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There has been a substantial evolution of anti-cancer therapies in the last decade, leading
to improved prognosis and disease-free survival of patients with melanoma. Due to the
number of patients that still develop resistance or to the high systemic toxicity and side
effects, new treatment options are still needed. Regardless of the type of therapeutic
interventions (except surgery), the reactive oxygen species (ROS) are a by-product or
contribute to the action mechanism of many successful therapies. In this context, medical
cold atmospheric plasma (CAP) arises as a promising tool, and studies are important to
prove the effectiveness of this new device.
Since combination therapies are the current standard way to treat melanoma, we explored
candidates to be combined with cold atmospheric plasma, with potential to become a
therapeutic option in the combination. Here, we tested the radiotherapy and clinically safe
mitochondrial inhibitor drugs. In the end of the study, both, ionizing radiation and four
mitochondrial-targeted-drugs showed to be promising candidates for the combination with
CAP. These combinations induced increased cytotoxicity and modulated the immune
system improving the anti-tumor immune response. Mitochondrial damage seems to be
the first stage to induce cellular deficiency and culminate in apoptotic cell death.
Furthermore the release of GM-CSF contribute to a pro inflammatory state and immune
system activation.
This dissertation showed that CAP serves as an excellent tool to boost melanoma cell
death and induce anti-tumor response. In addition, in our proposed therapeutic
combination, the intensity of plasma treatment could be decreased possibly resulting in
less systemic toxicity. Our results serves as model to be studied in other tumor entities.
Due to a variety of plasma sources in terms of type of discharge, energy yield, working gas or geometric factors, it is recommended to standardize the study protocol by choosing a plasma source and easy access to rugged tumor surfaces as demonstrated by the CAP-plasma-jet. The intention of the trial shall be to optimize the plasma jet for tumor site capability and operating room implementation.
It makes sense to start clinical trials in plasma medicine with the treatment of head and neck squamous cell carcinoma patients of infected wounds and ulcerations.
CAP is able to reduce contamination of cancer ulcerations and the typical fetid odor that often accompanies head and neck cancer patients. The intention of the trial shall be to evaluate the efficiency of decontamination in head and neck cancer ulcerations in terms of pathogenic species, amount of reduction and reliability.
Standardize study protocol:
Phase I, clinical explorative single-arm, randomized, open, multicenter
Primary objective
Reduction of microbial burden of cancer ulcerations by application of CAP
Secondary objective:
Reduction of tumor following local CAP application
Inclusion:
20 Patients suffering from locally advanced oral cavity carcinoma with open tumor surfaces, treated with palliative intention and no more curative treatment options
Exclusion:
No wish for treatment, no compliance and understanding the protocol of the clinical study
Efficacy:
reduction of microbial burden; Documentation of visible changes by photography; Pathohistological and biochemical examination of specimen, taken from the tumor area and control areas
Procedure:
Plasma is applied for 1 minute per cm², spot area of 3 mm diameter distance between nozzle and tumor surface of 14 mm. 3 times/week with a break of 1 week followed by a repeated cycle for another week.
Conclusion:
The most important intention of the trial from the clinician’s point of view shall be to make CAP-treatment an effective and well-accepted addition to standard cancer therapy based upon EBM at least in palliative medicine.
