, a total of 28 patients with bilateral gynecomastia were treated with LAL. Patients had a mean age of 36.5 years (range 24 to 56 years). LAL was performed with a 980-nm diode laser (continuous emission, 15 W power, 8-12 kJ total energy per breast) after tumescent anesthetic infiltration. The breast was evaluated objectively by two physicians who compared chest circumference and photographs. Patients were also asked to score the results using a visual analogue scale: 75 to 100 (very good), 50-74 (good), 25 to 49 (fair) and 0 to 24 (poor). The postoperative period for all patients was incident-free. After 6 months, 18 patients (64.3%) scored the results as "very good", 6 as "good" (21.4%), 3 as "fair" (10.7%) and 1 "poor" (3.6%). Mean chest circumferences pre- and postoperatively were, respectively, 117.4 ± 11.1 cm and 103.3 ± 7.5 cm (p < 0.001), corresponding to a mean difference of 14.1 cm. Physicians scored the photographs as "very good" in 22 patients (78.6%), as "good" in five patients (17.9%), and as "fair" in one patient (3.6%). LAL in gynecomastia is safe and produces significant effects on fatty tissue, with a reduction in breast volume, together with significant skin tightening. Provided an appropriate amount of energy is delivered by an experienced operator, the results are both significant and consistent.

Vibrational Relaxation of N2O (v2) by Atomic Oxygen Measured by Tunable Diode Laser Absorption Spectroscopy

Through the use of Transient Diode Laser Absorption Spectroscopy (TDLAS), the rate coefficient for the vibrational relaxation of N2O (ν2) by O(3P) at room temperature (32 ºC)) was determined to be (1.51 ± 0.11)x10-12 cm3molecule-1sec-1. A Q-switched, frequency quadrupled (266 nm) Nd:YAG laser pulse was used as the pump for this experiment. This pulse caused the photodissociation of O3 into O2 and O atoms.Excited oxygen (O(1D)) was collisionally quenched to ground state (O(3P)) by Ar and/or Xe. Photodissociation also caused a temperature jump within the system, exciting the ν2 state of N2O molecules. Population in the ν2 state was monitored through a TDLASobservation of a ν3 transition. Data were fit using a Visual Fortran 6.0 Global Fitting program. Analysis of room temperature data taken using only Ar to quench O atoms to the ground state gave the same rate coefficient as analysis of data taken using an Ar/Xe mixture, suggesting Ar alone is a sufficient bath gas. Experimentation was alsoperformed at -27 ºC and -82 ºC for a temperature dependence analysis. A linear regression analysis gave a rate coefficient dependence on temperature of ... for the rate coefficient of the vibrational relaxation of N2O (ν2) by atomic oxygen.

Multi-stage ytterbium fiber-amplifier seeded by a gain-switched laser diode

We demonstrated all-fiber amplification of 11 ps pulses from a gain-switched laser diode at 1064 nm. The diode was driven at a repetition rate of 40 MHz and delivered 13 µW of fiber-coupled average output power. For the low output pulse energy of 325 fJ we have designed a multi-stage core pumped pre-amplifier in order to keep the contribution of undesired amplified spontaneous emission as low as possible. By using a novel time-domain approach for determining the power spectral density ratio (PSD) of signal to noise, we identified the optimal working point for our pre-amplifier. After the pre-amplifier we reduced the 40 MHz repetition rate to 1 MHz using a fiber coupled pulse-picker. The final amplification was done with a cladding pumped Yb-doped large mode area fiber and a subsequent Yb-doped rod-type fiber. With our setup we reached a total gain of 73 dB, resulting in pulse energies of >5.6 µJ and peak powers of >0.5 MW. The average PSD-ratio of signal to noise we determined to be 18/1 at the output of the final amplification stage.