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Thin Films - Science topic

From different processes (CVD, PVD, SPIN, etc)
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I am trying to figure out a way of calculating the dielectric constant of a thin film of Yb2O3 on ITO. Assuming that the thickness of the Yb2O3 is known and that it's <5 nm, how does one proceed?
At this point, I hypothesize that this question is composed of two things that I need to figure out:
1. What is the dielectric constant of the thin film of Yb2O3 without any substrate effect?
2. What is the dielectric constant of the combined system?
I would rather be interested in a theoretical approach (simulations) rather than experimentally, but any comments/help are appreciated!
Thanks!
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  1. Dielectric functions are intrinsic properties of each material and do not generally depend on other materials within the device.
  2. There is no such thing as the dielectric constant of the combined system. The system must be studied as a stack of materials, each material with well defined dielectric functions.
Now, out of the ideal world, every thin film material optical properties depend on the deposition method and underlying materials. For example: in ITO, the ratio of oxide, tin and indium has a profile that depend on deposition method. Also, in certain cases, a "combined" dielectric function does exist (effective dielectric function), but this depends, among others, on the sample characteristics and the wavelength regime (dielectric "constants" are not constants, they are wavelength dependent).
Saying the above, as a first step, you can use material's dielectric functions from the literature and simulate the system response.
How to model the system? it depends on what do you want to model.
How to measure the dielectric functions? It depends on the sample characteristics and wavelength regime (dielectric "constants" are not constants, they are wavelength dependent). Ellipsometry is usually the best way to go.
See the following article on the determination of dielectric functions/optical constants on a stack system, as well as the modeling of the combined system:
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I'm trying to achieve bonding between two different substrates through thermocompression using indium as an adhesion layer. After depositing indium through e-beam evaporation, the thin film is white and not metallic like the pellets. Is this common or an issue?
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Thank you so much for your answer.
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Is the relationship A=-Log T applicable for calculating the absorbance, in the case of thin layers?
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I am trying to understand the influence of polymer films sliding against each other. For the simulation, I saw many molecular dynamics simulations, like LAMMPS, GROMACS, etc. I am new to this field. Can someone who has experience with these methods suggest which one is the best one for the particular case?
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Dear,
I have tried to thin film calculation. What is the difference from bulk calculation.
The vacuum added in the z-direction is enough in all calculation (scf, vc-relax and band)
Many thanks
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Roberto D'Agosta many thanks i added k points mesh with 10 10 1 as your suggestion (have a mesh in the Brillouin Zone that has only one point in the z direction)
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We are trying to sputter a metallic target. We can clearly see the plasma however after depositing for more than 30 minutes there is no deposition on the substrate. What can be the reason for this? need expert advice.
Thanks!
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I think that the gas pressure is a critical factor. Increasing the gas pressure will raise the collision frequency and the sputtering rate, but it will reduce the average mean free path of the sputtered atoms to reach the substrate and will also reduce the adhesion.
So, it is better to control the gas pressure in low range to have better adhesion and allow a longer mean free path of the sputtered atoms reaching the substrate.
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I have obtained XRD results for thin film in bulk mode, kindly suggest different methods to evaluate the residual stresses.
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For this, please refer to the preprint article link http://dx.doi.org/10.13140/RG.2.2.23849.40808, titled “Determining and quantifying chemically produced stresses in (atoms of) electronic and crystalline materials”
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I want to characterize the residual stress in copper thin film deposited on fused silica. Kindly let me know how to do that.
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For this, please refer to the preprint article link http://dx.doi.org/10.13140/RG.2.2.23849.40808, titled “Determining and quantifying chemically produced stresses in (atoms of) electronic and crystalline materials”
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We used CBD method for deposition of Al doped PbS thin films. We observed that thickness of the films decreased with Al increase of Al concentration. But refractive index values are increase with decrease of film thickness or increase of Al concentration.
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Konsantrasyon kırıcılık indisi ile doğru orantılı.
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I think that the XRD for thin film also measured the grain size
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Hey there Nadir Fadhil Habubi! Great question. When the crystallite size estimated by XRD matches the grain size for thin films, it typically means that the XRD analysis is indeed capturing the grain size accurately. In thin films, XRD can provide valuable insights into both the crystal structure and the size of the crystallites or grains within the film. When these two measurements align, it suggests that the XRD technique is effectively probing the structure of the thin film, including the grain size. So, to answer your Nadir Fadhil Habubi question directly, yes, XRD for thin films can indeed measure the grain size, and when the estimated crystallite size aligns with the observed grain size, it indicates a reliable assessment of the film's structure.
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I have introduced soc in VASP and I am getting these changes in the bandstructure when I change the SAXIS from 110 (0 deg) to 010(45 deg), also my magmom is in z direction . You can see, near the fermi energy (0 eV). Moreover, it is a calculation of thin film with a substrate MgO. The bands get kindoff splitted. What is actually happening in this?
P.S.- need articles for spin orbit coupling in solids
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If your crystal structure is cubic, then ideally SAXIS = 0 0 1 or 0 1 0 or 1 0 0 shouldn't make any difference. But, be careful with the MAGMOM flag.
Suppose if you are taking the default value of SAXIS say 001, then you should set MAGMOM in xyz direction, and take ISYM = 0.
I have tried this test for many systems that for particular SAXIS, changing the MAGMOM in different directions also leads to different ground state energies, where for SAXIS= 001, MAGMOM = 1 1 1 is found to be the most stable, at least for my systems.
You can also test it for your system. Keep SAXIS fixed and change MAGMOM directions, then you can analyze the most stable one. And experimentalists also do such things, so it is a good exercise I believe.
Hope this helps!
Best regards,
Payal
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Hi All
I am trying to understand the Akono scratch test method to find the fracture toughness of thin film. I am scratching the films with a probe radius of 4um (Spherical) with load below the film critical load. this means that the scratch path has no sudden change. For the data analysis, I only using a lateral load segment of scratch and divide it with the spherical shape function. can someone help to understand what is best way is to do this scratch and how to analyze the data.
Thanks for your help.
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Hey there Faisal Amir!
Understanding the Akono scratch test method for determining the fracture toughness of thin films is a wise pursuit. Utilizing a probe radius of 4um and ensuring the load remains below the film's critical load is crucial for maintaining a consistent scratch path without sudden changes.
For conducting the scratch, ensure a controlled and steady application of the load along the surface of the thin film. The scratch should be performed with precision, maintaining a constant velocity to avoid variations that could affect the results.
When it comes to analyzing the data, focusing on the lateral load segment of the scratch and dividing it by the spherical shape function is a sound approach. This division allows for normalization and comparison across different samples, enhancing the accuracy of the fracture toughness determination.
Consider employing techniques such as optical microscopy or atomic force microscopy to visualize the scratch morphology and accurately measure its dimensions. Additionally, mathematical modeling and simulation can aid in interpreting the data and deriving meaningful conclusions about the fracture toughness of the thin film.
Remember to document each step meticulously and validate the results through repeated experiments to ensure reliability. Collaboration with peers and experts in the field can also provide valuable insights and guidance throughout the process.
Keep up the meticulous work, and don't hesitate to reach out if you Faisal Amir have any further questions or need assistance along the way. Happy scratching!
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I have deposited Al doped PbS thin films using CBD method at different concentrations from 0,2,4,6 and 8%. I was observed that thickness of the films decreases with increase of Al concentration. Can explain about the reason
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The addition of Al dopants can alter the chemical reactions occurring during film deposition. This modification may lead to changes in precursor availability, reactivity, or stability, ultimately affecting the growth rate and resulting in thinner films. Also, Al dopants may influence the crystallite size and orientation of the PbS thin films. Higher concentrations of aluminum ions could lead to smaller crystallite sizes due to the incorporation of Al atoms into the PbS lattice or the formation of secondary phases. Smaller crystallite sizes often result in thinner films due to decreased grain coalescence during film growth.
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The TPM treatment ensures the film adheres to the substrate after curing. I use N,N-Methylenebis(acrylamide) as the crosslinker, Darocur as the photoinitiator and DMSO as the solvent. I have tried replicating procedures from a few papers with little luck. I need uniform films less than 1.5 microns thick so I can characterize them with ellipsometry.
Thanks
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In my experience you could easily spin coat PNIPAM dissolved in water. Dpending what thickness you want you make thicker concentration or thinner. After spinning it is still dissolved in water. You have to polimerise it by electron beam, UV etc. And them exposed aeras will be attached to the surface.
