MB Scientific AB Angular-Resolved Photoemission Spectroscopy System MBS A1SYS_V

Size: px
Start display at page:

Download "MB Scientific AB Angular-Resolved Photoemission Spectroscopy System MBS A1SYS_V"

Transcription

1 Products catalogue MB Scientific AB Angular-Resolved Photoemission Spectroscopy System MBS A1SYS_V 1/15

2 MBS A1SYS_V; Angular-Resolved Photoemission Spectroscopy System MBS A1SYS_V is MB Scientific AB s complete system for Angular-Resolved Photoemission Spectroscopy at Ultra High Resolution. This system has basic but state of the art components for the UPS, XPS* including ARPES measurements. (*X-ray system is optional) Here is a description of our system; Speciality 1. Smart, easy handling UHV system. 2. Extremely high energy resolution photoelectron analyser combined with ultra narrow energy line multi-gas VUV photon source provides absolute front line science at your own lab. 3. Compactly designed, but with full capability for expansion of the system with various options. Basic content of MBS A1SYS_V system; 1. UHV chambers and Aluminum Frame 2. UHV components including Sample cleaver SKTH Photoelectron energy analyser: MBS A-1 with lens4 4. VUV photon source: MBS L-1 (He gas) MBS T-1 (multi gas including Xe) 5. UHV dual grating Monochromator MBS TM-1 for VUV photon sources 6. UHV sample manipulator with low temperature cryostat 7. Water cooling unit 8. Air cooling unit 9. Baking system Options; 1. Different working energy range of electronics 2. Extra pumping system 3. Additional component i.e. X-ray source, Sputtering Ion source, Electron source, LEED- Auger, evaporator. 4. Additional detection system such as Spin polarimeter, Gated MCP detector and so on. There is a flexible choice of the system configuration. For your specific requirements please contact info@mbscientific.se 2/15

3 MBS A1SYS_V; Angular-Resolved Photoemission Spectroscopy System Detailed contents and technical specifications of the system components; 1. UHV chambers with Aluminum frame 1-1 Sample Chamber piece 1-2 Vacuum manifold set 1-3 Sample preparation chamber set 1-4 Al frame set Image photo* *Actual design might deviate from the picture. 2-1 Sample chamber: a. Mu-metal/ Permalloy UHV chamber with 3mm thickness as body material. (All flanges are SUS316L) b. Guaranteed residual magnetic field at sample point less than 500nT c. Guaranteed sample chamber reachable vacuum level less than 2 x 10-8 Pa d. Multiple ports for viewing and optional equipment e. Baking temperature up to 200 degree Celsius d. Every system which contain the Mu-metal/Permalloy chamber supplied with heat treatment certificate 2-2 Vacuum manifold: a. UHV chamber/connection tube made by SUS316L b. Guaranteed reachable vacuum level less than 2 x 10-8 Pa c. Baking temperature up to 200 degree Celsius 2-3 Sample preparation chamber: a. UHV chamber made by SUS316L b. Multiple ports for the sample treatments such as cleaving, evaporation*, annealing* also LEED-AES* optics with convenient opening/pumping. It has also ports for viewing and optional equipment. c. Guaranteed reachable vacuum level less than 2 x 10-8 Pa d. Baking temperature up to 200 degree Celsius *: optional component 3/15

4 2-4 Aluminum frame: a. Flexible standard extruded aluminum frame b. Stable but right weight with high extendibility c. Easy to mount/dismount with stably fastened feet and wheels for transport A-1_#11 UPS system with Aluminium Frame installed at Konan University in Japan 4/15

5 MBS A1SYS; Angular-Resolved Photoemission Spectroscopy System 2. UHV components 1-1 Turbo molecular pumps pcs 1-2 Ion pump 300l pce 1-3 Scroll dry pumps pcs 1-4 UHV gate valves pcs 1-5 MFC:s pcs 1-6 Ion gauges pcs 1-7 Q-mass pce 1-8 Sample cleaver pce 1-9 Magnet coupled rotary feedthrough with Ti Allen key for fastening sample --- 1pcs 1-10 Sampletransfer feedthroughs with magnet coupling pcs 1-11 Vacuum connection tubes and parts --- q.s. Fig. Sample preparation side photo of the A-1SYS #0001 at Shiga University 5/15

6 MBS A1SYS; Angular-Resolved Photoemission Spectroscopy System 2-1 Above components make to reach/allow following condition: a. Guaranteed reachable vacuum level less than 2 x 10-8 Pa in the sample chamber b. Baking temperature up to 200 degree Celsius c. In case of power cut the sample chamber with photoelectron energy analyzer can be kept in a good vacuum by closing 5 gate valves. Fig. UHV system schematic Fig. A-1SYS_#0001 photographed from the light source side 6/15

7 MBS A1SYS_V; Angular-Resolved Photoemission Spectroscopy System 3. Photoelectron energy analyzer_mbs A-1 analyser 1-1 UHV chambers set 1-2 Electron static lens Lans set 1-3 Hemispherical electron energy analyser set 1-4 2D MCP-CCD detection system set 2-1 UHV chambers: a. A1 analyser dome is made of Mu-metal/Permalloy with 3mm thickness as body material. (All flanges, base plate and lens chamber are SUS316L) b. SUS316L parts are electro polished as standard c. Double Mu-metal/Permalloy shield d. Guaranteed reachable vacuum level less than 2 x 10-8 Pa e. CF100/ICF150 pumping port for hemisphere part f. All parts used inside is nonmagnetic material g. 72 hour/ 300 C vacuum fired insulators f. CF40/ICF70 port for mounting ion gauge 2-2 Electrostatic lens: MBS A-1 Lens4 a. Multiple angular modes: 4, 7 and 36 degree total acceptance standard set b. Applicable kinetic energy range UPS ev, XPS ev c. In vacuum adjustable lens axis d. Very good focusing and flexibility by using 7 elements and electrostatic x-y deflector e. All inner surfaces is coated by proprietary 'micro graphite' f. Wide input acceptance angle (36degree) with 35 mm working distance. g. Double Mu-metal/Permalloy shielded h. Mounting flange size is CF200/ICF253, port length 300 mm. i. Angular Resolution (along the slit) within an angular interval of ±3.5 degree Less than 0.1 degree* (Ang3d5) *in the case of 1mmΦ spot size, if spot size is 2mmΦ resolution be less than 0.3 degree 7/15

