Specific Process Knowledge/Characterization/XRD/XRD SmartLab/Instrumental broading in T2T

From LabAdviser
Revision as of 08:40, 31 July 2024 by Eves (talk | contribs) (Created page with " This page describes the values of instrumental broadening in θ/2θ measurements and can be used as a reference for peak broadening in grain size calculation. The most common slit configuration cases are chosen, both with and without the Ge220 monochromator. The instrumental broadening has been measured by using standard Si and LaB<sub>6</sub> powder. Scherrer formula: <math>D=\frac{K\cdot\lambda}{\beta_{sample}\cdot cos\theta}</math> where: K is Scherrer constant...")
(diff) ← Older revision | Latest revision (diff) | Newer revision → (diff)

This page describes the values of instrumental broadening in θ/2θ measurements and can be used as a reference for peak broadening in grain size calculation. The most common slit configuration cases are chosen, both with and without the Ge220 monochromator.


The instrumental broadening has been measured by using standard Si and LaB6 powder.

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 that crystallite size causes Cauchy-type broadening, while strain broadening is associated with a Gaussian profile. Real measurements contain contributions from both Lorentzian (Cauchy) and Gaussian distributions.

Both LaB6 and Si powder provided the best fit with a Gaussian function. Therefore, all the results below are presented using a Gaussian fit.

It also seems necessary to use a high-quality single crystal to include both Lorentzian and Gaussian contributions and fit with a Pseudo-Voight approach.



Full scans

Here the full scans of LaB6 and Si powder are presented. Each sample was measured with and without the Ge220 monochromator on the incident side, with the Incident Slit (IS) set to either 0.5 mm or 1 mm. On the receiving side, RS1 = 0.5 mm and RS2 = 0.525 mm were used for IS = 0.5 mm, and RS1 = 1 mm and RS2 = 1.125 mm were used for IS = 1 mm. The step width was 0.01° and the speed was 2°/min for all scans. A Soller slit of 5° was selected as the Receiving Parallel Slit (RPS) for all scans. In the case of the IPS adapter, the Soller slit of 5° was used.

case1 - LaB6 with Ge220 monochromator

LaB6 Ge220 monochromator on incident side
IS = 0.5 mm
Orientation 2θ (°) Integral breadth (°) Integral breadth (rad) FWHM (°) FWHM (rad)
100 21.337 0.10739 0.00187 0.10089 0.00176
110 30.3523 0.13819 0.0024 0.12982 0.0023
111 37.4169 0.12657 0.0022 0.1189 0.0021
200 43.4813 0.12415 0.0022 0.11663 0.0020
210 48.9438 0.19641 0.0034 0.12504 0.0022
211 53.9726 0.14188 0.0025 0.13328 0.0023
220 63.2028 0.12865 0.0022 0.12086 0.0021
? 67.5401 0.12066 0.0021 0.11335 0.0020
? 71.7371 0.10965 0.0019 0.10301 0.0018
310 75.8311 0.10923 0.0019 0.10262 0.0018
320 87.7842 0.13106 0.0023 0.12312 0.0021
410 99.6432 0.13603 0.0024 0.12779 0.0022
411 103.6716 0.14652 0.0026 0.13765 0.0024
421 116.2506 0.14605 0.0025 0.1372 0.0024
IS = 1.0 mm
Orientation 2θ (°) Integral breadth (°) Integral breadth (rad) FWHM (°) FWHM (rad)
100 21.3112 0.24000 0.0042 0.22547 0.0039
110 30.3476 0.23945 0.0042 0.22494 0.0039
111 37.4059 0.22363 0.0039 0.21009 0.0037
200 43.471 0.23381 0.0041 0.21965 0.0038
210 48.9311 0.23146 0.0040 0.21744 0.0038
211 53.9635 0.21833 0.0038 0.2051 0.0036
220 63.2056 0.21683 0.0038 0.20369 0.0036
? 67.6308 0.22749 0.0040 0.21371 0.0037
? 71.7340 0.24789 0.0043 0.23288 0.0041
310 75.8186 0.22282 0.0039 0.20933 0.0037
320 87.7794 0.22295 0.0039 0.20945 0.0037
410 99.6445 0.21801 0.0038 0.20481 0.0036
411 103.6522 0.20431 0.0036 0.21748 0.0038
421 116.2526 0.2521 0.0044 0.23683 0.0041


