There are 3 main drivers in specifying an EDS detector:
• Energy resolution @ Mn k-alpha
• Sensitivity
• Solid angle
How relevant are these specifications in determining the performance of an EDS detector?
How do I choose the right detector for your lab?
Scanning Electron Microscope- Energy - Dispersive X -Ray Microanalysis (Sem E...Nani Karnam Vinayakam
The document discusses scanning electron microscopy (SEM) and energy-dispersive X-ray spectroscopy (EDX or EDS) analysis. It provides details on:
- How an SEM works by scanning a sample with a focused electron beam and detecting signals from electron interactions with the sample.
- The components of an SEM including the electron gun, detectors for secondary electrons and backscattered electrons.
- How EDX analysis identifies elements by measuring the energy of X-rays emitted when electrons change energy levels.
- Parameters that affect EDX analysis such as count rate, accelerating voltage, and take-off angle.
EDS softwares INCA and EDAX_EM forum_Yina Guo_May 2016YinaGuo
The document discusses energy dispersive spectroscopy (EDS) using scanning electron microscopy (SEM) and transmission electron microscopy (TEM). It provides an overview of how EDS works, factors that influence resolution and detection limits, and tips for acquisition and analysis using EDS software. Examples are given of multipoint analysis, elemental mapping, and line scans to identify phases in a steel sample.
X-ray photoelectron spectroscopy (XPS) or Electron spectroscopy for chemical analysis (ESCA) is used to investigate the chemistry at the surface of the samples. The basic mechanism behind an XPS instrument is that the photons of a specific energy are used to excite the electronic states of atoms at and just below the surface of the sample.
There are several areas suited to measurement by XPS:
1. Elemental composition
2. Empirical formula determination
3. Chemical state
4. Electronic state
5. Binding energy
6. Layer thickness in the upper portion of surfaces
XPS has many advantages, such as it is is good for identifying all but two elements, identifying the chemical state on surfaces, and is good with quantitative analysis. XPS is capable of detecting the difference in the chemical state between samples. XPS is also able to differentiate between oxidations states of molecules.
XPS has also some limitations, for instance, samples for XPS must be compatible with the ultra high vacuum environment. XPS is limited to measurements of elements having atomic numbers of 3 or greater, making it unable to detect hydrogen or helium. XPS spectra also take a long time to obtain. The use of a monochromator can also reduce the time per experiment.
Energy dispersive x-ray diffraction (EDD) uses a fixed-angle detector to measure diffracted x-rays by energy rather than angle. This allows analysis of bulk samples without movement but with some resolution and overlap limitations. New pixelated detectors may help overcome these issues. Tomographic EDD can provide 3D imaging of density and composition within samples. The document discusses EDD applications and the author's related work developing computational techniques and an analysis program for EDD data collection and processing.
X-ray photoelectron spectroscopy (XPS) is a surface-sensitive technique that uses X-rays to eject core electrons from the surface of a sample. It can be used to identify the elements present in the sample and provide information about the chemical and electronic states of the elements. In XPS, X-rays eject core electrons, which are then analyzed based on their kinetic energy. This kinetic energy is related to the electron binding energy and can be used to identify the element and chemical environment. XPS requires ultra-high vacuum to avoid surface contamination and provide high-resolution spectra with sharp elemental peaks and broader Auger peaks.
Xps (x ray photoelectron spectroscopy)Zaahir Salam
The document provides an overview of X-ray photoelectron spectroscopy (XPS) technology. XPS works by irradiating a sample surface with x-rays and measuring the kinetic energy and number of electrons that escape from the top 1-10 nm of the material. This allows one to determine the sample's elemental composition and chemical/electronic states. Key aspects discussed include the use of ultra-high vacuum conditions to prevent surface contamination and allow for accurate analysis. Characteristic XPS spectra are produced that contain peaks corresponding to different elemental binding energies.
X-Ray photoelectron spectroscopy, XPS was used to investigate the chemistry at the surface of the samples. The basic mechanism behind an XPS instrument is that the photons of a specific energy are used to excite the electronic states of atoms at and just below the surface of the sample.
There are several areas suited to measurement by XPS:
1. Elemental composition
2. Empirical formula determination
3. Chemical state
4. Electronic state
5. Binding energy
6. Layer thickness in the upper portion of surfaces
XPS has many advantages, such as it is is good for identifying all but two elements, identifying the chemical state on surfaces, and is good with quantitative analysis. XPS is capable of detecting the difference in chemical state between samples. XPS is also able to differentiate between oxidations states of molecules.
XPS has also some limitations, for instance, samples for XPS must be compatible with the ultra high vacuum environment. XPS is limited to measurements of elements having atomic numbers of 3 or greater, making it unable to detect hydrogen or helium. XPS spectra also take a long time to obtain. The use of a monochromator can also reduce the time per experiment.
The document discusses the functions and working principles of an energy dispersive spectrometer (EDS). EDS can determine the chemical composition of materials down to the micron scale by detecting the characteristic x-rays emitted when the material is exposed to an electron beam. The EDS system includes an x-ray detector that converts x-ray energies into electrical signals and a multi-channel analyzer to separate the signals by energy into an elemental composition spectrum. Factors such as detector resolution, sample properties, and operating conditions can affect the accuracy of elemental quantification by EDS.
Scanning Electron Microscope- Energy - Dispersive X -Ray Microanalysis (Sem E...Nani Karnam Vinayakam
The document discusses scanning electron microscopy (SEM) and energy-dispersive X-ray spectroscopy (EDX or EDS) analysis. It provides details on:
- How an SEM works by scanning a sample with a focused electron beam and detecting signals from electron interactions with the sample.
- The components of an SEM including the electron gun, detectors for secondary electrons and backscattered electrons.
- How EDX analysis identifies elements by measuring the energy of X-rays emitted when electrons change energy levels.
- Parameters that affect EDX analysis such as count rate, accelerating voltage, and take-off angle.
EDS softwares INCA and EDAX_EM forum_Yina Guo_May 2016YinaGuo
The document discusses energy dispersive spectroscopy (EDS) using scanning electron microscopy (SEM) and transmission electron microscopy (TEM). It provides an overview of how EDS works, factors that influence resolution and detection limits, and tips for acquisition and analysis using EDS software. Examples are given of multipoint analysis, elemental mapping, and line scans to identify phases in a steel sample.
X-ray photoelectron spectroscopy (XPS) or Electron spectroscopy for chemical analysis (ESCA) is used to investigate the chemistry at the surface of the samples. The basic mechanism behind an XPS instrument is that the photons of a specific energy are used to excite the electronic states of atoms at and just below the surface of the sample.
There are several areas suited to measurement by XPS:
1. Elemental composition
2. Empirical formula determination
3. Chemical state
4. Electronic state
5. Binding energy
6. Layer thickness in the upper portion of surfaces
XPS has many advantages, such as it is is good for identifying all but two elements, identifying the chemical state on surfaces, and is good with quantitative analysis. XPS is capable of detecting the difference in the chemical state between samples. XPS is also able to differentiate between oxidations states of molecules.
XPS has also some limitations, for instance, samples for XPS must be compatible with the ultra high vacuum environment. XPS is limited to measurements of elements having atomic numbers of 3 or greater, making it unable to detect hydrogen or helium. XPS spectra also take a long time to obtain. The use of a monochromator can also reduce the time per experiment.
Energy dispersive x-ray diffraction (EDD) uses a fixed-angle detector to measure diffracted x-rays by energy rather than angle. This allows analysis of bulk samples without movement but with some resolution and overlap limitations. New pixelated detectors may help overcome these issues. Tomographic EDD can provide 3D imaging of density and composition within samples. The document discusses EDD applications and the author's related work developing computational techniques and an analysis program for EDD data collection and processing.
