THIN FILM GROWTH by PECVD

Size: px
Start display at page:

Download "THIN FILM GROWTH by PECVD"

Transcription

1 THIN FILM GROWTH by PECVD This manual consists of four sections: section 1 and 2 provide a brief introduction to chemical vapour deposition and plasma technique respectively, section 3 gives the detailed procedure of the experiments for thin film growth by plasma-enhanced CVD (PECVD), section 4 introduces several commonly used characterization techniques of the grown thin films. 1. ABOUT CVD Chemical vapor deposition (CVD) is a technique of modifying properties of solid (substrate) surfaces by depositing a layer or layers of materials of interest on the substrate through a vapor phase chemical reaction at elevated temperatures. CVD can offer many advantages, such as excellent conformal coverage of complex structures, simpler deposition equipment, low temperature film fabrication and the ease of large scale deposition. It has rapidly developed in recent years as a method to prepare thin films for a variety of applications in the solid-state-electronics and coating industries. Typical materials deposited by CVD, and applications of the CVD techniques are summarized in Table 1 and 2, respectively. Table 1 Material Metals Compounds Ceramics Typical Materials Deposited by CVD Example Al, As, Be, Bi, Co, Cr, Cu, Fe, Ge, Hf, Ar, Mo, Nb, Ni, Os, Pb, Pt, Rc, Rh, Ru, Sb, Si, Sn, Ta, Th, Ti, U, V, W, Zr, also carbon and boron II-VI and III-V compounds, borides, carbides, nitrides, and silicides of transition metals, as well as sulfides, phosphides, aluminides, etc. Al 2 0 3, AlN, B 2 O 3, BN, SiC, Si 3 N 4, UO 2, Y 2 0 3, ZrO 2, etc. Page 1 of 15

2 Table 2 Applications of the CVD Technique Tribological coatings Wear-resistant coatings Emissive coatings High-temperature coatings for oxidation resistance Coatings for fibre composites Photovoltaic films Decorative Films Superconducting Films Dielectric insulating films Free-standing structural shapes Optical/reflective films Powders and whiskers Three fundamental steps are involved in a CVD process (see Figure 1), i.e. the transportation of the component elements in the vapour phase (or often in a carrier gas), the chemical reaction which takes place in a gaseous medium surrounding the substrate at elevated temperatures, and the removal of volatile reaction-by-products. Therefore a modern CVD equipment generally contains the following units: gas or volatile liquid/solid sources, a gas distribution and mixing system, a reaction chamber (often, with a vacuum pumping system), a system for providing the energy for the reaction and for heating the substrates; and a neutralization (disposal/scrubber) system for the exhaust gases. Main flow of reactant gases Gaseous by-products Boundary layer Interface (negligible thickness) Substrate 1. Diffusion in of reactants through boundary layer 2. Absorption of reactants on substrate 3. Chemical reaction takes place 4. Desorption of absorbed species 5. Diffusion out of by-products Figure 1 Sequence of events during deposition Page 2 of 15

3 The chemical reactions between various constituents occur normally in the vapour phase over the heated substrate, and the film is deposited on the surface. In some cases, however, a film can also be formed from a reaction between the substrate surface and one or more of the constituents of the vapor phase. Therefore gas flow rate, gas composition, system pressure, deposition temperature, and chamber geometry are all important process variables by which thin film deposition is controlled. CVD reactor designs can be classified into the atmospheric-pressure and low-pressure CVD categories. Atmospheric-pressure CVD (APCVD) has disadvantages including the need for a large stream of carrier gas, large apparatus size, and high levels of contamination. Low-pressure ( torr) CVD (LPCVD) has undergone significant development in the past years. It allows removal of carrier gas and uses only small amounts of reactive gases at low partial pressures. In conventional CVD, the reaction is thermally activated. In what is called a hot-wall reactor the whole reactor reaches the process temperature, the substrate residing in an isothermal environment produced by uniform furnace heating. In a coldwall reactor the heated area is limited to the substrates or the substrate holder. There have been recently developed different variations of conventional CVD method in order to lower the reaction temperatures and to enhance the deposition efficiency. These include metalorganic CVD (MOCVD), laserinduced (LCVD), photo-enhanced CVD (photo-cvd), plasma-enhanced CVD (PECVD), and microwave electron cyclotron resonance CVD (ECRCVD). In the MOCVD process metalorganic compounds, which are sufficiently volatile and have low decomposition temperature to desired materials, are used as CVD precursors so that the reactive molecules can be transported in the gas phase in high enough concentrations to allow reasonable film deposition rates and low deposition temperatures. As for LCVD, photo-cvd and PECVD the activation of the chemical reaction and thus the low deposition temperature is achieved by using a laser (for LCVD), UV light (for photo-cvd), or plasma (for PECVD) source. LCVD can be divided into two broad categories, pyrolysis and photolysis, depending on the mechanism that initiates the chemical reaction. In the former case the ambient gases react with the locally heated substrate, while in latter photons of sufficient energy are absorbed mainly to activate gaseous reactant atoms or molecules. Photo CVD Page 3 of 15

4 relies on high energy photons for selective absorption. The commonly used sources are low pressure Hg discharge lamps or excimer lasers. PECVD is yet another versatile technique for depositing a variety of materials for microelectronic, photovoltaic, and many other applications. In the present experiment a PECVD system manufactured by PlasmaQuest is employed to grow films such as Si 3 N 4 or SiO 2 on Si(100), (111), KBr pellet, or other substrates. 2. ABOUT PLASMA A plasma is a complex gaseous state of matter comprising free radicals, electrons, photons, ions, and various neutral species at many different energy levels. Natural plasmas exist mainly as stars of our universe. Lightning is among few examples of natural plasmas on the earth. Manmade plasmas can be produced in thermonuclear reaction, electric arc, combustion flames, low pressure gas discharge and so on. In PECVD the plasma is generated and controlled by ionizing a gas with an rf electromagnetic field of sufficient power, although dc and microwave fields have also been used. The primary role of the plasma is to promote chemical reactions. While the bulk gas is at room temperature (~ ev), the temperatures (the kinetic energy) of free electrons in the ionized gas can be times higher, thus producing an unusual, chemically reactive environment at ambient temperatures, the average electron energies (1-20 ev) in the plasma being sufficient to ionize and dissociate most type of gas molecules. Although electrons are the ionizing source, collisions involving excited species can lead to the formation of free radicals and can assist the ionization process. Once ionized, excited gas species react with surface of materials placed in the gas glow discharge, resulting in dramatic modifications to the surface and enhancing the deposition efficiency. In addition high energy UV photons, resulting from combination and relaxation of dissociated species, may be absorbed by the substrate, creating even more active sites. The colour of the glow discharge depends on the plasma chemistry, and its intensity depends on the processing variables. Note that the plasma process modifies only several molecular layers, thus the appearance and bulk properties are usually unaffected. Page 4 of 15