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Recently, I cannot use thin-film hydration method to successfully prepare my DPPC MLV. I am sure I didn't change any parameters or steps in my protocol. However. instead of acquiring thin-film, I got transparent aggregation (see attached picture) at the bottom of round bottom beaker after rotavap overnight. The lipid and chloroform I used were purchased two weeks ago so I don't think it is due to the outdated chemicals. I ever doubt rotovaper problem since I found that I could easily pull out the connected beaker even at very high vacuum degree (6mbar). Then I connected a pressure gauge to the rotovaper to test if the rotovaper works well. I tested twice and the gauge pressure very corresponded to the value read from the rotovaper screen. Now, I am so confused, could someone give me any possible explanations about why? Many thanks!
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Robert Adolf Brinzer Kangdi Sun after rotary evaporation is it necessary to dry film further in vaccum or flushing with nitrogen gas?
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I have deposited iron titanate thin films by electrodeposition at different molar concentration.
Q #1. In XRD pattern of as deposited I don't observe any intensity peak while after performing MF annealing at 300 degree Celcius, I observed intensity peaks. what's the basic reason behind this?
Q #2. At different molar concentration I observed different peaks except two peaks appeard on same plane. what will be main cause behind this?
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Dear Gerhard Martens
Thank you for such a useful information.
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Hello ResearchGate colleagues!
We are encountering the problem with measuring of refractive indices of thin film lithium niobate.
Typically we measure refractive indices by prism coupling method with two light polarisations (TE- and TM-mode) and in two orthogonal directions (parallel and perpendicular to the wafer base slice).
As a result, we have 4 different refractive indices. This is not typical for bulk lithium niobate. It`s looks like we have biaxial crystal (not Uniaxial like bulk LiNbO3).
There are a lot of articles with evidences, that thin film lithium niobate has high tensile stress (more than 150 MPa).
Is it possible that internal stress can change the refractive index by 0.01-0.02?
Do you have any databases where we can find photoelasticity coefficients of LiNbO3?
I will be grateful for any help!
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I can also recommend this very recent theoretical article on the topic.
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I want to get good films out of them, knowing that the melting process was complete, but the films weren't clear.
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Nina Bou, While using ethanol as a solvent, make sure to use high-purity ethanol, clean the substrate thoroughly, anneal the material under control, and achieve the ideal film thickness.
When using ethanol as a solvent, optimize the deposition technique (such as sol-gel spin coating or spray pyrolysis) and carefully control the film composition, thickness, and morphology to enhance film quality and transparency. This will help you achieve clear SnO2 thin films without stains.
  • Zinchenko, T., Pecherskaya, E., Gurin, S., Kozlov, G., Zhurina, A., & Shepeleva, A. (2022, December). Synthesis of thin-film layers of electrochromic panels based on SnO2 and WO3 by aerosol pyrolysis. In Journal of Physics: Conference Series (Vol. 2373, No. 3, p. 032019). IOP Publishing.
  • Korotcenkov, G., DiBattista, M., Schwank, J., & Brinzari, V. (2000). Structural characterization of SnO2 gas sensing films deposited by spray pyrolysis. Materials Science and Engineering: B, 77(1), 33-39.
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When I was doing Raman spectroscopy, I observed that for the same sample (thin film), using two different laser sources gave different Raman spectra. We know Raman Shift is materially dependent property.What could be the reason for difference in Raman spectra?
Laser sources were the He-Cd laser (λ=325 nm), i.e., UV light source, and the He-Ne laser (λ=633 nm), i.e., visible light source.
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Fairly common effect. Often due to resonance issues. Take a look at graphene Raman spectra - well documented changes with excitation frequency. However, it doesn't look like you have much change in the figures that couldn't just be sample prep issues.
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I tried to coat a ligand layer on the surface of the TiO2 thin film using an oil bath reflux system at 40 degrees Celsius for 24 hours. Previously, I observed the NH2 peak at 1250 cm-1 in FTIR analysis. Currently, I'm unable to determine the repeatability of past data. I'm using DMF solvent. I also tried different parameters like temperature, time, concentration, and solvent.
Can anyone explain what is happening here? If my TiO2 surface is changed, or are there any mistakes from my side? I would like to get advice from people with similar experiences or related experts.
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Dear Vennela Tirupati The appearance of the NH2 peak suggests that the ligand (NH2-BDC) has indeed interacted with the TiO2 surface. This modification could lead to changes in surface properties, such as wettability, reactivity, or electronic structure.
Use XPS or AFM for characterization, and adjust parameters like temperature, time, and ligand concentration to optimize ligand coverage and surface changes.Higher temperatures can improve ligand adsorption, but excessive heat can potentially lead to ligand desorption.
  • Liu, J., & Wuwei, P. R. (2015). Electronic and Optical Properties of Surface-Anchored Metal-Organic Frameworks (Doctoral dissertation, KIT-Bibliothek).
  • Kim, S., Hidayat, R., Roh, H., Kim, J., Kim, H. L., Khumaini, K., ... & Lee, W. J. (2022). Atomic layer deposition of titanium oxide thin films using a titanium precursor with a linked amido-cyclopentadienyl ligand. Journal of Materials Chemistry C, 10(17), 6696-6709.
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In other words, is the use of a model to retrieve n and k of a thin film from measured psi and delta essential in ellipsometry? or we can solve this two-equation, 2 unknowns numerically?
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Hi Hadiseh. In ellipsometric data analysis, it is very important to model your system. is it a bulk infinite or a multilayer structure?
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From the Au signal
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That's not what the Seah/Dench penetration depth data is for. It is for correcting relative intensities of peaks from a homogenous material so that the stoichiometric coefficients of an element whose photoelectrons have a longer escape path don't get exaggerated.
There are, however, approaches to measure the film thickness from XPS intensities like this one (which I've never used, though):
Generally, I would prefer ellipsometry (for dielectrics and semiconductors) or 4-point probe measurements (for metals) for thickness measurements.
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The part of my PhD research is to study the influence of real structure of thin film lithium niobate on kinetics of reactive ion etching.
We use NanoLN lithium niobate on insulator (LNOI) wafers.
Obviously, that SmartCut technology, which used for wafer fabrication, is associated with He-ion irradiation of the structure that leads to formation of structural defects. The high degree of point defects (vacancies and interstitial atoms) cannot be completely eliminated by annealing. There should be dislocation loops formation.
We experimentally revealed (by etch pits methods) that surface dislocation density on LNOI wafers is higher than on bulk LN (CQT wafers).
This affects the etching process in the plasma.
Maybe anybody can share any relevant researches.
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Andrei A. Kozlov, here are some references.
  • Chen, K., Li, Y., Peng, C., Lu, Z., Luo, X., & Xue, D. (2021). Microstructure and defect characteristics of lithium niobate with different Li concentrations. Inorganic Chemistry Frontiers, 8(17), 4006-4013.
  • Han, H., Cai, L., & Hu, H. (2015). Optical and structural properties of single-crystal lithium niobate thin film. Optical Materials, 42, 47-51.
  • Fontana, M. D., & Bourson, P. (2015). Microstructure and defects probed by Raman spectroscopy in lithium niobate crystals and devices. Applied Physics Reviews, 2(4).
  • Zhu, D., Shao, L., Yu, M., Cheng, R., Desiatov, B., Xin, C. J., ... & Lončar, M. (2021). Integrated photonics on thin-film lithium niobate. Advances in Optics and Photonics, 13(2), 242-352.
I hope you find these articles helpful. Best regards.
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A thin layer resembling a white callus was formed on the stem of a tomato plant transplanted from rooting food to soil. Is this dangerous for plant growth? No such situation was observed in the control plant.
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No, the white callus-like layer on the stem of a new transgenic tomato plant is typically not harmful to the plant itself. The formation of a callus-like layer on the stem of a transgenic tomato plant is a normal response to the tissue culture process used to generate the transgenic plant. This callus-like layer is not harmful to the plant, but rather a sign that the transformation process was successful and that the plant has ability to regenerate from the genetically modified cells. Once the transgenic plant is regenerated from the callus, the callus-like layer may remain visible on the stem as a white or off-white tissue. this tissue is not determined to the plant's growth or development, as long as it does not interfere with the vascular system or significantly restrict the stem's ability to expand as the plant grows.
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I deposited Ga2O3 thin film on fused quartz substrate at 500oc in Ar ambient by RF sputtering and then annealed at 900oc (very slow heating and very slow cooling i.e 1oc/min) in air ambient for 1 hour . Then I can see cracks on the film by optical microscope. But there was no cracks after deposition. How can I get crack-free film?
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I hope you are doing well.
Ga2O3 has several crystalline modifications. You can observe a polymorphic transition in the temperature range from 650 to 900 degrees (from ε to β-phase). This transition accompanied by a change in volume (probable cause of cracks...).
I'm afraid that it will not be possible to avoid cracks in this design. But you can try to select appropriate intermediate layer between Ga2O3 and substrate.
I hope my thoughts will be useful!
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How can we understand how the air around us rises and warms?