X-ray photoelectron spectroscopy (XPS) is a surface-sensitive technique that uses X-rays to eject core electrons from the surface of a sample. It can be used to identify the elements present in the sample and provide information about the chemical and electronic states of the elements. In XPS, X-rays eject core electrons, which are then analyzed based on their kinetic energy. This kinetic energy is related to the electron binding energy and can be used to identify the element and chemical environment. XPS requires ultra-high vacuum to avoid surface contamination and provide high-resolution spectra with sharp elemental peaks and broader Auger peaks.
Xps (x ray photoelectron spectroscopy)Zaahir Salam
The document provides an overview of X-ray photoelectron spectroscopy (XPS) technology. XPS works by irradiating a sample surface with x-rays and measuring the kinetic energy and number of electrons that escape from the top 1-10 nm of the material. This allows one to determine the sample's elemental composition and chemical/electronic states. Key aspects discussed include the use of ultra-high vacuum conditions to prevent surface contamination and allow for accurate analysis. Characteristic XPS spectra are produced that contain peaks corresponding to different elemental binding energies.
X-Ray photoelectron spectroscopy, XPS was used to investigate the chemistry at the surface of the samples. The basic mechanism behind an XPS instrument is that the photons of a specific energy are used to excite the electronic states of atoms at and just below the surface of the sample.
There are several areas suited to measurement by XPS:
1. Elemental composition
2. Empirical formula determination
3. Chemical state
4. Electronic state
5. Binding energy
6. Layer thickness in the upper portion of surfaces
XPS has many advantages, such as it is is good for identifying all but two elements, identifying the chemical state on surfaces, and is good with quantitative analysis. XPS is capable of detecting the difference in chemical state between samples. XPS is also able to differentiate between oxidations states of molecules.
XPS has also some limitations, for instance, samples for XPS must be compatible with the ultra high vacuum environment. XPS is limited to measurements of elements having atomic numbers of 3 or greater, making it unable to detect hydrogen or helium. XPS spectra also take a long time to obtain. The use of a monochromator can also reduce the time per experiment.
The document discusses the functions and working principles of an energy dispersive spectrometer (EDS). EDS can determine the chemical composition of materials down to the micron scale by detecting the characteristic x-rays emitted when the material is exposed to an electron beam. The EDS system includes an x-ray detector that converts x-ray energies into electrical signals and a multi-channel analyzer to separate the signals by energy into an elemental composition spectrum. Factors such as detector resolution, sample properties, and operating conditions can affect the accuracy of elemental quantification by EDS.
The document describes the capabilities of an X-ray photoelectron spectroscopy (XPS) instrument called the K-Alpha XPS from Thermo Scientific. The K-Alpha provides high throughput analysis with micrometer-scale spatial resolution. It features an aluminum anode X-ray source for high chemical state resolution and a focused ion beam for sample cleaning and depth profiling. The document outlines how XPS can be used to identify elements, quantify elemental composition, and determine chemical bonding states at surfaces.
X-ray photoelectron spectroscopy (XPS) is a surface-sensitive technique that uses X-rays to eject core electrons from the surface of a material. The kinetic energy of the ejected electrons is measured to identify the elemental composition of the outermost layers of the material. XPS is based on the photoelectric effect discovered by Einstein and was developed in the 1960s by Kai Siegbahn and his research group. It functions under ultra-high vacuum and allows identifying elements, chemical states, and empirical formulas of the top 1-10 nm of materials.
Auger Electron Spectroscopy (AES) uses a focused electron beam to eject inner shell electrons from the surface of a sample. The vacancies are filled by higher-energy electrons, emitting characteristic "Auger electrons" that can be analyzed to determine the elemental composition of the top few atomic layers. The key components of an AES system are an electron gun, electron energy analyzer, electron detector, and ultra-high vacuum environment. AES provides surface sensitivity, elemental analysis, and depth profiling capabilities. Limitations include inability to analyze non-conductive samples and lack of hydrogen/helium detection.
This document discusses X-ray photoelectron spectroscopy (XPS), a technique used to analyze the surface chemistry of materials. XPS uses X-rays to excite photoelectrons from the top 1-10 nm of a sample, and measures their kinetic energy to determine the elemental composition, empirical formula, chemical and electronic states. It works by relating the photoelectrons' binding energy to the energy of the exciting X-ray photons minus the kinetic energy and work function. XPS can identify all elements except hydrogen and helium, and is useful for quantifying elemental composition and chemical bonding at surfaces.
Auger electron spectroscopy is an analytical technique used to study surfaces. It works by bombarding a sample with an electron beam, which causes ionization and the ejection of core electrons from atoms in the sample. As higher-energy electrons drop to fill these vacancies, their energy can be transferred to a secondary electron that is then ejected from the atom. This ejected electron is called an Auger electron. The instrument used in AES consists of an electron gun, sample, electron energy analyzer, electron detector, and output device to analyze and display the spectra of emitted Auger electrons.
Surface modification can be used to alter
or improve these characteristics, and so
surface analysis is used to understand
surface chemistry of material, and
investigate the efficacy of surface
engineering. From non-stick cookware
coatings to thin-film electronics and bioactive
surfaces, X-ray photoelectron
spectroscopy is one of the standard
tools for surface characterization.
Auger electron spectroscopy (AES) is an analytical technique used to analyze the surface chemistry of materials. It works by (1) removing a core electron from the sample using a high-energy electron beam, (2) causing an electron to fill the resulting vacancy and emit an Auger electron, and (3) analyzing the kinetic energy of the emitted Auger electrons to determine the elemental composition of the top 1-10 nanometers of the sample surface. AES can also be used to create depth profiles by combining it with argon ion sputtering to sequentially remove layers from the surface. Typical applications of AES include analyzing thin film layers, surface oxides, and corrosion processes.
The document provides an overview of the transmission electron microscope (TEM). It discusses key components of the TEM including the electron gun, condenser lenses, objective lens, and vacuum system. The document explains that TEM uses electromagnetic lenses to focus a beam of electrons onto a thin specimen, and forms an image from the interaction of electrons transmitted through the specimen. TEM allows higher magnification and resolution than light microscopes, and can be used to investigate the morphology, structure, and composition of materials down to the atomic scale.
XPS can be used to characterize polymers at the surface. It provides both elemental and chemical information about the top 10 nm of a sample. Elemental identification and quantification is possible from survey spectra. High resolution region spectra can identify functional groups and chemical environments through chemical shifts. XPS can map the distribution of elements and chemical states across a sample surface. Depth profiling with cluster ion beams maintains chemical information during sputtering and allows buried layers and interfaces to be analyzed. XPS was used to characterize a fluoropolymer coating on PET and PTFE, identifying the chemical structure and confirming it matched the expected structure from the plasma deposition process.
Dr. S. H. Burungale's document discusses scanning electron microscopy. It notes that Ernst Ruska won the Nobel Prize in Physics in 1986 for his work developing the first electron microscope. The document compares light microscopes and electron microscopes, noting that electron microscopes have much higher magnifications and resolving power but are more expensive. It explains that electron microscopes work by generating a beam of electrons that is accelerated, focused by electromagnetic lenses, and scanned across a specimen, with secondary electrons from the specimen detected to form an image.
