2011
DOI: 10.1107/s0909049511004250
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Revealing low-dose radiation damage using single-crystal spectroscopy

Abstract: The structural information and functional insight obtained from X-ray crystallography can be enhanced by the use of complementary spectroscopies. Here the information that can be obtained from spectroscopic methods commonly used in conjunction with X-ray crystallography and best-practice single-crystal UV-Vis absorption data collection are briefly reviewed. Using data collected with the in situ system at the Swiss Light Source, the time and dose scales of low-dose X-ray-induced radiation damage and solvated el… Show more

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Cited by 18 publications
(16 citation statements)
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References 32 publications
(44 reference statements)
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“…Note the rates we compare range from 126 kGy/s (monochromatic) to 4,500 kGy/s (pink beam, during the pulse), much higher than those considered earlier. 17 We consider three typical rates: monochromatic beam, characteristic of ID beamlines at a 3 rd generation synchrotron source; pink beam, produced at ID beamlines without the use of a monochromator; and an x-ray free electron laser beam, such as the one generated at LCLS. Experimentally, we observed greater than ~6.7×10 6 photons/µm 2 to ~1.1×10 7 photons/µm 2 (corresponding to 7.6×10 3 Gy to 1.3×10 4 Gy, note that this was calculated using the full sample thickness at an energy of 7.1keV) as the dosage limit for 5% damage from ~1mm of sample (monochromatic beam), 5 while the model calculations for such a thickness indicate a dosage threshold at ~2.5×10 6 photons/µm 2 (corresponding to 2.8×10 3 Gy, given the same parameters).…”
Section: Resultsmentioning
confidence: 99%
“…Note the rates we compare range from 126 kGy/s (monochromatic) to 4,500 kGy/s (pink beam, during the pulse), much higher than those considered earlier. 17 We consider three typical rates: monochromatic beam, characteristic of ID beamlines at a 3 rd generation synchrotron source; pink beam, produced at ID beamlines without the use of a monochromator; and an x-ray free electron laser beam, such as the one generated at LCLS. Experimentally, we observed greater than ~6.7×10 6 photons/µm 2 to ~1.1×10 7 photons/µm 2 (corresponding to 7.6×10 3 Gy to 1.3×10 4 Gy, note that this was calculated using the full sample thickness at an energy of 7.1keV) as the dosage limit for 5% damage from ~1mm of sample (monochromatic beam), 5 while the model calculations for such a thickness indicate a dosage threshold at ~2.5×10 6 photons/µm 2 (corresponding to 2.8×10 3 Gy, given the same parameters).…”
Section: Resultsmentioning
confidence: 99%
“…27 Various online spectroscopic techniques have been developed to monitor the redox state of metals in crystals. [80][81][82] Strategies to mitigate such reduction include merging of composite, low dose partial datasets 83 or helical data collection approaches. 84 Use of rapid X-ray detectors and cryogenic temperatures -typically 100 K -minimises but does not eliminate the effects of photoreduction or radiation damage to crystals.…”
Section: Xfel Structures Of Intact Redox States Of Cunirs By Serial Fmentioning
confidence: 99%
“…At 100 K aqueous electrons can move through the unit cell and rapidly react, with the result that their spectroscopic signature rapidly reaches a maximum (at $45 kGy; Owen et al, 2011) and then decays (Fig. 4).…”
Section: Figurementioning
confidence: 99%