8 j. Angular Mapping Mode 2-3 Hemispherical electron energy analyser : a. Double Mu-metal/Permalloy shielded b. Baking temperature up to 150 degree Celsius c. Guaranteed reachable vacuum level less than 2 x 10-8 Pa d. Applicable kinetic energy range UPS ev, XPS ev, HE ev e. 200mm mean radius f. Standard Slit Set 9 pairs of 25 mm long BeCu slits Straight: 0.05, 0.1, 0.1(wide aperture), 0.2, 0.4, 0.8, 1.6, 3.2 Curved: 0.2 mm with 1 mm Aperture for adjustments g. Guaranteed energy resolution less than 1meV h. Minimum pre defined pass energy 1eV i. All inner surfaces is coated by micro graphite j. Guaranteed residual magnetic field less than 10nT 2-4 2D MCP-CCD detection system: a. Chevron mount Φ50mm MCP plus fiber optic phosphor screen. b. 2D detection with high sensitivity CCD camera which has 525x910 pixels c. Real time view can be obtained with separate LCD-TV monitor 2-5 Other: a. Easy to be up graded to attach different optional detector such as Spin detector, Gate detector, or other. b. Interface program LabView.vi Energy Resolution -----Better than 1meV The following data was obtained by Dr. Seigo Souma at Tohoku University, Japan. The system consists of MBS A1 with spin option, MBS T1 multi-gas light source, in this case using Xenon gas excitation. 8/15

9 A-1SYS Outlook photo* *System might deviate from the picture depending on the options. 9/15

10 MBS A1SYS_V; Angular-Resolved Photoemission Spectroscopy System 4. VUV photon source_mbs L-1/T-1 lamp 1-1 MBS L-1 He Discharge head set 1-2 MBS T-1 Multi Gas Discharge head set 1-3 Microwave generator set 1-4 Power supply set 1-5 control unit set 2-1 Discharge head: a. Magnetron Microwave ECR (Electron Cyclotron Resonance) plasma. Can use all rare gases from He up to Xe b. Narrow peak wdith less than 0.15meV FWHM at Xe 8.436eV c. Extremely High Brightness More than photon/sr,s(xe) d. Cooling type: Model T-1 air and water, Model L-1 water e. CF40/ICF70 pumping port(s) 2-2 Microwave generator: a. Air cooling with fan T-1 Lamp Head Energies and approximate strengths of He lines HeI: ev 78% ev 8% ev 2% HeII: ev 10% ev 2% Illumination from Xe gas Microwave Generator 10/15

11 MBS A1SYS_V; Angular-Resolved Photoemission Spectroscopy System 5. UHV Monochromator for VUV photon source_mbs TM UHV Twin Monochromator set 2-1 UHV Twin Monochromator: a. Working wavelength between 0nm and 250nm b. Baking temperature up to 150 degree Celsius c. Blaze Wavelength 1350Å d. CF100/ICF150 pumping port e. Accept double gratings to be mounted f. Two ports for mounting L-1 and T-1 lamp head Monochromatised Xe I ( 8.5eV ) Test set up of the Xe VUV system with TM-1 mono 11/15

12 MBS A1SYS_V; Angular-Resolved Photoemission Spectroscopy System 12/15

13 MBS A1SYS_V; Angular-Resolved Photoemission Spectroscopy System 6. UHV sample manipulator with low temperature cryostat 1-1 UHV sample manipulator with Goniometer piece 2-1 UHV sample manipulator with Goniometer: a. Temperature range: 10K to 300K b. Minimum achievable temperature: refrigerator: 4.0K (As system: 10K guarantee) c. Thermal stability: ±0.2K d. Cryostat 1. Cryo capability: exceed 3/5W@60K at 1st Stage(50/60Hz), 0.1W@4.2K at 2nd Stage. 2. He hose:5m 3. Closed liquid He cycle flow e. Interface 1. Sample holder: Gold coated OFHC copper 2. Thermal shield: Body/Head: gold coated OFHC copper 3. Sample rod, Heater mount: Gold coated OFHC copper 4. Skirt: SUSφCF62/ICF114, 6PIN-2pieces f. Manipulation 1. XYZ: manual, Moving distance: XY-axis±10mm Z-axis more than 150mm 2. Rotation: manual 3. Mounting flange size: CF100/ICF Working distance: 250mm, +50mm, -100mm g. Temperature control 1. Temperature control: PID controlled 2. Thermo Heater: Si sensor 2pieces 3. Heater: 50w cartridge 1piece 4. Connection: GP-IB, RS232C h. Utility 1. Power supply for Cryostat AC100/240V, 1φ, 50/60Hz 2. Power supply for temperature control AC100/240V, 1φ, 50/60Hz,200VA 3. Working environment: less than 28 degree Celsius 4. Required vacuum level: less than Pa 13/15

14 MBS A1SYS_V ; Angular-Resolved Photoemission Spectroscopy System 7. Water cooling unit 1-1 Water cooling unit set 2-1 Water cooling unit: It is for cooling the L-1 VUV lamp and thickness monitor, and also for TMP cooling. 8. Air cooling unit 1-1 Air cooling unit set 2-1 Air cooling unit: a. It is for cooling the T-1 VUV lamp. b. Compressor power consumption maximum 2.2kW c. Maximum pressure up to 0.8MPa, controllable pressure between 0.6 and 0.8MPa d. Output air up to 250 l/min e. Power consumption less than 210W for the air dryer f. Relative humidity of output air 15 % within operational temperature 5 to 40 degree Celsius g. Up to 18 liter air tank h. Noise level less than 45dB 14/15

15 MBS A1SYS_V ; Angular-Resolved Photoemission Spectroscopy System 9. Baking system 1-1 Controller unit with thermocouple sets 1-2 Heating tapes 1-3 Fuse box set Heating tapes Controller units Fuse box 15/15