5 In order to ensure the high quality and the reproducibility of a given plasma process many parameters must be controlled with care, such as the pressure and the flow rate of the reagent gas or gas mixture, the discharge power density, the substrate temperature and the electric potential of the workpiece and so on. The film deposition rate depends on the rf energy, the mole fraction of the reactants, the total pressure, the substrate temperature, etc. Plasma equipment usually consists of six functions: vacuum system, power supply, matching network, power monitor, reactor chamber, and controller. Low-pressure plasma is generally produced in the pressure range from 0.1 to 10 torr, with a continuous gas flow into the reactor. The vacuum system must be able to maintain this pressure/flow regime. The plasma excitation power generally ranges from 50 to 5000 W (0 to 500 W for our PlasmaQuest system). The electromagnetic energy can be input by different coupling methods (inductive or capacitive), electrode configuration (a coil or two plates), and frequency (DC, AC, RF to MF). DC plasmas are not advantageous. Most plasma reactors use AC electrical power supplies, operating at audio-, radio-, or microwave frequencies. Commercial plasma systems usually operate in certain fixed frequencies, i.e. the ISM frequencies specific for industrial, scientific, medical applications other than telecommunications. These include low frequency (LF, khz), radio frequency (RF, or MHZ), and microwave (MW, 915 MHZ) frequencies. Although there has been a gradual shift from RF to MW in recent years, RF plasma is widely used because of easy, reliable operation as well as sufficient activity. For RF plasmas a matching network is necessary to match the impedance of the plasma to that at the generator output. Most plasma systems are designed for batch operation, which involves loading a batch of samples, evacuation, plasma processing, purging to atmospheric pressure, and the removal of the samples. 3. EXPERIMENTAL PROCEDURES The goal of the experiment is to deposit Si 3 N 4 (or SiO 2, or other materials of interest) thin films on both Si(100) and KBr substrates with PlasmaQuest, and then characterize the films grown with Fourier transform infrared spectroscopy (FTIR) or other analysis methods. Page 5 of 15

6 3.1 Preparation of the substrates Si chips cut from a Si(100) or (111) wafer are dipped in a concentrated HF solution for 5 mins, then rinsed with deionized/distilled water, and dried with a soft tissue paper. This pre-cleaning is designed to remove the native silicon oxide as well as contaminations from the substrate surface to facilitate the subsequent film growth. KBr pellets are prepared from pure KBr powder, which is wellgrounded, spread on a die, and pressed at < 8 tonne/m 2 pressure to give a self-supporting disk. The thickness of the pellets is around 1 mm, but not strictly important, in order to prevent the pellets from breaking into pieces during the process. 3.2 CVD reaction chamber with water cooling system The reaction chamber, which is made of welded stainless steel, is constructed of an RF biased gas showerhead and a non-biased resistively-heatable chuck, on which substrates are loaded (Figure 2). Figure 2 Schematic diagram of the PECVD system Page 6 of 15

7 Water cooling is provided for the chuck to chamber transition flange, turbo pump, and the RF matching network, to prevent overheating of the transition seal at ultra high chuck temperatures, and RF generator system. To start the experiment the chiller controller must first be turned on (the switch is located on the chiller, NESLAB RTE-111) so that the green light indicator of the deionizer (located near the chiller and the roughing pump) is on. Chiller reading should be set at 20 C (using "set point adjust" fine and coarse knobs). If the chilled water flow is not properly set, the RF power supply, RF matching system, chuck heater, or turbopump will be disabled. 3.3 Process vacuum system The process vacuum system consists of a turbomolecular pump backed by a mechanical pump (see Figure 2). This pump package provides the reaction chamber with sufficient pumping capacity to maintain high gas flows and low process pressure required for advanced processing. The process chamber should remain under vacuum at all times except during maintenance or sample loading. Turn on the roughing and backing pump switches (located on the wall of the lab) and be sure they are operating. 3.4 Electronics Rack Switches of the power supplies for the whole machine, computer, RF generator and automatic matching network are located in the front of the electronics rack with the main frame of the machine. To start the machine, turn on these switches one at a time, from the bottom to upper panel. 3.5 System computer In our PlasmaQuest system all the processes are automatically controlled by a microprocessor that can be programmed to remember Page 7 of 15

8 recipes, to determine all the machine parameters and the sequence of the processing steps. The processing information including the plasma power is displayed on a screen, so that the operator is constantly informed. Command entry is through the light pen or keyboard. ID and password are required for starting the computer, and they (PQ/752762) can be found from the label attached to the keyboard. Once the system software is booted up, it will be in the Status mode, and five icons, including Service, Edit, Run and Configuration, will be displayed for selection in all software modes. Using the mouse, enter into Service Mode and select System Reset (in the right column of the Service Mode screen) to automatically place the reactor in its idle condition by pumping down the process chamber to process base pressure setpoint (<3x10-5 torr). The chamber will be first pumped by the roughing pump through the roughing valve. At the pressure below 40 mtorr the throttle valve will be opened to speed up the pumping rate. When the process chamber reaches crossover set point (~ 20 mtorr), the roughing valves close. Turn on the turbo pump switch in the front of electronic rack, and the chamber is pumped by it. 3.6 Unloading/loading In order to load/unload samples the process chamber has to be vented with N 2. The valve to the N 2 cylinder should be opened now. By activating Service Mode, followed by selecting the System ATM and selecting Yes, the valves connected to the pumps will be closed and N 2 allowed into the chamber. The yellow clock on the computer screen will disappear when the chamber reaches atmospheric pressure. Once vented, turn clockwise the key switch in front of the chamber to open it. Turn the key back to its neutral position after the chamber wall (with the shower head) has been lifted to open. Page 8 of 15

9 Sample unloading/loading can be carried out now. The sample/substrate is put on the chuck. Close the chamber by turning the Key anticlockwise and pressing the break release button next to the Key to ease the chamber wall back to the original position. When the chamber is in the closed position, the machine will be automatically self-tested until the pumping speed of the turbo pump, displayed on panel 3 of the electronic rack, is ~ 830. To pump down the system use light pen to apply system Reset, as already stated in section 3.5. The chamber is then pumped down. Alternatively, pumping can be performed by using the mouse to activate the roughing, throttle (at < 40 mtorr), and hi vac valve (< 20 mtorr) in sequence. 3.7 Process control The process chamber is equipped with a Balzers full-range gauge, (which is used for atmospheric, crossover and base pressure monitoring, and will be separated from the chamber when the gases start to flow into the chamber) and one MKS Baratron absolute pressure transducers, (for process pressure monitoring between 20 mtorr and atmospheric pressure). Process gases enter the reactor chamber through an upstream gas manifold that controls gas flow through the showerhead. Once the chamber pressure is low enough (< 3x10-5 Torr), open the valves of the gas cylinders to be used, and the deposition can be started by activating Run Mode, which allows to execute a given process, whose recipe is stored in memory and can be picked up easily. Upon entry, the computer displays the last process recipe executed. To select an existing recipe (such as SiN and so on) to run, select the Recipe icon at the right side of the screen, and a file Page 9 of 15

10 selection box will be displayed. The user can adjust all parameters by activating Edit Mode through numeric input. The attached is the recipes for the deposition of Si 3 N 4 (see Appendix 1). The process procedures/parameters will be automatically shown on the computer screen. Ask demonstrator for more details. The chemical reaction involved is SiH 4 (g) + O 2 (g) = SiO 2 (s) + 2H 2 (g) for SiO 2 and 3SiH 4 (g)+ 4NH 3 (g)= Si 3 N 4 (s) + 12H 2 (g) for Si 3 N 4. After deposition allow the chuck to cool down (which may take many hours) and follow the unloading procedure in Section 3.6 to remove the sample out for characterization. 3.8 Safety Caution needs to be taken at all times during reactor operation. Some of the basic safety guidelines are listed in the attached paper (see Appendix 2). One Emergency Power Off (EPO) switch is located on the front of the system. Push it to turn off the machine in emergency cases. 3.9 Summary of operation 1. prepare substrates 2. open chamber 3. load substrates 4. close chamber 5. open roughing valve 6. after the chamber pressure lower than crossover pressure, close roughing valve and open high vacuum valve Page 10 of 15

