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Introduction
The concept of thermal ablation has proven a minimally invasive alternative or accompaniment to conventional tumour therapy. Patients with hepatic primary tumours or metastases are able to profit from it. Several modalities of thermal ablation exist, including radiofrequency ablation, microwave ablation and laser ablation. They differ in regards to their indications and their physical backgrounds, yet they all share the same aim: the hyperthermic ablation of tumorous target tissue.
At this point in time the maximum ablation diameter attained in a singular session using a singular applicator is about 30 mm. The maximum attainable volume is about 23 cm3. However, the mean and median of hepatic lesions exceed that number with about 50 mm. Most hepatic tumours therefore cannot be easily ablated in toto.
One of the main limitations of thermal ablation is the periprocedural transformation of vital tissue into a boundary layer. This boundary layer prevents efficient energy transmission into peripheral tissue and thus limits the potential of thermal ablation. The boundary layer is usually located centrally around the ablation applicator. In laser ablation the formation of this boundary layer is called carbonisation.
A technically simple, yet potentially effective approach to delay or prevent the formation of this boundary layer is the usage of a spacer. This perfused spacer cools the central zone surrounding the applicator. Therefore central temperatures remain beyond the point of carbonisation.
Methods
The development of two spacer prototypes took place in cooperation with the AG “Experimentelle Radiologie” of the University Clinic Charité. The first fully closed prototype featured an internal circulation of cooling fluid without tissue perfusion. The second open prototype perfused into tissue through an opened tip.
The conduct of this study included ex vivo experiments on bovine livers (n = 15) by means of laser ablation. Ablation diameter and ablation volume were recorded through MR-guided volumetry and manual displacement volumetry. The mean values of diameter and volume that were recorded when the stand-alone applicator system was used were then compared to the mean values recorded when using the closed spacer-supported applicator system and the open spacer-supported applicator system. The difference in values between the three applicator types were then examined for statistical significance using SPSS.
To exclude covariates a preliminary experiment was conducted which aimed to maximise power input of the laser and time interval while minimising the chance of carbonisation. For that, one of the variables was increased in intervals and the ablation diameter of all three applicator types was measured until carbonisation occurred.
Results
In the preliminary experiment it was found that following the increase of the pre-set power input of the laser a proportional increase of ablation diameter followed. However when increasing power input above 25 Watt almost instantaneous carbonisation of the central tissue occurred. This was the same for all three applicator types.
When increasing the time interval > 10 minutes the stand-alone applicator system showed central carbonisation, which was not the case when using the closed spacer-supported applicator system or the open spacer-supported applicator system. The two spacer prototypes only experienced carbonisation when a time interval of > 25 minutes was set. Thus the comparison of all three applicator types was conducted at 25 Watt and 10 minutes, whereas the comparison between the closed spacer-supported applicator system and the open spacer-supported applicator system was conducted at 25 Watt and 25 minutes.
During the first experiment the stand-alone applicator system achieved mean values of 37.50 mm ablation diameter and 23.61 cm3 ablation volume. This was a statistically significant (p < 0.001) increase to the values either spacer was able to attain: the closed spacer-supported applicator system recorded a mean value of 28.67 mm ablation diameter and 18.12 cm3 ablation volume, whereas the open spacer-supported applicator system recorded a mean value of 31.00 mm ablation diameter and 18.49 cm3 ablation volume. However, setting a longer time interval was not possible when the stand-alone applicator system was used for ablation. Due to this, a second experiment comparing mean ablation diameter and volume between the two spacer prototypes followed.
During the second experiment with a time interval of 25 minutes the closed spacer-supported applicator system attained a mean value of 52.07 mm ablation diameter and 75.25 cm3 ablation volume. These values showed a statistically significant (p < 0.001) difference in comparison to the open spacer-supported applicator system with mean values of 47.60 mm ablation diameter und 72.20 cm3 ablation volume.
Discussion
Within the framework of this study it was proven that the presence of a spacer between laser applicator and hepatic tissue was able to achieve a significant increase in ablation diameter and ablation volume. By using a closed spacer an increase in volume by a 3.19 factor of change was possible. The open spacer obtained an increase in volume by a 3.06 factor of change. The concept of using a spacer in thermal ablation as a proof of concept study is therefore valid and suitable for further pre-clinical studies.