ARPES (Angular Resolved Photoemission Spectroscopy) with a Gas Discharge Lamp

ARPES (Angular Resolved Photoemission Spectroscopy) with a Gas Discharge Lamp ARPES (Angular Resolved Photoemission Spectroscopy) with a Gas Discharge Lamp Outline - Experimental Setup - Individual Components - How to conduct an experiment - VUV lamps - Electron analyzer essentials

More information

Technical description of photoelectron spectrometer Escalab 250Xi

Technical description of photoelectron spectrometer Escalab 250Xi Technical description of photoelectron spectrometer Escalab 250Xi Resource center Physical Methods of Surface Investigations 2014 Table of contents Common description 3 Analytical chamber 8 Preparation

More information

Microscopy Cryostat System

Microscopy Cryostat System OF AMERICA, INC. Microscopy Cryostat System RC102-CFM Microscopy Cryostat offers fast cooldown, high efficiency, lowest thermal drift, excellent temperature stability and ultra low vibration Optical cryostat

More information

UV Source Series. UVS 10/35 gas discharge, UVS 300 duoplasmatron. Key Features

UV Source Series. UVS 10/35 gas discharge, UVS 300 duoplasmatron. Key Features UV Source Series UVS 10/35 gas discharge, UVS 300 duoplasmatron and UVLS microwave source for UPS and arpes Key Features Ultimate intensity and stability UV sources Ease of operation Variable excitation

More information

The Use of Synchrotron Radiation in Modern Research

The Use of Synchrotron Radiation in Modern Research The Use of Synchrotron Radiation in Modern Research Physics Chemistry Structural Biology Materials Science Geochemical and Environmental Science Atoms, molecules, liquids, solids. Electronic and geometric

More information

PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy

PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy PHI 5000 Versaprobe-II Focus X-ray Photo-electron Spectroscopy The very basic theory of XPS XPS theroy Surface Analysis Ultra High Vacuum (UHV) XPS Theory XPS = X-ray Photo-electron Spectroscopy X-ray

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

Photoemission Spectroscopy

Photoemission Spectroscopy FY13 Experimental Physics - Auger Electron Spectroscopy Photoemission Spectroscopy Supervisor: Per Morgen SDU, Institute of Physics Campusvej 55 DK - 5250 Odense S Ulrik Robenhagen,

More information

Experimental 2.1 Introduction. Ultra high vacuum.

Experimental 2.1 Introduction. Ultra high vacuum. 2 Experimental 2.1 Introduction. Ultra high vacuum. The interest in solid-gas (or solid-vacuum) interfaces has been increasing rapidly during the last three decades. On one hand this is due to the practical

More information

Lecture 5. X-ray Photoemission Spectroscopy (XPS)

Lecture 5. X-ray Photoemission Spectroscopy (XPS) Lecture 5 X-ray Photoemission Spectroscopy (XPS) 5. Photoemission Spectroscopy (XPS) 5. Principles 5.2 Interpretation 5.3 Instrumentation 5.4 XPS vs UV Photoelectron Spectroscopy (UPS) 5.5 Auger Electron

More information

Lecture 5-8 Instrumentation

Lecture 5-8 Instrumentation Lecture 5-8 Instrumentation Requirements 1. Vacuum Mean Free Path Contamination Sticking probability UHV Materials Strength Stability Permeation Design considerations Pumping speed Virtual leaks Leaking

More information

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7

Advanced Lab Course. X-Ray Photoelectron Spectroscopy 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT Qualitative analysis Chemical Shifts 7 Advanced Lab Course X-Ray Photoelectron Spectroscopy M210 As of: 2015-04-01 Aim: Chemical analysis of surfaces. Content 1 INTRODUCTION 1 2 BASICS 1 3 EXPERIMENT 3 3.1 Qualitative analysis 6 3.2 Chemical

More information

Atomic Absorption Spectrometer ZEEnit P series

Atomic Absorption Spectrometer ZEEnit P series Atomic Absorption Spectrometer ZEEnit P series Technical Data ZEEnit series Update 07/2014 OBue 1/ 5 ZEEnit P series Variable high-end AA Spectrometer with Deuterium and Zeeman Background Correction with

More information

3. Experimental Methods and Instrumentation.

3. Experimental Methods and Instrumentation. 3. Experimental Methods and Instrumentation. 3.1 UHV Setup An ultrahigh vacuum chamber pumped by a turbo molecular pump with a base pressure in the low 10-10 mbar range was used (figure 3.1). This chamber

More information

A photoelectron spectrometer for k-space mapping above the Fermi level

A photoelectron spectrometer for k-space mapping above the Fermi level A photoelectron spectrometer for k-space mapping above the Fermi level T. Greber a) Physik Institut der Universität Zürich, Winterthurerstr. 190, CH-8057 Zürich, Switzerland O. Raetzo Institut de Physique,

More information

X-ray Photoelectron Spectroscopy (XPS)

X-ray Photoelectron Spectroscopy (XPS) X-ray Photoelectron Spectroscopy (XPS) As part of the course Characterization of Catalysts and Surfaces Prof. Dr. Markus Ammann Paul Scherrer Institut markus.ammann@psi.ch Resource for further reading:

More information

Studying Metal to Insulator Transitions in Solids using Synchrotron Radiation-based Spectroscopies.