11 7. edit recipe 8. after the chamber pressure lower than base pressure, open the gas cylinder valves, run recipe 9. turn off turbo-pump after the recipe finishes, and close gas cylinder valves 10. after cooling to the room temperature, take out the samples. Note if SiH 4 is used in deposition, N 2 purge the SiH 4 gas line is needed before opening the chamber. 4. CHARACTERIZATION of the GROWN FILMS Fourier Transform Infrared Spectroscopy (FTIR), Scanning Electron Microscopy (SEM), Atomic Force Microscope (AFM), X-ray photoelectron spectroscopy (XPS) and other analytic methods can be employed to characterize the film grown by PECVD. AFM and SEM are used to observe the surface morphology, and XPS is used for analysis of surface composition and bonding structure of the grown thin film. Here only FTIR is briefly introduced. The goal of the basic infrared experiment is to determine changes in the intensity of a beam of infrared radiation as a function of wavelength or frequency ( µm or cm -1 ) after it interacts with the sample. If the IR is absorbed by the sample, it may be converted into vibrational energy of molecules (pairs or groups of bonded atoms) in the sample. As the vibrational energy is characteristic of molecules, FTIR can identify specific functional groups, providing chemical bonding information about the sample. A complete assignment of all the absorption bands is possible in favourable cases (e.g. see Figure 3 for the IR spectrum of Si 3 N 4 ). Many reference books are available for the interpretation of IR spectra. These include Infrared and Raman Spectra of Inorganic and Coordination Compounds, 4th edition, by Nakamoto and Spectrometric identification of organic compounds, 5th edition, by Silverstein, Bassler and Morrill. Page 11 of 15

12 WAVELENGTH [µm] (a) 1620 Å Si-O 1090 cm -1 TRANSMISSION [a.u.] N-H(S) 3340 cm -1 (b) 3 µm CO 2 (AIR) N-H(B) 1200 cm -1 Si-N(A.S) ~850 cm -1 SUB. Si-N(S) WAVENUMBER [cm -1 ] Figure 3 Infrared transmission for (a) thin (162.0 nm) and (b) thick (3000 nm) silicon nitride films pyrolitic-deposited on silicon substrates with NH 3 /SiH 4 =200. In this experiment the sample using KBr pellets as the substrate can be tested using transmission FTIR, in which the absorption bands are obtained by passing infrared beam through the sample since KBr is transparent to IR. For the films deposited on Si chips transmission FTIR can also be used, in which Si wafer should be recorded firstly as background. The alternative way is using specular or diffuse reflection absorption techniques, where IR beams reflected will be recorded to give IR spectra. REFERENCES PlasmaQuest Series H Operation Manual Joy George, Preparation of thin films C.E. Morosanu, Thin films by chemical vapour deposition, D. Satas, Coatings technology handbook, LJY Page 12 of 15

13 APPENDIX 1 PROCESS DEMO System: 157 Type: Si 3 N 4 Demo: Results: SiO 2 Demo: Results: Series II NH 3 = 18 sccm; 5% SiH 4 in Ar = 130 sccm; Process Pressure = 700 mtorr; RF Power = 40 Watts; Temperature = 350 C; Time duration = 150 sec. Center = 2.08 r.i.; nm; Avg. = ± 1.7 nm; Uniformity 1.5% based on 9 measurements; Rate = 43.5 nm/min. Sample repeatable from wafer to wafer. O 2 = 12 sccm; 5% SiH 4 in Ar = 130 sccm; Process Pressure = 580 mtorr; RF Power = 40 Watts; Temperature = 350 C; Time duration = 60 sec. Center = 1.46 r.i.; nm; Avg. = ± 5.2 nm; Uniformity 4.9% based on 9 measurements; Rate = nm/min. Sample repeatable from wafer to wafer. Page 13 of 15

14 APPENDIX 2 SAFETY GUIDELINES Followings are some of the basic safety guidelines for working with the reactor: 1. Operation of this reactor may involve use of highly toxic and hazardous gases which can be lethal in case of an accident or if not handled properly. It is strongly recommended that a minimum of two people be present when hazardous or toxic gas is being used in the reactor. Respirator masks should be available in case an accident occurs. 2. When connecting or disconnecting gas lines it is strongly recommended that a minimum of two people be present when hazardous or toxic gas is plumbed to the machine. Respirator masks should be worn when working on hazardous or toxic gas lines. It is good practice to wear a respirator mask when working on gas lines of any type. 3. High pressure compressed gas cylinders should be stored in vented gas cabinets or in a contained gas storage area and securely fastened with belts or chains to the wall. 4. Toxic or hazardous gases should be shut off at the cylinder when not in use (overnight, over the weekend) or in the event of fire, earthquake, or other emergency. 5. Automatic cut off valves, N 2 purged interlock systems, and gas detectors are recommended for toxic and hazardous gases. 6. High voltages are present in the system, and caution should be taken when electrical components or wires are to be worked on. Turn off the power circuit breaker to the system component that is to be serviced. 7. Potential danger from high-voltage sources has been minimized as much as possible in the design of the reactor. Voltages have been labelled according to their degree of hazard, however the operator needs to exercise care when working near the following high voltage components: * Turbomolecular pumps & controllers * RF generators * RF network and controllers Page 14 of 15

15 * Main power distribution enclosure * Internal power distribution box * Remote power distribution box * Transformer trailers, for systems requiring 50 Hz operation. 8. Chamber cleanup may expose reaction by-products which can be extremely hazardous. The degree of hazard will depend on the process used in the reactor. The operator should wear safety glasses, acid gas respirator, rubber gloves, and lab coat with long sleeves to minimize exposure to hazardous residue by-products while cleaning the reactor chamber. 9. The heated chuck can reach high temperatures and should be allowed time to cool before working on or near the chuck. 10. Mechanical pump oil may contain acidic or toxic residues. Wear rubber gloves, safety glasses, and an acid gas respirator when changing pump oils. 11. Safety precautions and warnings in the component manuals, located in volume 2 of this manual, should also be read and understood by the user. Page 15 of 15

DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD

DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD Chapter 4 DEPOSITION OF THIN TiO 2 FILMS BY DC MAGNETRON SPUTTERING METHOD 4.1 INTRODUCTION Sputter deposition process is another old technique being used in modern semiconductor industries. Sputtering

More information

Modern Methods in Heterogeneous Catalysis Research: Preparation of Model Systems by Physical Methods

Modern Methods in Heterogeneous Catalysis Research: Preparation of Model Systems by Physical Methods Modern Methods in Heterogeneous Catalysis Research: Preparation of Model Systems by Physical Methods Methods for catalyst preparation Methods discussed in this lecture Physical vapour deposition - PLD

More information

Plasma Deposition (Overview) Lecture 1

Plasma Deposition (Overview) Lecture 1 Plasma Deposition (Overview) Lecture 1 Material Processes Plasma Processing Plasma-assisted Deposition Implantation Surface Modification Development of Plasma-based processing Microelectronics needs (fabrication

More information

TMT4320 Nanomaterials November 10 th, Thin films by physical/chemical methods (From chapter 24 and 25)

TMT4320 Nanomaterials November 10 th, Thin films by physical/chemical methods (From chapter 24 and 25) 1 TMT4320 Nanomaterials November 10 th, 2015 Thin films by physical/chemical methods (From chapter 24 and 25) 2 Thin films by physical/chemical methods Vapor-phase growth (compared to liquid-phase growth)

More information

k T m 8 B P m k T M T

k T m 8 B P m k T M T I. INTRODUCTION AND OBJECTIVE OF THE EXPERIENT The techniques for evaporation of chemicals in a vacuum are widely used for thin film deposition on rigid substrates, leading to multiple applications: production

More information

Chapter 7 Plasma Basic

Chapter 7 Plasma Basic Chapter 7 Plasma Basic Hong Xiao, Ph. D. hxiao89@hotmail.com www2.austin.cc.tx.us/hongxiao/book.htm Hong Xiao, Ph. D. www2.austin.cc.tx.us/hongxiao/book.htm 1 Objectives List at least three IC processes

More information

CVD: General considerations.

