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Selective silicon and germanium nanoparticle deposition on amorphous surfacesCoffee, Shawn Stephen, 1978- 28 August 2008 (has links)
This dissertation describes the development of a process for the precise positioning of semiconductor nanoparticles grown by hot wire chemical vapor deposition and thermal chemical vapor deposition on amorphous dielectrics, and it presents two studies that demonstrate the process. The studies entailed growth and characterization using surface science techniques and scanning electron microscopy. The two systems, Ge nanoparticles on HfO₂ and Si nanoparticles on Si₃N₄, are of interest because their electronic properties show potential in flash memory devices. The positioning technique resulted in nanoparticles deposited within 20 nm diameter feature arrays having a 6x10¹⁰ cm⁻² feature density. Self-assembling diblock copolymer poly(styrene-b-methyl methacrylate) thin films served as the patterning soft mask. The diblock copolymer features were transferred using a CHF₃/O₂ reactive ion etch chemistry into a thin film SiO₂ hard mask to expose the desired HfO₂ or Si₃N₄ deposition surface underneath. Selective deposition upon exposed pore bottoms was performed at conditions where adatom accumulation occurred on the HfO₂ or Si₃N₄ surfaces and not upon the SiO₂ mask template. The selective deposition temperatures for the Ge/HfO₂ and Si/Si₃N₄ systems were 700 to 800 K and 900 to 1025 K, respectively. Germanium nucleation on HfO₂ is limited from hot wire chemical vapor deposition by depositing nanoparticles within 67% of the available features. Unity filling of features with Ge nanoparticles was achieved using room temperature adatom seeding before deposition. Nanoparticle shape and size are regulated through the Ge interactions with the SiO₂ feature sidewalls with the adatom removal rate from the features being a function of temperature. The SiO₂ mask limited Ge nanoparticle growth laterally to within ~5 nm of the hard mask at 800 K. Silicon deposition on patterned Si₃N₄ has multiple nanoparticles, up to four, within individual 20 nm features resulting from the highly reactive Si₃N₄ deposition surface. Silicon nucleation and continued nanoparticle growth is a linear function of deposition flux and an inverse function of sample temperature. Diblock copolymer organization can be directed into continuous crystalline domains having ordered minority phases in a process known as graphoepitaxy. In graphoepitaxy forced alignment within microscopic features occurs provided certain dimensional constraints are satisfied. Graphoepitaxy was attempted to precisely locate 20 nm diameter features for selective Ge or Si deposition and initial studies are presented. In addition to precise nanoparticle positioning studies, kinetic studies were performed using the Ge/HfO₂ material system. Germanium hot wire chemical vapor deposition on unpatterned HfO₂ surfaces was interpreted within the mathematical framework of mean-field nucleation theory. A critical cluster size of zero and critical cluster activation energy of 0.4 to 0.6 eV were estimated. Restricting HfO₂ deposition area to a 200 nm to 100 [mu]m feature-width range using SiO₂ decreases nanoparticle density compared to unpatterned surfaces. The studies reveal the activation energies for surface diffusion, nucleation, and Ge etching of SiO₂ are similar in magnitude. Comparable activation energies for Ge desorption, surface diffusion and cluster formation obscure the change with temperature an individual process rate has on nanoparticle growth characteristics as the feature size changes. / text
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Chemical Vapor Deposition of Thin Film Materials for Copper Interconnects in MicroelectronicsAu, Yeung Billy 24 July 2012 (has links)
The packing density of microelectronic devices has increased exponentially over the past four decades. Continuous enhancements in device performance and functionality have been achieved by the introduction of new materials and fabrication techniques. This thesis summarizes the thin film materials and metallization processes by chemical vapor deposition (CVD) developed during my graduate study with Professor Gordon at Harvard University. These materials and processes have the potential to build future generations of microelectronic devices with higher speeds and longer lifetimes. Manganese Silicate Diffusion Barrier: Highly conformal, amorphous and insulating manganese silicate \((MnSi_xO_y)\) layers are formed along the walls of trenches in interconnects by CVD using a manganese amidinate precursor vapor that reacts with the surfaces of the insulators. These \((MnSi_xO_y)\) layers are excellent barriers to diffusion of copper, oxygen and water.