With the growing importance of advanced lighting technologies, customers expect additional functionality and higher comfort from fluorescent lamps. However, the ability to regulate light intensity (dimmed operation), in particular, exerts enormous stress on fluorescent lamps’ electrodes, leading to increased electrode erosion and significantly reduced lifetimes. During the operation of a fluorescent lamp, free barium (the main compound of the electrode emitter) is produced at the electrode responsible for lowering the work function in order to enable energy-efficient and durable electrodes with lifetimes of up to 20,000 hours. Despite their relatively long lifetimes, electrodes remain the lifetime-limiting factor of a fluorescent lamp. Therefore, for practical applications (e.g., maintaining quality control, adjusting operational parameters, and evaluating new electrode designs), electrode erosion is of special interest. The actual erosion-measurement methods determine a time-averaged erosion level over several hundred operation hours. Thus, a quasi-instantaneous measuring method (short measurement) is still necessary to determine erosion during operation. Such a method would allow us to compare erosion under different discharge conditions (currents, frequencies, or heating currents) from the same electrode in the same lamp. This work focuses on the determination of absolute electrode erosion during the stationary operation of commonly used fluorescent lamps. Commercial T8 lamps (fluorescent lamps with a diameter of 8/8 inch) are investigated at the operating mode of commonly used electronic ballasts with frequencies of several kHz. Operations under standard and dimmed conditions with an additional heating current to reduce electrode erosion are investigated. Electrode erosion is characterized by the erosion of barium, the main compound of the electrode. Therefore, laser-induced fluorescence (LIF), which is the most sensitive method for this application, is applied to determine the absolute densities of the eroded barium in the electrode region. These densities are affected by the plasma in the electrode region and do not directly represent the absolute barium erosion. To overcome this limitation, a new method based on a special measurement technique in combination with a barium-diffusion-model is developed to determine the absolute barium erosion based on the measured densities. It has been found that the barium densities in the electrode region are lower than the equilibrium pressures produced by the reduction of the barium oxide. This could be caused either by a reduced reaction rate, the reduced diffusion of the reactant (primarily barium oxide) or by reduced barium transport through the porous emitter. However, these results suggest that barium erosion depends on temperature and emitter structure, which vary over an electrode’s lifetime. For currents significantly higher than the nominal lamp current, a drastic increase in emitter evaporation is found. Such, an increase in the lamp current from 300 mA to 500 mA leads to an increase in emitter evaporation by a factor of five. Using the lamp for a long period of time under these conditions therefore reduces the lifetime by a factor of five. Notably, at this dramatically increased erosion level, the hot spot temperature only increases from 1120 K to 1170 K. Investigation of various frequencies from 50 Hz to 5 kHz revealed no significant dependence of emitter evaporation on frequency.
The laser-matter interaction is a topic of current research. In this context, the interaction of intensive laser radiation with atomic clusters is of special interest. Du to the small cluster size, the laser field can penetrate the whole cluster volume, which leads to a high absorption of energy in the cluster. As a result, plasmas with high density and high temperature are produced. In the early phase of the laser-cluster interaction, free electrons are initially created in the cluster due to tunnel ionization or photoionization. Via collisions of these electrons with the cluster atoms, the ionization is increased and thus a dense nanoplasma is produced, which is heated by the laser. If free electrons leave the cluster during the laser-cluster interaction (outer ionization), a positive charge buildup is created. The associated charge repulsion finally can lead to the fragmentation of the cluster due to Coulomb explosion. Experimentally, interesting phenomena emerging from laser-excited clusters are observed, e.g., the creation of fast electrons, the production of highly charged ions, and X-ray emission. In this dissertation, the interaction of Gaussian laser pulses in the infrared regime with argon and xenon clusters is simulated by means of a nanoplasma model. Considering laser intensities in the non-relativistic regime, the relevant processes such as ionization, heating and expansion are theoretically described in this model with a set of coupled rate equations and hydrodynamic equations. One focus of the thesis is on the heating of the nanoplasma via inverse bremsstrahlung (IB), which is due to the absorption of laser photons in electron-ion collisions. In particular, the important question is investigated whether the consideration of the ionic structure – that means, the nuclear charge and the bound electrons – modifies the electron-ion collisions and thus the IB heating rate. Starting from a quantum statistical description, effective electron-ion potentials are used which account for both the screening due to the dense plasma and the inner ionic structure. Within the quantum mechanical first Born approximation, the consideration of the ionic structure leads to a drastic increase of the IB heating rate, in particular for high nuclear charges and low ionic charge states. However, for the parameters relevant in experiments, the applicability of the first Born approximation is questionable. Therefore, quantum mechanical calculations going beyond the first-order perturbation theory are performed. In addition, the IB heating rate is investigated with different classical methods. These are based either on transport cross sections for elastic electron-ion scattering or on classical simulations of inelastic scattering processes. Also within the classical approaches, the consideration of the ionic structure leads to an increase of the heating rate. However, this increase is shown to be only moderate. In a further part, the thesis focuses on the question how the dynamics of the laser-cluster interaction is influenced by the consideration of excited states. This is explored exemplarily for argon clusters excited by single or double laser pulses. The consideration of excitation processes in the nanoplasma leads to a decrease of the electron temperature and to an increase of the density of free electrons. Moreover, it is shown that the consideration of excitation processes results in an essential acceleration of the ionization dynamics. As a consequence, the mean ionic charge state in the plasma as well as the number of highly charged ions is significantly increased. For the population of ground states and excited states within an ionic charge state Z, collisional deexcitation processes play an important role. By means of an analytical relation between excitation and deexcitation cross sections, the rates for the respective processes in the presence of the laser field are calculated. The role of deexcitation processes is studied in detail, showing that the inclusion of these processes is essential for the correct theoretical description of the photon emission from laser-excited clusters. Based on these results, the photon yield is calculated for selected radiative transitions resulting from highly charged argon ions in the UV and X-ray regime.