CVD: General considerations. CVD: General considerations. PVD: Move material from bulk to thin film form. Limited primarily to metals or simple materials. Limited by thermal stability/vapor pressure considerations. Typically requires

More information

Etching Issues - Anisotropy. Dry Etching. Dry Etching Overview. Etching Issues - Selectivity

Etching Issues - Anisotropy. Dry Etching. Dry Etching Overview. Etching Issues - Selectivity Etching Issues - Anisotropy Dry Etching Dr. Bruce K. Gale Fundamentals of Micromachining BIOEN 6421 EL EN 5221 and 6221 ME EN 5960 and 6960 Isotropic etchants etch at the same rate in every direction mask

More information

EE143 Fall 2016 Microfabrication Technologies. Lecture 6: Thin Film Deposition Reading: Jaeger Chapter 6

EE143 Fall 2016 Microfabrication Technologies. Lecture 6: Thin Film Deposition Reading: Jaeger Chapter 6 EE143 Fall 2016 Microfabrication Technologies Lecture 6: Thin Film Deposition Reading: Jaeger Chapter 6 Prof. Ming C. Wu wu@eecs.berkeley.edu 511 Sutardja Dai Hall (SDH) 1 Vacuum Basics Units 1 atmosphere

More information

Chapter 7. Plasma Basics

Chapter 7. Plasma Basics Chapter 7 Plasma Basics 2006/4/12 1 Objectives List at least three IC processes using plasma Name three important collisions in plasma Describe mean free path Explain how plasma enhance etch and CVD processes

More information

UNIT 3. By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun

UNIT 3. By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun UNIT 3 By: Ajay Kumar Gautam Asst. Prof. Dev Bhoomi Institute of Technology & Engineering, Dehradun 1 Syllabus Lithography: photolithography and pattern transfer, Optical and non optical lithography, electron,

More information

ETCHING Chapter 10. Mask. Photoresist

ETCHING Chapter 10. Mask. Photoresist ETCHING Chapter 10 Mask Light Deposited Substrate Photoresist Etch mask deposition Photoresist application Exposure Development Etching Resist removal Etching of thin films and sometimes the silicon substrate

More information

Device Fabrication: Etch

Device Fabrication: Etch Device Fabrication: Etch 1 Objectives Upon finishing this course, you should able to: Familiar with etch terminology Compare wet and dry etch processes processing and list the main dry etch etchants Become

More information

XPS/UPS and EFM. Brent Gila. XPS/UPS Ryan Davies EFM Andy Gerger

XPS/UPS and EFM. Brent Gila. XPS/UPS Ryan Davies EFM Andy Gerger XPS/UPS and EFM Brent Gila XPS/UPS Ryan Davies EFM Andy Gerger XPS/ESCA X-ray photoelectron spectroscopy (XPS) also called Electron Spectroscopy for Chemical Analysis (ESCA) is a chemical surface analysis

More information

Fabrication Technology, Part I

Fabrication Technology, Part I EEL5225: Principles of MEMS Transducers (Fall 2004) Fabrication Technology, Part I Agenda: Microfabrication Overview Basic semiconductor devices Materials Key processes Oxidation Thin-film Deposition Reading:

More information

Chemistry Instrumental Analysis Lecture 34. Chem 4631

Chemistry Instrumental Analysis Lecture 34. Chem 4631 Chemistry 4631 Instrumental Analysis Lecture 34 From molecular to elemental analysis there are three major techniques used for elemental analysis: Optical spectrometry Mass spectrometry X-ray spectrometry

More information

Lecture 6 Plasmas. Chapters 10 &16 Wolf and Tauber. ECE611 / CHE611 Electronic Materials Processing Fall John Labram 1/68

Lecture 6 Plasmas. Chapters 10 &16 Wolf and Tauber. ECE611 / CHE611 Electronic Materials Processing Fall John Labram 1/68 Lecture 6 Plasmas Chapters 10 &16 Wolf and Tauber 1/68 Announcements Homework: Homework will be returned to you on Thursday (12 th October). Solutions will be also posted online on Thursday (12 th October)

More information

T: +44 (0) W:

T: +44 (0) W: Ultraviolet Deposition of Thin Films and Nanostructures Ian W. Boyd ETC Brunel University Kingston Lane Uxbridge Middx UB8 3PH UK T: +44 (0)1895 267419 W: etcbrunel.co.uk E: ian.boyd@brunel.ac.uk Outline

More information

Supporting Information s for

Supporting Information s for Supporting Information s for # Self-assembling of DNA-templated Au Nanoparticles into Nanowires and their enhanced SERS and Catalytic Applications Subrata Kundu* and M. Jayachandran Electrochemical Materials

More information

CHAPTER 6: Etching. Chapter 6 1

CHAPTER 6: Etching. Chapter 6 1 Chapter 6 1 CHAPTER 6: Etching Different etching processes are selected depending upon the particular material to be removed. As shown in Figure 6.1, wet chemical processes result in isotropic etching

More information

Thin Film Deposition. Reading Assignments: Plummer, Chap 9.1~9.4

Thin Film Deposition. Reading Assignments: Plummer, Chap 9.1~9.4 Thin Film Deposition Reading Assignments: Plummer, Chap 9.1~9.4 Thermally grown Deposition Thin Film Formation Thermally grown SiO 2 Deposition SiO 2 Oxygen is from gas phase Silicon from substrate Oxide

More information

Wafer holders. Mo- or Ta- made holders Bonding: In (Ga), or In-free (clamped) Quick and easy transfer

Wafer holders. Mo- or Ta- made holders Bonding: In (Ga), or In-free (clamped) Quick and easy transfer Wafer holders Mo- or Ta- made holders Bonding: In (Ga), or In-free (clamped) Quick and easy transfer Image: In-free, 3-inch sample holder fitting a quarter of a 2- inch wafer Reflection High Energy Electron

More information

MS482 Materials Characterization ( 재료분석 ) Lecture Note 12: Summary. Byungha Shin Dept. of MSE, KAIST

MS482 Materials Characterization ( 재료분석 ) Lecture Note 12: Summary. Byungha Shin Dept. of MSE, KAIST 2015 Fall Semester MS482 Materials Characterization ( 재료분석 ) Lecture Note 12: Summary Byungha Shin Dept. of MSE, KAIST 1 Course Information Syllabus 1. Overview of various characterization techniques (1

More information

Etching: Basic Terminology

Etching: Basic Terminology Lecture 7 Etching Etching: Basic Terminology Introduction : Etching of thin films and sometimes the silicon substrate are very common process steps. Usually selectivity, and directionality are the first

More information

CHEMICAL VAPOR DEPOSITION (CVD)