Studying Metal to Insulator Transitions in Solids using Synchrotron Radiation-based Spectroscopies. PY482 Lecture. February 28 th, 2013 Studying Metal to Insulator Transitions in Solids using Synchrotron Radiation-based Spectroscopies. Kevin E. Smith Department of Physics Department of Chemistry Division

More information

Angle-resolved photoemission spectroscopy (ARPES) Overview-Physics 250, UC Davis Inna Vishik

Angle-resolved photoemission spectroscopy (ARPES) Overview-Physics 250, UC Davis Inna Vishik Angle-resolved photoemission spectroscopy (ARPES) Overview-Physics 250, UC Davis Inna Vishik Outline Review: momentum space and why we want to go there Looking at data: simple metal Formalism: 3 step model

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

novaa 800 D Atomic Absorption Spectrometer

novaa 800 D Atomic Absorption Spectrometer Technical Data Atomic Absorption Spectrometer Cpt : +27 (0) 21 905 0476 Jhb : +27 (0) 11 794 Dbn : +27 (0) 31 266 2454 1/7 General The is a compact atomic absorption spectrometer with deuterium background

More information

M2 TP. Low-Energy Electron Diffraction (LEED)

M2 TP. Low-Energy Electron Diffraction (LEED) M2 TP Low-Energy Electron Diffraction (LEED) Guide for report preparation I. Introduction: Elastic scattering or diffraction of electrons is the standard technique in surface science for obtaining structural

More information

Chapter 3. Experimental Techniques. 3.1 Optical bending beam method

Chapter 3. Experimental Techniques. 3.1 Optical bending beam method Chapter 3 Experimental Techniques Stress measurements using optical bending beam method can be applied for UHV system as well as in air. However, the magnetic properties of ultra thin films are better

More information

MSE 321 Structural Characterization

MSE 321 Structural Characterization Auger Spectroscopy Auger Electron Spectroscopy (AES) Scanning Auger Microscopy (SAM) Incident Electron Ejected Electron Auger Electron Initial State Intermediate State Final State Physical Electronics

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

The Standard Auger Electron Spectra in The AIST DIO-DB(111); Ge(111)

The Standard Auger Electron Spectra in The AIST DIO-DB(111); Ge(111) Paper The Standard Auger Electron Spectra in The AIST DIO-DB(111); Ge(111) K. Goto, a,* Adel Alkafri, b Y. Ichikawa, b A.Kurokawa, c and Y. Yamauchi a a AIST-Chubu Center, Anagahora 2266, Moriyama-ku,

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

Photoelectron spectroscopy Instrumentation. Nanomaterials characterization 2

Photoelectron spectroscopy Instrumentation. Nanomaterials characterization 2 Photoelectron spectroscopy Instrumentation Nanomaterials characterization 2 RNDr. Věra V Vodičkov ková,, PhD. Photoelectron Spectroscopy general scheme Impact of X-ray emitted from source to the sample

More information

CRYOGENIC CONDUCTION COOLING TEST OF REMOVABLE PANEL MOCK-UP FOR ITER CRYOSTAT THERMAL SHIELD

CRYOGENIC CONDUCTION COOLING TEST OF REMOVABLE PANEL MOCK-UP FOR ITER CRYOSTAT THERMAL SHIELD CRYOGENIC CONDUCTION COOLING TEST OF REMOVABLE PANEL MOCK-UP FOR ITER CRYOSTAT THERMAL SHIELD K. Nam, a D. K. Kang, a W. Chung, a C. H. Noh, a J. Yu, b N. I. Her, b C. Hamlyn-Harris, b Y. Utin, b and K.

More information

Vibration-Free Pulse Tube Cryocooler System for Gravitational Wave Detectors I

Vibration-Free Pulse Tube Cryocooler System for Gravitational Wave Detectors I 1 Vibration-Free Pulse Tube Cryocooler System for Gravitational Wave Detectors I - Vibration-Reduction Method and Measurement - T. Tomaru A, T. Suzuki A, T. Haruyama A, T. Shintomi A, N. Sato A, A. Yamamoto

More information

Ma5: Auger- and Electron Energy Loss Spectroscopy

Ma5: Auger- and Electron Energy Loss Spectroscopy Ma5: Auger- and Electron Energy Loss Spectroscopy 1 Introduction Electron spectroscopies, namely Auger electron- and electron energy loss spectroscopy are utilized to determine the KLL spectrum and the

More information

Ion Implanter Cyclotron Apparatus System

Ion Implanter Cyclotron Apparatus System Ion Implanter Cyclotron Apparatus System A. Latuszyñski, K. Pyszniak, A. DroŸdziel, D. M¹czka Institute of Physics, Maria Curie-Sk³odowska University, Lublin, Poland Abstract In this paper the authors

More information

Atomic Spectra HISTORY AND THEORY

Atomic Spectra HISTORY AND THEORY Atomic Spectra HISTORY AND THEORY When atoms of a gas are excited (by high voltage, for instance) they will give off light. Each element (in fact, each isotope) gives off a characteristic atomic spectrum,

More information

Parts Manual R410A Models

Parts Manual R410A Models Parts Manual R410A Models PTAC - PD Series (Electronic Controls) Packaged Terminal Air Conditioners Packaged Terminal Heat Pumps PTAC PARTS E (1-2010) Table of Contents Unit Identification... 2 PTAC System

More information

CIG B5. Capitolato Tecnico Technical requirements

CIG B5. Capitolato Tecnico Technical requirements Gara a procedura aperta per l'affidamento della fornitura di uno strumento per X-ray Photoelectron Spetroscopy (XPS) destinato alla Nanochemistry Facility dell Istituto Italiano di Tecnologia CIG 05092316B5

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

A DIVISION OF ULVAC-PHI

A DIVISION OF ULVAC-PHI A DIVISION OF ULVAC-PHI X-ray photoelectron spectroscopy (XPS/ESCA) is the most widely used surface analysis technique and has many well established industrial and research applications. XPS provides

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

JARA FIT Ferienprakticum Nanoelektronik Experiment: Resonant tunneling in quantum structures

JARA FIT Ferienprakticum Nanoelektronik Experiment: Resonant tunneling in quantum structures JARA FIT Ferienprakticum Nanoelektronik 2013 Experiment: Resonant tunneling in quantum structures Dr. Mihail Ion Lepsa, Peter Grünberg Institut (PGI 9), Forschungszentrum Jülich GmbH 1. Introduction The

More information

The ISIS Penning H - SPS and Diagnostic Developments at RAL

The ISIS Penning H - SPS and Diagnostic Developments at RAL The ISIS Penning H - SPS and Diagnostic Developments at RAL D.C. Faircloth 1, A.P. Letchford 1, J. Pozimski 1+2, M.O. Whitehead 1, T. Wood 1, S. Jolly 2, P. Savage 2, M. Haigh 3, J. Morrison 3, I. Yew

More information

5) Surface photoelectron spectroscopy. For MChem, Spring, Dr. Qiao Chen (room 3R506) University of Sussex.

