000154651 001__ 154651
000154651 005__ 20210407101424.0
000154651 037__ $$aDESY-2013-01010
000154651 041__ $$aEnglish
000154651 1001_ $$0P:(DE-H253)PIP1010228$$aBurkhardt, Anja$$b0$$eCorresponding author
000154651 1112_ $$a28th Meeting of the European Crystallographic Association$$cWarwick$$d2013-08-25 - 2013-08-29$$gECM28$$wUnited Kingdom
000154651 245__ $$aThe Crystallography Endstation at Beamline P11 at PETRA III
000154651 260__ $$c2013
000154651 3367_ $$0PUB:(DE-HGF)24$$2PUB:(DE-HGF)$$aPoster$$bposter$$mposter$$s1383833880_14422
000154651 3367_ $$2DRIVER$$aconferenceObject
000154651 3367_ $$2BibTeX$$aINPROCEEDINGS
000154651 3367_ $$033$$2EndNote$$aConference Paper
000154651 502__ $$cWarwick University
000154651 520__ $$aBeamline P11 at PETRA III is dedicated to imaging anddiffraction experiments of biological samples. Thebeamline provides two experimental endstations: anX-ray microscope and a crystallography experiment.The P11 X-ray optics consist of a LN2 cooled doublecrystal monochromator and two horizontal deflectingand one vertical deflecting X-ray mirrors. The mirrorsare dynamically bendable and are used to generate anintermediate focus at 65.5 m from the source with a sizeof 16 × 96 μm2 rms (v × h).The crystallography endstation is installed on top of a 8meter long granite block which is the key element of theP11 experimental hutch. The sample position is locatedat 72.9 m from the source. A CVD diamond basedX-ray feedback system provides a long term beamposition stability of better than 1 μm. Thecrystallography experiment is equipped with a highprecision single axis goniometer with a combinedsphere of confusion of smaller than 100 nm. Theinstrument provides an on-axis microscope for easycrystal centering and beam alignment. Diffractionexperiments can be performed at energies between4 and 30 keV. The beamsize can be adjusted between6 × 12 μm2 FWHM (v × h) with a photon flux of about2 × 1012 ph/s and 300 × 300 μm2 FWHM (v × h) with1 × 1013 ph/s. Due to the very small beam divergenceP11 is ideally suited to measure large unit cell systems,such as viruses or large molecular complexes. Thebeamline is equipped with a Pilatus 6M-F detectorwhich allows fast data collection with frame rates of upto 25 Hz. In addition to the standard data collectionfeatures the beamline control software at P11 provides agrid scan capability for crystal centering andmeasurement of micro crystals (with and without crystalrotation) and an interface for serial crystallography. Anautomatic sample changer is under construction and willbe available to users in 2014. The robot will be able tomount samples within 10 s and the large dewar willallow storage of more than 300 samples.
000154651 536__ $$0G:(DE-H253)POF2-P11-20130405$$aPETRA Beamline P11 (POF2-54G14)$$cPOF2-54G14$$fPOF II$$x0
000154651 693__ $$0EXP:(DE-H253)P-P11-20150101$$1EXP:(DE-H253)PETRAIII-20150101$$6EXP:(DE-H253)P-P11-20150101$$aPETRA III$$fPETRA Beamline P11$$x0
000154651 7001_ $$0P:(DE-H253)PIP1001724$$aReime, Bernd$$b1
000154651 7001_ $$0P:(DE-H253)PIP1007563$$aPakendorf, Tim$$b2
000154651 7001_ $$0P:(DE-H253)PIP1013364$$aRoever, Jan$$b3
000154651 7001_ $$0P:(DE-H253)PIP1017872$$aWarmer, Martin$$b4
000154651 7001_ $$0P:(DE-H253)PIP1011949$$aGoeries, Dennis$$b5
000154651 7001_ $$0P:(DE-H253)PIP1015025$$aStuebe, Nicolas$$b6
000154651 7001_ $$0P:(DE-H253)PIP1016998$$aMeyer, Jan$$b7
000154651 7001_ $$0P:(DE-H253)PIP1000022$$aPanneerselvam, Saravanan$$b8
000154651 7001_ $$0P:(DE-H253)PIP1011948$$aFischer, Pontus$$b9
000154651 7001_ $$0P:(DE-H253)PIP1006208$$aMeents, Alke$$b10
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000154651 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1006208$$aDeutsches Elektronen-Synchrotron$$b10$$kDESY
000154651 9131_ $$0G:(DE-HGF)POF2-54G14$$1G:(DE-HGF)POF2-540$$2G:(DE-HGF)POF2-500$$3G:(DE-HGF)POF2$$4G:(DE-HGF)POF$$9G:(DE-H253)POF2-P11-20130405$$aDE-H253$$bStruktur der Materie$$lForschung mit Photonen, Neutronen, Ionen$$vPETRA III$$x0
000154651 9141_ $$y2013
000154651 9201_ $$0I:(DE-H253)FS-PE-20120731$$kFS-PE$$lExperimentebetreuung PETRA III$$x0
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