This document provides an overview of electron spectroscopy techniques, including X-ray photoelectron spectroscopy (XPS), Auger electron spectroscopy (AES), and ultraviolet photoelectron spectroscopy (UPS). It discusses the basic principles, instrumentation, applications, and advantages/limitations of each technique. XPS is described as using X-rays to eject core electrons and measure their kinetic energy to determine elemental composition. AES uses electrons to eject core electrons which cause additional electrons to fall into the vacancy, emitting energy measured to identify elements. UPS uses UV light to eject valence electrons and measure their kinetic energy to determine molecular orbital energies.
Identifying elements by the peaks in auger electron spectroscopyAwais72700
This document discusses the process of identifying elements in an Auger electron spectroscopy analysis. It begins by defining Auger electron spectroscopy as a technique that uses an electron beam to excite a sample's surface and emit Auger electrons, which are then analyzed by an electron energy analyzer to determine the elemental composition of the top few atomic layers. It then outlines the standard equipment used, importance of sample preparation, and qualitative analysis procedure to identify peaks by comparing their energies and shapes to known elemental spectra. The procedure involves methodically matching peaks of decreasing intensity to identify all elements present.
X-RAY PHOTOELECTRON SPECTROSCOPY AND ELECTRON SPIN RESONANCEKishan Kasundra
INTRODUCTION OF XPS
MECHANISM OF XPS
CHEMICAL SHIFT IN XPS
STRENGTHS AND LIMITATIONS OF XPS
INTRODUCTION OF ESR
MECHANISM OF ESR
PRESENTATION OF ESR SPECTRUM
APPLICATION OF ESR
ADVANTAGES AND DISADVANTAGES OF ESR
Instrumentation presentation - Auger Electron Spectroscopy (AES)Amirah Basir
Group 5-AES
Normaizatul Hanissa Binti Hamdan
Amirah Binti Basir
-Introduction/Backgroud /History, fundamental/basic principle and
elaboration of the principle, related pictures, related
equations/expressions/derivations, components and it functions,
related models/brands, technologies and applications
The document discusses the Auger process and Auger electron spectroscopy (AES) technique. It explains that the Auger process involves ejection of an inner shell electron by an incoming electron, followed by relaxation through emission of an Auger electron. AES can be used to identify elements on a sample surface through measurement of the kinetic energies of emitted Auger electrons. It also allows for elemental mapping, depth profiling, and quantification of elemental composition.
X ray photoelectron spectroscopy (xps) iit kgpak21121991
The document provides an overview of X-ray photoelectron spectroscopy (XPS) and its applications in analyzing semiconductor devices and materials. It discusses how XPS can be used to determine elemental composition, chemical state and electronic state. Examples are given of how XPS has been used to analyze metal-insulator-semiconductor contacts, high-k dielectric films, titanium dioxide structures, molybdenum disulfide, aluminum oxide thin films and nickel silicide. Both XPS and ultraviolet photoelectron spectroscopy are discussed. In summary, the document outlines the capabilities of XPS and gives several examples of its use in characterizing semiconductor materials and devices.
Electron Energy Loss Spectroscopy (EELS) involves analyzing the energy distribution of electrons that have undergone inelastic scattering in a transmission electron microscope. The technique provides information about a sample's composition, bonding properties, and local structure from features in the EELS spectrum including peaks corresponding to ionization edges that identify elements and fine structures related to bonding and coordination. However, EELS has limitations in usable sample thickness, especially for heavier elements where thickness must be less than 20 nm.
Auger electron spectroscopy (AES) is an analytical technique used to determine the composition of surface layers of a sample. It involves three steps: (1) removing a core electron from an atom via ionization, typically using a 2-10 keV electron beam; (2) an electron dropping to fill the vacancy, releasing energy; (3) this energy causes the emission of an Auger electron. AES collects these low-energy (20-2000 eV) Auger electrons that escape from within 50 angstroms of the surface, allowing it to provide compositional information about just the sample's surface.
This document discusses Silicon Drift Detectors (SDD) for use in synchrotron energy dispersive X-ray fluorescence (EDXRF) spectroscopy. It begins with an introduction to SDDs, explaining their structure and operating principle. It then describes the features and high performance of SDDs, including high count rates up to 500,000 counts per second and excellent energy resolution of 125 eV FWHM at 5.9 keV. Applications of SDDs in EDXRF spectroscopy and portable XRF devices are also mentioned. In the concluding remarks, the key advantages of SDDs are summarized as having lower capacitance than conventional silicon detectors, allowing better energy resolution at higher count rates.
The Thermo Scientific NextGuard x-ray detection system provides cost-effective and sensitive detection of foreign objects in packaged food products. It uses a unique non-linear x-ray detector design that eliminates inspection blind spots and ensures 100% detection for any product size or shape. The system offers options for customization, easy maintenance, and is designed for use in compliance with worldwide food safety standards.
The document describes the capabilities of an X-ray photoelectron spectroscopy (XPS) instrument called the K-Alpha XPS from Thermo Scientific. The K-Alpha provides high throughput analysis with micrometer-scale spatial resolution. It features an aluminum anode X-ray source for high chemical state resolution and a focused ion beam for sample cleaning and depth profiling. The document outlines how XPS can be used to identify elements, quantify elemental composition, and determine chemical bonding states at surfaces.
X-ray photoelectron spectroscopy (XPS) is a surface-sensitive technique that uses X-rays to eject core electrons from the surface of a material. The kinetic energy of the ejected electrons is measured to identify the elemental composition of the outermost layers of the material. XPS is based on the photoelectric effect discovered by Einstein and was developed in the 1960s by Kai Siegbahn and his research group. It functions under ultra-high vacuum and allows identifying elements, chemical states, and empirical formulas of the top 1-10 nm of materials.
Auger Electron Spectroscopy (AES) uses a focused electron beam to eject inner shell electrons from the surface of a sample. The vacancies are filled by higher-energy electrons, emitting characteristic "Auger electrons" that can be analyzed to determine the elemental composition of the top few atomic layers. The key components of an AES system are an electron gun, electron energy analyzer, electron detector, and ultra-high vacuum environment. AES provides surface sensitivity, elemental analysis, and depth profiling capabilities. Limitations include inability to analyze non-conductive samples and lack of hydrogen/helium detection.
This document discusses X-ray photoelectron spectroscopy (XPS), a technique used to analyze the surface chemistry of materials. XPS uses X-rays to excite photoelectrons from the top 1-10 nm of a sample, and measures their kinetic energy to determine the elemental composition, empirical formula, chemical and electronic states. It works by relating the photoelectrons' binding energy to the energy of the exciting X-ray photons minus the kinetic energy and work function. XPS can identify all elements except hydrogen and helium, and is useful for quantifying elemental composition and chemical bonding at surfaces.
Auger electron spectroscopy is an analytical technique used to study surfaces. It works by bombarding a sample with an electron beam, which causes ionization and the ejection of core electrons from atoms in the sample. As higher-energy electrons drop to fill these vacancies, their energy can be transferred to a secondary electron that is then ejected from the atom. This ejected electron is called an Auger electron. The instrument used in AES consists of an electron gun, sample, electron energy analyzer, electron detector, and output device to analyze and display the spectra of emitted Auger electrons.
Surface modification can be used to alter
or improve these characteristics, and so
surface analysis is used to understand
surface chemistry of material, and
investigate the efficacy of surface
engineering. From non-stick cookware
coatings to thin-film electronics and bioactive
surfaces, X-ray photoelectron
spectroscopy is one of the standard
tools for surface characterization.