Non-healing wounds pose a major burden to patients and health care systems alike. These wounds are chronically stuck in the inflammatory phase of the healing process without transitioning to the proliferative phase. They are also characterized by the excessive presence of leukocytes which are assumed to provoke the persistent inflammation observed in pathological wound healing. Recent studies suggested a beneficial role of cold physical plasma in the treatment of chronic wounds. Hence, it was the central question, whether exposure to cold physical plasma would affect the viability and/or function of human leukocytes. Cold plasma displays various properties of which the generation of reactive molecules, such as reactive oxygen and nitrogen species (ROS/RNS), where found to be central in mediating redox changes in leukocytes. Oxidative stress was present especially in lymphocytes that readily underwent apoptosis after exposure to plasma. This was largely a direct consequence of plasma-generated hydrogen peroxide but not superoxide or RNS. Amount of apoptosis was comparable among several lymphocyte subpopulations, with the wound healing-relevant γδ T cells being least affected. Lymphocyte apoptosis was accompanied by mitochondrial membrane depolarization, caspase 3 activation, DNA fragmentation, and phosphatidylserine exposure. These results are in line with previous characterizations of the intrinsic apoptotic pathway in redox biology, and suggest that plasma-induced apoptosis was not mediated by alternative molecular mechanisms. An important immune response mechanism, the proliferation of lymphocytes, was not interrupted in plasma-treated but non-apoptotic cells. In wounds, a central role of leukocytes is to orchestrate the healing response via the release of small communication molecules called cytokines. Non-healing wounds are associated with elevated amounts of pro-inflammatory IL-1β, IL-6, and TNFα, and plasma-treatment of leukocytes strongly decreased their concentrations. At the same time, the expression of anti inflammatory cytokines (IL-10, TGFβ) was markedly increased. The pro inflammatory chemokine IL-8 was the only molecule to be significantly increased in supernatants of plasma-treated cells. IL-8 is the major chemo-attractant for neutrophil granulocytes. Neutrophils are frequently associated with non-healing wounds. These professional phagocytes are the first to migrate to the site of injury where they inactivate invading pathogens by various mechanisms. Importantly, highly relevant effector functions remained mostly unaffected by plasma treatment: the phagocytosis of bacteria, the oxidative burst, and the intracellular killing of microbes. Of note, plasma induced a strong induction of neutrophil extracellular traps (NETs). Decorated with antimicrobial proteins, NETs are web-like chromatin extrusions that entrap pathogens. These results have several implications for wound healing. Plasma-treated neutrophils were still capable of eradicating bacteria, which are frequently associated with non-healing wounds. In addition, plasma-induced NETs could aid in wound healing by providing an antibacterial scaffold to safeguard against further dissemination of microorganisms. Chronic wounds display a state of sustained inflammation and plasma induced apoptosis but not necrosis in lymphocytes. This was an important finding as necrosis, the involuntary cell death, is associated with the release of intracellular content, enhancing inflammation. By contrast, apoptosis dampens it as dead cells are cleared by macrophages inducing anti inflammatory responses. Further, the cytokine signature of plasma-treated leukocytes was largely non inflammatory, which could further decrease inflammation in wounds. Altogether, this work provided first insight with regard to effects and mechanisms of cold physical plasma treatment of wound-relevant leukocytes. Generally, these cells were affected by a plasma mediated modulation of their redox state. Future studies should include the possibility of redox modulation into their experimental approach to further elucidate the role of ROS/RNS in inflammation and possibly to improve existing wound healing therapies.
Non-thermal atmospheric pressure plasma has recently been shown to have broad application potential for medical as well as industrial purposes. Improved wound healing and tissue decontamination have been described as consequences of non- thermal plasma treatment. However, thus far the underlying molecular mechanisms in human tissues have only been partially characterized. In this work a two-dimensional difference in-gel electrophoresis (2D-DIGE) approach was used and an analysis-workflow to study the response of human cells to atmospheric pressure non-thermal plasma was established. Human S9 bronchial epithelial cells were used as a model for airway epithelial cells. They were treated with atmospheric pressure plasma jet (APPJ) for different periods of time. Subsequently, time-resolved comparative proteome analysis was used to study the complex cellular adaptation reactions after a 120 sec plasma treatment, which accelerated wound healing in a clinically relevant model. The results indicate, that intracellular oxidative stress due to the non-thermal plasma treatment either leads to cell death or to proliferation. The oxidative stress response, mediated by Nrf2, appears to play a pivotal role in molecular signalling and might be a key pathway determining the fate of stressed cells. This thesis demonstrates changes in Nrf2-expression after non-thermal plasma treatment. Furthermore, potential protein biomarker candidates for evaluation of oxidative stress after non-thermal plasma treatment were identified. Finally, it is shown, that the cytosolic concentrations of IL-1beta and IL-33 were decreased following non-thermal plasma treatment. Thus, modulation of innate immune response by non-thermal plasma treatment of epithelial cells (ENTplas treatment) is concluded.
Beams of ions and electrons are a source of free energy which can be transferred to waves via an instability. Beams exist in almost all plasma environments, but their instabilities are particularly important for the dynamics of space plasmas. In the absence of collisions, the instability drives waves to large amplitudes and forms nonlinear structures such as solitary waves. The electric fields in these waves can scatter particles in the background plasma, or disrupt currents. Both of these effects are important for the overall dynamics of the plasma. In this thesis, both electron and ion beam plasma instabilities have been investigated in the linear plasma device VINETA and using a Particle-in-Cell simulation. The electron beam instability has been demonstrated by previous authors to be a useful diagnostic for the plasma density. The spatial resolution of previous results was confirmed at a few millimetres, and a temporal resolution of 1ms was shown for the first time. An ion beam was generated with a double plasma discharge. Compared to space, this environment and indeed most laboratory plasmas have considerably higher collisionality and a limited spatial extent which introduces gradients in the plasma. Gradients perpendicular to the beam propagation direction are linked to a decrease of both the wavelength and amplitude of the instability. It was observed in both experiment and simulation that gradients in sheaths at the boundaries of the plasma not only affect the time averaged plasma parameters, but also excite instabilities. Fluctuations within the sheath spread the beam in velocity space, effectively increasing its temperature. Warmer beams require a higher drift velocity to excite an instability. This was also confirmed by experimental and numerical results. Collisions are shown to be the dominant damping force for the electron beam instability. For ions, collisions play an important role in the simulation, but appear to be overshadowed by Landau damping from impurities in the experiment. When boundary conditions are removed from the simulation, wave amplitudes increase and nonlinear effects become important. Saturation by particle trapping and coalescence of phase space holes is observed, which could eventually lead to the solitary waves as they are observed in space plasmas.