CHEMICAL VAPOR DEPOSITION (CVD) CHEMICAL VAPOR DEPOSITION (CVD) A process of formation of a non-volatile solid film on a substrate from the reaction of vapor phase chemical reactants containing the right proportion of constituents. ELEMETRY

More information

A HYDROGEN SENSITIVE Pd/GaN SCHOTTKY DIODE SENSOR

A HYDROGEN SENSITIVE Pd/GaN SCHOTTKY DIODE SENSOR Journal of Physical Science, Vol. 17(2), 161 167, 2006 161 A HYDROGEN SENSITIVE Pd/GaN SCHOTTKY DIODE SENSOR A.Y. Hudeish 1,2* and A. Abdul Aziz 1 1 School of Physics, Universiti Sains Malaysia, 11800

More information

PHYSICAL AND CHEMICAL PROPERTIES OF ATMOSPHERIC PRESSURE PLASMA POLYMER FILMS

PHYSICAL AND CHEMICAL PROPERTIES OF ATMOSPHERIC PRESSURE PLASMA POLYMER FILMS PHYSICAL AND CHEMICAL PROPERTIES OF ATMOSPHERIC PRESSURE PLASMA POLYMER FILMS O. Goossens, D. Vangeneugden, S. Paulussen and E. Dekempeneer VITO Flemish Institute for Technological Research, Boeretang

More information

EE C245 ME C218 Introduction to MEMS Design Fall 2007

EE C245 ME C218 Introduction to MEMS Design Fall 2007 EE C245 ME C218 Introduction to MEMS Design Fall 2007 Prof. Clark T.-C. Nguyen Dept. of Electrical Engineering & Computer Sciences University of California at Berkeley Berkeley, CA 94720 Lecture 4: Film

More information

Introduction to Plasma

Introduction to Plasma What is a plasma? The fourth state of matter A partially ionized gas How is a plasma created? Energy must be added to a gas in the form of: Heat: Temperatures must be in excess of 4000 O C Radiation Electric

More information

ION Pumps for UHV Systems, Synchrotrons & Particle Accelerators. Mauro Audi, Academic, Government & Research Marketing Manager

ION Pumps for UHV Systems, Synchrotrons & Particle Accelerators. Mauro Audi, Academic, Government & Research Marketing Manager ION Pumps for UHV Systems, Synchrotrons & Particle Accelerators Mauro Audi, Academic, Government & Research Marketing Manager ION Pumps Agilent Technologies 1957-59 Varian Associates invents the first

More information

Electronic Supplementary Information: Synthesis and Characterization of Photoelectrochemical and Photovoltaic Cu2BaSnS4 Thin Films and Solar Cells

Electronic Supplementary Information: Synthesis and Characterization of Photoelectrochemical and Photovoltaic Cu2BaSnS4 Thin Films and Solar Cells Electronic Supplementary Material (ESI) for Journal of Materials Chemistry C. This journal is The Royal Society of Chemistry 2017 Electronic Supplementary Information: Synthesis and Characterization of

More information

Chemical Vapor Deposition *

Chemical Vapor Deposition * OpenStax-CNX module: m25495 1 Chemical Vapor Deposition * Andrew R. Barron This work is produced by OpenStax-CNX and licensed under the Creative Commons Attribution License 3.0 note: This module was developed

More information

Repetition: Practical Aspects

Repetition: Practical Aspects Repetition: Practical Aspects Reduction of the Cathode Dark Space! E x 0 Geometric limit of the extension of a sputter plant. Lowest distance between target and substrate V Cathode (Target/Source) - +

More information

6.5 Optical-Coating-Deposition Technologies

6.5 Optical-Coating-Deposition Technologies 92 Chapter 6 6.5 Optical-Coating-Deposition Technologies The coating process takes place in an evaporation chamber with a fully controlled system for the specified requirements. Typical systems are depicted

More information

Clean-Room microfabrication techniques. Francesco Rizzi Italian Institute of Technology

Clean-Room microfabrication techniques. Francesco Rizzi Italian Institute of Technology Clean-Room microfabrication techniques Francesco Rizzi Italian Institute of Technology Miniaturization The first transistor Miniaturization The first transistor Miniaturization The first transistor Miniaturization

More information

Atmospheric Analysis Gases. Sampling and analysis of gaseous compounds

Atmospheric Analysis Gases. Sampling and analysis of gaseous compounds Atmospheric Analysis Gases Sampling and analysis of gaseous compounds Introduction - External environment (ambient air) ; global warming, acid rain, introduction of pollutants, etc - Internal environment

More information

Table of Content. Mechanical Removing Techniques. Ultrasonic Machining (USM) Sputtering and Focused Ion Beam Milling (FIB)

Table of Content. Mechanical Removing Techniques. Ultrasonic Machining (USM) Sputtering and Focused Ion Beam Milling (FIB) Table of Content Mechanical Removing Techniques Ultrasonic Machining (USM) Sputtering and Focused Ion Beam Milling (FIB) Ultrasonic Machining In ultrasonic machining (USM), also called ultrasonic grinding,

More information

Metal Deposition. Filament Evaporation E-beam Evaporation Sputter Deposition

Metal Deposition. Filament Evaporation E-beam Evaporation Sputter Deposition Metal Deposition Filament Evaporation E-beam Evaporation Sputter Deposition 1 Filament evaporation metals are raised to their melting point by resistive heating under vacuum metal pellets are placed on

More information

Effect of Spiral Microwave Antenna Configuration on the Production of Nano-crystalline Film by Chemical Sputtering in ECR Plasma

Effect of Spiral Microwave Antenna Configuration on the Production of Nano-crystalline Film by Chemical Sputtering in ECR Plasma THE HARRIS SCIENCE REVIEW OF DOSHISHA UNIVERSITY, VOL. 56, No. 1 April 2015 Effect of Spiral Microwave Antenna Configuration on the Production of Nano-crystalline Film by Chemical Sputtering in ECR Plasma

More information

CVD-3 LFSIN SiN x Process

CVD-3 LFSIN SiN x Process CVD-3 LFSIN SiN x Process Top Electrode, C Bottom Electrode, C Pump to Base Time (s) SiH 4 Flow Standard LFSIN Process NH 3 Flow N 2 HF (watts) LF (watts) Pressure (mtorr Deposition Time min:s.s Pump to

More information

LECTURE 5 SUMMARY OF KEY IDEAS

LECTURE 5 SUMMARY OF KEY IDEAS LECTURE 5 SUMMARY OF KEY IDEAS Etching is a processing step following lithography: it transfers a circuit image from the photoresist to materials form which devices are made or to hard masking or sacrificial

More information

Lecture 10. Vacuum Technology and Plasmas Reading: Chapter 10. ECE Dr. Alan Doolittle

Lecture 10. Vacuum Technology and Plasmas Reading: Chapter 10. ECE Dr. Alan Doolittle Lecture 10 Vacuum Technology and Plasmas Reading: Chapter 10 Vacuum Science and Plasmas In order to understand deposition techniques such as evaporation, sputtering,, plasma processing, chemical vapor

More information

Plasmonic Hot Hole Generation by Interband Transition in Gold-Polyaniline

Plasmonic Hot Hole Generation by Interband Transition in Gold-Polyaniline Supplementary Information Plasmonic Hot Hole Generation by Interband Transition in Gold-Polyaniline Tapan Barman, Amreen A. Hussain, Bikash Sharma, Arup R. Pal* Plasma Nanotech Lab, Physical Sciences Division,

More information

VACUUM TECHNOLOGIES NEEDED FOR 3D DEVICE PROCESSING

VACUUM TECHNOLOGIES NEEDED FOR 3D DEVICE PROCESSING VACUUM TECHNOLOGIES NEEDED FOR 3D DEVICE PROCESSING Future ICs will use more 3D device structures such as finfets and gate-all-around (GAA) transistors, and so vacuum deposition processes are needed that

More information

Lab Day and Time: Instructions. 1. Do not open the exam until you are told to start.

