diff --git a/chap01.aux b/chap01.aux index b693d744e09a8d922850c8020c584bc063526fbb..e5c23d5fcbb22d1ab6b638453a9d8c08e5c7ef1e 100644 --- a/chap01.aux +++ b/chap01.aux @@ -91,7 +91,7 @@ \newlabel{sub@fig:mask_aligner_nomenclature_capacitances_motors}{{a}{23}{\relax }{figure.caption.20}{}} \newlabel{fig:mask_aligner_nomenclature_capacitances_mask}{{1.16b}{23}{\relax }{figure.caption.20}{}} \newlabel{sub@fig:mask_aligner_nomenclature_capacitances_mask}{{b}{23}{\relax }{figure.caption.20}{}} -\newlabel{fig:mask_aligner_nomenclature_capacitances}{{\caption@xref {fig:mask_aligner_nomenclature_capacitances}{ on input line 319}}{23}{Capacitive distance measurements}{figure.caption.20}{}} +\newlabel{fig:mask_aligner_nomenclature_capacitances}{{\caption@xref {fig:mask_aligner_nomenclature_capacitances}{ on input line 322}}{23}{Capacitive distance measurements}{figure.caption.20}{}} \@writefile{lof}{\contentsline {figure}{\numberline {1.16}{\ignorespaces (\subref {fig:mask_aligner_nomenclature_capacitances_motors}) cross-section of the Mask Aligner showing the labeling and rough positioning of the capacitance sensors on the mask (inner \textcolor {tab_red}{red} triangle) in relation to the three piezo motor stacks. (\subref {fig:mask_aligner_nomenclature_capacitances_mask}) diagram of the mask's dimensions as well as labeling of the mask's sensors. The inset shows the dimensions of the holey part of the mask, which is used to create patterns. Below is a cross section of the materials used.}}{23}{figure.caption.20}\protected@file@percent } \@writefile{lof}{\contentsline {figure}{\numberline {1.17}{\ignorespaces Diagram showing how communication with the RHK and the Lock-in amplifier is done and how they interact with elements in vacuum. Red lines are input, black lines are output lines. The capacitance relay is used to measure $C_i$ one after another. The RHK relay controls, which motor is currently driven.}}{24}{figure.caption.21}\protected@file@percent } \newlabel{fig:diagram_MA_circ}{{1.17}{24}{Diagram showing how communication with the RHK and the Lock-in amplifier is done and how they interact with elements in vacuum. Red lines are input, black lines are output lines. The capacitance relay is used to measure $C_i$ one after another. The RHK relay controls, which motor is currently driven}{figure.caption.21}{}} diff --git a/chap02.tex b/chap02.tex index 4fe6432646971e172414030ec088aa46dcc2a4a7..23171b272e27edb6d5819e33ed540df3d404f45e 100644 --- a/chap02.tex +++ b/chap02.tex @@ -15,15 +15,16 @@ The setup of an electron beam evaporator is shown in Figure \ref{fig:e-beam_evap %The crucible is also heated during the evaporation process, in order to prevent it from being damaged, a material with a high melting point is chosen. Tungsten with a melting point of 3695 K ~\cite{Tungsten_melt} is usually chosen. %Additionally, the crucible usually has to be water cooled to avoid outgassing during the evaporation process. -In order to heat the source material it is hit with a high voltage electron beam ($\mathcal{O}$($1$~kV)), emitted by either an electron gun or a filament. This beam usually is focused using magnetic fields to hit the source material. Energy transfer heats the hit atoms and eventually leads to the evaporation according to its vapor pressure.\\ +To heat the source material, it is bombarded with a high-voltage electron beam ($\mathcal{O}$($1$~kV)), which is emitted by either an electron gun or a filament. This beam usually is focused using magnetic fields to hit the source material. Energy transfer heats the hit atoms and eventually leads to the evaporation according to its vapor pressure.