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Method for visualizing detailed profiles of synchrotron X-ray beams using diamond-thin films and silicon drift detectors

MetadataDetails
Publication Date2025-04-22
JournalJournal of Synchrotron Radiation
AuthorsTogo Kudo, Shinji Suzuki, Mutsumi Sano, Toshiro Itoga, Hiroyasu Masunaga
InstitutionsJapan Synchrotron Radiation Research Institute
AnalysisFull AI Review Included

Technical Documentation & Analysis: Diamond Films for Synchrotron Beam Monitoring

Section titled “Technical Documentation & Analysis: Diamond Films for Synchrotron Beam Monitoring”

This document analyzes the research paper “Method for visualizing detailed profiles of synchrotron X-ray beams using diamond-thin films and silicon drift detectors” (Kudo et al., J. Synchrotron Rad. 2025) and outlines how 6CCVD’s advanced MPCVD diamond materials and customization capabilities directly support and enable this critical synchrotron diagnostics technology.


The research successfully demonstrates a high-precision, energy-resolved method for visualizing synchrotron undulator beam profiles using a thin Single-Crystal Diamond (SCD) film as a scatterer.

  • Core Value Proposition: Accurate determination of the true X-ray beam center by effectively eliminating contamination from nearby bending magnet radiation.
  • Material Requirement: A high-purity, thin (70 ”m) SCD film was essential for scattering the pink X-ray beam while minimizing heat load and absorption.
  • Technical Achievement: Achieved high energy resolution (ΔE = 140 eV FWHM) using a Silicon Drift Detector (SDD) coupled with pinhole imaging.
  • Spatial Resolution: Demonstrated a spatial resolution limit of 50 ”m, enabling detailed visualization of beam splitting and convergence patterns across various energy levels.
  • Methodology: Two distinct scanning methods (SDD scan for high spatial resolution and FES scan for wide-field visualization) were validated against SPECTRA simulations.
  • 6CCVD Relevance: 6CCVD specializes in producing the required high-purity SCD films with precise thickness control (0.1 ”m to 500 ”m) and custom metalization necessary for robust mounting in high-vacuum synchrotron environments.

The following hard data points were extracted from the experimental setup and results:

ParameterValueUnitContext
Diamond MaterialSingle Crystal Diamond (SCD)N/AUsed as the X-ray scatterer
Diamond Thickness70”mCritical dimension for scattering efficiency and heat load
SDD Energy Resolution (ΔE)140eV (FWHM)Resolution used to filter bending magnet contamination
Spatial Resolution Limit50”mEstablished by Pinhole 1 diameter
FES Aperture (High Resolution Scan)1.5 x 1.5mmFixed aperture during SDD 2D scan
FES Aperture (Wide Field Scan)0.4 x 0.4mmScanned aperture during FES 2D scan
Undulator Gap (SDD Scan)26mmFirst harmonic peak at 17.3 keV
Undulator Gap (FES Scan)14.8mmFirst harmonic peak at 10 keV
Beam Center FWHM (Vertical, 16.9 keV)~500”mMeasured beam size, significantly smaller than FES aperture
Contamination Reduction4 orders of magnitudeN/AReduction of bending magnet flux near beam center

The experiment utilized a semi-nondestructive approach combining high-purity diamond scattering films with energy-resolved detection.

  1. Diamond Scatterer Integration: A 70 ”m thick Single-Crystal Diamond (SCD) film was installed in a vacuum chamber (35.407 m from the light source) to scatter the pink synchrotron beam.
  2. Beam Definition: A Front-End Slit (FES) was used upstream of the monochromator to define the beam aperture (e.g., 1.5 mm x 1.5 mm for high-resolution scans).
  3. Pinhole Camera Setup: Forward-scattered X-rays were extracted through a Be window and imaged using a pinhole camera system (Pinhole 1: 50 ”m diameter; Pinhole 2: 200 ”m diameter).
  4. High-Spatial Resolution Measurement (SDD Scan): The SDD detector assembly (with Pinhole 2) was scanned in 2D (200 ”m increments) across the beam profile to achieve high spatial detail (50 ”m limit).
  5. Wide-Field Measurement (FES Scan): The FES aperture was reduced (0.4 mm x 0.4 mm) and scanned in 2D (0.1 mm pitch) across a 5 mm range, while the SDD remained fixed, enabling visualization of the full pre-slit profile (up to 4 mm aperture).
  6. Energy Filtering: The high energy resolution of the SDD (ΔE = 140 eV) was crucial for analyzing energy-resolved intensity maps and isolating the undulator radiation from lower-energy bending magnet contamination.