Lab Day and Time: Instructions. 1. Do not open the exam until you are told to start. Name: Lab Day and Time: Instructions 1. Do not open the exam until you are told to start. 2. This exam is closed note and closed book. You are not allowed to use any outside material while taking this

More information

Section 3: Etching. Jaeger Chapter 2 Reader

Section 3: Etching. Jaeger Chapter 2 Reader Section 3: Etching Jaeger Chapter 2 Reader Etch rate Etch Process - Figures of Merit Etch rate uniformity Selectivity Anisotropy d m Bias and anisotropy etching mask h f substrate d f d m substrate d f

More information

Vacuum Pumps. Two general classes exist: Gas transfer physical removal of matter. Mechanical, diffusion, turbomolecular

Vacuum Pumps. Two general classes exist: Gas transfer physical removal of matter. Mechanical, diffusion, turbomolecular Vacuum Technology Vacuum Pumps Two general classes exist: Gas transfer physical removal of matter Mechanical, diffusion, turbomolecular Adsorption entrapment of matter Cryo, sublimation, ion Mechanical

More information

A Novel Approach to the Layer Number-Controlled and Grain Size- Controlled Growth of High Quality Graphene for Nanoelectronics

A Novel Approach to the Layer Number-Controlled and Grain Size- Controlled Growth of High Quality Graphene for Nanoelectronics Supporting Information A Novel Approach to the Layer Number-Controlled and Grain Size- Controlled Growth of High Quality Graphene for Nanoelectronics Tej B. Limbu 1,2, Jean C. Hernández 3, Frank Mendoza

More information

Dynamic Equipment and Process Simulation for Atomic Layer Deposition Technology

Dynamic Equipment and Process Simulation for Atomic Layer Deposition Technology Dynamic Equipment and Process Simulation for Atomic Layer Deposition Technology Wei Lei, Yuhong Cai, Laurent Henn-Lecordier and Gary W. Rubloff Department of Materials Science and Engineering and Institute

More information

Lab Day and Time: Instructions. 1. Do not open the exam until you are told to start.

Lab Day and Time: Instructions. 1. Do not open the exam until you are told to start. Name: Lab Day and Time: Instructions 1. Do not open the exam until you are told to start. 2. This exam is closed note and closed book. You are not allowed to use any outside material while taking this

More information

E SC 412 Nanotechnology: Materials, Infrastructure, and Safety Wook Jun Nam

E SC 412 Nanotechnology: Materials, Infrastructure, and Safety Wook Jun Nam E SC 412 Nanotechnology: Materials, Infrastructure, and Safety Wook Jun Nam Lecture 10 Outline 1. Wet Etching/Vapor Phase Etching 2. Dry Etching DC/RF Plasma Plasma Reactors Materials/Gases Etching Parameters

More information

Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped

Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped Supplementary Figure 1 Detailed illustration on the fabrication process of templatestripped gold substrate. (a) Spin coating of hydrogen silsesquioxane (HSQ) resist onto the silicon substrate with a thickness

More information

Etching Capabilities at Harvard CNS. March 2008

Etching Capabilities at Harvard CNS. March 2008 Etching Capabilities at Harvard CNS March 2008 CNS: A shared use facility for the Harvard Community and New England CNS Provides technical support, equipment and staff. Explicitly multi-disciplinary w/

More information

Supplementary Information. Atomic Layer Deposition of Platinum Catalysts on Nanowire Surfaces for Photoelectrochemical Water Reduction

Supplementary Information. Atomic Layer Deposition of Platinum Catalysts on Nanowire Surfaces for Photoelectrochemical Water Reduction Supplementary Information Atomic Layer Deposition of Platinum Catalysts on Nanowire Surfaces for Photoelectrochemical Water Reduction Neil P. Dasgupta 1 ǂ, Chong Liu 1,2 ǂ, Sean Andrews 1,2, Fritz B. Prinz

More information

Chemical Vapor Deposition (CVD)

Chemical Vapor Deposition (CVD) Chemical Vapor Deposition (CVD) source chemical reaction film substrate More conformal deposition vs. PVD t Shown here is 100% conformal deposition ( higher temp has higher surface diffusion) t step 1

More information

Atomic layer deposition of titanium nitride

Atomic layer deposition of titanium nitride Atomic layer deposition of titanium nitride Jue Yue,version4, 04/26/2015 Introduction Titanium nitride is a hard and metallic material which has found many applications, e.g.as a wear resistant coating[1],

More information

Importance of in situ Monitoring in MOCVD Process and Future Prospects

Importance of in situ Monitoring in MOCVD Process and Future Prospects G u e s t F o r u m Guest Forum Series of Lectures by Screening Committees of the Second Masao Horiba Awards Importance of in situ Monitoring in MOCVD Process and Future Prospects Hiroshi Funakubo Tokyo

More information

DAY LABORATORY EXERCISE: SPECTROSCOPY

DAY LABORATORY EXERCISE: SPECTROSCOPY AS101 - Day Laboratory: Spectroscopy Page 1 DAY LABORATORY EXERCISE: SPECTROSCOPY Goals: To see light dispersed into its constituent colors To study how temperature, light intensity, and light color are

More information

OES - Optical Emission Spectrometer 2000

OES - Optical Emission Spectrometer 2000 OES - Optical Emission Spectrometer 2000 OES-2000 is used to detect the presence of trace metals in an analyte. The analyte sample is introduced into the OES-2000 as an aerosol that is carried into the

More information

EBSS: Hands-on Activity #8. Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder

EBSS: Hands-on Activity #8. Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder EBSS: Hands-on Activity #8 Operation of an electromagnetic isotope separator (EMIS) Dan Stracener Jon Batchelder Schematic of RIB Production at the HRIBF ISOL: Isotope Separation On-Line 2 Managed by UT-Battelle

More information

Application of Rarefied Flow & Plasma Simulation Software

Application of Rarefied Flow & Plasma Simulation Software 2016/5/18 Application of Rarefied Flow & Plasma Simulation Software Yokohama City in Japan Profile of Wave Front Co., Ltd. Name : Wave Front Co., Ltd. Incorporation : March 1990 Head Office : Yokohama

More information

X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu

X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu X-Ray Photoelectron Spectroscopy (XPS) Prof. Paul K. Chu X-ray Photoelectron Spectroscopy Introduction Qualitative analysis Quantitative analysis Charging compensation Small area analysis and XPS imaging

More information

Film Deposition Part 1

Film Deposition Part 1 1 Film Deposition Part 1 Chapter 11 : Semiconductor Manufacturing Technology by M. Quirk & J. Serda Spring Semester 2013 Saroj Kumar Patra Semidonductor Manufacturing Technology, Norwegian University of

More information

Plasma Chemistry Study in an Inductively Coupled Dielectric Etcher

Plasma Chemistry Study in an Inductively Coupled Dielectric Etcher Plasma Chemistry Study in an Inductively Coupled Dielectric Etcher Chunshi Cui, John Trow, Ken Collins, Betty Tang, Luke Zhang, Steve Shannon, and Yan Ye Applied Materials, Inc. October 26, 2000 10/28/2008

More information

Graphene films on silicon carbide (SiC) wafers supplied by Nitride Crystals, Inc.