\\ %The penetration depth of electron with ($<5$ kV) is less than 0.4 $\mu$m (estimated using CASINO Monte Carlo software)~\cite{CASINO} so the heating occurs only very near to the source material's surface. This allows for less energy loss and more controlled evaporation as the crucible and the rest of the system is not heated by the electron beam directly, but only by the radiant heat emitted by the source material.\\ -When the material's vapor pressure exceeds the surrounding environments pressure, a vapor forms. The sample is kept at a temperature much colder than the source material's temperature, due to this the material beam will condense on the substrate's surface forming a thin film. A shutter is used to control the deposition of the material.\\ +When the material's vapor pressure exceeds the surrounding environments pressure, a vapor forms. The sample is kept at a temperature much colder than the source material's temperature, due to this the material beam will condense on the substrate's surface forming a thin film. To regulate the deposition process, a shutter is employed, allowing for controlled release of the material. \\ -In order to ensure the material beam reaches the sample in a direct path, the mean free path (MFP) of a traveling particle has to be larger than the distance to the sample's surface. For this reason, high vacuum (HV) (MFP of $10$ cm to $1$ km) or ultra-high vacuum conditions (UHV) (MFP of $1$ km to $10^5$ km) are used. +In order to ensure the material beam reaches the sample in a direct path, the mean free path (MFP) of a traveling particle has to be larger than the distance to the sample's surface. For this reason, high vacuum (HV) (MFP of $10$ cm to $1$ km) or ultra-high vacuum conditions (UHV) (MFP of $1$ km to $10^5$ km) are needed. The deposition rate of the evaporator can be measured using a molecular flux monitor. The deposition rate of a material is described by the Hertz-Knudsen equation: + \begin{equation} \frac{dN}{A dt} = \frac{\alpha (p_\text{e} - p)}{\sqrt{2 \pi m k_\text{B} T}} \label{eq:hertz_knudsen} @@ -97,8 +98,8 @@ The motor module consists of three piezo motors. They move the mask along the z The direction is specified by mathematical sign, where $-$ specifies the approach direction, while $+$ specifies retract (Fig. \ref{fig:mask_aligner_nomenclature_motors}).\\ \section{Slip stick principle} -In order to control the movement of the mask stage using the mask aligner, three motors of six piezo stacks each made up of four piezo crystals are used. Piezo crystals expand/contract upon being supplied with a DC voltage. To enable the piezo crystals to move the stage, a sapphire prism is clamped between the six piezo stacks. When one applies a voltage amplitude to the piezo stacks, the prism is moved by the stacks. An illustration of the principle is shown in Figure \ref{fig:slip_stick_diagram}. \\ -First a slowly rising pulse is applied to the piezo moving the prism along with the piezo. This pulse is referred to as the "slow flank". Afterward, a very fast pulse ($<1$ $\mu$s) is applied, contracting the piezo back into its original position. The prism however due to inertia remains in position. This pulse is referred to as the "fast flank". When repeated, the prism can be moved. The direction depends on the voltage amplitude signal polarity. The simplest pulse shape allowing for this is the saw tooth wave, but other signal shapes that follow the principle can be used. +The movement of the mask stage is controlled by the mask aligner, which utilizes a system consisting of three motors, each comprising six piezo stacks. Each piezo stack is made up of four piezo crystals that expand or contract when a DC voltage is applied. To facilitate the movement of the stage, a sapphire prism is clamped between the six piezo stacks. When a voltage amplitude is applied to the piezo stacks, the prism