Specific Process Knowledge/Characterization/XRD/XRD SmartLab/Instrumental broading in GiXRD: Difference between revisions

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Created page with "This page describes values of Instrumental broadening in GiXRD measurements, and can be used as a reference for peak broadening in 2θ - scans. Most four common slit configuration cases are chosen. The instrumental broadening has been measured by using standard Si powder sample. Scherrer formula: <math>D=\frac{K\cdot\lambda}{\beta_{sample}\cdot cos\theta}</math> where: K is Scherrer constant (typically close to unity K=0.9-1)<br> λ is a wavelength of X-ray radiatio..."
 
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This page describes values of Instrumental broadening in GiXRD measurements, and can be used as a reference for peak broadening in 2θ - scans. Most four common slit configuration cases are chosen.
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This page describes values of Instrumental broadening in [[Specific_Process_Knowledge/Characterization/XRD/Process_Info#2θ_scan._Graizing_Incident_X-ray_Diffraction_(GiXRD)|GiXRD measurements]], and can be used as a reference for peak broadening in 2θ - scans. Most four common slit configuration cases are chosen.
The instrumental broadening has been measured by using standard Si powder sample.  
The instrumental broadening has been measured by using standard Si powder sample.  



Latest revision as of 17:40, 9 November 2023

Feedback to this page: click here


This page is written by Evgeniy Shkondin @DTU Nanolab if nothing else is stated.
All images and photos on this page belongs to DTU Nanolab.
The fabrication and characterization described below were conducted in 2023 by Evgeniy Shkondin, DTU Nanolab.


This page describes values of Instrumental broadening in GiXRD measurements, and can be used as a reference for peak broadening in 2θ - scans. Most four common slit configuration cases are chosen. The instrumental broadening has been measured by using standard Si powder sample.

Scherrer formula:

where: K is Scherrer constant (typically close to unity K=0.9-1)
λ is a wavelength of X-ray radiation (λ Cu-Kα1 = 1.540562 Å, and in case both Cu-Kα1 and Cu-Kα2 are present λ Cu-Kα1,2 = 1.541871 Å)
θ is Bragg angle
βsample is a peak broadening. The technical point should be noted that intergal breadth and/or FWHM have to be inserted in radians.


in the case where the peaks obey Lorentzian (or Cauchy) distribution profile.

in the case of Gaussian distribution profile.

Experimental results implied crystallite size to cause a Cauchy-type broadening while strain broadening was associated with a Gauss profile. Real measurement contains contributions of both Lorentzian (Cauchy) and Gaussian distributions.


Full scans

case1

IS=0.5 mm and ω=2°


Peak number 2θ (°) FWHM (°) FWHM (rad) Integral breadth (°) Integral breadth (rad)
1 28.4077 0.2923 0.0051 0.3232 0.0056
2 47.2895 0.3109 0.0054 0.3395 0.0059
3 56.1274 0.3004 0.0052 0.3368 0.0059
4 69.1426 0.3082 0.0054 0.3325 0.0058
5 76.3659 0.2585 0.0045 0.2936 0.0051
6 88.0122 0.3174 0.0055 0.3609 0.0063
7 94.9581 0.3126 0.0055 0.3434 0.0060
8 106.7351 0.3317 0.0058 0.3637 0.0063

case2

IS=0.5 mm and ω=1°


Peak number 2θ (°) FWHM (°) FWHM (rad) Integral breadth (°) Integral breadth (rad)
1 28.4185 0.2961 0.0052 0.3246 0.0057
2 47.2935 0.2961 0.0052 0.3214 0.0056
3 56.1085 0.2881 0.0050 0.3206 0.0056
4 69.1297 0.3009 0.0053 0.3203 0.0056
5 76.3485 0.3110 0.0054 0.3525 0.0062
6 88.0310 0.2972 0.0052 0.3234 0.0056
7 94.9806 0.2872 0.0050 0.3114 0.0054
8 106.7100 0.2838 0.0050 0.3024 0.0053

case3

IS=1 mm and ω=2°


Peak number 2θ (°) FWHM (°) FWHM (rad) Integral breadth (°) Integral breadth (rad)
1 28.3469 0.3041 0.0053 0.3237 0.0056
2 47.2945 0.3009 0.0053 0.3242 0.0057
3 56.1208 0.3064 0.0053 0.3322 0.0058
4 69.1388 0.3363 0.0059 0.3598 0.0063
5 76.3682 0.2689 0.0047 0.3100 0.0054
6 88.0168 0.3443 0.0060 0.3811 0.0067
7 94.9673 0.3018 0.0053 0.3289 0.0057
8 106.7248 0.3344 0.0058 0.3655 0.0064

case4

IS=1 mm and ω=1°


Peak number 2θ (°) FWHM (°) FWHM (rad) Integral breadth (°) Integral breadth (rad)
1 28.4186 0.2981 0.0052 0.3187 0.0056
2 47.2990 0.2998 0.0052 0.3192 0.0056
3 56.0990 0.2991 0.0052 0.3418 0.0060
4 69.1210 0.2992 0.0052 0.3318 0.0058
5 76.3549 0.3070 0.0054 0.3386 0.0059
6 88.0328 0.3053 0.0053 0.3437 0.0060
7 94.9712 0.2838 0.0050 0.3127 0.0055
8 106.7197 0.2799 0.0049 0.2980 0.0052