Abstract: Methods and systems for feed-forward of multi-layer and multi-process information using XPS and XRF technolgies are disclosed. In an example, a method of thin film characterization includes measuring first XPS and XRF intensity signals for a sample having a first layer above a substrate. A thickness of the first layer is determined based on the first XPS and XRF intensity signals. The information for the first layer and for the substrate is combined to estimate an effective substrate. Second XPS and XRF intensity signals are measured for a sample having a second layer above the first layer above the substrate. The method also involves determining a thickness of the second layer based on the second XPS and XRF intensity signals, the thickness accounting for the effective substrate.

Abstract: Systems and approaches for silicon germanium thickness and composition determination using combined XPS and XRF technologies are described. In an example, a method for characterizing a silicon germanium film includes generating an X-ray beam. A sample is positioned in a pathway of said X-ray beam. An X-ray photoelectron spectroscopy (XPS) signal generated by bombarding said sample with said X-ray beam is collected. An X-ray fluorescence (XRF) signal generated by bombarding said sample with said X-ray beam is also collected. Thickness or composition, or both, of the silicon germanium film is determined from the XRF signal or the XPS signal, or both.

Abstract: Methods and systems for measuring periodic structures using multi-angle X-ray reflectance scatterometry (XRS) are disclosed. For example, a method of measuring a sample by X-ray reflectance scatterometry involves impinging an incident X-ray beam on a sample having a periodic structure to generate a scattered X-ray beam, the incident X-ray beam simultaneously providing a plurality of incident angles and a plurality of azimuthal angles. The method also involves collecting at least a portion of the scattered X-ray beam.

Abstract: Methods and systems for fabricating platelets of a monochromator for X-ray photoelectron spectroscopy (XPS) are disclosed. For example, a method of fabricating a platelet of a monochromator for X-ray photoelectron spectroscopy involves placing a crystal on a stage of an X-ray measuring apparatus, the crystal having a top surface. The method also involves measuring, by X-ray reflection, an orientation of a crystal plane of the crystal, the crystal plane beneath the top surface of the crystal and having a primary axis. The method also involves measuring a surface angle of the top surface of the crystal by measuring a light beam reflected from the top surface of the crystal.

Abstract: Systems and methods for characterizing films by X-ray photoelectron spectroscopy (XPS) are disclosed. For example, a system for characterizing a film may include an X-ray source for generating an X-ray beam having an energy below the k-edge of silicon. A sample holder may be included for positioning a sample in a pathway of the X-ray beam. A first detector may be included for collecting an XPS signal generated by bombarding the sample with the X-ray beam. A second detector may be included for collecting an X-ray fluorescence (XRF) signal generated by bombarding the sample with the X-ray beam. Monitoring/estimation of the primary X-ray flux at the analysis site may be provided by X-ray flux detectors near and at the analysis site. Both XRF and XPS signals may be normalized to the (estimated) primary X-ray flux to enable film thickness or dose measurement without the need to employ signal intensity ratios.

Abstract: A method to determine a distribution profile of an element in a film. The method comprises exciting an electron energy of an element deposited in a first film, obtaining a first spectrum associating with the electron energy, and removing a background spectrum from the first spectrum. Removing the background value generates a processed spectrum. The method further includes matching the processed spectrum to a simulated spectrum with a known simulated distribution profile for the element in a film comparable to the first film. A distribution profile is obtained for the element in the first film based on the matching of the processed spectrum to a simulated spectrum selected from the set of simulated spectra.

Abstract: A method to determine a distribution profile of an element in a film. The method comprises exciting an electron energy of an element deposited in a first film, obtaining a first spectrum associating with the electron energy, and removing a background spectrum from the first spectrum. Removing the background value generates a processed spectrum. The method further includes matching the processed spectrum to a simulated spectrum with a known simulated distribution profile for the element in a film comparable to the first film. A distribution profile is obtained for the element in the first film based on the matching of the processed spectrum to a simulated spectrum selected from the set of simulated spectra.