is displaced by the stacks, enabling precise movement of the stage. The operating principle of this mechanism is illustrated in Figure \ref{fig:slip_stick_diagram}. \\ +The movement of the prism is achieved through a two-stage process. Initially, a slowly increasing pulse, known as the "slow flank," is applied to the piezo, causing it to move the prism. This is followed by a rapid pulse, lasting less than $1$ $\mu$s, which contracts the piezo back to its original position. However, due to inertia, the prism remains in its new position. This rapid pulse is referred to as the "fast flank." By repeating this sequence, the prism can be moved in a controlled manner. The direction of movement is determined by the polarity of the voltage amplitude signal. The simplest waveform that can achieve this movement is a sawtooth wave, although other signal shapes that adhere to this principle can also be used. \begin{figure}[H] \centering @@ -110,12 +111,14 @@ First a slowly rising pulse is applied to the piezo moving the prism along with \section{Shadow mask alignment} \subsection{Motor screw configuration} -In order to make sure the motors can all give similar step sizes, there are 3 -screws (see Figure \ref{fig:screw_firmness_screw_image}). One is located on each motor's leaf spring. They can control the amount of force the front plate applies to the prism and thus the friction between the prism and piezo stacks. In order to achieve similar step size for the three motors. The step size in dependence of the screw firmness has to be determined. This is done by measuring -the time it takes for a motor to travel a known distance. For example the -distance of one solder anchor can be used as it is known -to be $2$ mm. This gives a measurement fast and precise enough to determine a suitable number of rotations. -An example for how the screw firmness affects the step size can be seen in Figure \ref{fig:screw_firmness_plot}. +To ensure that the three motors produce similar step sizes, the friction between the prism and the piezo stacks is adjusted. This is achieved through the use of three screws, one located on each motor's leaf spring (as shown in Figure \ref{fig:screw_firmness_screw_image}). By adjusting these screws, the force applied by the front plate to the prism can be controlled, thereby influencing the friction between the prism and the piezo stacks. To determine the optimal screw firmness for achieving similar step sizes among the three motors, the relationship between screw firmness and step size must be established. This is done by measuring the time it takes for a motor to travel a known distance. This method provides a fast and precise way to determine a suitable number of rotations. An example of how screw firmness affects step size is illustrated in Figure \ref{fig:screw_firmness_plot}. +% +%In order to make sure the motors can all give similar step sizes, there are 3 +%screws (see Figure \ref{fig:screw_firmness_screw_image}). One is located on each motor's leaf spring. They can control the amount of force the front plate applies to the prism and thus the friction between the prism and piezo stacks. In order to achieve similar step size for the three motors. The step size in dependence of the screw firmness has to be determined. This is done by measuring +%the time it takes for a motor to travel a known distance. For example the +%distance of one solder anchor can be used as it is known +%to be $2$ mm. This gives a measurement fast and precise enough to determine a suitable number of rotations. +%An example for how the screw firmness affects the step size can be seen in Figure \ref{fig:screw_firmness_plot}. \begin{figure}[H] \centering @@ -153,9 +156,9 @@ The step size calibration procedure involves the following