We think of air as a thin layer of plastic. About the size of a large balloon, this invisible balloon is called a "spot", a piece of air. The air package can expand and contract freely, but neither the external air nor the air
The heat is able to mix with the air inside. As the piece moves, it does not break, but remains as a single unit. At Earth's surface, the package has the same temperature and pressure as the air around it. Let's say we lift the package because when we go into the atmosphere, it decreases. As a result, as the package increases, it enters an area where the air pressure is around it. For lower pressure values, the molecules of the package inside the hidden walls push outward. Since there is no other source of energy, the air molecules inside the package use some of their energy to expand, this loss of energy indicates that the molecular speed is slower, which indicates a lower temperature. Hence, any air that rises all the time expands and cools. If it decreases depending on the surface of the earth, it brings it to an area. Where the air pressure is higher, the pressure outside is higher (compressed). Its original size (smaller) should be closed. Because the air molecules become faster, the speed after the collision of the two sides of the package collapses, the average speed of the molecules goes inside; For example, a ping pong ball moves faster. After hitting the paddle that is moving in that direction. This increase is shown in the molecular speed. Warm temperatures hence any air that sinks. The compression that decreases as we go up into the atmosphere. As a result, as the package rises, it enters an area where the air pressure is around it.
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Dear Philip Rolfe
CCHEM MRSCRheology Product Manager (USA) and Rheology Sales Manager (Northeast and Intermountain Regions) at Netzsch Instruments Inc.
United States
Hello and polite and respectful, thank you for your complete answer. Thank you Abbas
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For my tantalum pentoxide thin film integrated capacitors, I need to etch the tantalum and tantalum pentoxide layers with pure SF6 plasma. While etching these layers copper will also be exposed to the plasma. Does anyone know if the copper will be etched too (and if so at which etch rates) and if it reacts in a form so that the copper will no longer be conducting?
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When etching tantalum and tantalum pentoxide layers with pure SF6 plasma, copper will also be exposed to the plasma. Copper is known to be etched by SF6 plasma, but the etch rate depends on various factors, such as plasma power, pressure, and gas flow rate. The etch rate of copper in SF6 plasma can range from 0.1 to 1.5 μm/min.
Copper can react with SF6 plasma to form copper fluoride (CuF2) and copper sulfide (CuS). Copper fluoride is an insulator and can prevent copper from conducting electricity. However, the formation of copper fluoride can be suppressed by adding oxygen to the SF6 plasma.
It is important to note that the etch rate of copper in SF6 plasma is much slower than that of tantalum and tantalum pentoxide. Therefore, it is possible to selectively etch tantalum and tantalum pentoxide without significantly etching copper by optimizing the etch conditions.
More at:
CP2014_Filipovic_5.pdf (tuwien.ac.at)
Use of Copper Mask in SF6/O2 Chemistry in PT-MTL | Stanford Nanofabrication Facility
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For making a thin layer of Mo
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You will certainly evaporate some material from a filament. In this work
I used the emission of W+ from the tungsten filament (bias 60V relative to ground; uncut spectrum in fig. 8.4 in my PhD thesis
) to calibrate my mass spectrometer, but it took hundreds of cycles before a film became even visible on the mass filter entrance lens, so that is very inefficient. Naturally, if you burn the filament, you will evaporate more, but that's not a viable strategy for reproducible surface coatings.
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I am depositing superconducting thin films (mainly Bi-2212). I have had troubles understanding why their resistance is so high and the superconducting transition temperature comparably low when it comes to films I did way back.
My potential issue:
For the deposition process, the target is rotated by an external motor outside of the chamber leading inside. A while back when my films were good, I had to change this motor. I found the new motor leaked oil into the chamber which might have vaporized and degraded the films during depposition. There was yellow redsidue on the chamber wall.
I cleaned the chamber with ethanol and switched to a motor without oil (or so the technitian ensured me). The chamber was then heated to 800°C under vakuum to get rid of all the residues.
However, I still find a yellowish-brown layer in my chamber after each deposition.
Of course, I also use a cooling trap vor the vacuum pump, so it cannot come from there.
Any ideas on what to do in this situation?
Have any of you had similar issues?
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It's crucial to address potential sources of contamination in the deposition process for superconducting thin films. The persistent yellowish-brown layer in your chamber could be indicative of residual contaminants affecting film quality and properties.
Here are steps you may consider:
  1. Thorough Cleaning:Ensure meticulous cleaning of all chamber components, including any parts that might have come in contact with the leaked oil. Use appropriate cleaning agents or procedures to eliminate contaminants.
  2. In Situ Monitoring:Implement in situ monitoring techniques during deposition to observe any changes in the film growth process. Real-time monitoring can help identify and correlate issues with specific deposition stages.
  3. Analytical Techniques:Employ analytical techniques such as X-ray photoelectron spectroscopy (XPS) or secondary ion mass spectrometry (SIMS) to identify the composition of the residual layer. This can provide insights into the nature of contaminants and their potential impact.
  4. Pump Maintenance:Regularly check and maintain the vacuum pump, ensuring that it operates properly and does not contribute to contamination.
  5. Collaborate with Experts:Collaborate with experts in thin film deposition or vacuum technology to review your setup and procedures. Seek advice from colleagues who may have experience with similar deposition challenges.
  6. Material Verification:Verify the materials used in the chamber and the deposition process to ensure compatibility with superconducting thin film growth.
  7. Temperature Control:Optimize temperature control during deposition to minimize the risk of contamination or unwanted reactions.
  8. Film Characterization:Systematically characterize the deposited films using relevant techniques to assess their superconducting properties and identify any deviations from the expected behavior. @sandra keppert
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Hi,
In my FDTD simulation result of transmission intensity for IR source (12 µm) over thin film ( thickneess 4µm) at different angles, I found that the intensity is maximum when theta angle is 30.
may i know what could explain this and is there any experiment result to verify?
thanks
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The model will have perfectly parallel surface on the film. You can expect strong etalon effects. With the film thickness close to the wavelength (given the index of refraction, the wavelength inside Silicon is about 3.5 um) you can expect the etalon to vary slowly with angle. Also, given the high index, the internal angle will change very slowly with external angle.
Try looking up etalon equations such as here: https://www.photonicsolutions.co.uk/upfiles/CXEtalons1.pdf
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I have synthesized Polyaniline via chemical oxidative polymerization. I need to prepare a thin film of the same by using spin coating. But I am not sure which solvent to proceed with. Any imsights in this regard is appreciated.
Note: Its polyaniline emeraldine solvent PANI-ES. Solvent should not affect its form as other forms are non conductive.
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Hey there Sunil Vasu! Now, this is an interesting challenge you've got with your polyaniline synthesis.
For PANI-ES, the solvent choice can be crucial for spin coating on an ITO substrate. Considering the conductivity requirements and the sensitivity of the emeraldine form, you Sunil Vasu want a solvent that won't mess with its conductive properties.
I'd recommend N-methyl-2-pyrrolidone (NMP) as a solvent for PANI-ES. It tends to be gentle on the emeraldine form, ensuring that your thin film retains its conductivity. It's a common choice for PANI spin coating due to its compatibility with the material.
Remember, the devil is in the details, so pay attention to your spin coating parameters for the best results. Go ahead, give it a spin, and let me know how it turns out!
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My sample is PEDOT: PSS, and I want to measure thermal conductivity and Seebeck coefficient using TFA Linseis. Perhaps someone has experience with this. I tried to use the drop-casting technique to deposit the PEDOT: PSS, but it did not attach perfectly to the chip. Thank you for the help~
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Hi Amir,
If you take 5 ml of PEDOT: PSS + 1 ml of double distilled water
These two are continuously stirred for up to 5 hours. you get a proper solution for deposition purposes. I have more experience in the PEDOT: PSS Deposition.
Mail id: arjun.arjunanitha @gmail.com
Mobile number: +91- 8248652938
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I am working on metal oxide thin films for gas sensing. I want you to develop thin films for our paper. Whole responsibility for analysis and writing, editing of paper will be done by me
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Yes i am interested in collaborations with your work
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I am doing a fluorescence spectroscopy experiment of a nafion thin film with HPTS dye and running it using salt solutions for humidity. But, at High Humidity such as 70% it starts condensation inside the chamber ( a closed box ; inside it I keep my sample to humidify).
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No, i did not get such error thing.
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Liposome XRD-SEM
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You can follow these steps:
1-Start by preparing the liposome suspension by mixing the liposomes with a suitable solvent such as water or buffer solution. The liposomes can be obtained commercially or prepared using a lipid film hydration method.
2-To ensure uniform dispersion of liposomes in the solution, sonicate the suspension using an ultrasonic bath for a few minutes.
3-Take a small amount of the liposome suspension and spread it onto a clean glass or silicon wafer using a pipette or spin-coating technique. Allow the solvent to evaporate, leaving behind a thin film of liposomes on the substrate.