Abstract: A method to determine a distribution profile of an element in a film. The method comprises exciting an electron energy of an element deposited in a first film, obtaining a first spectrum associating with the electron energy, and removing a background spectrum from the first spectrum. Removing the background value generates a processed spectrum. The method further includes matching the processed spectrum to a simulated spectrum with a known simulated distribution profile for the element in a film comparable to the first film. A distribution profile is obtained for the element in the first film based on the matching of the processed spectrum to a simulated spectrum selected from the set of simulated spectra.

Abstract: A method and a system for calibrating an X-ray photoelectron spectroscopy (XPS) measurement are described. The method includes using an X-ray beam to generate an XPS signal from a sample and normalizing the XPS signal with a measured or estimated flux of the X-ray beam. The system includes an X-ray source for generating an X-ray beam and a sample holder for positioning a sample in a pathway of the X-ray beam. A detector is included for collecting an XPS signal generated by bombarding the sample with the X-ray beam. Also included are a flux detector for determining a measured or estimated flux of the X-ray beam and a computing system for normalizing the XPS signal with the measured or estimated flux of the X-ray beam.

Abstract: A semiconductor substrate processing apparatus and a method for processing semiconductor substrates are provided. The method may include providing a semiconductor substrate having a surface and a plurality of features on the surface, each feature being positioned on the surface at a first respective point in a first coordinate system, plotting the position of each feature at a second respective point in a second coordinate system; and generating a translation between the first and the second coordinate systems. The generating of the translation may include calculating an offset between the first and the second coordinate systems. The calculating of the offset may include calculating an offset distance between a reference point of the first coordinate system and a reference point of the second coordinate system and calculating an offset angle between an axis of the first coordinate system and an axis of the second coordinate system.

Abstract: A method to determine a distribution profile of an element in a film. The method comprises exciting an electron energy of an element deposited in a first film, obtaining a first spectrum associating with the electron energy, and removing a background spectrum from the first spectrum. Removing the background value generates a processed spectrum. The method further includes matching the processed spectrum to a simulated spectrum with a known simulated distribution profile for the element in a film comparable to the first film. A distribution profile is obtained for the element in the first film based on the matching of the processed spectrum to a simulated spectrum selected from the set of simulated spectra.

Abstract: According to one aspect of the invention, a semiconductor substrate processing apparatus and a method for processing semiconductor substrates are provided. The method may include providing a semiconductor substrate having a surface and a plurality of features on the surface, each feature being positioned on the surface at a first respective point in a first coordinate system, plotting the position of each feature at a second respective point in a second coordinate system; and generating a translation between the first and the second coordinate systems. The generating of the translation may include calculating an offset between the first and the second coordinate systems. The calculating of the offset may include calculating an offset distance between a reference point of the first coordinate system and a reference point of the second coordinate system and calculating an offset angle between an axis of the first coordinate system and an axis of the second coordinate system.

Abstract: An electronic device. The device comprises a printed circuit board, a multilayered capacitor formed on the printed circuit board, and a conductive strip disposed on a top surface of the printed circuit board. The conductive strip interconnects to the multilayered capacitor. The multilayered capacitor includes a plurality of capacitance plates and a plurality of dielectric layers wherein each dielectric layer is disposed between two of the capacitance plates. The printed circuit board further comprises ground plated sidewalls disposed about the printed circuit board. Each of the ground plated sidewalls extends from a top surface to a bottom surface of the printed circuit board.

Abstract: A method comprising obtaining a first set of spectral data for a first sample film measured by a first system, extracting intensities for one or more elemental species associated with the first sample film to provide a first set of extracted intensities using a function, and determining a first quantitative characteristic associated with the first sample film using the first set of extracted intensities. Next, obtain a second set of spectral data measured for a comparable sample film measured by a second photoelectron spectroscopy system. Next, apply the same function and continually adjust the function to extract intensities for the respective elemental species associated with the comparable sample film to provide a second set of corrected-extracted intensities. A second quantitative characteristic for the comparable sample is determined. The function is continually adjusted until the determined second quantitative characteristic closely or substantially matches the first quantitative characteristic.