steps: \end{itemize} An example of this process for motors Z1 and Z2 is shown in Figure \ref{fig:calibration_uhv_example_driving} for a $1000$-step measurement. \\ -The procedure for step size calibration is: $2000$, $4000$, -$6000$, $8000$ and $10000$ steps are driven. After each set of steps the distance -the prism has traveled in the image of the camera is measured. This is done with the Bresser MicroCam II software. In the software a line is drawn at the initial position, from a remarkable point on the motor (Fig. \ref{fig:calibration_uhv_points_of_interest}). After driving another line is drawn at the end position. The distance between these is measured using the software. An example for motor Z1 and Z2 is shown in Figure \ref{fig:calibration_uhv_example_driving} for a $1000$ step measurement. If changes to the motors have been performed a calibration has to be performed outside of UHV before reinsertion into UHV. Afterwards the motors have to be calibrated in UHV. \\ +%The procedure for step size calibration is: $2000$, $4000$, +%$6000$, $8000$ and $10000$ steps are driven. After each set of steps the distance +%the prism has traveled in the image of the camera is measured. This is done with the Bresser MicroCam II software. In the software a line is drawn at the initial position, from a remarkable point on the motor (Fig. \ref{fig:calibration_uhv_points_of_interest}). After driving another line is drawn at the end position. The distance between these is measured using the software. An example for motor Z1 and Z2 is shown in Figure \ref{fig:calibration_uhv_example_driving} for a $1000$ step measurement. If changes to the motors have been performed a calibration has to be performed outside of UHV before reinsertion into UHV. Afterwards the motors have to be calibrated in UHV. \\ \begin{figure}[H] \centering @@ -456,11 +459,10 @@ One concern regarding reproducibility is whether the approach curve is significa \label{fig:approach_replicability} \end{figure} -Reinsertion of the mask resulted in a substantial change in the approach curve, which can likely be attributed to newly induced tilt on the mask. This shift is evident in the difference between the green and red curves shown in Figure \ref{fig:approach_replicability}. \ref{fig:approach_replicability}. - -Alternatively, minor movement of the mask frame on the Nd magnets, causing the mask to tilt, could also be a contributing factor. This issue is inherent to the current design of the Mask Aligner and cannot be resolved without a fundamental redesign. \\ +Reinsertion of the mask resulted in a substantial change in the approach curve, which can likely be attributed to newly induced tilt on the mask. This shift is evident in the difference between the green and red curves shown in Figure \ref{fig:approach_replicability}.\\ +Alternatively, minor movement of the mask frame on the \ce{Nd} magnets, causing the mask to tilt, could also be a contributing factor. This issue is inherent to the current design of the Mask Aligner and cannot be resolved without a fundamental redesign. \\ -Reinsertion of the sample also resulted in a difference in approach curves, although this difference is relatively small, as shown in Figure \ref{fig:approach_replicability} (blue and green curves). The overall trend of the curve remains consistent, but the absolute values exhibit a slight change. However, the peak in dC underwent a significant shift. A stop condition determined based on the green curve (e.g., 0.04 pF) would exceed the point of first contact on the blue curve. This implies that after switching samples, a conservative stop condition must be selected to avoid overshooting. \\ +Reinsertion of the sample also resulted in a difference in approach curves of $\approx 