Auger electron spectroscopy (AES) is an analytical technique used to analyze the surface chemistry of materials. It works by (1) removing a core electron from the sample using a high-energy electron beam, (2) causing an electron to fill the resulting vacancy and emit an Auger electron, and (3) analyzing the kinetic energy of the emitted Auger electrons to determine the elemental composition of the top 1-10 nanometers of the sample surface. AES can also be used to create depth profiles by combining it with argon ion sputtering to sequentially remove layers from the surface. Typical applications of AES include analyzing thin film layers, surface oxides, and corrosion processes.
The document provides an overview of the transmission electron microscope (TEM). It discusses key components of the TEM including the electron gun, condenser lenses, objective lens, and vacuum system. The document explains that TEM uses electromagnetic lenses to focus a beam of electrons onto a thin specimen, and forms an image from the interaction of electrons transmitted through the specimen. TEM allows higher magnification and resolution than light microscopes, and can be used to investigate the morphology, structure, and composition of materials down to the atomic scale.
XPS can be used to characterize polymers at the surface. It provides both elemental and chemical information about the top 10 nm of a sample. Elemental identification and quantification is possible from survey spectra. High resolution region spectra can identify functional groups and chemical environments through chemical shifts. XPS can map the distribution of elements and chemical states across a sample surface. Depth profiling with cluster ion beams maintains chemical information during sputtering and allows buried layers and interfaces to be analyzed. XPS was used to characterize a fluoropolymer coating on PET and PTFE, identifying the chemical structure and confirming it matched the expected structure from the plasma deposition process.
Dr. S. H. Burungale's document discusses scanning electron microscopy. It notes that Ernst Ruska won the Nobel Prize in Physics in 1986 for his work developing the first electron microscope. The document compares light microscopes and electron microscopes, noting that electron microscopes have much higher magnifications and resolving power but are more expensive. It explains that electron microscopes work by generating a beam of electrons that is accelerated, focused by electromagnetic lenses, and scanned across a specimen, with secondary electrons from the specimen detected to form an image.
This document provides an overview of electron spectroscopy techniques, including X-ray photoelectron spectroscopy (XPS), Auger electron spectroscopy (AES), and ultraviolet photoelectron spectroscopy (UPS). It discusses the basic principles, instrumentation, applications, and advantages/limitations of each technique. XPS is described as using X-rays to eject core electrons and measure their kinetic energy to determine elemental composition. AES uses electrons to eject core electrons which cause additional electrons to fall into the vacancy, emitting energy measured to identify elements. UPS uses UV light to eject valence electrons and measure their kinetic energy to determine molecular orbital energies.
Identifying elements by the peaks in auger electron spectroscopyAwais72700
This document discusses the process of identifying elements in an Auger electron spectroscopy analysis. It begins by defining Auger electron spectroscopy as a technique that uses an electron beam to excite a sample's surface and emit Auger electrons, which are then analyzed by an electron energy analyzer to determine the elemental composition of the top few atomic layers. It then outlines the standard equipment used, importance of sample preparation, and qualitative analysis procedure to identify peaks by comparing their energies and shapes to known elemental spectra. The procedure involves methodically matching peaks of decreasing intensity to identify all elements present.
X-RAY PHOTOELECTRON SPECTROSCOPY AND ELECTRON SPIN RESONANCEKishan Kasundra
INTRODUCTION OF XPS
MECHANISM OF XPS
CHEMICAL SHIFT IN XPS
STRENGTHS AND LIMITATIONS OF XPS
INTRODUCTION OF ESR
MECHANISM OF ESR
PRESENTATION OF ESR SPECTRUM
APPLICATION OF ESR
ADVANTAGES AND DISADVANTAGES OF ESR
Instrumentation presentation - Auger Electron Spectroscopy (AES)Amirah Basir
Group 5-AES
Normaizatul Hanissa Binti Hamdan
Amirah Binti Basir
-Introduction/Backgroud /History, fundamental/basic principle and
elaboration of the principle, related pictures, related
equations/expressions/derivations, components and it functions,
related models/brands, technologies and applications
The document discusses the Auger process and Auger electron spectroscopy (AES) technique. It explains that the Auger process involves ejection of an inner shell electron by an incoming electron, followed by relaxation through emission of an Auger electron. AES can be used to identify elements on a sample surface through measurement of the kinetic energies of emitted Auger electrons. It also allows for elemental mapping, depth profiling, and quantification of elemental composition.
X ray photoelectron spectroscopy (xps) iit kgpak21121991
The document provides an overview of X-ray photoelectron spectroscopy (XPS) and its applications in analyzing semiconductor devices and materials. It discusses how XPS can be used to determine elemental composition, chemical state and electronic state. Examples are given of how XPS has been used to analyze metal-insulator-semiconductor contacts, high-k dielectric films, titanium dioxide structures, molybdenum disulfide, aluminum oxide thin films and nickel silicide. Both XPS and ultraviolet photoelectron spectroscopy are discussed. In summary, the document outlines the capabilities of XPS and gives several examples of its use in characterizing semiconductor materials and devices.
Electron Energy Loss Spectroscopy (EELS) involves analyzing the energy distribution of electrons that have undergone inelastic scattering in a transmission electron microscope. The technique provides information about a sample's composition, bonding properties, and local structure from features in the EELS spectrum including peaks corresponding to ionization edges that identify elements and fine structures related to bonding and coordination. However, EELS has limitations in usable sample thickness, especially for heavier elements where thickness must be less than 20 nm.
Auger electron spectroscopy (AES) is an analytical technique used to determine the composition of surface layers of a sample. It involves three steps: (1) removing a core electron from an atom via ionization, typically using a 2-10 keV electron beam; (2) an electron dropping to fill the vacancy, releasing energy; (3) this energy causes the emission of an Auger electron. AES collects these low-energy (20-2000 eV) Auger electrons that escape from within 50 angstroms of the surface, allowing it to provide compositional information about just the sample's surface.
This document discusses Silicon Drift Detectors (SDD) for use in synchrotron energy dispersive X-ray fluorescence (EDXRF) spectroscopy. It begins with an introduction to SDDs, explaining their structure and operating principle. It then describes the features and high performance of SDDs, including high count rates up to 500,000 counts per second and excellent energy resolution of 125 eV FWHM at 5.9 keV. Applications of SDDs in EDXRF spectroscopy and portable XRF devices are also mentioned. In the concluding remarks, the key advantages of SDDs are summarized as having lower capacitance than conventional silicon detectors, allowing better energy resolution at higher count rates.
The Thermo Scientific NextGuard x-ray detection system provides cost-effective and sensitive detection of foreign objects in packaged food products. It uses a unique non-linear x-ray detector design that eliminates inspection blind spots and ensures 100% detection for any product size or shape. The system offers options for customization, easy maintenance, and is designed for use in compliance with worldwide food safety standards.
1. The document discusses two types of wavelength dispersive spectrometers (WDS): Rowland circle WDS and parallel beam WDS.
2. Rowland circle WDS uses curved diffractors to focus diffracted x-rays, but suffers from low intensities for low energy x-rays when used on SEMs.
3. Parallel beam WDS uses a collimating optic near the sample and flat diffractors, providing excellent intensities across all energies without complicated geometry.
Silicon Drift Detectors for Energy Dispersive X- Ray Fluorescence ( SDDEXRF)Saleh Qutaishat
This document discusses Silicon Drift Detectors (SDD) for use in synchrotron energy dispersive X-ray fluorescence (EDXRF) spectroscopy. It begins with an introduction to SDDs, explaining their structure and operating principle. It then describes the features and high performance of SDDs, including their high count rate, good energy resolution, and large active area. The document presents spectra from an Fe55 source taken with an SDD and includes diagrams of detector modules, cooling systems, and integration with spectroscopy systems. It concludes by emphasizing the key advantages of SDDs for spectroscopy applications like their lower noise and ability to operate at higher count rates than conventional semiconductor detectors.
