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Hybrid photon-counting detectors are widely established at third-generation synchrotron facilities and the specifications of the Pilatus3 X CdTe were quickly recognized as highly promising in charge-density investigations. This is mainly attributable to the detection efficiency in the high-energy X-ray regime, in combination with a dynamic range and noise level that should overcome the perpetual problem of detecting strong and weak data simultaneously. These benefits, however, come at the expense of a persistent problem for high diffracted beam flux, which is particularly problematic in single-crystal diffraction of materials with strong scattering power and sharp diffraction peaks. Here, an in-depth examination of data collected on an inorganic material, FeSb2, and an organic semiconductor, rubrene, revealed systematic differences in strong intensities for different incoming beam fluxes, and the implemented detector intensity corrections were found to be inadequate. Only significant beam attenuation for the collection of strong reflections was able to circumvent this systematic error. All data were collected on a bending-magnet beamline at a third-generation synchrotron radiation facility, so undulator and wiggler beamlines and fourth-generation synchrotrons will be even more prone to this error. On the other hand, the low background now allows for an accurate measurement of very weak intensities, and it is shown that it is possible to extract structure factors of exceptional quality using standard crystallographic software for data processing (SAINT-Plus, SADABS and SORTAV), although special attention has to be paid to the estimation of the background. This study resulted in electron-density models of substantially higher accuracy and precision compared with a previous investigation, thus for the first time fulfilling the promise of photon-counting detectors for very accurate structure factor measurements.

Supporting information

cif

Crystallographic Information File (CIF) https://doi.org/10.1107/S1600576720003775/kc5106sup1.cif
Contains datablock I

hkl

Structure factor file (CIF format) https://doi.org/10.1107/S1600576720003775/kc5106Isup2.hkl
Contains datablock I

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S1600576720003775/kc5106sup3.pdf
Additional figures and tables

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S1600576720003775/kc5106sup4.pdf
Plots of exposure time at constant attentuation

pdf

Portable Document Format (PDF) file https://doi.org/10.1107/S1600576720003775/kc5106sup5.pdf
Plots of attenuation at constant exposure time

zip

Zip compressed file https://doi.org/10.1107/S1600576720003775/kc5106sup6.zip
Additional XD files for FeSb2

zip

Zip compressed file https://doi.org/10.1107/S1600576720003775/kc5106sup7.zip
Additional XD files for rubrene

CCDC reference: 1990530

Computing details top

Program(s) used to refine structure: Volkov et al., (2006); molecular graphics: Volkov et al., (2006); software used to prepare material for publication: Volkov et al., (2006).