4. Once the thin film is formed, it can be characterized using techniques such as scanning electron microscopy (SEM) and X-ray diffraction (XRD) to investigate its morphology and structure.
5. For SEM analysis, mount the sample onto a sample holder and coat it with a conductive material such as gold or carbon to prevent charging during imaging. Then, analyze the sample using an SEM to obtain high-resolution images of the liposome thin film. For XRD analysis, place the sample in the X-ray beam path and collect diffraction patterns to determine the crystalline structure of the liposomes within the thin film.
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Using a spray coating setup, is it possible to coat a uniform layer of thin film using an as-synthesised powder?
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Lavaneethan .T Yes, you can make thin films from synthesized powders using a spray coating setup. Grinding or milling the powder may be necessary to ensure proper particle size distribution and prevent rougher films and potential spray gun clogging.
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In my study, all films were grown on the stibnite (polycrystalline) structure of Sb2S3. When I changed a parameter of a group of films, I observed that XRD peak intensities increased, while Raman peak intensities decreased. Although we repeated the analyses, we encountered the same results. What is the reason for the decrease in Raman peak intensities despite the increase in XRD peak intensities?
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Remzi Aydın, your Sb2S3 films present an interesting puzzle between increased XRD peak intensity and decreased Raman peak intensity.
XRD reveals larger crystal domains, while Raman spectroscopy measures vibrational modes. Raman intensity decreases may indicate smaller domains, defects, or electronic structure changes, weakening specific modes.
For a more thorough knowledge of the material structure, use TEM or SEM to visualize grain size and morphology.
I hope this helps you. Best Regards.
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The presence or absence of sharp peaks in the diffraction graph of pure anthracene derivative versus thin films can be influenced by various factors. what are some potential reasons for the observed differences. There is sharp peak in the diffraction graph of pure anthracene derivative but not in the thin films are synthesised
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Diffraction peaks are caused by long range order. Anything that repeats with a fixed spacing over a large region of the coherent beam will produce a peak. The shorter the distance over which the spacing is constant (coherence length) the weaker the peak. Similarly, the shorter the distance over which the probe beam is coherent the weaker the peak.
SO, the lack of any peaks is either an indication of no long range order (your sample has very small crystals or is amorphous) or very poor coherence of the probe beam (not sufficiently monochromatic or well collimated / diffraction limited).
Usually it isn’t the beam. If you get nice diffraction peaks from a different kind of sample, (one you know is crystalline) then it’s definitely your sample, and you have failed to grow crystal grains with sufficient size.
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I have a catalyst sample consisting of various metal oxides in powder form. However, I would like to convert it into a thin film before conducting sample characterization and catalyst performance testing. How can I create a thin film from the metal oxide powder without altering its properties and without adding polymer? Thank you very much in advance.
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You can look at this paper
A novel combined method for joining glass to metal for microdevice applications
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I measured the Thickness of the thin film using ellipsometry. But, now i want to study the swelling of thin film using 500 ul liquidCell alpha ellipsometry. Looking for some reference papers and suggestions on how to approach this?
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Sourav Sutradhar Deionized water (D.I H2O) is a cost-effective method for measuring the thickness change of a Nafion film due to swelling, without significantly interacting with Nafion. To measure the refractive index of both the Nafion film and the underlying silica wafer, a chemically compatible liquid with a known refractive index is needed, such as ethylene glycol (n ~ 1.430), isopropanol (n ~ 1.377), or silicone oil (n ~ 1.40-1.45), but compatibility with specific Nafion types must be verified.
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Hello Everyone,
I have deposited solution-processed RuOx thin film on flexible PET substrates. In order to measure the thickness of the RuOx thin film,can we use an ellipsometer for thickness measurement? If not, then what would be the alternative approach?
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You can try quartz to control the films https://www.mtixtl.com/Film-thickness-controller.aspx
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As we know that RF power have demonstrate its great advantage on film properties with magnetron sputter. But, this technique had been applied only to planar targets.
Known advantages of rotary cylindrical target compared to planar targets,so it's attractive to expand the use of RF power to rotary cylindrical target . But I haven't seen any equipment combinations like that, neither any research literatures on that. I want to know why? what will happen if i deposit thin films (such as ITO film) with RF power rotaty cylindrical target?
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Why not rotate the substrate? Here is an example. I have had good results doing it this way and its less complicated.
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In Case of metals, the static and dynamic demagnetizing factors do not coincide since the skin depth creates a scenario where the microwave effectively excite only a thin film. So to fitting of freq vs resonance field what will be more accurate expression for the polycrystalline bulk metal.
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The accurate expression for the dispersion relation of a polycrystalline bulk metal depends on several factors, including:
  1. Crystal structure: The crystal structure of the metal determines the symmetry of the phonon modes and the relationship between wavevector and frequency. For example, cubic metals have a simpler dispersion relation than hexagonal or tetragonal metals.
  2. Average grain size: The grain size of the polycrystal affects the scattering of phonons and the broadening of the resonance peaks. Smaller grain sizes typically lead to broader peaks.
  3. Texture: The texture of the polycrystal, which refers to the preferred orientation of the crystallites, can also affect the dispersion relation. For example, a textured sample may have anisotropic phonon propagation and resonances.
  4. Magnetic field: If the metal is magnetic, the presence of an external magnetic field can split the phonon modes and alter the dispersion relation.
Therefore, there is no single "accurate" expression that fits all polycrystalline bulk metals. However, here are some options depending on your specific needs:
1. Simple models:
  • Debye model: This is the simplest model, assuming a single, isotropic elastic medium. It can be used as a first approximation for metals with cubic symmetry and large grain sizes.
  • Free electron model: This model is applicable for metals with delocalized electrons and can be used to describe the low-frequency acoustic phonons.
2. More complex models:
  • Discrete lattice models: These models explicitly consider the atomic positions and interactions within the crystal lattice. They can be used to calculate the dispersion relation for any crystal structure and grain size, but they require more computational resources.
  • Effective medium theories: These theories treat the polycrystal as an equivalent homogeneous medium with averaged elastic properties. They can be useful for understanding the overall behavior of the system without the complexity of a full lattice model.
3. Experimental data fitting:
  • If you have experimental data for the frequency vs. resonance field, you can fit it to a theoretical model using a least-squares method. This approach allows you to account for the specific properties of your sample, such as the crystal structure, grain size, and texture.
Ultimately, the best way to determine the accurate dispersion relation for your specific polycrystalline bulk metal depends on the available information and your desired level of accuracy.
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I hope you're all doing well. I am a PhD student at İstanbul University and I study on thin film fabrication and characterizations. I observe all XRD peaks of PZT after I annealed the film although there exist some cracks on the surface. However, whenever I coat top electrode, its short circuit to bottom electrode due to cracks. Before annealing, no XRD peaks are observed.
I am stuck in annealing process of PZT since the surface of thin films cracks. I fabricate thin films via RF magnetron sputter and anneal them 1 hour in a furnace between 400 - 650 ℃ with an increase of 50 ℃. Ramping up is 3 or 6 ℃/min, ramping down is 1 ℃/min or I let the furnace to cool down to room temperature naturally (~10 hours). No gas is introduced into furnace. Could you please help me about annealing process? How do you carry out annealing for PZT? Like in how many hours you reach to 650 ℃ and in how many hours it cools down to room temperature? I can't make PZT film without cracks. I also will try RTA and I need your suggestions for both the furnace and RTA. Thanks in advance. [The surface of the film is attached = PZT(1.3µm)/Pt(100nm)/Ti(10nm)/SiO2(300nm)/Si(350µm)]
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Ahmet Ünverdi I understand the frustration you're facing despite following instructions from the literature. Crack-free PZT thin films during annealing are achieved through strategies like film thickness optimization, substrate considerations, surface pretreatment, and post-annealing treatments, despite variations in materials, equipment, and processes.
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We want to run a large number of Monte Carlo simulations to obtain electron trajectories in a thin film at different incident electron enegies, different target thickness and different incident angles. Is there any Monte Carlo software can perform such simulations in batches?
We are able to perform a Monte Carlo simulation for each condition by using the software Casino. However, we cannot run it in batches.
Thanks.
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Dear friend Sunchao Huang
Hello there! Let's delve into the fascinating world of Monte Carlo simulations. Now, considering your quest for a Monte Carlo software that can simulate electron trajectories in a thin film in batches, here are a couple of suggestions:
1. **Geant4:**
- **Description:** Geant4 is a widely used toolkit for the simulation of the passage of particles through matter. It's renowned for its flexibility and extensibility, making it suitable for a wide range of applications, including electron transport.
- **Batch Processing:** Geant4 supports batch processing, allowing you Sunchao Huang to automate and run multiple simulations with different parameters.