Energy-Dispersive X-Ray Spectroscopy Procedure for Analysing Cellular Element...iosrjce
Four phototrophic bacterial species Blastochloris sulfoviridis, Rhodocista pekingensis,
Rhodopseudomonas palustris and Rhodomicrobium vannielii, isolated from hot springs were analysed for
cellular elemental affinity between them and to determine possible relationship between physiological features
and the constituent elements. A novel methodology using Energy-dispersive X-ray spectroscopy (EDS/EDX) of
pigments produced by the bacteria was adopted and applied. Results did show close affinity of cellular elements
with little or no difference in weighted and atomic percentages of the constituent elements. There was also little
or no inference in the effects of these elements on the pigments and other features of the bacteria such as colour
and morphological differences could not be fully attributed to the elemental inclusions. It was concluded that
systemic factors that were responsible for extraneous features such as pigmentation, pigment density etc, could
be a combination of elemental inclusion variations, genetics and other factors in-between rather than one.
Required energy sources and metabolic factors were assumed to play key roles in contents and types of cellular
elements in relation to pigmentation.
This document discusses X-ray fluorescence (XRF), a technique used to analyze the chemical composition of materials. XRF works by exciting a sample with an X-ray source, which causes fluorescent X-rays to be emitted from the sample that are characteristic of its elemental composition. The document covers the basic principles of XRF, how it is used to generate spectra to analyze samples, common instrumentation including X-ray sources and detectors, sample preparation methods, applications in fields like mining and environmental analysis, and limitations of the technique.
This document provides an overview of X-ray fluorescence (XRF) spectroscopy. It discusses XRF theory, instrumentation, hardware, and applications. XRF uses X-rays to excite a sample, and a detector then measures the fluorescent X-rays emitted from the sample that are characteristic of its elemental composition. The document compares wavelength dispersive XRF and energy dispersive XRF, and describes the components of XRF systems including X-ray sources, detectors, filters, and electronics. It provides examples of XRF applications in qualitative and quantitative elemental analysis across various industries.
XRF & XRD analysis techniques are used to analyze materials. X-rays were discovered in 1895 by Wilhelm Conrad Roentgen. Over time, scientists developed an understanding of X-ray diffraction and how to use it for crystallography. By the mid-20th century, powder diffractometry techniques and databases had been established. X-rays are electromagnetic waves or photon beams with wavelengths between 0.01 to 10 nm, corresponding to energies from 0.125 to 125 keV. They can be hazardous due to their ionizing properties, requiring safety precautions as they are invisible, travel in straight lines at the speed of light, and can cause serious injury.
The document discusses X-ray fluorescence (XRF) theory and applications. XRF involves bombarding a sample with X-rays, which causes fluorescent X-rays to be emitted from the sample that are characteristic of its elemental composition. This allows for both qualitative and quantitative elemental analysis. Key advantages of XRF include rapid, nondestructive analysis of major and trace elements in various materials. Common applications include analysis of soils, minerals, metals, and more in fields like geology, archaeology, and environmental analysis.
Study of AC Power Loss of High Frequency Gapped InductorsYoussef Kandeel
This document discusses a study of AC power loss in high frequency gapped inductors. It begins with an introduction discussing the importance of reducing size in power electronics and the role of inductors in DC-DC converters. It then provides an overview of recent approaches to calculating AC power loss such as the Steinmetz Equation and its modifications. The objective of the thesis is to improve correlation between calculated and measured AC power loss of inductors operating at high frequencies. It will validate the accuracy of recent AC power loss prediction methods and propose improvements.
This document summarizes research being conducted by the Army Research Office on nanoscience and quantum information science. It discusses several applications of nanoscience including electronic and photonic band engineering, chemical and biological agent detection, and technologies to benefit soldiers such as lightweight armor and power sources. It also outlines research on quantum information science, including quantum communication techniques like quantum cryptography and quantum teleportation that could provide unbreakable secure communication, as well as the potential for quantum computing to solve certain problems much faster than classical computers.
Fiber Optic Sensors, Fiber Optical Temperature Sensor - Rugged Monitoringrugged_monitoring
Check what is Fiber Optic Sensor? The sensor which uses optical fiber as sensing device. Rugged Monitoring have top fiber optic temperature sensors team on monitors, Software accessories, E-mobility, medical, energy, RF/Microwave, research labs etc.
Check what is Fiber Optic Sensor? The sensor which uses optical fiber as sensing device. Rugged Monitoring have top fiber optic temperature sensors team on monitors, Software accessories, E-mobility, medical, energy, RF/Microwave, research labs etc
Before LEDs, if we measured illuminance with a quality lux meter that was in good condition and calibrated, there was a high level of confidence that the reading it gave was an accurate representation of what you saw with your eye. However the introduction of phosphor based LED lighting has brought that into question due to their strong blue light component. This presentation will look at some of the recommendations given when measuring LED light, such as applying a SP ratio and reflect on its effectiveness. It will also detail a method for simulating the illuminance reading that a lux meter will give and use it to compare and contrast the performance of a variety of lux meters under different lighting conditions, including LED light.
Talk by Ivan Perre, London Underground
- Lux meters are calibrated to measure incandescent light accurately but may not accurately measure LED and other light sources due to spectral differences.
- Good quality lux meters that have consistent spectral response curves can measure LED light with a correction factor, while cheap meters have inconsistent responses.
- To assess the accuracy of a lux meter for LED measurement, check the spectral response curve against the CIE curve and consider doing test measurements with known light sources. Looking at the manufacturer's spectral response data sheet is also recommended.
Inductive Non-Contact Position/Displacement Sensing: Technology-Application-O...Design World
Dan Spohn from Kaman Precision Products presented on inductive non-contact position sensing technology. He discussed the basic operating principles of linear inductive sensors using electromagnetic fields. Key application concerns like target material, size, environment, range, and speed were covered. Common error sources and standard sensor options like cable length, oscillator frequency, and temperature compensation were also summarized. Example applications demonstrated how inductive sensors can be customized for applications like engraving heads, ammunition primers, and projectile velocity measurements.
Liquid Sensing: Visible light absorption spectroscopy and colorimetry are two fundamental tools used in chemical analysis. Most of these light-based systems use photodiodes as the light sensor, and require similar high input impedance signal chains. This session examines the different components of a photodiode amplifier signal chain, including a programmable gain transimpedance amplifier, a hardware lock-in amplifier, and a Σ-Δ ADC that can measure a sample and reference channel to greatly reduce any measurement error due to variations in intensity of the light source.
Gas Sensing: Many industrial processes involve toxic compounds, and it is important to know when dangerous concentrations exist. Electrochemical sensors offer several advantages for instruments that detect or measure the concentration of toxic gases. This session will describe a portable toxic gas detector using an electrochemical sensor. The system presented here includes a potentiostat circuit to drive the sensor, as well as a transimpedance amplifier to take the very small output current from the sensor and translate it to a voltage that can take advantage of the full-scale input of an ADC.
The document describes an experiment to study how the current flowing through a light dependent resistor (LDR) varies with changes in the power and distance of an incandescent light source. The LDR's resistance decreases when exposed to light, increasing the current. The experiment found that the current increased as the light source's power increased or its distance from the LDR decreased. Common applications of LDRs include camera light meters, photocopying machines, and automatic lighting controls.