5) Surface photoelectron spectroscopy. For MChem, Spring, Dr. Qiao Chen (room 3R506) University of Sussex. For MChem, Spring, 2009 5) Surface photoelectron spectroscopy Dr. Qiao Chen (room 3R506) http://www.sussex.ac.uk/users/qc25/ University of Sussex Today s topics 1. Element analysis with XPS Binding energy,

More information

Nova 600 NanoLab Dual beam Focused Ion Beam IITKanpur

Nova 600 NanoLab Dual beam Focused Ion Beam IITKanpur Nova 600 NanoLab Dual beam Focused Ion Beam system @ IITKanpur Dual Beam Nova 600 Nano Lab From FEI company (Dual Beam = SEM + FIB) SEM: The Electron Beam for SEM Field Emission Electron Gun Energy : 500

More information

General Physics II Summer Session 2013 Review Ch - 16, 17, 18

General Physics II Summer Session 2013 Review Ch - 16, 17, 18 95.104 General Physics II Summer Session 2013 Review Ch - 16, 17, 18 A metal ball hangs from the ceiling by an insulating thread. The ball is attracted to a positivecharged rod held near the ball. The

More information

Replication Of MHI Transmutation Experiment By D 2 Gas Permeation Through Pd Complex

Replication Of MHI Transmutation Experiment By D 2 Gas Permeation Through Pd Complex Higashiyama, T., et al. Replication Of MHI Transmutation Experiment By D2 Gas Permeation Through Pd Complex. in Tenth International Conference on Cold Fusion. 2003. Cambridge, MA: LENR-CANR.org. This paper

More information

Results on a-c tubes subjected to synchrotron irradiation

Results on a-c tubes subjected to synchrotron irradiation Results on a-c tubes subjected to synchrotron irradiation V. Baglin, P. Chiggiato, P. Costa-Pinto, B. Henrist (CERN, Geneva) V. Anashin, D. Dorokhov. A. Semenov, A. Krasnov, D. Shwartz, A. Senchenko (,

More information

Vacuum. Kai Schwarzwälder, Institut für Physik Universität Basel October 6 th 2006

Vacuum. Kai Schwarzwälder, Institut für Physik Universität Basel October 6 th 2006 Physics,, Technology and Techniques of the Vacuum Kai Schwarzwälder, Institut für Physik Universität Basel October 6 th 2006 Outline Introduction and basics Defintion of Vacuum Vacuum A vacuum is a volume

More information

1) Introduction 2) Photo electric effect 3) Dual nature of matter 4) Bohr s atom model 5) LASERS

1) Introduction 2) Photo electric effect 3) Dual nature of matter 4) Bohr s atom model 5) LASERS 1) Introduction 2) Photo electric effect 3) Dual nature of matter 4) Bohr s atom model 5) LASERS 1. Introduction Types of electron emission, Dunnington s method, different types of spectra, Fraunhoffer

More information

Mass Spectrometers. for Surface Analysis SURFACE ANALYSIS

Mass Spectrometers. for Surface Analysis SURFACE ANALYSIS Mass Spectrometers for Surface Analysis SURFACE ANALYSIS MASS SPECTROMETERS for Surface Analysis Hiden Analytical have been designing and developing the highest quality quadrupole mass spectrometer based

More information

Chemistry 524--Final Exam--Keiderling May 4, :30 -?? pm SES

Chemistry 524--Final Exam--Keiderling May 4, :30 -?? pm SES Chemistry 524--Final Exam--Keiderling May 4, 2011 3:30 -?? pm -- 4286 SES Please answer all questions in the answer book provided. Calculators, rulers, pens and pencils are permitted. No open books or

More information

PARTS CATALOG MUZ-FE09NA MUZ-FE09NA - 1 MUZ-FE09NAH MUZ-FE12NA MUZ-FE12NA1 MUZ-FE12NAH MUZ-FE18NA OUTDOOR UNIT. No. OBB543 REVISED EDITION-C.

PARTS CATALOG MUZ-FE09NA MUZ-FE09NA - 1 MUZ-FE09NAH MUZ-FE12NA MUZ-FE12NA1 MUZ-FE12NAH MUZ-FE18NA OUTDOOR UNIT. No. OBB543 REVISED EDITION-C. SPLIT-TYPE AIR CONDITIONERS Revision C: H and FE12NAH have been added. Please void OBB543 REVISED EDITION-B. OUTDOOR UNIT PARTS CATALOG No. OBB543 REVISED EDITION-C Models - 1 H FE12NA FE12NA1 FE12NAH

More information

Multi-technique photoelectron spectrometer for micro-area spectroscopy and imaging

Multi-technique photoelectron spectrometer for micro-area spectroscopy and imaging Multi-technique photoelectron spectrometer for micro-area spectroscopy and imaging U. Manju, M. Sreemony and A. K. Chakraborty In this note we present the new multipurpose photoelectron spectroscopy facility

More information

object objective lens eyepiece lens

object objective lens eyepiece lens Advancing Physics G495 June 2015 SET #1 ANSWERS Field and Particle Pictures Seeing with electrons The compound optical microscope Q1. Before attempting this question it may be helpful to review ray diagram

More information

Defining quality standards for the analysis of solid samples

Defining quality standards for the analysis of solid samples Defining quality standards for the analysis of solid samples Thermo Scientific Element GD Plus Glow Discharge Mass Spectrometer Redefine your quality standards for the elemental analysis of solid samples

More information

ARGUS VI. Static Vacuum Mass Spectrometer. Static Vacuum ARGUS VI. Multicollection Low Volume Precision

ARGUS VI. Static Vacuum Mass Spectrometer. Static Vacuum ARGUS VI. Multicollection Low Volume Precision ARGUS VI Static Vacuum Mass Spectrometer Static Vacuum ARGUS VI Multicollection Low Volume Precision Based on more than 20 years of experience in noble gas mass spectrometry instrumentation, we have developed