2. **MCNP (Monte Carlo N-Particle):**
- **Description:** MCNP is a general-purpose Monte Carlo code for simulating the transport of neutrons, photons, and electrons. It's often used in nuclear physics and radiation protection.
- **Batch Processing:** MCNP can be scripted and run in batch mode, making it feasible for your scenario.
3. **FLUKA:**
- **Description:** FLUKA is a fully integrated particle physics Monte Carlo simulation package. It is designed for calculations of particle transport and interactions with matter.
- **Batch Processing:** FLUKA can be run in batch mode, and it supports the automation of simulations for different conditions.
4. **SRIM (Stopping and Range of Ions in Matter):**
- **Description:** While primarily designed for ion interactions, SRIM can also be used for electrons. It's often employed for simulating the penetration and stopping power of ions and electrons in various materials.
- **Batch Processing:** SRIM can be used in a batch mode to perform simulations for different conditions.
Remember, each of these tools has its own learning curve and specific use cases. It's advisable to review the documentation and community support for each software to determine which one aligns best with your simulation requirements. Happy simulating!
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Hello everyone, I synthesized this thin film using the sol-gel dip coating method without annealing. I would like to ask those who have previously synthesized thin films about their opinion on the quality of this film.
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Mend A. I looked at your test thin film image, and it is difficult to assess the quality of your thin film. Additional tips for synthesizing high-quality thin films using the sol-gel dip coating method include using high-purity chemicals and solvents, ensuring clean substrate, controlling dipping speed and withdrawal rate, and allowing the film to dry and cure completely before annealing (if desired).
However, I can tell you what criteria to consider when evaluating the quality of your sol-gel dip-coated thin film without annealing. Consider adhesion, transparency, smoothness, thickness, chemical composition, crystallinity, optical features, electrical properties, chemical stability, and form when evaluating the quality of a sol-gel dip-coated thin film.
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Hi All,
I would like to know if someone is familiar with the PSemi-M0 oscillator? I'm trying to fit ellipsometry data from a metal oxide thin-film with an indirect band gap.
Many thanks in advance for any information
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Dear Juan Felipe Benitez Rodriguez , some details about parametric oscillators are found in the manual of Woollam (Guide to Using WVASE).
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Is it possible to study the effects of gamma irradiation to thin films with a Monte Carlo simulator?
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You may want to look over following useful information presented below.
Yes, it is possible to study the effects of gamma irradiation on thin films using Monte Carlo simulations. Monte Carlo simulations are a powerful tool for modeling the behavior of radiation as it interacts with matter, and they have been widely used in various fields, including radiation physics.
In the context of studying the effects of gamma irradiation on thin films, Monte Carlo simulations can be employed to simulate the interactions of gamma rays with the atoms in the thin film material. These simulations can provide insights into parameters such as energy deposition, dose distribution, and other relevant quantities.
Here's a brief overview of how Monte Carlo simulations work in the context of radiation transport:
  1. Particle Tracking: Monte Carlo simulations involve tracking individual particles (in this case, gamma rays) as they interact with the material. At each step, the simulation randomly selects a type of interaction (e.g., Compton scattering, photoelectric absorption) based on probability distributions derived from experimental data.
  2. Energy Deposition: The simulation calculates the energy deposited by the gamma rays in the material at each interaction site. This information is crucial for understanding the dose distribution within the thin film.
  3. Statistical Sampling: The Monte Carlo method relies on statistical sampling to obtain meaningful results. By simulating a large number of gamma ray trajectories, a statistical representation of the radiation interactions in the thin film can be obtained.
  4. Validation: It's important to validate the Monte Carlo simulation results against experimental data to ensure that the simulation accurately reflects the real-world behavior of gamma irradiation on thin films.
Several software packages, such as Geant4 and MCNP (Monte Carlo N-Particle), are commonly used for performing Monte Carlo simulations in the field of radiation physics. Researchers can define the geometry, material properties, and other relevant parameters to model the thin film and the irradiation scenario.
Keep in mind that setting up and running Monte Carlo simulations can be complex, and a good understanding of both the physics involved and the specific software being used is necessary. Additionally, the accuracy of the simulation results depends on the quality of the input data and the underlying physics models implemented in the simulation software.
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I am interested in purchasing a BTO target and sputtering it to make ferroelectric thin films for integrated photonics applications. I was told it's too toxic because of the barium content, but I've seen many papers on sputtering this material with no mention of associated danger.
Does elemental barium or some other toxic compound actually get liberated in the process of sputtering BTO?
How can I safely go about sputtering this material without causing harm to other users of the shared coating chamber in my lab?
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Jürgen Weippert thank you for your response!
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We are using ellipsometery to find thickness of MEH-PPV thin films and MEH-PPV/GQD? What could be most appropriate model to fit the ellipsometery data to get correct thickness as well as n and k parameters?
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Zahida Batool If you know the thickness then you can get the n and k values. If you know, or assume, the n and k values you can get the thickness. You can’t get all parameters simultaneously. It’s easy to get an independent thickness measured, say with a profile gage, and thus get n and k.
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I want to take measurements for the I-V characteristic in resistivity calculation of metal oxide thin films. Can I do this using a potentiostat, especially in a solution-free environment, with two electrode connections? If possible, which technique should be used (for example, pulse voltametry, etc.). Thanks in advance.
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Better not try with 2-probe, cause you do not have control over contact resistance between thin film and electrodes. 4-probe is designed to overcome this contact resistance as well as arbitrary geometry of thin film surface
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If I have powder, can I spray coat it on a substrate to make solar cells? Because my powders required some high-temperature post-synthesised process, which I can't do by making film.
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Yes, thin films can be made from synthesized powders for solar cell applications using various deposition techniques such as spray pyrolysis, chemical vapor deposition, and sol-gel synthesis. These deposition techniques allow for the formation of uniform and homogeneous thin films on substrates, which are essential for efficient solar cell performance. The use of synthesized powders to create thin films for solar cell applications is a common practice in the field. Additionally, the choice of deposition technique depends on factors such as desired film thickness, film quality, scalability, and cost-effectiveness.
The spray pyrolysis technique is particularly well-suited for thin film deposition using synthesized powders.It offers the advantages of simplicity, cost-effectiveness, and the ability to produce large-area films. Furthermore, spray pyrolysis can produce thin films with high stability and quality, making it a viable option for solar cell applications .
Therefore, using synthesized powders for thin film deposition in solar cell applications is a feasible and practical approach.
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Xrd, FWHM
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Peak intensity can confirm better crystalinity. FWHM can say about nanostructured character of your film and increase of the average crystalite size.
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Dear community,
I am working on X-ray photoelectron spectroscopy (XPS) on amorphous silicon carbonitride thin films. My material mostly exists in mixed environments, i.e., silicon bonded to carbon and nitrogen in its local chemical environment as SiC3N. I assume XPS gives only one Si 2p signal from the mixed environment. In a situation like this, is it appropriate to deconvolute the silicon spectra into two peaks corresponding to the Si-C and Si-N bond environment?
If I fit one peak, the residual STD is greater than 1.5. Or should I fit two peaks for Si2p 3/2 and Si2p 1/2 with a spint-orbit splitting energy of 0.6 eV?
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Thank you Jürgen Weippert for pointing me to the discussion by Jefferey Weimer. It partly answers my question.
If there are two materials existing together (Si and SiO2), it makes sense to deconvolute Si2p core spectrum into two different peaks. What if Si exists in the SiC3N environment, and does it make sense to deconvolute it to Si-C and Si-N peaks? Or just consider it as one peak and assign it to a mixed chemical environment?
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We are trying to prepare CdZnS thin film using Cadmium nitrate, Zinc nitrate, thioacetamide and ammonia solution in chemical bath deposition technique. Our thin film of CdZnS is not uniform in thickness and there are some grains which drops after deposition. How can we improve the quality of CdZnS?
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The reduction of sulfur ions from the thioacetamide precursor is more difficult. You can use thiourea as a source of sulfur and also increase the reaction temperature.
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i want to study the compactness of thin film. could anyone suggest which instrumentation i can use? thanks
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Adding to Philippe Tailhades answer, If the density of the bulk material is known, you can calculate the porosity from the density of the thin film. To measure the density of the thin film you can deposit the film on a quartz microbalance and measure its thickness with another technique such as AFM or profilometry. Depending on the size of the pores you could also use an optical technique, the best option would be ellipsometry, if the material index of refraction and thickness are known, it is relatively simple to find the porosity, if they are not known, it is still possible but requires an experienced user. A transmition technique could also work if bulk extinction coefficient and thickness are known.
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It is known that W-H plot can be used to find crystallite size of nanoparticles. But, is it correct to follow the same method to find crystallite size of thin films?