Graphene films on silicon carbide (SiC) wafers supplied by Nitride Crystals, Inc. 9702 Gayton Road, Suite 320, Richmond, VA 23238, USA Phone: +1 (804) 709-6696 info@nitride-crystals.com www.nitride-crystals.com Graphene films on silicon carbide (SiC) wafers supplied by Nitride Crystals,

More information

IR LASER-INDUCED CARBOTHERMAL REDUCTION OF TITANIUM MONOXIDE: CARBON- PHASE SHIELD TO NANOSIZED TiO OXIDATION

IR LASER-INDUCED CARBOTHERMAL REDUCTION OF TITANIUM MONOXIDE: CARBON- PHASE SHIELD TO NANOSIZED TiO OXIDATION IR LASER-INDUCED CARBOTHERMAL REDUCTION OF TITANIUM MONOXIDE: CARBON- PHASE SHIELD TO NANOSIZED TiO OXIDATION Věra JANDOVÁ a, Zdeněk BASTL b, Jan ŠUBRT c, Josef POLA a a Institute of Chemical Process Fundamentals,

More information

Chapter 3 Engineering Science for Microsystems Design and Fabrication

Chapter 3 Engineering Science for Microsystems Design and Fabrication Lectures on MEMS and MICROSYSTEMS DESIGN and MANUFACTURE Chapter 3 Engineering Science for Microsystems Design and Fabrication In this Chapter, we will present overviews of the principles of physical and

More information

Section 5: Thin Film Deposition part 1 : sputtering and evaporation. Jaeger Chapter 6. EE143 Ali Javey

Section 5: Thin Film Deposition part 1 : sputtering and evaporation. Jaeger Chapter 6. EE143 Ali Javey Section 5: Thin Film Deposition part 1 : sputtering and evaporation Jaeger Chapter 6 Vacuum Basics 1. Units 1 atmosphere = 760 torr = 1.013x10 5 Pa 1 bar = 10 5 Pa = 750 torr 1 torr = 1 mm Hg 1 mtorr =

More information

Combinatorial RF Magnetron Sputtering for Rapid Materials Discovery: Methodology and Applications

Combinatorial RF Magnetron Sputtering for Rapid Materials Discovery: Methodology and Applications Combinatorial RF Magnetron Sputtering for Rapid Materials Discovery: Methodology and Applications Philip D. Rack,, Jason D. Fowlkes,, and Yuepeng Deng Department of Materials Science and Engineering University

More information

Case Study of Electronic Materials Packaging with Poor Metal Adhesion and the Process for Performing Root Cause Failure Analysis

Case Study of Electronic Materials Packaging with Poor Metal Adhesion and the Process for Performing Root Cause Failure Analysis Case Study of Electronic Materials Packaging with Poor Metal Adhesion and the Process for Performing Root Cause Failure Analysis Dr. E. A. Leone BACKGRUND ne trend in the electronic packaging industry

More information

INTRODUCTION TO THE HYBRID PLASMA EQUIPMENT MODEL

INTRODUCTION TO THE HYBRID PLASMA EQUIPMENT MODEL INTRODUCTION TO THE HYBRID PLASMA EQUIPMENT MODEL Prof. Mark J. Kushner Department of Electrical and Computer Engineering 1406 W. Green St. Urbana, IL 61801 217-144-5137 mjk@uiuc.edu http://uigelz.ece.uiuc.edu

More information

Introduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960

Introduction to X-ray Photoelectron Spectroscopy (XPS) XPS which makes use of the photoelectric effect, was developed in the mid-1960 Introduction to X-ray Photoelectron Spectroscopy (XPS) X-ray Photoelectron Spectroscopy (XPS), also known as Electron Spectroscopy for Chemical Analysis (ESCA) is a widely used technique to investigate

More information

EXPERIMENT 15. The Frank Hertz Experiment. 1. Pre-Laboratory Work [2 pts] Lab section: Partner's name(s): Grade:

EXPERIMENT 15. The Frank Hertz Experiment. 1. Pre-Laboratory Work [2 pts] Lab section: Partner's name(s): Grade: Name: Date: Course number: MAKE SURE YOUR TA OR TI STAMPS EVERY PAGE BEFORE YOU START! Lab section: Partner's name(s): Grade: EXPERIMENT 15 The Frank Hertz Experiment 1. Pre-Laboratory Work [2 pts] 1.

More information

FINE PATTERN ETCHING OF SILICON USING SR-ASSISTED IONIZATION OF CF4 GAS

FINE PATTERN ETCHING OF SILICON USING SR-ASSISTED IONIZATION OF CF4 GAS Technical Paper Journal of Photopolymer Science and Technology Volume 6, Number 4(1993) 617-624 1993TAPJ FINE PATTERN ETCHING OF SILICON USING SR-ASSISTED IONIZATION OF CF4 GAS YASUO NARA, YosHIHto SUGITA,

More information

Reporting Category 1: Matter and Energy

Reporting Category 1: Matter and Energy Name: Science Teacher: Reporting Category 1: Matter and Energy Atoms 8.5A Fill in the missing information to summarize what you know about atomic structure. Name of Subatomic Particle Location within the

More information

Extrel is widely respected for the quality of mass spectrometer systems that are

Extrel is widely respected for the quality of mass spectrometer systems that are Extrel is widely respected for the quality of mass spectrometer systems that are available to the world's top research scientists. In response to increasing requests for complete turn-key systems built

More information

Technology for Micro- and Nanostructures Micro- and Nanotechnology

Technology for Micro- and Nanostructures Micro- and Nanotechnology Lecture 10: Deposition Technology for Micro- and Nanostructures Micro- and Nanotechnology Peter Unger mailto: peter.unger @ uni-ulm.de Institute of Optoelectronics University of Ulm http://www.uni-ulm.de/opto

More information

Plasma Modeling with COMSOL Multiphysics

Plasma Modeling with COMSOL Multiphysics Plasma Modeling with COMSOL Multiphysics Copyright 2014 COMSOL. Any of the images, text, and equations here may be copied and modified for your own internal use. All trademarks are the property of their

More information

Application of the GD-Profiler 2 to the PV domain

Application of the GD-Profiler 2 to the PV domain Application of the GD-Profiler 2 to the PV domain GD Profiler 2 RF GDOES permits to follow the distribution of the elements as function of depth. This is an ultra fast characterisation technique capable

More information

R I T. Title: GCA Stepper Operations. Semiconductor & Microsystems Fabrication Laboratory Revision: F Rev Date: 08/09/ SCOPE

R I T. Title: GCA Stepper Operations. Semiconductor & Microsystems Fabrication Laboratory Revision: F Rev Date: 08/09/ SCOPE Approved by: Process Engineer / / / / Equipment Engineer 1 SCOPE The purpose of this document is to detail the use of the GCA Stepper. All users are expected to have read and understood this document.