More information

Physics 24, Spring 2007 Lab 2 - Complex Spectra

Physics 24, Spring 2007 Lab 2 - Complex Spectra Physics 24, Spring 2007 Lab 2 - Complex Spectra Theory The optical spectra of isolated atoms consist of discrete, unequally spaced lines. This fact could not be understood on the basis of classical atomic

More information

The photoelectric effect

The photoelectric effect The photoelectric effect E K hν-e B E F hν E B A photoemission experiment Lifetime broadening ΔE.Δτ~ħ ΔE~ħ/Δτ + Experimental resolution Hüfner, Photoelectron Spectroscopy (Springer) A photoemission experiment

More information

X-Rays From Laser Plasmas

X-Rays From Laser Plasmas X-Rays From Laser Plasmas Generation and Applications I. C. E. TURCU CLRC Rutherford Appleton Laboratory, UK and J. B. DANCE JOHN WILEY & SONS Chichester New York Weinheim Brisbane Singapore Toronto Contents

More information

Beamlines on Indian synchrotron radiation source Indus-1

Beamlines on Indian synchrotron radiation source Indus-1 Beamlines on Indian synchrotron radiation source Indus-1 R. V. Nandedkar Centre for Advanced Technology, Indore 452 013, India In India, at the Center for Advanced Technology (CAT), Indore a 450 MeV electron

More information

Methods of surface analysis

Methods of surface analysis Methods of surface analysis Nanomaterials characterisation I RNDr. Věra Vodičková, PhD. Surface of solid matter: last monoatomic layer + absorbed monolayer physical properties are effected (crystal lattice

More information

Thermo Scientific K-Alpha + XPS Spectrometer. Fast, powerful and accessible chemical analysis for surface and thin film characterization

Thermo Scientific K-Alpha + XPS Spectrometer. Fast, powerful and accessible chemical analysis for surface and thin film characterization Thermo Scientific K-Alpha + XPS Spectrometer Fast, powerful and accessible chemical analysis for surface and thin film characterization X-ray Photoelectron Spectroscopy Quantitative, chemical identification

More information

Atomic and Nuclear Physics

Atomic and Nuclear Physics Atomic and Nuclear Physics Nuclear physics Rutherford scattering LD Physics Leaflets P6.5.2.1 Rutherford scattering: measuring the scattering rate as a function of the scattering angle and the atomic number

More information

Flight Demonstration of Electrostatic Thruster Under Micro-Gravity

Flight Demonstration of Electrostatic Thruster Under Micro-Gravity Flight Demonstration of Electrostatic Thruster Under Micro-Gravity Shin SATORI*, Hiroyuki MAE**, Hiroyuki OKAMOTO**, Ted Mitsuteru SUGIKI**, Yoshinori AOKI # and Atsushi NAGATA # * Hokkaido Institute of

More information

Spin-resolved photoelectron spectroscopy

Spin-resolved photoelectron spectroscopy Spin-resolved photoelectron spectroscopy Application Notes Spin-resolved photoelectron spectroscopy experiments were performed in an experimental station consisting of an analysis and a preparation chamber.

More information

UPGRADE AND COMMISSIONING OF THE PIAVE-ALPI ECR INJECTOR AT LNL

UPGRADE AND COMMISSIONING OF THE PIAVE-ALPI ECR INJECTOR AT LNL UPGRADE AND COMMISSIONING OF THE PIAVE-ALPI ECR INJECTOR AT LNL A. Galatà, M. Sattin, L. Bertazzo, L. Boscagli, S. Contran, A. Dainese, A. Lombardi, D. Maniero, M. Poggi, F. Scarpa, A. Facco, INFN-LNL,

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

PHOTOELECTRON SPECTROSCOPY (PES)

PHOTOELECTRON SPECTROSCOPY (PES) PHOTOELECTRON SPECTROSCOPY (PES) NTRODUCTON Law of Photoelectric effect Albert Einstein, Nobel Prize 1921 Kaiser-Wilhelm-nstitut (now Max-Planck- nstitut) für Physik Berlin, Germany High-resolution electron

More information

KP Technology System Catalogue

KP Technology System Catalogue Sample: Al Tip: 2mm S/S Sig Ave: 60 WF Ave: 2 T: 18.9 C Gain: 4 KP Technology System Catalogue Winter 2013-2014 Al Relative Humidity Ramp Test (10% steps) @ 2 Hr/step 09-10/Nov/2013 RH (%) 92 90 88 86

More information

MSE 321 Structural Characterization

MSE 321 Structural Characterization Auger Spectroscopy Auger Electron Spectroscopy (AES) Scanning Auger Microscopy (SAM) Incident Electron Ejected Electron Auger Electron Initial State Intermediate State Final State Physical Electronics

More information

Practice Final Name. m 3 /s b) 8.75 x 10 4 c) 8.21 x 10 4 d) 7.45 x 10 4 e) 7.21 x 10 4 Ans: a

Practice Final Name. m 3 /s b) 8.75 x 10 4 c) 8.21 x 10 4 d) 7.45 x 10 4 e) 7.21 x 10 4 Ans: a I included more than 35 problems only for practice purposes. In the final you will have 35 problems, as I stated during the last class meeting on Thursday, December 7, 2006. Practice Final Name 1) In a

More information

A beam of coherent monochromatic light from a distant galaxy is used in an optics experiment on Earth.