case2 - LaB6 with IPS adaptor

LaB6 IPS on incident side
IS = 0.5 mm
Orientation 2θ (°) Integral breadth (°) Integral breadth (rad) FWHM (°) FWHM (rad)
100 21.3385 0.16688 0.0029 0.15677 0.0027
110 30.3784 0.7473 0.0030 0.16415 0.0029
111 37.4424 0.18775 0.0033 0.17638 0.0031
200 43.5157 0.21383 0.0037 0.20088 0.0035
210 48.9575 0.16613 0.0029 0.15607 0.0027
211 53.9741 0.13757 0.0024 0.12924 0.0023
220 63.2098 0.16157 0.0028 0.15179 0.0026
? 67.5436 0.13682 0.0024 0.12853 0.0022
? 71.74000 0.13819 0.0024 0.12982 0.0023
310 75.84990 0.15249 0.0027 0.14326 0.0025
320 87.79290 0.13792 0.0024 0.12956 0.0023
410 99.6461 0.14402 0.0025 0.13529 0.0024
411 103.6695 0.14404 0.0025 0.13532 0.0024
421 116.2607 0.16243 0.0028 0.15259 0.0027
IS = 1.0 mm
Orientation 2θ (°) Integral breadth (°) Integral breadth (rad) FWHM (°) FWHM (rad)
100 21.3354 0.25476 0.0044 0.23933 0.0042
110 30.3763 0.24934 0.0044 0.23424 0.0041
111 37.4454 0.25983 0.0045 0.24409 0.0043
200 43.5167 0.26947 0.0047 0.25315 0.0044
210 48.9694 0.26146 0.0046 0.24562 0.0043
211 53.9866 0.24426 0.0043 0.22947 0.0040
220 63.2297 0.27671 0.0048 0.25995 0.0045
? 67.5594 0.27847 0.0049 0.26161 0.0046
? 71.7568 0.26005 0.0045 0.2443 0.0043
310 75.8530 0.27326 0.0048 0.25671 0.0045
320 87.7921 0.25544 0.0045 0.23997 0.0042
410 99.6463 0.23764 0.0041 0.22324 0.0039
411 103.664 0.23902 0.0042 0.22454 0.0039
421 116.2617 0.25501 0.0045 0.23957 0.0042


case3 - Si powder with Ge220 monochromator

Si powder Ge220 monochromator on incident side
IS = 0.5 mm
Orientation 2θ (°) Integral breadth (°) Integral breadth (rad) FWHM (°) FWHM (rad)
111 28.4124 0.15459 0.0027 0.14522 0.0025
220 47.2829 0.13319 0.0023 0.12512 0.0022
311 56.1009 0.1342 0.0023 0.12608 0.0022
331 76.3771 0.17568 0.0031 0.16504 0.0029
511 88.0381 0.14264 0.0025 0.1340 0.0023
440 - - - - -
531 - - - - -
422 - - - - -
IS = 1.0 mm
Orientation 2θ (°) Integral breadth (°) Integral breadth (rad) FWHM (°) FWHM (rad)
111 28.3944 0.2392 0.0042 0.22471 0.0039
220 47.2802 0.20108 0.0035 0.1889 0.0033
311 56.1069 0.22110 0.0039 0.20771 0.0036
331 76.3585 0.20981 0.0037 0.1971 0.0034
422 88.0277 0.2230 0.0039 0.20949 0.0037
511 94.9552 0.23689 0.0041 0.22255 0.0039
440 106.6949 0.19242 0.0034 0.18076 0.0032
531 114.0880 0.22245 0.0039 0.20898 0.0036


case4 - Si powder with IPS adaptor

Si powder IPS on incident side
IS = 0.5 mm
Orientation 2θ (°) Integral breadth (°) Integral breadth (rad) FWHM (°) FWHM (rad)
111 28.4386 0.23378 0.0041 0.14883 0.0026
220 47.3197 0.22441 0.0039 0.21082 0.0037
311 56.1199 0.14714 0.0026 0.13823 0.0024
331 76.3703 0.13962 0.0024 0.13116 0.0023
511 88.0354 0.15322 0.0027 0.14394 0.0025
440 94.9602 0.15685 0.0027 0.14735 0.0026
531 106.7178 0.16969 0.0030 0.15941 0.0028
422 114.1167 0.18994 0.0033 0.17844 0.0031
IS = 1.0 mm
Orientation 2θ (°) Integral breadth (°) Integral breadth (rad) FWHM (°) FWHM (rad)
111 28.4311 0.24618 0.0043 0.23127 0.0040
220 47.3122 0.27804 0.0049 0.2612 0.0046
311 56.1430 0.27204 0.0047 0.25557 0.0045
331 76.3978 0.27933 0.0049 0.26241 0.0046
422 88.0267 0.24578 0.0043 0.23089 0.0040
511 94.957 0.26134 0.0046 0.24551 0.0043
440 106.7393 0.29928 0.0052 0.28116 0.0049
531 114.1079 0.2957 0.0052 0.27779 0.0048