UV-visible detectors are commonly used to detect and quantify organic compounds in HPLC. They work by exciting electrons in sample molecules using light from a lamp, with different compounds absorbing different wavelengths. Key factors that affect detector performance include optics design, lamp type and intensity, flow cell design, slit width, data collection rate, time constant, and use of a reference signal to reduce noise. Optimizing these parameters can improve sensitivity, robustness, and quantitation.
compiter radiography and digital radiography Unaiz Musthafa
This document discusses computed radiography (CR) and digital radiography (DR). CR uses reusable imaging plates instead of film, which are read by a laser scanner. DR uses a digital detector incorporated into x-ray equipment to provide direct digital output. Both have greater exposure latitude than screen-film and allow computer post-processing to enhance images. Technologists must monitor exposure indices to avoid overexposure with CR and DR systems. The document also covers digital fluoroscopy techniques like frame averaging.
Let’s think for a moment:
What are the methods available to test an LED ?
How can board topologies affect the test coverage for LED?
Can these be done at the ICT – REALLY?
This presentation is by John Coonrod from the Advanced Circuit Materials Division at Rogers Corporation. It addresses how to determine the dielectric constant (Dk) in circuit materials for printed circuit boards and electronics.
LED TECHNOLOGY FOR WONDERING FUTURE(PPT)Rahul Kumar
LED technology has advanced significantly. LEDs are now commonly used for lighting applications due to their energy efficiency and long lifespan. LEDs operate by passing electricity through crystalline solids unlike conventional lighting methods. Early LEDs could only produce red light but advances in materials allow different colors to be produced. White LEDs use a blue LED combined with yellow phosphor. Manufacturing LEDs is a complex process involving growing semiconductor wafers, dicing dies, packaging, and testing. Proper heat management is important for LED lifespan and performance. LEDs have many applications from indoor lighting to automotive due to their controllability and flexibility. Further advances may allow multi-color chips and integrated circuits on LEDs.
Introduction to applying X-Ray imaging techniques to industrial machine vision applications. This presentation was given at the "Vision Show" in 2009 in Phoenix, AZ. It provides as overview of possible sensors to convert X-Rays into photons for imaging.
1) The document discusses various types of neutron detectors, their detection principles, energy response characteristics, and challenges in accurately measuring neutron dose equivalent rates. It focuses on REM balls but also covers other technologies like TEPC, mixed gas detectors, and CLYC.
2) Key points covered include how detector response varies with neutron energy spectrum, factors of over or under response depending on energy, and importance of characterizing the neutron field energy spectrum. It also highlights challenges in accounting for directionality and mixed gamma/neutron exposures.
3) Newer portable neutron detectors like mixed gas, Domino, and CLYC provide alternatives to REM balls and aim to improve gamma rejection, energy response, and form factor for radiological
Infrared Technology - Seeing the Invisible (Part Two: Camera Technology)Allied Vision
Through specific applications examples with sample images, this presentation introduces you to the basics of infrared (IR) imaging technology. You will learn that in the IR-world things look different and that you can visualize with an IR camera things which you cannot see with your own eyes. To understand “the why”, we touch on some basics about IR radiation and corresponding imaging sensor technologies.
This document discusses electromagnetic positioning sensors and their design factors. It describes how electromagnetic positioning works using principles from Maxwell's equations and how factors like frequency, range, radiation pattern, and positioning methods are important in the design of these sensors. It also covers advantages and challenges of electromagnetic positioning as well as relevant legislation.
Similar to Choosing the right EDS detector - Thermo Scientific (20)
The technology uses reclaimed CO₂ as the dyeing medium in a closed loop process. When pressurized, CO₂ becomes supercritical (SC-CO₂). In this state CO₂ has a very high solvent power, allowing the dye to dissolve easily.
EWOCS-I: The catalog of X-ray sources in Westerlund 1 from the Extended Weste...Sérgio Sacani
Context. With a mass exceeding several 104 M⊙ and a rich and dense population of massive stars, supermassive young star clusters
represent the most massive star-forming environment that is dominated by the feedback from massive stars and gravitational interactions
among stars.
Aims. In this paper we present the Extended Westerlund 1 and 2 Open Clusters Survey (EWOCS) project, which aims to investigate
the influence of the starburst environment on the formation of stars and planets, and on the evolution of both low and high mass stars.
The primary targets of this project are Westerlund 1 and 2, the closest supermassive star clusters to the Sun.
Methods. The project is based primarily on recent observations conducted with the Chandra and JWST observatories. Specifically,
the Chandra survey of Westerlund 1 consists of 36 new ACIS-I observations, nearly co-pointed, for a total exposure time of 1 Msec.
Additionally, we included 8 archival Chandra/ACIS-S observations. This paper presents the resulting catalog of X-ray sources within
and around Westerlund 1. Sources were detected by combining various existing methods, and photon extraction and source validation
were carried out using the ACIS-Extract software.
Results. The EWOCS X-ray catalog comprises 5963 validated sources out of the 9420 initially provided to ACIS-Extract, reaching a
photon flux threshold of approximately 2 × 10−8 photons cm−2
s
−1
. The X-ray sources exhibit a highly concentrated spatial distribution,
with 1075 sources located within the central 1 arcmin. We have successfully detected X-ray emissions from 126 out of the 166 known
massive stars of the cluster, and we have collected over 71 000 photons from the magnetar CXO J164710.20-455217.
Sexuality - Issues, Attitude and Behaviour - Applied Social Psychology - Psyc...PsychoTech Services
A proprietary approach developed by bringing together the best of learning theories from Psychology, design principles from the world of visualization, and pedagogical methods from over a decade of training experience, that enables you to: Learn better, faster!
(June 12, 2024) Webinar: Development of PET theranostics targeting the molecu...Scintica Instrumentation
Targeting Hsp90 and its pathogen Orthologs with Tethered Inhibitors as a Diagnostic and Therapeutic Strategy for cancer and infectious diseases with Dr. Timothy Haystead.
Authoring a personal GPT for your research and practice: How we created the Q...Leonel Morgado
Thematic analysis in qualitative research is a time-consuming and systematic task, typically done using teams. Team members must ground their activities on common understandings of the major concepts underlying the thematic analysis, and define criteria for its development. However, conceptual misunderstandings, equivocations, and lack of adherence to criteria are challenges to the quality and speed of this process. Given the distributed and uncertain nature of this process, we wondered if the tasks in thematic analysis could be supported by readily available artificial intelligence chatbots. Our early efforts point to potential benefits: not just saving time in the coding process but better adherence to criteria and grounding, by increasing triangulation between humans and artificial intelligence. This tutorial will provide a description and demonstration of the process we followed, as two academic researchers, to develop a custom ChatGPT to assist with qualitative coding in the thematic data analysis process of immersive learning accounts in a survey of the academic literature: QUAL-E Immersive Learning Thematic Analysis Helper. In the hands-on time, participants will try out QUAL-E and develop their ideas for their own qualitative coding ChatGPT. Participants that have the paid ChatGPT Plus subscription can create a draft of their assistants. The organizers will provide course materials and slide deck that participants will be able to utilize to continue development of their custom GPT. The paid subscription to ChatGPT Plus is not required to participate in this workshop, just for trying out personal GPTs during it.