A beam of coherent monochromatic light from a distant galaxy is used in an optics experiment on Earth. Waves_P2 [152 marks] A beam of coherent monochromatic light from a distant galaxy is used in an optics experiment on Earth. The beam is incident normally on a double slit. The distance between the slits

More information

High Resolution Photoemission Study of the Spin-Dependent Band Structure of Permalloy and Ni

High Resolution Photoemission Study of the Spin-Dependent Band Structure of Permalloy and Ni High Resolution Photoemission Study of the Spin-Dependent Band Structure of Permalloy and Ni K. N. Altmann, D. Y. Petrovykh, and F. J. Himpsel Department of Physics, University of Wisconsin, Madison, 1150

More information

H. R. Hirsch R. J. Hull R. H. Kohler Mrs. Ilana Levitan K. K. Y. Li J. H. Loehlin

H. R. Hirsch R. J. Hull R. H. Kohler Mrs. Ilana Levitan K. K. Y. Li J. H. Loehlin IIIL - -~ V. NUCLEAR MAGNETIC RESONANCE AND HYPERFINE STRUCTURE Prof. F. Bitter Prof. L. C. Bradley III Prof. J. S. Waugh Dr. H. H. Stroke Dr. J. F. Waymouth B. B. Aubrey M. Ciftan H. R. Hirsch R. J. Hull

More information

Instructions for the advanced lab course Angle-resolved photoelectron spectroscopy

Instructions for the advanced lab course Angle-resolved photoelectron spectroscopy Instructions for the advanced lab course Angle-resolved photoelectron spectroscopy Contents 1 Introduction 2 2 References 2 3 Preparation 3 3.1 Basics of Condensed Matter Physics............... 3 3.2 Photoelectron

More information

How to distinguish EUV photons from out-of-band photons

How to distinguish EUV photons from out-of-band photons How to distinguish EUV photons from out-of-band photons Thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Physics Author: Student ID: Supervisors: 2 nd

More information

HELIX SFT. Static Vacuum ARGUS VI HELIX SFT. Static Vacuum Mass Spectrometer Static Vacuum Mass Spectrometer

HELIX SFT. Static Vacuum ARGUS VI HELIX SFT. Static Vacuum Mass Spectrometer Static Vacuum Mass Spectrometer ARGUS VI HELIX SFT Static Vacuum Mass Spectrometer Static Vacuum Mass Spectrometer Static Vacuum HELIX SFT Low Volume Multicollection High Mass Resolution 3 Based on more than 20 years of experience in

More information

X-ray Photoelectron Spectroscopy/ Electron spectroscopy for chemical analysis (ESCA), By Francis Chindeka

X-ray Photoelectron Spectroscopy/ Electron spectroscopy for chemical analysis (ESCA), By Francis Chindeka X-ray Photoelectron Spectroscopy/ Electron spectroscopy for chemical analysis (ESCA), By Francis Chindeka X-ray photoelectron spectroscopy (XPS) or Electron spectroscopy for chemical analysis (ESCA), Surface

More information

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source

Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source 3rd International EUVL Symposium NOVEMBER 1-4, 2004 Miyazaki, Japan Visualization of Xe and Sn Atoms Generated from Laser-Produced Plasma for EUV Light Source H. Tanaka, A. Matsumoto, K. Akinaga, A. Takahashi

More information

Harmonic Generation for Photoionization Experiments Christian J. Kornelis Physics REU Kansas State University

Harmonic Generation for Photoionization Experiments Christian J. Kornelis Physics REU Kansas State University Harmonic Generation for Photoionization Experiments Christian J. Kornelis Physics REU Kansas State University The Basic Setup for the KLS Photoionization Experiment V. Kumarappan Femtosecond Pump-Probe

More information

LIBSlab ANALYZERS ANALYZERS

LIBSlab ANALYZERS ANALYZERS ANALYZERS ANALYZERS Chemical multi-elemental analysis with LIBS in modular benchtop design LIBSlab LIBSpector compact sample chamber for the LIBS analysis of solid, liquid and gaseous samples. Sample chamber

More information

Which Optistat is right for you?

Which Optistat is right for you? OPTISTAT Optistat liquid cryogen optical cryostats for spectroscopy Which Optistat is right for you? Our easy to use, compact and efficient Optistat cryostats offer a wide range of options to suit most

More information

HELIX MC Plus. Static Vacuum. ARGUS VI Thermo Scientific HELIX MC Plus Static Vacuum Mass Spectrometer Static Vacuum Mass Spectrometer

HELIX MC Plus. Static Vacuum. ARGUS VI Thermo Scientific HELIX MC Plus Static Vacuum Mass Spectrometer Static Vacuum Mass Spectrometer ARGUS VI Thermo Scientific HELIX MC Plus Static Vacuum Mass Spectrometer Static Vacuum Mass Spectrometer Static Vacuum HELIX MC Plus Dynamic range Multi collection High mass resolution Based on more than

More information

Direct Neutrino Mass Measurement with KATRIN. Sanshiro Enomoto (University of Washington) for the KATRIN Collaboration

Direct Neutrino Mass Measurement with KATRIN. Sanshiro Enomoto (University of Washington) for the KATRIN Collaboration Direct Neutrino Mass Measurement with KATRIN Sanshiro Enomoto (University of Washington) for the KATRIN Collaboration DBD16, Osaka, Japan, 8 Nov 2016 Neutrino Mass Measurement with Single Beta Decay 2

More information

Birck Nanotechnology Center XPS: X-ray Photoelectron Spectroscopy ESCA: Electron Spectrometer for Chemical Analysis

Birck Nanotechnology Center XPS: X-ray Photoelectron Spectroscopy ESCA: Electron Spectrometer for Chemical Analysis Birck Nanotechnology Center XPS: X-ray Photoelectron Spectroscopy ESCA: Electron Spectrometer for Chemical Analysis Dmitry Zemlyanov Birck Nanotechnology Center, Purdue University Outline Introduction

More information

PHYSICS QUESTION PAPER CLASS-XII

PHYSICS QUESTION PAPER CLASS-XII PHYSICS QUESTION PAPER CLASS-XII Time : 3.00 Hours] [Maximum Marks : 100 Instructions : There are four sections and total 60 questions in this question paper. ( 1) (2) All symbols used in this question

More information

Beetle UHV VT AFM / STM

Beetle UHV VT AFM / STM UHV VT AFM / STM RHK Technology Imaging the Future of Nanoscience UHV VT AFM / STM Engineered Excellence Everyday, in university and government labs around the globe, RHK research platforms lead to new

More information

Because light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency.