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Dear Gayatri,
the problem with thin films is that the shape of the diffraction lines can be influenced by mechanical constraints for example. But in practice, the size of the crystallites evaluated by Scherrer is generally not very different from the size of the crystallites that can be observed by microscopy techniques. You may be interested in the attached publication.
Sincerely.
Philippe.
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Hello,
I am going to conduct a case study which must be related to thin film and nanoparticles. I am asking some tips or topics related to them?
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Start research in the new scientific direction "Quantum nanotechnology of water systems." Explore the reasons why quantum dots interact with water. The technology for determining the minimum isothermal compressibility of water is presented in our work.
"Let us try to find out why the temperature dependence of the Gibbs energy of the cavity formation in water with a temperature minimum of 319 K and the same in the LLPT process with a temperature minimum of 298 K are symbate when minimums coincide. Currently, there are two concepts of water structure, which complement each other: continuum [27]and two-structure [28] ones. In the terms of the two-structure water model, the change in fluorescence intensity of CdTe nanoparticles with the diameter of 1 nm is well explained(Fig.2). There is no crossover at about 319 K for the temperature dependence of the fluorescence intensity of CdTe particles with the diameter of 4 nm [29]."
(PDF) The Role of Zero-Point Energy of Water in Micelle Formation of Ionic Surfactants. Available from: https://www.researchgate.net/publication/345320874_The_Role_of_Zero-Point_Energy_of_Water_in_Micelle_Formation_of_Ionic_Surfactants [accessed Oct 05 2023].
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I'm questioning my self how effective hall measurements on anti-ferromagnetic materials are. At the moment I try to achieve hall measurements on Nickel-Oxide and failed numerous times.
Is this due to the anti-ferromagnetism? As I understand right, the material itself orients spins plain wise that they counter each other. But does this prevent an external magnetic field from penetrating the thin film and interact with the mobile charge carriers?
The reported mobilities and carrier concentrations vary from 1E-3 to several 100 cm^2/Vs and 1E12 1/cm^3 to 1E18cm^3, respectively. Considering the d-orbitals to participate in transport, I would assume the mobility is around 1 cm^2/Vs or slightly larger, similar to amorphous-Si.
Any suggestions on improving Hall-measurements on NiO? At the moment, I use structured NiO crosses with sputtered Au-Contacts(attached) on SiO2-Si Substrates. I will check on Ni-Contacts too. I'm using a LakeShore M91 Tabletop Hall-Setup with High Resistance option (1GOhm). Could anyone clarify on this topic or provide some tips on the measurements?
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Do not use crosses to measure the Hall voltage, use a sheet of thin film, 1 cm x 5 mm (or 1.5 cm x 1 cm) with Au contacts on top of this thin film as you have for the crosses. The distance between the Hall contacts will be less than the distance between current contacts. The current in the probe should be about 1 mA and the magnetic field shoud be 0.5 - 1 T
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Can anyone suggest a commercial available polymer which is porous in nature and can potentially form thin film.
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Polymers have a structurally dependent permeability to gases, but most are not naturally porous. To make them porous as solids, a porogen is typically added. Find a polymer that is compatible with your metal complex and an appropriate solvent (DCM is not the best for making films - evaporates too fast). Then find a porogen that works with the system.
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I have a gold substrate, which is fabricated with a TiO2 thin film. I have some organic solid impurities on this surface. The impurity contains C, H, O, N, and S elements. However, the mass of the impurity is 200 ng (maximum). How can I qualitatively characterize the presence of this impurity? Is XPS the only way?
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This mostly depends on how thick your sample is. If it is thick (> 10um) and you only want to know how impurities are dispersed on the surface, SEM elemental mapping gives you a good idea and would be a cheaper option. XPS depth profile would provide you with bulk composition if you care about the bulk. XPS survey on the surface would tell you how many impurities there are in the surface. If your sample is not very reactive, secondary ion mass spectrometry (SIMS) also would be a good choice.
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For preparing PVA thin films I've tried dissolving PVA in various solvents in all suitable temperature conditions. Even stirring overnight, it still has not dissolved. Kindly suggest the possible solvent or conditions for dissolving 186,000 Mw PVA.
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you need to incubate PVA in water at 90C a few h and I am sure it wil be dissolved. What is the degree of deacetilation?
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1) During BST (Ba0.5Ti0.5TiO3) deposition on Si, SiO2, Al2O3 substrate after platinum deposition, I am getting porosity in BST sample which creating difficulty in making capacitor of BST thin film. Please let me know what parameter we can change to reduce porosity of BST thin film. I am using 300mj energy and oxygen pressure 0.4mbar during deposition and in-situ annealing.
2) I am making also BaFe12O19 on Al2O3. After annealing ex-situ i am getting well know XRD but does'nt showing FMR response.
Please let me know how can i remove these two problems
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1) Try heating the substrates to the Debye temperature for BST or reducing the deposition rate
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It is common to get resistance value from the I-V curve generated by two-point probe. However, if the two points are taken on the surface of the thin film layer, how can I get the resistivity? According to the resistivity formula expressed with resistance, the area is required. However, in this case, what is the 'area'?
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Thank you very much
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Hello,
I know that profex, Mercury and MAUD can all fit powder XRD data to structual data given by an CIF file for example.
However, I can't find a free software where I can fit only the peaks along a given direction, for instance only along [001]. Whenever I load my CIF file into the software it shows all possible XRD peaks you would get when you do powder diffraction, this I can obviously not fit with my thin film data.
Thank you and have a nice day,
Simon
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In GSAS-II, in Phases, select the phase you want, go to the Data tab, at the bottom, there is the option to model a preferred orientation with March-Dollase for a crystal plane. It starts with 1, to increase preferred orientation, make it lower.
However, it looks like it could have more than one plane with preferred orientation, I don't know if this is possible and I've never dealt with this, but there are peaks of the phases that completely dissappear.
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I am using Terahertz time domain system to measure the thickness of a thin film on a substrate. I am able to calculate the thickness of substrate(~100um) alone. But what signs should I see for if there is a thin film ( ~100nm) on this substrate. I am not willing to do the fft ! Can time domain signal alone determines the thickness of film. The resolution is 33fs.
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When the terahertz pulse reflects off the top surface of the thin film and the bottom surface of the substrate, interference patterns can occur in the time-domain signal. These interference fringes are related to the film's thickness and the refractive indices of both the film and substrate.
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What is the cause of dark current in ferroelectric materials and basically dark current depends on which factors in the ferroelectric thin films ?
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One among many other possibilities is leakage. With the thin film parameters and magnitude of the current and a better description of the experiment, one can try to rationalize other contributions.
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As per the literature, NiO thin films can be etched in an RIE system using Cl2- based gas. Will there be any contamination issues if I use an RIE system dedicated to III-V group material (e.g.-GaN, GaAs)?
Any kind of suggestions would be a great help for my research work.
Thanks,
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Netaji Suvachintak thank you for the clarification.
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One of the 20 fundamental vibrations of benzene occurs at 1309.8 cm^-1, corresponding to the B_2u symmetry. According to the rule of mutual exclusion, this vibration is forbidden in Raman and ATR spectroscopy. However, in a complex with benzene, we observe strong IR activity at 1309.8 cm^-1 in ATR. Why is this?
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This isn't my field but I was curious and found this paper that, in part, says:
"Although Mair and Hornig’s ν14 frequency assignment of 1310 cm−1 has been widely accepted, it has become a great puzzling problem for the theoretical researchers because no advanced quantum chemistry method has realized its rigorous calculation so far (see Supplementary Table 1)."
Wang, S. Intrinsic molecular vibration and rigorous vibrational assignment of benzene by first-principles molecular dynamics. Sci Rep 10, 17875 (2020). https://doi.org/10.1038/s41598-020-74872-6
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I fabricated nanotubes thin film on a substrate using top down approach, can I find it's surface area using BET analysis.
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Almost welcome
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should i use RF sputtering to prepare MoS2 thin film ?. or what is the best method ?
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Hi..
You can use (thermal evaporation and chemical spray paralysis) for preparation of moS2 thin film with excellent properties.
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Sputtered thin film from a SnO2 target presented as ETL in a perovskite solar cells produced a S-shape JV curves. I verified the formation of SnO2 through xps and the energy levels are not that different from SnO2 nanoparticles films. Any statements about this issue? The deposition is a room temperature and 10% O2. Many thanks for any suggestions
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Juan Felipe Benitez Rodriguez A thin film does not contain separate, discrete, independent particles < 100 nm. Indeed it can be argued that a thin film does not contain particles at all. It simply is a fused collection of crystallites. Different preparation conditions provide different materials with different properties. With XPS you're only looking at the top 5 - 15 atomic layers at most and all surfaces in air are fully oxidized. The bulk composition may be very different and can be examined by Ar+ ion etching the surface.