Describing and Interpreting an Immersive Learning Case with the Immersion Cub...Leonel Morgado
Current descriptions of immersive learning cases are often difficult or impossible to compare. This is due to a myriad of different options on what details to include, which aspects are relevant, and on the descriptive approaches employed. Also, these aspects often combine very specific details with more general guidelines or indicate intents and rationales without clarifying their implementation. In this paper we provide a method to describe immersive learning cases that is structured to enable comparisons, yet flexible enough to allow researchers and practitioners to decide which aspects to include. This method leverages a taxonomy that classifies educational aspects at three levels (uses, practices, and strategies) and then utilizes two frameworks, the Immersive Learning Brain and the Immersion Cube, to enable a structured description and interpretation of immersive learning cases. The method is then demonstrated on a published immersive learning case on training for wind turbine maintenance using virtual reality. Applying the method results in a structured artifact, the Immersive Learning Case Sheet, that tags the case with its proximal uses, practices, and strategies, and refines the free text case description to ensure that matching details are included. This contribution is thus a case description method in support of future comparative research of immersive learning cases. We then discuss how the resulting description and interpretation can be leveraged to change immersion learning cases, by enriching them (considering low-effort changes or additions) or innovating (exploring more challenging avenues of transformation). The method holds significant promise to support better-grounded research in immersive learning.
ESR spectroscopy in liquid food and beverages.pptxPRIYANKA PATEL
With increasing population, people need to rely on packaged food stuffs. Packaging of food materials requires the preservation of food. There are various methods for the treatment of food to preserve them and irradiation treatment of food is one of them. It is the most common and the most harmless method for the food preservation as it does not alter the necessary micronutrients of food materials. Although irradiated food doesn’t cause any harm to the human health but still the quality assessment of food is required to provide consumers with necessary information about the food. ESR spectroscopy is the most sophisticated way to investigate the quality of the food and the free radicals induced during the processing of the food. ESR spin trapping technique is useful for the detection of highly unstable radicals in the food. The antioxidant capability of liquid food and beverages in mainly performed by spin trapping technique.
PPT on Direct Seeded Rice presented at the three-day 'Training and Validation Workshop on Modules of Climate Smart Agriculture (CSA) Technologies in South Asia' workshop on April 22, 2024.
Mending Clothing to Support Sustainable Fashion_CIMaR 2024.pdfSelcen Ozturkcan
Ozturkcan, S., Berndt, A., & Angelakis, A. (2024). Mending clothing to support sustainable fashion. Presented at the 31st Annual Conference by the Consortium for International Marketing Research (CIMaR), 10-13 Jun 2024, University of Gävle, Sweden.
The binding of cosmological structures by massless topological defectsSérgio Sacani
Assuming spherical symmetry and weak field, it is shown that if one solves the Poisson equation or the Einstein field
equations sourced by a topological defect, i.e. a singularity of a very specific form, the result is a localized gravitational
field capable of driving flat rotation (i.e. Keplerian circular orbits at a constant speed for all radii) of test masses on a thin
spherical shell without any underlying mass. Moreover, a large-scale structure which exploits this solution by assembling
concentrically a number of such topological defects can establish a flat stellar or galactic rotation curve, and can also deflect
light in the same manner as an equipotential (isothermal) sphere. Thus, the need for dark matter or modified gravity theory is
mitigated, at least in part.
2. 2 Proprietary & Confidential
EDS and SEM go hand-in-hand
Electron Microscopy provides the imaging
EDS provides the “chemistry”
3. 3 Proprietary & Confidential
EDS provides a look at material composition
Point & Shoot, Line Scan and Mapping
4. 4 Proprietary & Confidential
Electron Microscopes
• Material Science
• Electronics
• Petrochemical
• Mining
• Metals
• Semiconductor
• Life Science
Many options for
electron microscopes
Many options for EDS
5. 5 Proprietary & Confidential
EDS detector advances
Larger active areas
Various tube size… even oval tubes
Faster Acquisitions
6. 6 Proprietary & Confidential
• There are 3 main drivers in specifying an EDS
detector
• Energy resolution @ Mn k-alpha
• Sensitive to
• Solid angle
• How relevant are these specifications in determining
the performance of an EDS detector?
• How do I choose the right detector for my lab?
8. 8 Proprietary & Confidential
Energy resolution
Measured:
Width of the Mn k-alpha peak @
half the peak height
- Why does this spread occur?
- What is good enough?
- Is this a valuable metric?
9. 9 Proprietary & Confidential
How x-ray detection works:
X-rays generate a small current of e- – hole pairs
Next stage: charge-sensitive pre-amplifier stage
Next stage: Pulse processor measures the amplitude
10. 10 Proprietary & Confidential
Signal
Time
Function of Silicon Drift Detector
Charge
Collection:
Event 1 signal 1
Event 2 signal 2
Event 3 signal 3
1
2
3
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0
5
10
15
20
25
30
35
0 100 200 300 400
Voltage
Time
0
0.2
0.4
0.6
0.8
1
1.2
50 60 70 80 90 100 110 120 130 140 150
Energy (keV)
Counts
Peaking time
X-ray induced
voltagestep
Every system has noise. This noise drives energy resolution
12. 12 Proprietary & Confidential
Sources of uncertainty: Noise
• Internal or “system”
• Inherent in the system: SDD module, wire bonding, cabling, electronics and
other overall architecture design
• Measured in the factory in a “golden” environment.
• External or “Environmental”
• Any external noise source: motors, old equipment, switching circuits, EM
interference, UPS, poor power, ground-loops and so forth
13. 13 Proprietary & Confidential
System noise
• In a SiLi-based EDS, the capacitance is directly related to the active
area of the device.
• Capacitance starts as BIG
• As active area increases, capacitance increases
Needs LN
14. 14 Proprietary & Confidential
Get much smaller
And have potential to get smaller still.
15. 15 Proprietary & Confidential
Move averaging, less uncertainty, better resolution
Less averaging, more uncertainty, worse resolution
16. 16 Proprietary & Confidential
Longer integration times result in superior energy resolution
Shorter integration times are required for high count rates
18. 18 Proprietary & Confidential
What does high count rate resolution look like?
123 eV @ 6.4 sec
183 eV @ 0.2 sec
EDS detectors are routinely specified @ 2,000 – 3,000 cps
19. 19 Proprietary & Confidential
Take-away points
• Energy resolution
• Laboratory noise impacts performance
• speed matters: faster acquisition = worse resolution
• Detectors are specified at slow rates
20. 20 Proprietary & Confidential
What does high count rate resolution look like?
Often-times 185 eV is just fine
2000 eV
peak-to-peak
2000 eV
peak-to-peak
21. 21 Proprietary & Confidential
What does high count rate resolution look like?
Sometimes we need 4 eV
22. 22 Proprietary & Confidential
Take-away points
• Energy resolution
• Laboratory noise impacts performance
• speed matters: faster acquisition = worse resolution
• Detectors are specified at slow rates
• Sometimes poor resolution is just fine
• Other times the resolution will never be good enough
23. 23 Proprietary & Confidential
What does high count rate look like?
128 eV @ 6.4 sec
160 eV @ 0.4 sec
How about down here?
(input cps)
Standard EDS
24. 24 Proprietary & Confidential
What does high count rate look like?
Difficult to even define resolution
@ 1,000,000 cps
(input cps)
Standard EDS
25. 25 Proprietary & Confidential
Can we improve on this?
It is possible to design an SDD with excellent low energy performance
76 eV
78 eV
114 eV
66 eV
67 eV
90 eV
55 eV
61 eV
114 eV
(input cps)
Extreme EDS
26. 26 Proprietary & Confidential
Can we improve on this?