Manganese Capping Layer: A selective CVD manganese capping process strengthens the interface between copper and dielectric insulators to improve the electromigration reliability of the interconnects. High selectivity is achieved by deactivating the insulator surfaces using vapors containing reactive methylsilyl groups. Manganese at the Cu/insulator interface greatly increases the strength of adhesion between the copper and the insulator. Bottom-up Filling of Copper and Alloy in Narrow Features: Narrow trenches, with widths narrow than 30 nm and aspect ratios up to 9:1, can be filled with copper or copper-manganese alloy in a bottom-up fashion using a surfactant-catalyzed CVD process. A conformal manganese nitride \((Mn_4N)\) layer serves as a diffusion barrier and adhesion layer. Iodine atoms chemisorb on the \(Mn_4N\) layer and are then released to act as a catalytic surfactant on the surface of the growing copper layer to achieve void-free, bottom-up filling. Upon post-annealing, manganese in the alloy diffuses out from the copper and forms a self-aligned barrier in the surface of the insulator. Conformal Seed Layers for Plating Through-Silicon Vias: Through-silicon vias (TSV) will speed up interconnections between chips. Conformal, smooth and continuous seed layers in TSV holes with aspect ratios greater than 25:1 can be prepared using vapor deposition techniques. \(Mn_4N\) is deposited conformally on the silica surface by CVD to provide strong adhesion at Cu/insulator interface. Conformal copper or Cu-Mn alloy seed layers are then deposited by an iodine-catalyzed direct-liquid-injection (DLI) CVD process. / Chemistry and Chemical Biology
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Chemical Vapor Deposition of Cobalt-based Thin Films for MicroelectronicsYang, Jing January 2013 (has links)
In microelectronics, the device size continues to shrink to improve the performance and functionality, which sets technical challenges for the integrated circuit (IC) fabrication. Novel materials and processing techniques are developed to maintain excellent device performances and structural reliability. Cobalt-based thin films possess numerous applications in microelectronics with the potential to enhance the device performance and reliability. This thesis explores the fabrication, characterization and application of cobalt-based thin films for microelectronics. Chemical vapor deposition (CVD) technique has been applied for depositing cobalt-based thin films, because CVD can produce high quality thin films with excellent conformality in complex 3D architectures required for future microelectronics. / Engineering and Applied Sciences
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Dynamic feature analysis of an industrial PECVD tool with connection to operation-dependent degradation modelingBleakie, Alexander Q. 23 December 2010 (has links)
An analysis that is based on the monitoring of dynamic features from in-situ sensors of an industrial PECVD tool is presented. Linear Discriminant Analysis is used to determine which features are the most sensitive to various changes in the tool condition. The concept of Confidence Values (CVs) is used to quantify statistical changes of these dynamic features as the condition of the tool changed. Two data sets were collected from a PECVD tool in the facilities of a well-known equipment supplier. Dynamic features coming from the RF plasma power and matching capacitors’ sensors are shown to be sensitive to various changes in the cleaning cycles for Si-N, Si-O₂, and TEOS depositions. Quantifying the statistical distributions of the sensitive sensor features during tool condition changes is important for determining which sensor features are necessary to monitor in order to predict the tool chamber health. Results show that these RF plasma sensors could be used to track changes inside the tool chamber. / text
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Χημική εναπόθεση μικροκρυσταλλικού υδρογονωμένου πυριτίου με πλάσμα υψηλής πυκνότητας ηλεκτρονίωνΔημητρακέλλη, Παναγιώτης 27 May 2014 (has links)
Το μικροκρυσταλλικό υδρογονωμένο πυρίτιο (μc-Si:H) βρίσκει εφαρμογή ως ενδογενής ημιαγωγός σε φωτοβολταϊκές ιδιοσυσκευές λεπτών υμενίων πυριτίου απλής και ανάστροφης δομής (tandem). Η τυπική μέθοδος παρασκευής του υλικού είναι η χημική εναπόθεση ατμών ενισχυμένη με πλάσμα (Plasma Enhanced Chemical Vapor Deposition – PECVD) με χρήση χωρητικών εκκενώσεων υψηλής αραίωσης σιλανίου (SiH4) σε υδρογόνο (H2). Εξαιτίας της χαμηλής απορρόφησης στο ορατό φάσμα απαιτείται αρκετά μεγάλο πάχος της ενδογενούς στοιβάδας του μc-Si:H, ωστόσο με τα υπάρχοντα δεδομένα οι ρυθμοί εναπόθεσης είναι αρκετά χαμηλοί με αποτέλεσμα οι χρόνοι εναπόθεσης να είναι απαγορευτικοί για τη βιομηχανία. Έτσι γίνεται επιτακτική η ανάγκη για υψηλούς ρυθμούς εναπόθεσης (> 5 Å/s) ούτως ώστε να είναι εφικτή η παραγωγή φωτοβολταϊκών κελιών χαμηλού κόστους.