0.5 \pm 0.2$ pF, as shown in Figure \ref{fig:approach_replicability} (blue and green curves). The overall trend of the curve remains consistent, but the absolute values exhibit a change. However, the peak in $dC$ underwent a significant shift. A stop condition determined based on the green curve (e.g., $0.04$ pF) would exceed the point of first contact on the blue curve. This implies that after switching samples, a conservative stop condition must be selected to avoid overshooting. \\ % %\subsection{Capacitance correlations} \label{subsec:cross_cap} diff --git a/chap04.tex b/chap04.tex index 09730d7c306b0995c036d219d3b21f4bbefd5bf7..aa34dff835a8b134109590c321fa66a13b77a212 100644 --- a/chap04.tex +++ b/chap04.tex @@ -290,6 +290,7 @@ To establish the optimal screw setup and verify the effectiveness of the modific \label{fig:calibration_after_repair} \end{figure} -The calibration results, as shown in Figure \ref{fig:calibration_after_repair}, indicate that the three motors exhibit similar performance in the approach direction. The deviation between Z2 and the other motors is within $2\sigma$, while the difference between Z3 and Z1 is up to $6$ nm/step, which is within $6\sigma$ of each other. Assuming a worst-case difference of $6$ nm, the data suggests an angular tilt per step of approximately $(5.73 × 10^-6)^circ$. This corresponds to a height difference on the sample of approximately $0.5$ nm/step, resulting in a penumbra difference of $1.2$ nm for every $100$ steps. \\ +The calibration results, as shown in Figure \ref{fig:calibration_after_repair}, indicate that the three motors exhibit similar performance in the approach direction. The deviation between Z2 and the other motors is within $2\sigma$, while the difference between Z3 and Z1 is up to $6$ nm/step, which is within $6\sigma$ of each other. Assuming a worst-case difference of $6$ nm, the data suggests an angular tilt per step of approximately $(5.73 \times 10^{-6})^\circ$. This corresponds to a height difference on the sample of approximately $0.5$ nm/step, resulting in a penumbra difference of $1.2$ nm for every $100$ steps. \\ + In the retract direction, the difference between motors is within the margin of error for Z2 and Z1, but Z3 deviates by about $4\sigma$ from the others. However, since the mask is aligned during approach, deviations in retract have a lesser impact on alignment. After each evaporation, the mask is retracted to approximately $50$ $\mu$m to prevent damage to the sample. This results in a tilt of $1.2$ $\mu$m over the evaporation field, corresponding to an angle of approximately $0.004^\circ$. This difference would cause a deviation of approximately $38$ nm in penumbra. However, by driving the Z1 and Z2 motors $100$ steps up after retraction, this deviation can be almost fully compensated, resulting in an error of at most approximately $6$ nm of additional penumbra induced by tilt. \\ diff --git a/pdfa.xmpi b/pdfa.xmpi index 9ac23145892c0deedb34636bf77bf642c5154b36..a4b240669fa72bd6435a8e0ab214b6c9fed5b7a9 100644 --- a/pdfa.xmpi +++ b/pdfa.xmpi @@ -73,15 +73,15 @@ </rdf:Description> <rdf:Description rdf:about="" xmlns:xmp="http://ns.adobe.com/xap/1.0/"> <xmp:CreatorTool>LaTeX with hyperref</xmp:CreatorTool> - <xmp:ModifyDate>2024-10-22T19:59:44+02:00</xmp:ModifyDate> - <xmp:CreateDate>2024-10-22T19:59:44+02:00</xmp:CreateDate> - <xmp:MetadataDate>2024-10-22T19:59:44+02:00</xmp:MetadataDate> + <xmp:ModifyDate>2024-10-22T20:59:27+02:00</xmp:ModifyDate> + <xmp:CreateDate>2024-10-22T20:59:27+02:00</xmp:CreateDate> + <xmp:MetadataDate>2024-10-22T20:59:27+02:00</xmp:MetadataDate> </rdf:Description> <rdf:Description rdf:about="" xmlns:xmpRights = "http://ns.adobe.com/xap/1.0/rights/"> </rdf:Description> <rdf:Description