Asymmetrical capacitively coupled RF discharges in oxygen, argon and hydrogen have been experimentally investigated with the innovative technique of the phase resolved optical emission spectroscopy. This diagnostic tool allows to measure spatio-temporally resolved emission intensities of electronically excited species with a high resolution. The spatial (axial) resolution was better than 1 mm and a temporal resolution of about 1.5 ns has been achieved. Therefore the plasma induced optical emission within the RF cycle (TRF = 73.75 ns) from the RF sheath region with a typical mean sheath thickness of about 5mm has been studied. Spatio-temporally resolved optical emission patterns of the following optical transitions have been measured for a total gas pressure in the range of 20 to 100 Pa and self-bias voltages between -50 and -550 V: Oxygen plasma Emission at 777.4 nm and 844.6 nm (atomic oxygen) Argon plasma Emission at about 751 nm and 841 nm (argon) Hydrogen plasma Emission at 656.3nm (atomic hydrogen, H alpha-line) These transitions are the most prominent ones of the investigated excited species in these plasmas as could be shown from overview spectra of the plasma induced optical emission in the range from 350 to 850 nm. For the first time such extensive PROES measurements in oxygen CCRF plasmas are presented in this work. The additional investigations of argon and hydrogen plasmas serve as a reference and for a direct comparison with results from the literature. The temporal behavior of the emission intensity is influenced by the effective lifetime of the emitting states which is on the order of the nanosecond time scale of the RF cycle. Therefore, it does not represent the real temporal behavior of the excitation. A simple method has been applied to calculate relative excitation rates from the measured emission intensities to distinguish different excitation mechanisms and their correct relative temporal behavior. In a close collaboration within the framework of the Sonderforschungsbereich Transregio 24 'Fundamentals of Complex Plasmas' a newly 1d3v PIC-MCC code for simulations of capacitive RF discharges in oxygen has been developed by Matyash et al. The very close coupling of experiment and modeling allowed a really detailed and microscopic understanding of the processes and dynamics from the sheath to the bulk plasma in CCRF discharges. The spatio-temporally resolved excitation rate profiles show four different excitation structures (I-IV). Excitation processes due to the following mechanisms in CCPs could be identified and characterized: I Electrons expelled from growing sheath II Electrons detached from negative ions (collisions with neutrals) + secondary electrons from the electrode surface (ion bombardment) III Field-reversal effect, reduced mobility of electrons (electron-neutral collisions) IV Heavy-particle collisions These excitation mechanisms are characterized by different temporal and spatial behaviors of the excitation rate within the RF cycle. Additionally it has been shown that the excitation by electron impact in the investigated oxygen plasmas results mainly from dissociative electron impact excitation (O2 + e -> O + O* + e) and not from direct electron impact excitation (O + e -> O* + e). Actinometry measurements show that the results are not really credible. Thus actinometry is not applicable on the investigated oxygen RF plasma. A challenge in interpretation is the observed excitation pattern IV. Pattern IV has to be caused in connection with heavy particle collisions nearby the electrode surface and could be observed in all the three plasmas oxygen, argon and hydrogen. It is located directly in front of the powered electrode and appears during almost the whole RF cycle. The temporal modulation is nearly sinusoidal and weak in comparison to the first three patterns. This is due to the weak RF modulation of the ion flux towards the electrode surface which has been proven by a PIC simulation. It could be shown that the modulation degree of pattern IV depends on the transition time of the corresponding positive ions through the RF sheath which is influenced by the ion mass. In oxygen as well as in argon CCRF plasmas pattern IV is less modulated than in hydrogen CCRF plasmas due to the heavier ions in oxygen and argon. Additionally the modulation degree increases with increasing pressure due to the more confined plasma at higher pressures which is yielding in a stronger modulated ion current towards the powered electrode.