Σκοπός της παρούσας εργασίας είναι η μελέτη εναλλακτικών τεχνικών ενίσχυσης του ρυθμού εναπόθεσης λεπτών υμενίων μc-Si:H όπως η χρήση πηγής πλάσματος υψηλής πυκνότητας ηλεκτρονίων (Hollow Cathode) και η χρήση δισιλανίου (Si2H6) ως επιπρόσθετο του τυπικού μίγματος SiH4/H2. Στο πρώτο μέρος παρουσιάζεται η κατασκευή δύο ηλεκτροδίων hollow cathode διαφορετικής γεωμετρίας και ο ηλεκτρικός χαρακτηρισμός τους σε εκκενώσεις Η2 με σκοπό τη βελτίωση της γεωμετρίας της πηγής και των συνθηκών στις οποίες επιτυγχάνεται υψηλή πυκνότητα ηλεκτρονίων στην εκκένωση. Επιπλέον παρουσιάζονται μετρήσεις ρυθμού εναπόθεσης λεπτών υμενίων με την πηγή hollow cathode διερευνώντας διαφορετικές παραμέτρους της διεργασίας και πραγματοποιείται σύγκριση με την προϋπάρχουσα πηγή χωρητικής σύζευξης. Αποδείχθηκε ότι με τη χρήση καθοδικών κοιλοτήτων μεγάλης διαμέτρου (20 mm) η πυκνότητα των ηλεκτρονίων αυξάνει σημαντικά και οι ρυθμοί εναπόθεσης είναι έως και τρεις φορές υψηλότεροι σε σχέση με την πηγή χωρητικής σύζευξης. Στο δεύτερο μέρος παρουσιάζεται η επίδραση της προσθήκης μικρής ποσότητας Si2H6 στο μίγμα SiH4/H2 στο ρυθμό εναπόθεσης και την κρυσταλλικότητα των λεπτών υμενίων πυριτίου, πραγματοποιείται βελτιστοποίηση της διεργασίας όσον αφορά την πίεση και συγκρίνεται η χρήση Si2H6 με την αύξηση της παροχής του μίγματος SiH4/H2. Η προσθήκη Si2H6 σε περιοχή πιέσεων 2-3 Torr αποδείχθηκε ευεργετική για το ρυθμό εναπόθεσης των υμενίων (έξι φορές αύξηση) λόγω ενίσχυσης της πυκνότητας ηλεκτρονίων και του ρυθμού διάσπασης του SiH4. Επίσης η προσθήκη Si2H6 οδηγεί σε υψηλότερη απόδοση εναπόθεσης συγκριτικά με την αύξηση της συνολικής παροχής του μίγματος SiH4/H2 ή της περιεκικότητας σε SiH4. / Microcrystalline hydrogenated silicon (μc-Si:H) is widely used as intrinsic layer in thin film solar cells of single or tandem structure. This material is most commonly produced via Plasma enhanced Chemical Vapor Deposition (PECVD) from highly diluted silane (SiH4) in hydrogen (H2). However, the rather low absorption coefficient of the intrinsic material in the visible spectrum imposes higher layer thickness in order to ensure high device efficiency. The key obstacle for the production of cost-effective solar cells is the relatively low growth rate of the intrinsic μc-Si:H and thus the research is focused on the increase of the deposition rate while maintaining the thin film quality.