Abstract: Characterization of a sample, e.g., a depth profile, may be attained using one or more of the following parameters in an electron spectroscopy method or system. The one or more parameters may include using low ion energy ions for removing material from the sample to expose progressively deeper layers of the sample, using an ion beam having a low ion angle to perform such removal of sample material, and/or using an analyzer positioned at a high analyzer angle for receiving photoelectrons escaping from the sample as a result of x-rays irradiating the sample. Further, a correction algorithm may be used to determine the concentration of components (e.g., elements and/or chemical species) versus depth within the sample, e.g., thin film formed on a substrate. Such concentration determination may include calculating the concentration of components (e.g, elements and/or chemical species) at each depth of a depth profile by removing from depth profile data collected at a particular depth (i.e.

Abstract: According to one embodiment of the invention, photoelectron spectroscopy is used to determine the thickness of one or more layers in a single or multi-layer structure on a substrate. The thickness may be determined by measuring the intensities of two photoelectron species or other atom-specific characteristic electron species emitted by the structure when bombarded with photons. A predictive intensity function that is dependent on the thickness of a layer is determined for each photoelectron species. A ratio of two predictive intensity functions is formulated, and the ratio is iterated to determine the thickness of a layer of the structure. According to one embodiment, two photoelectron species may be measured from a single layer to determine a thickness of that layer. According to another embodiment, two photoelectron species from different layers or from a substrate may be measured to determine a thickness of a layer.

Abstract: A method to determine a distribution profile of an element in a film. The method comprises exciting an electron energy of an element deposited in a first film, obtaining a first spectrum associating with the electron energy, and removing a background spectrum from the first spectrum. Removing the background value generates a processed spectrum. The method further includes matching the processed spectrum to a simulated spectrum with a known simulated distribution profile for the element in a film comparable to the first film. A distribution profile is obtained for the element in the first film based on the matching of the processed spectrum to a simulated spectrum selected from the set of simulated spectra.

Abstract: According to one aspect of the present invention, a substrate processing system is provided. The system may include a chamber wall enclosing a chamber, a substrate support positioned within the chamber to support a substrate, an electromagnetic radiation source to emit electromagnetic radiation onto the substrate on the substrate support, the electromagnetic radiation causing photoelectrons to be emitted from a material on the substrate, an analyzer to capture the photoelectrons emitted from the substrate, and a magnetic field generator to generate a magnetic field within the chamber and guide the photoelectrons from the substrate to the analyzer.

Abstract: According to one aspect of the invention a robust anode structure and methods of making and using said structure to produce ionizing radiation are disclosed. An ionizing radiation producing layer is bonded to the target side of a highly conductive diamond substrate, by a metal carbide layer. The metal carbide layers improves the strength and durability of the bond, thus improving heat removal from the anode surface and reducing the risk of delaminating the ionizing radiation producing layer, thus reducing degradation and extending the anode's life. A smoothing dopant is alloyed into the radiation producing layer to facilitate keeping the layer surface smooth, thus improving the quality of the x-ray beam emitted from the anode. In an embodiment, the heat sink comprises a metal carbide skeleton cemented diamond material. In another embodiment, the heat sink is bonded to the diamond substrate structure in a high temperature reactive brazing process.

Abstract: According to one embodiment of the invention, a method for analyzing data from an instrument is disclosed. The raw data generated by the instrument, along with configuration data generated by a user, is packaged into a calling model. The raw data may include, for example, counts having a certain kinetic energy when analyzing photoelectron spectroscopy data. The configuration data may include several parameters selected by the user based on the composition and configuration of the structure being measured. The calling model may serve as an interface between the instrument and an engine for generating an algorithm for returning desired results to the user. The engine then generates the algorithm as well as the results specified by the user, and the calling model returns the results to the user. This allows a specific algorithm and results for a specific measured sample or structure to be generated using known algorithms and functions.