This research highlights the critical role of high-quality, precisely manufactured diamond films in advanced synchrotron diagnostics. 6CCVD is uniquely positioned to supply the materials and engineering support required to replicate and advance this technology.

The success of this method relies entirely on the purity, crystallinity, and precise thickness of the diamond scatterer.

Research Requirement6CCVD SolutionMaterial Specification
High Purity ScattererOptical Grade Single Crystal Diamond (SCD)High-purity MPCVD SCD ensures minimal absorption and low background noise, crucial for accurate energy-resolved measurements.
Precise Thickness (70 ”m)Custom SCD Wafers6CCVD offers SCD thickness control from 0.1 ”m up to 500 ”m, allowing researchers to optimize the scattering cross-section versus heat load for specific beamlines.
High Heat Load ManagementThermal Grade SCDFor future high-power applications, 6CCVD can supply SCD with thermal conductivity > 2000 W/mK, essential for managing heat load on the optics system (a limitation noted in the paper).

The experimental setup requires highly specific component dimensions and integration features, which 6CCVD provides as standard services.

  • Custom Dimensions: While the paper used a specific size, 6CCVD can supply SCD plates and wafers up to 125 mm (PCD) and custom-cut SCD pieces to fit any vacuum chamber mount or FES geometry.
  • Precision Polishing: To maintain beam quality and minimize surface scattering artifacts, 6CCVD guarantees ultra-smooth surfaces. We offer polishing down to Ra < 1 nm for SCD, ensuring the highest optical quality for beam monitoring applications.
  • Integrated Metalization Services: The diamond film must be robustly mounted for thermal sinking and structural integrity in the UHV environment. 6CCVD offers in-house metalization capabilities, including Ti/Pt/Au, W, Cu, and Pd coatings, optimized for brazing or clamping into water-cooled mounts, directly addressing the heat load limitations discussed in the paper.

The challenges noted in the paper—specifically optimizing thickness for heat load and achieving faster measurement times—require expert material consultation.

  • Application Expertise: 6CCVD’s in-house PhD team specializes in material selection for high-flux X-ray beam diagnostics and beam position monitors (XBPMs). We can assist researchers in optimizing diamond thickness and purity for similar Synchrotron Beam Profile Monitoring projects.
  • Advanced Detector Integration: We provide consultation on integrating diamond films with advanced detectors, including multi-element SDDs, to reduce measurement time from hours to seconds, as suggested for future work in the paper.

For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.

View Original Abstract

Contamination from nearby bending magnet radiation hinders precise and accurate determination of the true beam center of undulator radiation. To solve this problem, a semi-nondestructive method was developed to visualize the detailed profile of a synchrotron radiation beam by using a thin diamond film as a scatterer. As the beam passed through the diamond film, scattered X-rays were imaged using a pinhole camera and measured with a two-dimensional silicon drift detector (SDD) scan. With this configuration, the beam center was accurately determined by visualizing the radiation pattern distribution for each energy level of a pink X-ray beam within an aperture size of 1.5 mm × 1.5 mm, shaped by a front-end slit (FES) positioned upstream of the monochromator. Additionally, by scanning the FES in two dimensions with a reduced aperture of 0.4 mm × 0.4 mm, energy-resolved images were successfully obtained using the SDD at a fixed position. These images revealed the profile of undulator radiation over a broad area (with an aperture extending up to 4 mm) in a pre-slit positioned upstream of the FES, demonstrating good alignment with SPECTRA calculations. This method effectively eliminates contamination from nearby bending magnet radiation, a significant issue in previous approaches, enabling a direct and highly accurate determination of the true beam center.