In this work we aim to study alternative techniques in order to enhance the μc-Si:H thin films growth rate such as the utilization of high electron density plasma source (hollow cathode) and the small disilane (Si2H6) addition to the SiH4/H2 gas mixture. In the first part is presented the construction of two novel hollow electrodes and their electrical characterization in H2 discharges aiming to investigate the conditions that ensure a high electron density in the discharge. Moreover, deposition rate measurements are presented for the hollow cathode source and compared to the already existing CCP source. It was proved that for the larger hollows (20mm diameter) the average electron density increased abruptly and the corresponding deposition rate was about 3 times higher comparatively to the CCP source. In the next part of this study is presented the effect of the small Si2H6 addition to the gas mixture to the silicon thin films growth rate and crystallinity, the process is optimized in terms of the total gas pressure and compared to the case of the SiH4/H2 total flow rate increase. The small Si2H6 addition in the narrow pressure region of 2-3 Torr proved beneficial for the film growth rate (six times increase) due to the sharp enhancement of the electron density and the SiH4 dissociation rate. The Si2H6 addition also resulted in much higher deposition efficiency as compared with the increase of the SiH4/H2 flow rate or the SiH4 molar fraction.
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Properties and Processing of Chemical Vapor Deposited Zinc SulfideMcCloy, John S. January 2008 (has links)
The structure and properties of chemical vapor deposited zinc sulfide (CVD ZnS) were assessed before and after heat treatments, involving different annealing and hot isostatic pressing (HIPing) profiles. Samples were characterized using optical microscopy, SEM, TEM, electron diffraction, polycrystalline and powder x-ray diffraction, x-ray chemical microanalysis, photoluminescence, ultraviolet through longwave infrared transmission, and mechanical testing. Before heat treatment, CVD ZnS consists of lamellar twinned structures in 10 to 100 nm layers aggregated into domains which compose grains typically 5 to 10 μm in diameter with an overall crystallographic texture on the {100} planes. The scattering behavior of CVD ZnS was investigated and described by a surface scattering model based on internal surface roughness and refractive index variations due to onedimensional stacking disorder. The two to five percent hexagonality measured by x-ray diffraction is believed to form due to oxygen impurities at the twin boundaries which cause nanostructural polytypism and result in differential refractive index and scattering. CVD ZnS variants in low temperature deposited red ZnS and sulfur precursor elemental ZnS are examined as well. Color in CVD ZnS is believed to be due to band edge position, probably due to oxygen content, and not directly related to the hydride absorption at 6 μm. After annealing or hot isostatic pressing above 850 °C for sufficient time, CVD ZnS recrystallizes and becomes strongly textured on the {111} planes. This recrystallization is required to remove stacking disorder, resulting in a structure with less than half a percent hexagonality and low visible scattering. The recrystallization is believed to proceed by diffusing the oxygen at the nano-twin boundaries back into the lattice, thus unpinning the boundaries and allowing them to move and grow into the tabular recrystallized morphology by polytype induced exaggerated grain growth. The presence of active metals like platinum, silver, copper, or nickel during hot isostatic pressing causes a reaction with sulfur and lowers the temperature required for recrystallization. The optical scattering model is consistent in describing standard CVD ZnS, elemental ZnS, and multispectral recrystallized ZnS as having successively lower birefringence at internal surfaces.
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A Deformation Induced Quantum DotWoodsworth, Daniel James 05 1900 (has links)
Due to their extraordinary electronic properties, Quantum Dots (QDs) are potentially very useful
nanoscale devices and research tools. As their electrons are confined in all three dimensions, the
energy spectra of QDs is descrete, similar to atoms and molecules. Because the gaps between
these energy levels is inversely related to the size of the QD, very small QDs are desirable.
Carbon nanotubes have long been touted as fundamental units of nanotechnology, due to
their structural, optical and electronic properties, many of which are a result of the confinement
of electrons in the trans-axial plane of the nanotube. It is known that their band gap structure
is altered under deformation of their cross section.