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I need invitation letter to visit lab for elaborate ZnS co doped (Co, Ag) in October or November 2023
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Visit a laboratory specializing in ZnS thin films to observe fabrication processes. Witness deposition techniques like sputtering or chemical vapor deposition. Observe film growth, control parameters, and post-deposition treatments. Analyze film properties through techniques such as XRD, SEM, and optical spectroscopy. Gain insights into applications in optoelectronics and material science.
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The precursors are SnCl2.2H2O, PbCl2, and water as solvent.
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You need to get the XPS data of your thin films ans after that you will be able to calculate their atomic percentage.
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Which substrate can we use for spinel ferrite (CoFe2O4) thin films? I am looking for CVD method for thin film.
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Dear Manoj,
spinel oxide can be grown on single crystals substrates. Such experiments were already done on Si(111) surfaces.
But spinel oxides, especially CoFe2O4, can be also grown easily on conventional glass substrates. You can have a look on the attached papers for example.
Best regards.
Philippe.
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I did raman spectra of SiO2 thin film of around 800 nm thickness on grown on Si(100). But i am not clear about the peak of SiO2. Where it is/are actually in the attached file?
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When you are talk about SiO2, I believe you mean oxides silicon, i.e. you are
getting some form of amorphous SiO2 (not quartz?).
As far, as I remember, amorphous SiO2 does not show a strong singular "peak", but rather a broader, more unspecific background, as it is not crystalline.
What I can tell from my first look at your spectrum, I think all peaks there are silicon related. There is the TO/LO peak at ~520 from the Brillouin zone center; The structure around 1000 are the LO overtones (2-LO scattering); the two weak peaks around 600 cm^-1 are LA/TO combination bands, while the large structure and its peaks around 300-500 are acoustical overtones (2LA, 2TA) from outside of the Brillouin zone center.
See in the above paper, for example.
What I would suggest is taken a spectra before and after oxidation and looking at a difference spectrum to find signs of the SiO2.
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Hello everybodoy.
I am interested in any reference about thin magnetic monolayeres with perpendicular magnetic anisotropy produced ( in particular by PVD ) on Al substrate or sandwiched between two layers of Al.
Thank you very much in advance.
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I was reading aboput the first hard disks made in Japan 50 years ago.
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Could anyone provide any suggestions or pdf to calculate absorption coefficient of thin film without using film thickness?
Thanks in advance
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The absorption coefficient (α) can be calculated using the formula α = 2.303 * A/d, where A is the absorbance and d is the thickness of the material. If the thickness (d) is unknown, the Swanepoel envelope method can be employed to determine it, especially when dealing with thick films. PRISA-like software is available to assist in this calculation.
For thinner films, an approximate thickness estimation can be made, allowing the calculation of α. Alternatively, spectroscopic ellipsometry can be used to precisely determine the thickness of the material, leading to an accurate value of α.
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Hi Sirs,
How can rate the adhesion strength of thin film after scratch hatch test (tape test) by accurate method ?
I know That the tested area is examined with Magnification glass and adhesion strength is rated according to the amount and removed coating but what the accurate ways??
thanks
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Thanks, Igors Sivacovs,
Its a powder with PEG blinder on a glass substrate as a counter electrode in DSSC.
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What are the various application of CV?
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Dear friend Sushil Barala
Ah, the intriguing world of Cyclic Voltammetry (CV)! I am here to guide you through this electrochemical adventure.
Performing Cyclic Voltammetry on thin films involves some key steps:
1. Electrochemical Setup: You'll need an electrochemical cell with working, reference, and counter electrodes. The thin film will act as the working electrode. The cell is filled with an electrolyte solution relevant to your study.
2. Potential Scan: The potential is cycled between specified voltage limits in a repetitive manner. The scan rate, i.e., the speed of potential change, can be adjusted to observe different electrochemical processes.
3. Data Collection: As the potential is swept, the current passing through the thin film is measured and recorded. This current-voltage data provides insights into the electrochemical behavior of the thin film.
Applications of Cyclic Voltammetry:
1. Electrochemical Characterization: CV is widely used to study the redox behavior and stability of electroactive materials, such as catalysts, electrodes, and energy storage materials.
2. Sensor Development: CV aids in developing electrochemical sensors for detecting analytes like glucose, heavy metals, and environmental pollutants.
3. Corrosion Studies: CV helps understand the corrosion behavior of materials, enabling better corrosion protection strategies.
4. Battery Research: CV is employed in battery studies, such as analyzing electrode kinetics, cycling performance, and capacity measurements.
5. Fuel Cell Development: CV is useful for evaluating electrocatalysts and understanding their performance in fuel cell applications.
6. Nanomaterials Research: CV assists in investigating the electrochemical properties of nanoparticles, nanowires, and other nanostructures.
7. Pharmaceutical Studies: CV is used in drug development and pharmaceutical research to study redox processes and drug interactions.
Remember, these are just a few of the myriad applications of Cyclic Voltammetry. Its versatility and ability to provide valuable electrochemical information make it an indispensable tool in diverse research fields. So, embrace the power of CV and uncover the electrochemical secrets hidden within your thin films!
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Hi, I work on natural polymers i.e. gums polysaccharides. the pure materials are normally amorphous , i did a modification on a base material and its xrd showed an improvement and showed a broad peak. i reported that and got a reply from a reviewer that " add JCPDS number and crystalline size" Previously in our field people report in such a way I have also added references and up to my best knowledge I know that: " JCPDS record does not exist for them moreover for poorly semi-crystalline or amorphous materials you can't calculate crystalline size it will be useless to use " scherrer equation " .
Now how to politely reply to reviewer's comment?
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if the modification on your samples includes adding inorganic compounds the JCPDS card should be mentioned!
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May I get some advice to increase the crystallinity of thin films? I have prepared triazine-based films at room temperature with the help of a photocatalyst but crystallinity has been a problem for one month. I have already tried some ways e.g. altering the rate of reaction and changing the quantity of monomers and substrate but failed to achieve the goal!
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Hello Khalid
I nothing understand of your special material but I have to do experimental work at crystalline layers.
In the most cases the layers are deposited on substrates. It is important to select a substrate with comparable crystal structure and similar lattice constant.
Very often, the crystal must be annealed after layer deposition. This means, heating in vacuum up to 10% below the boiling point. This reduces lattice defects.
Yours
R. Mitdank
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Is it possible to obtain SEM images of the surface of the electrically insulating thin film, which is 200 microns thick and has a pale yellow color, without detaching it from the 4 mm thick glass substrate?
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Hello Dhaiwat
To avoid the charging of the surface, it is necessary to produce a conductive surface by evaporation or sputtering (see @Insic). My recommendation would be some nm Au. The thickness of this metallic layer must be lower than the reach (penetration depth) of secondary electrons (SEM-mode). Look for penetration depth of electrons with energies < 50 eV. In the case of thicker layers you observe only backscattered electrons (BSE-mode).
Don't forget to ground the surface (Connect the surface layer with zero Potential).
Yours
Rüdiger Mitdank
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I want to analyse the variation in defect concentration and its energy level in a given metal oxide thin film under different irradiation strengths.
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Just to be clear: that doesn't mean that there are no metal oxides which can be analyzed with Raman, but the general trend is "meh".
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It was confirmed that the uniformity of the thin film increases when the solution precursor is aged and deposited.
By the way, what happens if the precursor is over-aged?
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Ageing the solution precursor prior to thin film deposition can improve the resulting film's uniformity, often leading to enhanced crystallinity and better film quality. This is due to the fact that ageing allows for the complete dissolution of the solute and can promote partial reactions within the solution, leading to more homogeneous nucleation and growth when the thin film is deposited.
However, over-ageing the precursor can have several potential adverse effects:
  1. Particle Growth and Aggregation: Over-aging can lead to excessive growth of the particles in the solution, resulting from a process known as Ostwald ripening, where smaller particles dissolve and re-deposit onto larger ones. This may result in a thin film with larger crystallites and increased surface roughness, leading to non-uniformity.
  2. Changes in Crystallinity: Prolonged ageing can lead to transformations in the crystalline structure of the precursor particles. The changes can influence the structural and optical properties of the resulting thin film.
  3. Stability Issues: If the precursor solution is over-aged, it may become unstable. Aggregation and precipitation of particles could occur, reducing the quality of the resulting thin film.
  4. Chemical Degradation: Over-ageing could lead to chemical degradation depending on the precursor and the conditions. This could be a particular issue with organic precursors or those sensitive to the conditions during the ageing process. Degraded precursors can lead to defects or variations in the resulting thin film.