(I) top
Crystal data top
a = 26.7958 (18) ÅV = 2716.1 (3) Å3
b = 7.1586 (5) ÅZ = 4
c = 14.1598 (11) ÅCell parameters from 9573 reflections
α = 90°θ = 2.2–20.1°
β = 90°T = 20 K
γ = 90°
Data collection top
Rint = 0.047k =
h = l =
Refinement top
Refinement on F2175 parameters
Least-squares matrix: full0 restraints
R[F2 > 2σ(F2)] = 0.038 w2 = 1/[s2(Fo2)]
wR(F2) = 0.025(Δ/σ)max < 0.001
S = 1.03Δρmax = 0.19 e Å3
26442 reflectionsΔρmin = 0.17 e Å3
Fractional atomic coordinates and isotropic or equivalent isotropic displacement parameters (Å2) top
xyzUiso*/Ueq
C10.527359 (2)00.50.005
C20.553273 (1)0.144732 (4)0.549013 (2)0.005
C30.526872 (1)0.296485 (4)0.587617 (2)0.005
C40.552186 (1)0.448163 (5)0.634051 (3)0.007
C50.526568 (1)0.591265 (5)0.675635 (3)0.008
C60.607681 (1)0.135037 (4)0.572756 (2)0.006
C70.623084 (1)0.023845 (5)0.648770 (3)0.008
C80.672640 (2)0.025107 (6)0.679443 (3)0.009
C90.707480 (2)0.140262 (6)0.634825 (3)0.01
C100.692331 (1)0.252881 (6)0.559422 (3)0.009
C110.642978 (1)0.249454 (5)0.528376 (3)0.007
H40.592620.4477160.6361650.021
H50.5466160.7033530.7109610.021
H70.5956010.0626530.6843690.021
H80.6834790.0631870.7382950.025
H90.7459390.1433220.6589250.026
H100.7190640.3438990.5246530.025
H110.6315750.33670.4696710.021
Atomic displacement parameters (Å2) top
U11U22U33U12U13U23
C10.004675 (10)0.004714 (10)0.005698 (11)000.001007 (8)
C20.004862 (7)0.004918 (7)0.005903 (8)0.000187 (6)0.000163 (6)0.000931 (6)
C30.005485 (8)0.004817 (7)0.005858 (8)0.000225 (6)0.000005 (6)0.001021 (6)
C40.006767 (9)0.005983 (8)0.007680 (9)0.000988 (7)0.000324 (7)0.001989 (7)
C50.008343 (10)0.005959 (8)0.008402 (10)0.000730 (7)0.000230 (7)0.002360 (7)
C60.005008 (7)0.005938 (8)0.005954 (8)0.000493 (6)0.000224 (6)0.000095 (6)
C70.006838 (9)0.008906 (10)0.006967 (9)0.000727 (7)0.000760 (7)0.001564 (7)
C80.007731 (10)0.011965 (12)0.008345 (10)0.000247 (8)0.002070 (8)0.001426 (8)
C90.006031 (9)0.012166 (12)0.010684 (12)0.000279 (8)0.001450 (8)0.000472 (9)
C100.005667 (8)0.009553 (10)0.011155 (12)0.001240 (8)0.000692 (8)0.000280 (8)
C110.005938 (8)0.007348 (9)0.008293 (9)0.000747 (7)0.000503 (7)0.001046 (7)
H40.0116430.0234630.0292140.0017210.0004620.005032
H50.0223690.0166760.0234440.0059150.0018620.007394
H70.0181330.0241190.0221880.005090.0018080.008126
H80.0235010.0303240.0210750.002050.0061040.010101
H90.0122790.0359520.0310590.0019450.006850.002949
H100.0170360.0266970.0304070.0077150.0031910.006673
H110.0210590.0221560.0207840.000160.0018670.009474
Geometric parameters (Å, º) top
C1—C1i1.4662C6—C71.4009
C1—C1ii1.4662C6—C111.4001
C1—C21.4273C7—C81.3971
C1—C2iii1.4273C7—H71.0862
C2—C31.4069C8—C91.3965
C2—C61.4978C8—H81.0855
C3—C3ii1.4401C9—C101.3981
C3—C41.4392C9—H91.0858
C4—C51.3665C10—C111.3938
C4—H41.0839C10—H101.0863
C5—C5ii1.4238C11—H111.0837
C5—H51.0875
C1iv—C1—C2119.1102C2—C6—C7119.0503
C1iv—C1—C2119.1103C2—C6—C11121.9844
C1iv—C1—C2119.1102C7—C6—C11118.5693
C1iv—C1—C2119.1103C6—C7—C8121.0107
C2iv—C1—C2121.7795C6—C7—H7118.7326
C1—C2—C3120.3167C8—C7—H7120.2519
C1—C2—C6123.3016C7—C8—C9119.9037
C1—C2—C3120.3167C7—C8—H8119.2871
C1—C2—C6123.3016C9—C8—H8120.8075
C3—C2—C6115.9772C8—C9—C10119.4572
C2—C3—C3120.1874C8—C9—H9120.2786
C2—C3—C4121.5367C10—C9—H9120.2615
C3—C3—C4118.1188C9—C10—C11120.4101
C3—C4—C5121.7128C9—C10—H10120.0337
C3—C4—H4118.7840C11—C10—H10119.5561
C5—C4—H4119.5025C6—C11—C10120.6420
C4—C5—C5120.1551C6—C11—H11119.4032
C4—C5—H5120.2102C10—C11—H11119.9533
C5—C5—H5119.6028
Symmetry codes: (i) x+3/2, y+1/2, z+1; (ii) x+3/2, y+1/2, z; (iii) x, y, z+1; (iv) x, y, z+1.
 

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