It is proposed that one way to fabricate a very small quantum dot is by confining electrons
in the nanotube so that they may not freely move along its length. A structure to produce this
confinement has been described elsewhere, namely the carbon nanotube cross, consisting of two
carbon nanotubes, with the the one draped over the other at ninety degrees. It is thought that
this structure will induce local physical deformations in the nanotube, resulting in local changes
in electronic structure of the top nanotube at the junction of the cross. These band gap shifts
may cause metal-semiconductor transitions, resulting in tunnel barriers that axially the confine
electrons in the nanotube. This thesis investigates the possibility that the carbon nanotube cross
may exhibit QD behavior at the junction of the cross, due to these local band gap shifts.
A device for carbon nanotube growth, using Chemical Vapor Deposition, has been designed,
and may be built using microfabrication techniques. This device consists of electrodes (for electrical
measurements of the nanotubes) and catalyst regions (to initiate nanotube growth), lithographically
patterned in a configuration that promotes carbon nanotube formation. Unfortunately,
due to fabrication issues, this effort is a work in progress, and these devices have not yet
been constructed. However, an experimental methodolgy has been developed, which provides a
framework for eventually building a carbon nanotube cross, and investigating the possibility of
QD behavior at the junction of the cross.
This structure has also been investigated computationally. Molecular dynamics simulations
were used to obtain equilibrium geometries of the carbon nanotube cross, and it was found
that their are many different meta stable states, corresponding to different types of nanotube,
and different physical arrangements of these nanotubes. The electronic structure of the carbon
nanotube cross was calculated using the density functional theory. Band gap energies similar to
experimental values were obtained. A one-to-one spatial correlation between deformation and
band gap and conduction band shifts were observed in the top carbon nanotube of the nanotube
cross. Small tunnel barriers, inferred from both the calculated band gap and LUMO energies, are
observed, and could well be sufficient to confine electrons along the axis of the nanotube.
The results described in this thesis, while not definitive, certainly indicate that a QD probably
would form at the junction of a carbon nanotube cross, and that further investigation, both
experimental and computational, is warranted.
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Synthesis of millimeter-scale carbon nanotube arrays and their applications on electrochemical supercapacitorsCui, Xinwei Unknown Date
No description available.
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Combustion chemical vapor deposition of α-alumina, YSZ and multilayer α-alumina/YSZ filmsGriffin, Jack M. 05 1900 (has links)
No description available.
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Fabrication of surface enhanced Raman spectroscopy (SERS) active substrates based on vertically aligned nitrogen doped carbon nanotube forestAlam, Md Khorshed January 2015 (has links)
This thesis work describes the fabrication and surface enhanced Raman spectroscopy (SERS) characterization of vertically aligned nitrogen (N) doped multi walled carbon nanotube (MWCNT) forests coated by silver (Ag) and gold (Au) nanoparticles. In the present work, the CNT forests were grown from a catalyst metal layer by the chemical vapor deposition (CVD) process at temperature of 800 oC and a physical vapor deposition (PVD) and annealing processes were applied subsequently for the evaporation and diffusion of noble metal nanoparticles on the forest. Transistor patterning of 20, 50 and 100 μm were made onto the silicon-oxide (SiO2) wafers through the photolithography process with and without depositing a thickness of 10 nm titanium (Ti) buffer layer on the Si-surfaces. Iron (Fe) and cobalt (Co) were used together to deposite a thickness of 5 nm catalyst layer onto the Single Side Polished (SSP) wafers. As carbon and nitrogen precursor for the CNT growth was used pyridine. Two different treatment times (20 and 60 minutes) in the CVD process determined the CNT forest height. Scanning Electron Microscopy (SEM) imaging was employed to characterize the CNT forest properties and Ag and Au nanoparticle distribution along the CNT walls. The existence of “hot spots” created by the Ag and Au nanoparticles through the surface roughness and plasmonic properties was demonstrated by the SERS measurements. Accordingly, the peak intensity at wave number of 1076 cm-1 was picked up from each SERS spectra to establish the Ag- and Au-trend curves with different concentrations of 4-ATP solution. The SERS mapping was also carried out to study the Ag- and Au-coated CNT surface homogeneity and “hot spots” distribution on the CNT surface. The SERS enhancement factors (EF) were calculated by applying an analyte solution of ethanolic 4-ATP on the CNT surface. The calculated values of EF from Ag- and Au-coated CNT forests were 9×106 and 2.7×105 respectively.
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