More information

ELEMENT2 High Resolution- ICP-MS INSTRUMENT OVERVIEW

ELEMENT2 High Resolution- ICP-MS INSTRUMENT OVERVIEW ELEMENT2 High Resolution- ICP-MS INSTRUMENT OVERVIEW Inductively Coupled Plasma Mass Spectrometry (ICP-MS) What is a Plasma? - The magnetic field created by a RF (radio frequency) coil produces

More information

Effects of plasma treatment on the precipitation of fluorine-doped silicon oxide

Effects of plasma treatment on the precipitation of fluorine-doped silicon oxide ARTICLE IN PRESS Journal of Physics and Chemistry of Solids 69 (2008) 555 560 www.elsevier.com/locate/jpcs Effects of plasma treatment on the precipitation of fluorine-doped silicon oxide Jun Wu a,, Ying-Lang

More information

SUPPLEMENTARY NOTES Supplementary Note 1: Fabrication of Scanning Thermal Microscopy Probes

SUPPLEMENTARY NOTES Supplementary Note 1: Fabrication of Scanning Thermal Microscopy Probes SUPPLEMENTARY NOTES Supplementary Note 1: Fabrication of Scanning Thermal Microscopy Probes Fabrication of the scanning thermal microscopy (SThM) probes is summarized in Supplementary Fig. 1 and proceeds

More information

Production of Graphite Chloride and Bromide Using Microwave Sparks

Production of Graphite Chloride and Bromide Using Microwave Sparks Supporting Information Production of Graphite Chloride and Bromide Using Microwave Sparks Jian Zheng, Hongtao Liu, Bin Wu, Chong-an Di, Yunlong Guo, Ti Wu, Gui Yu, Yunqi Liu, * and Daoben Zhu Key Laboratory

More information

Atmospheric pressure Plasma Enhanced CVD for large area deposition of TiO 2-x electron transport layers for PV. Heather M. Yates

Atmospheric pressure Plasma Enhanced CVD for large area deposition of TiO 2-x electron transport layers for PV. Heather M. Yates Atmospheric pressure Plasma Enhanced CVD for large area deposition of TiO 2-x electron transport layers for PV Heather M. Yates Why the interest? Perovskite solar cells have shown considerable promise

More information

Introduction to Thin Film Processing

Introduction to Thin Film Processing Introduction to Thin Film Processing Deposition Methods Many diverse techniques available Typically based on three different methods for providing a flux of atomic or molecular material Evaporation Sputtering

More information

Direct Measurement of Metallic Impurities in 20% Ammonium Hydroxide by 7700s/7900 ICP-MS

Direct Measurement of Metallic Impurities in 20% Ammonium Hydroxide by 7700s/7900 ICP-MS Direct Measurement of Metallic Impurities in 20% Ammonium Hydroxide by 7700s/7900 ICP-MS Application Note Semiconductor Authors Junichi Takahashi Agilent Technologies Tokyo, Japan Abstract Ammonium hydroxide

More information

- A spark is passed through the Argon in the presence of the RF field of the coil to initiate the plasma

- A spark is passed through the Argon in the presence of the RF field of the coil to initiate the plasma THE PLASMA Inductively Coupled Plasma Mass Spectrometry (ICP-MS) What is a Plasma? - The magnetic field created by a RF (radio frequency) coil produces a current within a stream of Argon (Ar) gas, which

More information

Reactive Ion Etching (RIE)

Reactive Ion Etching (RIE) Reactive Ion Etching (RIE) RF 13.56 ~ MHz plasma Parallel-Plate Reactor wafers Sputtering Plasma generates (1) Ions (2) Activated neutrals Enhance chemical reaction 1 2 Remote Plasma Reactors Plasma Sources

More information

Nanostructure. Materials Growth Characterization Fabrication. More see Waser, chapter 2

Nanostructure. Materials Growth Characterization Fabrication. More see Waser, chapter 2 Nanostructure Materials Growth Characterization Fabrication More see Waser, chapter 2 Materials growth - deposition deposition gas solid Physical Vapor Deposition Chemical Vapor Deposition Physical Vapor

More information

Title: ASML Stepper Semiconductor & Microsystems Fabrication Laboratory Revision: B Rev Date: 12/21/2010

Title: ASML Stepper Semiconductor & Microsystems Fabrication Laboratory Revision: B Rev Date: 12/21/2010 Approved by: Process Engineer / / / / Equipment Engineer 1 SCOPE The purpose of this document is to detail the use of the ASML PAS 5500 Stepper. All users are expected to have read and understood this

More information

Auger Electron Spectroscopy (AES)

Auger Electron Spectroscopy (AES) 1. Introduction Auger Electron Spectroscopy (AES) Silvia Natividad, Gabriel Gonzalez and Arena Holguin Auger Electron Spectroscopy (Auger spectroscopy or AES) was developed in the late 1960's, deriving

More information

Automated multi-vapor gravimetric sorption analyzer for advanced research applications

Automated multi-vapor gravimetric sorption analyzer for advanced research applications Automated multi-vapor gravimetric sorption analyzer for advanced research applications Automated multi-vapor gravimetric sorption analyzer for advanced research applications Key benefits of the DVS Advantage

More information

NUCLEAR TRANSMUTATION IN DEUTERED PD FILMS IRRADIATED BY AN UV LASER

NUCLEAR TRANSMUTATION IN DEUTERED PD FILMS IRRADIATED BY AN UV LASER Castellano, et al. Nuclear Transmutation in Deutered Pd Films Irradiated by an UV Laser. in 8th International Conference on Cold Fusion. 2000. Lerici (La Spezia), Italy: Italian Physical Society, Bologna,

More information

Infrared Spectroscopy

Infrared Spectroscopy Reminder: These notes are meant to supplement, not replace, the laboratory manual. Infrared Spectroscopy History and Application: Infrared (IR) radiation is simply one segment of the electromagnetic spectrum

More information

Previous Lecture. Electron beam lithoghraphy e - Electrons are generated in vacuum. Electron beams propagate in vacuum

Previous Lecture. Electron beam lithoghraphy e - Electrons are generated in vacuum. Electron beams propagate in vacuum Previous Lecture Electron beam lithoghraphy e - Electrons are generated in vacuum Electron beams propagate in vacuum Lecture 6: Vacuum & plasmas Objectives From this vacuum lecture you will learn: What

More information

Safety in the Chemistry Laboratory

Safety in the Chemistry Laboratory Safety in the Chemistry Laboratory CHAPTER1 Safety must be everyone s primary concern in the chemistry lab. Understanding and following all safety rules in the organic chemistry lab is critical to your

More information

EE 527 MICROFABRICATION. Lecture 24 Tai-Chang Chen University of Washington

EE 527 MICROFABRICATION. Lecture 24 Tai-Chang Chen University of Washington EE 527 MICROFABRICATION Lecture 24 Tai-Chang Chen University of Washington EDP ETCHING OF SILICON - 1 Ethylene Diamine Pyrocatechol Anisotropy: (100):(111) ~ 35:1 EDP is very corrosive, very carcinogenic,

More information

How many grams of sodium metal is required to completely react with 2545 grams of chlorine gas?

How many grams of sodium metal is required to completely react with 2545 grams of chlorine gas? EXAMPLE PROBLEM: How many grams of sodium metal is required to completely react with 2545 grams of chlorine gas? 1 - Convert 2545 grams of chlorine to moles chlorine using formula weight 2 - Convert moles

More information

FTIR INVESTIGATION OF THE AGEING PROCESS OF CARBON NANOWALLS

FTIR INVESTIGATION OF THE AGEING PROCESS OF CARBON NANOWALLS Romanian Reports in Physics, Vol. 68, No. 3, P. 1108 1114, 2016 FTIR INVESTIGATION OF THE AGEING PROCESS OF CARBON NANOWALLS V. MĂRĂSCU 1, 2,*, S. VIZIREANU 2, S. D. STOICA 2, V. BARNA 1, A. LAZEA- STOYANOVA

More information