Because light behaves like a wave, we can describe it in one of two ways by its wavelength or by its frequency. Light We can use different terms to describe light: Color Wavelength Frequency Light is composed of electromagnetic waves that travel through some medium. The properties of the medium determine how light

More information

Development of a High-Speed VUV Camera System for 2-Dimensional Imaging of Edge Turbulent Structure in the LHD

Development of a High-Speed VUV Camera System for 2-Dimensional Imaging of Edge Turbulent Structure in the LHD Development of a High-Speed VUV Camera System for 2-Dimensional Imaging of Edge Turbulent Structure in the LHD Masaki TAKEUCHI, Satoshi OHDACHI and LHD experimental group National Institute for Fusion

More information

Puebla, C.P , Mexico; ABSTRACT 1. INTRODUCTION 2. CRYOSTAT INTEGRATION

Puebla, C.P , Mexico; ABSTRACT 1. INTRODUCTION 2. CRYOSTAT INTEGRATION Integration and characterization of the cryogenic system of MEGARA Ferrusca R.,D.* a, Cisneros G., M. E. a, Velázquez, M. a, Zenteno H., J. A. a, Gil de Paz, A. b, Gallego, J. b, Carrasco, E. a, Sánchez-Moreno

More information

Plasma Spectroscopy in ISTTOK

Plasma Spectroscopy in ISTTOK Plasma Spectroscopy in ISTTOK J. Figueiredo 1, R. B. Gomes 1, T. Pereira 1, H. Fernandes 1, A. Sharakovski 2 1 Associação EURATOM/IST, Centro de Fusão Nuclear, IST, 1049-001 Lisboa, Portugal 2 Association

More information

Emission Spectrum of Atomic Gases. Prelab Questions

Emission Spectrum of Atomic Gases. Prelab Questions Emission Spectrum of Atomic Gases Prelab Questions Before this coming to this lab, please review your text for the physics of the spectrum of visible light and of diffraction grating spectrometer.. Which

More information

ORMS HARS. SpectrA LAB EQUIPMENTS Optical Rotation Resolution nm Wavelength Range 0.1nm Wavelength Resolution -70 C Cooling 10 Vacuum

ORMS HARS. SpectrA LAB EQUIPMENTS Optical Rotation Resolution nm Wavelength Range 0.1nm Wavelength Resolution -70 C Cooling 10 Vacuum All Products are manufactured and marketed by Opto-Mechatronics Pvt. Ltd HARS ADVANCED RESEARCH SYSTEMS & SOLUTIONS FARADAY & KERR OPTO-MECHATRONICS PVT.LTD OPTICAL ROTATION MEASUREMENT SYSTEM 0-3 0.005

More information

Cover Page. The handle holds various files of this Leiden University dissertation.

Cover Page. The handle   holds various files of this Leiden University dissertation. Cover Page The handle http://hdl.handle.net/1887/44295 holds various files of this Leiden University dissertation. Author: Badan, C. Title: Surface-structure dependence of water-related adsorbates on platinum

More information

AES - Auger Electron Spectrosopy

AES - Auger Electron Spectrosopy Advanced Materials - Lab Intermediate Physics Ulm University Institute of Solid State Physics AES - Auger Electron Spectrosopy Sebastian Schnurr March 13, 2013 Safety Precautions MAKE SURE THAT YOU UNDERSTAND

More information

Spectroscopic studies of impurities in the LHD plasmas

Spectroscopic studies of impurities in the LHD plasmas Spectroscopic studies of impurities in the LHD plasmas Visitor: Zhenwei Wu (the institute of plasma physics, CAS -ASIPP) Host: Shigeru Morita (the national institute for fusion science -NIFS) Content 1.

More information

This experiment is included in the XRP 4.0 X-ray solid state, XRS 4.0 X-ray structural analysis, and XRC 4.0 X-ray characteristics upgrade sets.

This experiment is included in the XRP 4.0 X-ray solid state, XRS 4.0 X-ray structural analysis, and XRC 4.0 X-ray characteristics upgrade sets. The intensity of characteristic X-rays as a TEP Related topics Characteristic X-radiation, energy levels, Bragg s law, and intensity of characteristic X-rays Principle The X-ray spectrum of an X-ray tube

More information

In the investigation, a pressure on the order of 10-6

In the investigation, a pressure on the order of 10-6 Production of a 131m Xe calibration source for Cyclotron Radiation Emission Spectroscopy and use with Project 8 setup Annie Ramey Physics Department and CENPA, University of Washington (Dated: August 23,

More information

= 6 (1/ nm) So what is probability of finding electron tunneled into a barrier 3 ev high?

= 6 (1/ nm) So what is probability of finding electron tunneled into a barrier 3 ev high? STM STM With a scanning tunneling microscope, images of surfaces with atomic resolution can be readily obtained. An STM uses quantum tunneling of electrons to map the density of electrons on the surface

More information

Thermo Scientific ELEMENT GD PLUS Glow Discharge Mass Spectrometer. Defining quality standards for the analysis of solid samples

Thermo Scientific ELEMENT GD PLUS Glow Discharge Mass Spectrometer. Defining quality standards for the analysis of solid samples Thermo Scientific ELEMENT GD PLUS Glow Discharge Mass Spectrometer Defining quality standards for the analysis of solid samples Redefine your quality standards for the elemental analysis of solid samples

More information

Lecture 3 Vacuum Science and Technology

Lecture 3 Vacuum Science and Technology Lecture 3 Vacuum Science and Technology Chapter 3 - Wolf and Tauber 1/56 Announcements Homework will be online from noon today. This is homework 1 of 4. 25 available marks (distributed as shown). This

More information

Introduction to Blackbody Sources

Introduction to Blackbody Sources Introduction to s This section contains dedicated blackbody sources for low uncertainty calibration of infrared thermometers. A range of portable primary blackbody sources combine high emissivity with

More information

A fast, parallel acquisition, electron energy analyzer: The hyperbolic field analyzer

A fast, parallel acquisition, electron energy analyzer: The hyperbolic field analyzer REVIEW OF SCIENTIFIC INSTRUMENTS VOLUME 70, NUMBER 5 MAY 1999 A fast, parallel acquisition, electron energy analyzer: The hyperbolic field analyzer M. Jacka a) and M. Kirk Department of Physics, University

More information