rdf:about="" xmlns:xmpMM="http://ns.adobe.com/xap/1.0/mm/"> <xmpMM:DocumentID>uuid:C8CFC28F-88E1-7995-E9AD-F6D12EAD346B</xmpMM:DocumentID> - <xmpMM:InstanceID>uuid:CC1D564D-DD9C-13EB-4F6A-EDC267DA7134</xmpMM:InstanceID> + <xmpMM:InstanceID>uuid:59A396FE-C5CD-2B08-7D15-ECB63B9792D8</xmpMM:InstanceID> </rdf:Description> </rdf:RDF> </x:xmpmeta> diff --git a/thesis.log b/thesis.log index f69f3203ab4dda41ed486cdd316f6736fe1dd871..f3300a1a4aac012302dc28784665788b882f0056 100644 --- a/thesis.log +++ b/thesis.log @@ -1,4 +1,4 @@ -This is pdfTeX, Version 3.141592653-2.6-1.40.25 (MiKTeX 24.1) (preloaded format=pdflatex 2024.9.29) 22 OCT 2024 19:59 +This is pdfTeX, Version 3.141592653-2.6-1.40.25 (MiKTeX 24.1) (preloaded format=pdflatex 2024.9.29) 22 OCT 2024 20:59 entering extended mode restricted \write18 enabled. %&-line parsing enabled. @@ -1699,6 +1699,12 @@ Package pdftex.def Info: img/EBeamDep.pdf used on input line 9. 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[67 <./img/Plots/Filtering.pdf> <./img/Plots/FilteringDone.pdf>] -<img/Plots/InvertedSginal.pdf, id=3213, 433.62pt x 289.08pt> +<img/Plots/InvertedSginal.pdf, id=3210, 433.62pt x 289.08pt> File: img/Plots/InvertedSginal.pdf Graphic file (type pdf) <use img/Plots/InvertedSginal.pdf> Package pdftex.def Info: img/Plots/InvertedSginal.pdf used on input line 126. (pdftex.def) Requested size: 225.75594pt x 150.50331pt. -<img/Plots/Switching01.pdf, id=3214, 433.62pt x 289.08pt> +<img/Plots/Switching01.pdf, id=3211, 433.62pt x 289.08pt> File: img/Plots/Switching01.pdf Graphic file (type pdf) <use img/Plots/Switching01.pdf> Package pdftex.def Info: img/Plots/Switching01.pdf used on input line 131. @@ -2823,13 +2829,13 @@ Underfull \hbox (badness 10000) in paragraph at lines 158--159 [] [69] -<img/Plots/Walker/WalkerApproach.pdf, id=3317, 867.24pt x 650.43pt> +<img/Plots/Walker/WalkerApproach.pdf, id=3314, 867.24pt x 650.43pt> File: img/Plots/Walker/WalkerApproach.pdf Graphic file (type pdf) <use img/Plots/Walker/WalkerApproach.pdf> Package pdftex.def Info: img/Plots/Walker/WalkerApproach.pdf used on input lin e 169. (pdftex.def) Requested size: 225.75594pt x 169.31622pt. -<img/Plots/Walker/WalkerRetract.pdf, id=3318, 867.24pt x 650.43pt> +<img/Plots/Walker/WalkerRetract.pdf, id=3315, 867.24pt x 650.43pt> File: img/Plots/Walker/WalkerRetract.pdf Graphic file (type pdf) <use img/Plots/Walker/WalkerRetract.pdf> Package pdftex.def Info: img/Plots/Walker/WalkerRetract.pdf used on input line @@ -2837,19 +2843,19 @@ Package pdftex.def Info: img/Plots/Walker/WalkerRetract.pdf used on input line (pdftex.def) Requested size: 225.75594pt x 169.31622pt. [70 <./img/Plots/Walker/WalkerApproach.pdf> <./img/Plots/Walker/WalkerRetract. pdf>] -<img/Plots/Walker/WalkerApproach_ff.pdf, id=3394, 867.24pt x 650.43pt> +<img/Plots/Walker/WalkerApproach_ff.pdf, id=3391, 867.24pt x 650.43pt> File: img/Plots/Walker/WalkerApproach_ff.pdf Graphic file (type pdf) <use img/Plots/Walker/WalkerApproach_ff.pdf> Package pdftex.def Info: img/Plots/Walker/WalkerApproach_ff.pdf used on input line 185. (pdftex.def) Requested size: 225.75594pt x 169.31622pt. -<img/Plots/Walker/WalkerRetract_ff.pdf, id=3395, 867.24pt x 650.43pt> +<img/Plots/Walker/WalkerRetract_ff.pdf, id=3392, 867.24pt x 650.43pt> File: img/Plots/Walker/WalkerRetract_ff.pdf Graphic file (type pdf) <use img/Plots/Walker/WalkerRetract_ff.pdf> Package pdftex.def Info: img/Plots/Walker/WalkerRetract_ff.pdf used on input l ine 189. (pdftex.def) Requested size: 225.75594pt x 169.31622pt. -<img/MA/SchaltDiagramWalker.pdf, id=3398, 544.13278pt x 385.4176pt> +<img/MA/SchaltDiagramWalker.pdf, id=3395, 544.13278pt x 385.4176pt> File: img/MA/SchaltDiagramWalker.pdf Graphic file (type pdf) <use img/MA/SchaltDiagramWalker.pdf> Package pdftex.def Info: