000154947 001__ 154947
000154947 005__ 20210407175446.0
000154947 037__ $$aDESY-2013-01181
000154947 041__ $$aEnglish
000154947 1001_ $$0P:(DE-H253)PIP1007496$$aLiermann, Hanns-Peter$$b0$$eCorresponding author
000154947 245__ $$aCurrent and future developments of dynamic experiments at extremes at DESY and the European XFEL$$f2011-05-24
000154947 3367_ $$0PUB:(DE-HGF)31$$2PUB:(DE-HGF)$$aTalk (non-conference)$$btalk$$mtalk$$s1397720785_12942$$xInvited
000154947 3367_ $$2DINI$$aOther
000154947 3367_ $$2BibTeX$$aINPROCEEDINGS
000154947 3367_ $$033$$2EndNote$$aConference Paper
000154947 502__ $$cBrookhaven National Laboratory
000154947 520__ $$aIn December 2010 the Extreme Condition Beamline (ECB) at PETRA III (3rd generation source) DESY, received first beam and entered the commissioning phase. At the same time the High-Energy Density Matter Experiment (HED) at the European XFEL has entered its design phase. Both beamlines will be used in to conducted dynamic diffraction and spectroscopy experiments. Within this presentation we outline some of the current capabilities of the ECB to conducted dynamic diffraction experiments at extreme conditions. Furthermore, we give an outlook on possible future developments of single exposure and pump and probe techniques that can be used at the ECB at PETRA III and HED once the XFEL becomes operational in 2015.
000154947 536__ $$0G:(DE-H253)POF2-P02.2-20140410$$aPETRA Beamline P02.2 (POF2-54G14)$$cPOF2-54G14$$fPOF II$$x0
000154947 693__ $$0EXP:(DE-H253)P-P02.2-20150101$$1EXP:(DE-H253)PETRAIII-20150101$$6EXP:(DE-H253)P-P02.2-20150101$$aPETRA III$$fPETRA Beamline P02.2$$x0
000154947 7001_ $$0P:(DE-H253)PIP1001329$$aTschentscher, Thomas$$b1
000154947 7001_ $$0P:(DE-H253)PIP1013606$$aKonopkova, Zuzana$$b2
000154947 7001_ $$0P:(DE-H253)PIP1006769$$aMorgenroth, Wolfgang$$b3
000154947 7001_ $$0P:(DE-H253)PIP1010563$$aPetitgirard, Sylvain$$b4
000154947 7001_ $$0P:(DE-H253)PIP1005928$$aFranz, Hermann$$b5
000154947 773__ $$y2011
000154947 909CO $$ooai:bib-pubdb1.desy.de:154947$$pVDB
000154947 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1007496$$aDeutsches Elektronen-Synchrotron$$b0$$kDESY
000154947 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1001329$$aDeutsches Elektronen-Synchrotron$$b1$$kDESY
000154947 9101_ $$0I:(DE-588b)16047298-2$$6P:(DE-H253)PIP1001329$$aThe European X-Ray Laser Project XFEL$$b1$$kXFEL
000154947 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1013606$$aExternes Institut$$b2$$kExtern
000154947 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1006769$$aDeutsches Elektronen-Synchrotron$$b3$$kDESY
000154947 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1006769$$aExternes Institut$$b3$$kExtern
000154947 9101_ $$0I:(DE-HGF)0$$6P:(DE-H253)PIP1010563$$aExternes Institut$$b4$$kExtern
000154947 9101_ $$0I:(DE-588b)2008985-5$$6P:(DE-H253)PIP1005928$$aDeutsches Elektronen-Synchrotron$$b5$$kDESY
000154947 9131_ $$0G:(DE-HGF)POF2-54G14$$1G:(DE-HGF)POF2-540$$2G:(DE-HGF)POF2-500$$3G:(DE-HGF)POF2$$4G:(DE-HGF)POF$$9G:(DE-H253)POF2-P02.2-20140410$$aDE-H253$$bStruktur der Materie$$lForschung mit Photonen, Neutronen, Ionen$$vPETRA III$$x0
000154947 9141_ $$y2011
000154947 9201_ $$0I:(DE-H253)FS-PE-20120731$$kFS-PE$$lExperimentebetreuung PETRA III$$x0
000154947 9201_ $$0I:(DE-H253)Eur_XFEL-20120731$$kEur.XFEL$$lEuropean XFEL$$x1
000154947 980__ $$atalk
000154947 980__ $$aVDB
000154947 980__ $$aUNRESTRICTED
000154947 980__ $$aI:(DE-H253)FS-PE-20120731
000154947 980__ $$aI:(DE-H253)Eur_XFEL-20120731