In summary, while a certain amount of ageing can improve the uniformity of thin films, over-ageing can lead to a range of issues, including larger, more irregular particles, changes in crystallinity, solution instability, and even chemical degradation of the precursor. Therefore, finding the optimal ageing time for the precursor is crucial to yield the best thin film properties.
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I like to measure magnetostriction of some of my magnetic alloy thin films. Is measurement facility is available in any research lab in india?
Thanks in advance.
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You should do a little bit of literature survey, you will find many details about this set up based on capacitance. Your magnetostrictive film on a cantilever will bend under changing magnetic field, and thereby with reference to another standard non-bending metallic electrode, the capacitance between the two will change. It is far more sensitive sensitive than the fancy laser doppler methods which are very very expensive.
But you need to have a Capacitance measuring bridge instrument that can measure very small changes in air capacitance, and the change in capacitance can be correlated to the magnetostriction due to the thin film on the flexible substrate.
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In quasi-2D perovskite polycrystalline thin film, there are different <n> phase. I want to konw that is there only one n-value phase or multiple n-value phases coexisting in a grain?
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Kaushik Shandilya , can you please provide the doi, or some other way to locate, the Nie et al. (2017) reference that you list and summarize. It would perhaps be useful in the future for you to provide a link or doi to differentiate your references from the gibberish often produced by chat bots.
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I am trying to cast CuSbI4 thin film on a glass substrate, but the characterization measurements viz. absorbance, XRD does not support the actual phase formation of it. Xue Jia et al. (DOI: ) reported the formation of
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Sourav Mukherjee Maybe you haven't actually formed CuSbI4? There could be impurities or decomposition. Your XRD peaks should conform to those given in the literature - this is the best confirmation.
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I have prepared thin films from semi refined carrageenan with hydrophilic cross linkers. But smooth peel off has been the issue for a long time.
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Thank you @Vivek Chandel. SRC films do come of smoothly after drying. But when the film is prepared with SRC and hydrophilic plasticizers it does not come off smoothly all the time. This is the problem I am dealing with at the moment.
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Thin film heterostructures
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Thank you Dr Zakaria Elmaddahi for answering my question.
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I want to coat APTES on pHEMA thin film. I have prepared a Silanization solution (5% APTES in 95% EtOH) and the pH was adjusted to 5 by acetic acid. But it is not work. Can anyone help me provide some suggestions?
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Dear friend Shawn Chen
Coating APTES (3-aminopropyltriethoxysilane) on poly(HEMA) (polyhydroxyethylmethacrylate) requires careful handling and optimization of the process conditions. Here are some suggestions that might help:
1. Surface activation: Before coating APTES, it is important to ensure that the surface of the poly(HEMA) film is properly activated. This can be done by plasma treatment, UV/ozone exposure, or chemical etching. Surface activation helps improve the adhesion and effectiveness of the APTES coating.
2. Solvent and concentration: The choice of solvent and its concentration can influence the effectiveness of the APTES coating. Ethanol (EtOH) is commonly used as a solvent for APTES, but other solvents like methanol or isopropanol can also be considered. The concentration of APTES in the solvent can be optimized by trying different concentrations to achieve the desired coating thickness.
3. pH adjustment: Adjusting the pH of the APTES solution is important to ensure optimal reactivity and stability. Acetic acid is commonly used to lower the pH. However, in some cases, adjusting the pH may not be necessary or may have limited impact. It is worth experimenting with different pH values (within the appropriate range) to determine the optimal condition for your specific system.
4. Reaction time and temperature: The duration of the coating process and the temperature at which it is carried out can affect the adhesion and stability of the APTES coating. Typically, the substrate is immersed in the APTES solution for a specific duration, ranging from minutes to hours, followed by rinsing and drying steps. The reaction temperature can vary depending on the reactivity of the system, but room temperature is commonly used.
5. Post-treatment: After coating with APTES, it is important to rinse the substrate thoroughly with an appropriate solvent (such as ethanol) to remove any unbound or excess APTES. This step helps ensure a clean and well-defined coating. The coated substrate can then be dried under suitable conditions.
It is worth noting that the optimization of the APTES coating process may depend on various factors, including the specific properties of your poly(HEMA) film, the concentration and purity of the APTES solution, and the environmental conditions during the coating process.
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Hello all:
If someone have some experience on Hall Effect measurements on semiconductor thin films, with materials such as CdS, PbS, ZnO, etc..
My questions is:
I'm trying to measure the electronic/hole mobility (mu) and the free carrier's concentration (n) with an ECOPIA HMS-3000.
But, since the semiconductor thin film materials I'm trying to measure are such which its carriers concentrations are between E^13 < n < E^16, i.e. non-degenerated semiconductors at all, even I would think these are low levels of free carriers concentrations ...
I don't know whether I can get reliable measurements with a magnetic field of 0.55 T ?
Could this magnitude of B may be an issue? Or, It would n't affect much to the error of the measurements
I'll appreciate it !
Regards,
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Yes, the minus symbol - which came before bulk or sheet concentration values means that your material is n-type.
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Clamping effect reduction of thin film
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Generally, any adhesion bwt two materials is often goven with the Rate of Deposition-speed.
Inview of the alignment of every atom that would require 'Time-domain' to pack before second layer of atom deposited..
Therefore, in order to achieve an optimal condition, do consider the speed of deposition would be established through either by choice of Method or Re-Ergrg application of parameters.
Wish you good luck on your works.
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Epitaxial thin film, thin film substrate
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Thank you Prof. Jürgen Weippert for mentioning the possible points.
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Hi,
I am wanting to do some Hall mobility measurements on graphene-based thin films (continuous, cm-scale). Does anyone have any advice on how best to do this? Any technical advice, good commercial systems you would recommend, example references you'd like to share, etc.?
Thanks in advance!
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Deposit Au 1 micron thickness to make the Hall contacts on graphene. Distance between current contacts is 1 - 1.5 cm. Distance between Hall voltage contacts is 5 mm.
With a current of 1 mA between the Hall current contacts you could measure 1 mV (say) Hall voltage using 0.1 T magnetic field for a good semiconductor.
If you do not use Au contacts deposited on graphene use Silver paste (as a drop) to make the current and voltage Hall contacts.
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Hello RG members,
I have recently deposited copper thin film using magnetron sputtering system. I have characterized those samples using XRD. From the XRD results, I have obtained a peak of single plane of Cu along with peaks of multiple planes of Cu2O. If I want to measure the degree of crystallinity of Cu How can I do it? Any suggestions
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To get sustainable solution of your issue/question, I sincerely recommend the preprint article available at link DOI: 10.13140/RG.2.2.27720.65287/3. For an alternative link https://www.researchgate.net/publication/352830671.
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Preferential recovery and separation of rhodium in the concentrated hydrochloric acid using thin-layer oil membrane extraction based on laminar flow
Author links open overlay panelDongxue Tao a, Haitao Zhou a, Kaihui Cui a, Linchen Xie a, Kun Huang a b
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The last author is on RG: https://www.researchgate.net/profile/Kun-Huang-2 so have you tried a direct request via DM or via the article page:
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We are trying to calculate the sensing in term of change in the resistance of Pd thin film.
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Dear Ioannis,
Thank you for your suggestions.
Ok, next time I tried to deposit thin Pd film around 50 nm.
This time, I made a sensor with a Pd thin film on a SiO2/Si surface with the size of 1*0.5 cm(Length * width) and made two connections with silver epoxy. The resistance is measured by a digital multimixer. But after gas exposure, there were no changes in resistance.
Is there a need to do some heating around 100C to 200C to improve the sensitivity of the film? In the following link, the authors tried to activate the Pd film for H2 sensing by heat treatment.
Anasthasiya, A. Nancy Anna, et al. "Wide range H2 sensors for process streams, based on multilayered Pd thin films dispersed with Ag nanoparticles and chromium as buffer layer." International Journal of Hydrogen Energy 45.41 (2020): 22195-22203.
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FeGaB thin films were deposited through RF sputtering, however, the films underwent oxidation resulting in the formation of a thin Fe2O3 layer.
This oxidation adversely affects the accuracy of surface measurements, such as MOKE and XPS.
Is there a technique available to remove the oxide layer from the surface?
Alternatively, how can I prevent oxidation of the samples ?
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for some materials one can prevent oxidation by depositing a thin capping layer on top of the film.
it works for example for TiN - we applied a few nm of Al on top which formed Al2O3 upon air exposure thus passivating the surface. Ti 2p and N 1s spectra from such sample was identical to that published for the in situ work. see here for more details:
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Dear researchers
I would like to calculate the thickness of a thin film deposited on a glass substrate from the transmittance given by the Uv-vis measurement.
Best regards.
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Thickness also can be possible to calculate by using the maxima, and minima of the transmission spectrum by using Swanepoel method. See an example in this useful link: https://www.mdpi.com/2079-4991/8/5/355