It is possible to design an SDD with excellent low energy performance
57 eV
67 eV
50 eV
62 eV
50 eV
62 eV
(input cps)
Extreme EDS
27. 27 Proprietary & Confidential
Take-away points
• Energy resolution
• Laboratory noise impacts performance
• speed matters: faster acquisition = worse resolution
• Detectors are specified at slow rates
• Sometimes poor resolution is just fine
• Other times the resolution will never be good enough
• Low energy part of the spectrum is affected more dramatically than the
moderate to higher part of the spectrum
28. 28 Proprietary & Confidential
• High quality light element energy resolution
• Low quality light element energy resolution
• Can we quantify the difference between these two
detector designs?
29. 29 Proprietary & Confidential
A look at the numbers
Group 1 = Standard EDS
Group 2 = Extreme EDS
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A look at the numbers
All “129 eV” detectors~ 10 eV difference in light element
Group 1 = Standard EDS
Group 2 = Extreme EDS
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How much of an impact?
Extreme detector, 10 kcps
Standard detector, 10 kcps
Standard detector, 1 Mcps
33. 33 Proprietary & Confidential
Take-away points
• Energy resolution
• Laboratory noise impacts performance
• speed matters: faster acquisition = worse resolution
• Detectors are specified at slow rates
• Sometimes poor resolution is just fine
• Other times the resolution will never be good enough
• Low energy part of the spectrum is affected more dramatically than the
moderate to higher part of the spectrum
• Energy resolution specifications up at Mn –ka (5.9 keV) are not
reflective of the performance in the low energy spectrum.
35. 35 Proprietary & Confidential
Light element sensitivity: “Sensitive to”
•EDS detectors often carry a light element
sensitivity specification termed as:
•“Sensitive to”
•Why this specification?
•What does it really indicate?
36. 36 Proprietary & Confidential
Light element sensitivity: “Sensitive to”
• The detector system absorbs x-rays
• Window between SEM chamber and crystal
• Thin metal layer on detector crystal to avoid cathodoluminescence
• Some detectors use N2 backfill
window
detector
crystal
pre-amp
cold finger
insulator
X-rays
liquid Nitrogen
38. 38 Proprietary & Confidential
X-ray absorption in windows
O
BLi Be
Li detection is not possible with a window and has challenges well beyond
window technology
39. 39 Proprietary & Confidential
Light element sensitivity: “Sensitive to Be”
Extreme EDS
40. 40 Proprietary & Confidential
Light element sensitivity: “Sensitive to BN”
Extreme EDS
41. 41 Proprietary & Confidential
Light element sensitivity: “Sensitive to B”
Compact EDS
Pure B metal
43. 43 Proprietary & Confidential
Light element sensitivity: “Sensitive to B”
8x sensitivity Extreme EDS
Compact EDS
44. 44 Proprietary & Confidential
Light element sensitivity: “Sensitive to B”
0
1000
2000
3000
4000
5000
6000
0
200
400
600
800
1000
1200
1400
1600
1800
2000
80 180 280 380 480
EDScounts
WDScounts
Energy eV)
B - WDS
B - EDS
Trace B (2% B in Fe-Cr) is harder
B
C
0
2000
4000
6000
8000
10000
0
20000
40000
60000
80000
100000
120000
80 180 280 380 480
EDScounts
WDScounts
Energy eV)
B - WDS
B - EDS
B metal is easy for EDS/WDS
B
45. 45 Proprietary & Confidential
Take-away points
• Energy resolution
• Laboratory noise impacts performance
• speed matters: faster acquisition = worse resolution
• Detectors are specified at slow rates
• Sometimes poor resolution is just fine
• Other times the resolution will never be good enough
• Low energy part of the spectrum is affected more dramatically than the
moderate to higher part of the spectrum
• Energy resolution specifications up at Mn –ka (5.9 keV) are not reflective of the
performance in the low energy spectrum.
• Sensitivity
• Detection to B isn’t always detection to B
46. 46 Proprietary & Confidential
•Is light element sensitivity just
about my detector and window
technology?
49. 49 Proprietary & Confidential
Light element sensitivity: Variable pressure mode
C Cu-L
Pure B metal
50. 50 Proprietary & Confidential
Light element sensitivity: Variable pressure mode
No VP
50 Pa
200 Pa
No VP
Extreme detector
Compact EDS detector
51. 51 Proprietary & Confidential
Take-away points
• Energy resolution
• Laboratory noise impacts performance
• speed matters: faster acquisition = worse resolution
• Detectors are specified at slow rates
• Sometimes poor resolution is just fine
• Other times the resolution will never be good enough
• Low energy part of the spectrum is affected more dramatically than the
moderate to higher part of the spectrum
• Energy resolution specifications up at Mn –ka (5.9 keV) are not
reflective of the performance in the low energy spectrum.
• Sensitivity
• Detection to B isn’t always detection to B
• Variable pressure mode has a major impact on light element detection
52. 52 Proprietary & Confidential
Light Element Detection – Li mapping
Windowless Extreme EDS detector
53. 53 Proprietary & Confidential
Take-away points
• Energy resolution
• Laboratory noise impacts performance
• speed matters: faster acquisition = worse resolution
• Detectors are specified at slow rates
• Sometimes poor resolution is just fine
• Other times the resolution will never be good enough
• Low energy part of the spectrum is affected more dramatically than the
moderate to higher part of the spectrum
• Energy resolution specifications up at Mn –ka (5.9 keV) are not
reflective of the performance in the low energy spectrum.
• Sensitivity
• Detection to B isn’t always detection to B
• Variable pressure mode has a major impact on light element detection
• The technology for light element detection exists today. You need to
specifically ask & plan for it.
54. 54 Proprietary & Confidential
Light element sensitivity: “Sensitive to”
•Determine what you need
•Is it important to your application?
• Light element detection? Or mapping?
• Transition metals?
• Do you work in VP mode?
• How critical is quant?
•Be specific & avoid ambiguity.
61. 61 Proprietary & Confidential
Multiphase Sample – Net Count Maps
Si_K
Ta_M
W_M
Si, Ta, W: No detector can separate these peaks
Peak deconvolution algorithms cleanly separate the peaks
63. 63 Proprietary & Confidential
Example – Mo, S, Ba – Raw Count Element Maps
64. 64 Proprietary & Confidential
Example – Mo, S, Ba – Net Count Maps
65. 65 Proprietary & Confidential
Example – Mo, S, Ba – Phase Maps
Distinguishing the three main phases is
not possible without robust peak
deconvolution
2100 2150 2200 2250 2300 2350 2400 2450 2500
eV
MoL SK
66. 66 Proprietary & Confidential
Take-away points
• Energy resolution
• Laboratory noise impacts performance
• Speed matters: faster acquisition = worse resolution
• Detectors are specified at slow rates
• Sometimes poor resolution is just fine
• Other times the resolution will never be good enough
• Low energy part of the spectrum is affected more dramatically than the moderate to higher part of the
spectrum
• Energy resolution specifications up at Mn –ka (5.9 keV) are not reflective of the performance in the
low energy spectrum.
• Sensitivity
• Detection to B isn’t always detection to B
• Variable pressure mode has a major impact on light element detection
• The technology for light element detection exists today. You need to specifically ask & plan for it.
• Post-processing algorithms
• Peak deconvolution, background subtraction and matrix correction algorithms are critical to high quality
mapping
• Phase mapping is even more powerful than these element mapping algorithms
67. 67 Proprietary & Confidential
• EDS detector have made many advances over the last several years
• 3 main drivers in specifying an EDS detector
• Energy resolution @ Mn k-alpha
• Sensitive to
• Solid angle
• Actually important
• Energy resolution in low energy
• Actual sensitivity of light element
• Actual throughput
• Most important: Peak deconvolution and net counts mapping
• The most important factor is careful discernment of the EDS detector and
the overall EDS system