img/MA/SchaltDiagramWalker.pdf used on input line 201 @@ -2950,7 +2956,7 @@ pdfTeX warning (ext4): destination with the same identifier (name{section.4.3}) \relax l.51 \section{Walker principle diagram} \label{app:walker_diagram} -<img/ElectronicsDiagramm.pdf, id=3620, 778.32848pt x 492.10774pt> +<img/ElectronicsDiagramm.pdf, id=3617, 778.32848pt x 492.10774pt> File: img/ElectronicsDiagramm.pdf Graphic file (type pdf) <use img/ElectronicsDiagramm.pdf> Package pdftex.def Info: img/ElectronicsDiagramm.pdf used on input line 54. @@ -2963,7 +2969,7 @@ Package pdftex.def Info: img/ElectronicsDiagramm.pdf used on input line 54. pdfTeX warning: pdflatex.exe (file ./img/Plots/Walker/MaskAlign Walker Signalel ektronik 1.0.pdf): PDF inclusion: found PDF version <1.7>, but at most version <1.5> allowed -<img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0.pdf, id=3628, 845.07724 +<img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0.pdf, id=3625, 845.07724 pt x 597.55246pt> File: img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0.pdf Graphic file ( type pdf) @@ -2992,7 +2998,7 @@ ektronik 1.0.pdf): PDF inclusion: found PDF version <1.7>, but at most version pdfTeX warning: pdflatex.exe (file ./img/Plots/Walker/MaskAlign Walker Signalel ektronik 1.0.pdf): PDF inclusion: found PDF version <1.7>, but at most version <1.5> allowed -<img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0.pdf, id=3631, page=1, 8 +<img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0.pdf, id=3628, page=1, 8 45.07724pt x 597.55246pt> File: img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0.pdf Graphic file ( type pdf) @@ -3032,7 +3038,7 @@ Package pdftex.def Info: img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0 pdfTeX warning: pdflatex.exe (file ./img/Plots/Walker/MaskAlign Walker Signalel ektronik 1.0.pdf): PDF inclusion: found PDF version <1.7>, but at most version <1.5> allowed -<img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0.pdf, id=3704, page=2, 8 +<img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0.pdf, id=3701, page=2, 8 45.07724pt x 597.55246pt> File: img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0.pdf Graphic file ( type pdf) @@ -3059,7 +3065,7 @@ Package pdftex.def Info: img/Plots/Walker/MaskAlign Walker Signalelektronik 1.0 pdfTeX warning: pdflatex.exe (file ./img/Plots/Walker/MaskAlign Walker Netzteil modifiziert 24-05-2024.pdf): PDF inclusion: found PDF version <1.7>, but at mo st version <1.5> allowed -<img/Plots/Walker/MaskAlign Walker Netzteil modifiziert 24-05-2024.pdf, id=3709 +<img/Plots/Walker/MaskAlign Walker Netzteil modifiziert 24-05-2024.pdf, id=3706 , 1194.98447pt x 845.07724pt> File: img/Plots/Walker/MaskAlign Walker Netzteil modifiziert 24-05-2024.pdf Gra phic file (type pdf) @@ -3088,7 +3094,7 @@ st version <1.5> allowed pdfTeX warning: pdflatex.exe (file ./img/Plots/Walker/MaskAlign Walker Netzteil modifiziert 24-05-2024.pdf): PDF inclusion: found PDF version <1.7>, but at mo st version <1.5> allowed -<img/Plots/Walker/MaskAlign Walker Netzteil modifiziert 24-05-2024.pdf, id=3712 +<img/Plots/Walker/MaskAlign Walker Netzteil modifiziert 24-05-2024.pdf, id=3709 , page=1, 1194.98447pt x 845.07724pt> File: img/Plots/Walker/MaskAlign Walker Netzteil modifiziert 24-05-2024.pdf Gra phic file (type pdf) @@ -3192,9 +3198,9 @@ ublic/lm/lmsy8.pfb><C:/Users/Luzifer/AppData/Local/Programs/MiKTeX/fonts/type1/ public/lm/lmtk10.pfb><C:/Users/Luzifer/AppData/Local/Programs/MiKTeX/fonts/type 1/public/lm/lmtt8.pfb><C:/Users/Luzifer/AppData/Local/Programs/MiKTeX/fonts/typ e1/public/lm/lmtti10.pfb> -Output written on thesis.pdf (99 pages, 253487523 bytes). +Output written on thesis.pdf (99 pages, 253486518 bytes). 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