000192786 001__ 192786 000192786 005__ 20250717112634.0 000192786 0247_ $$2doi$$a10.1063/1.4902141 000192786 0247_ $$2ISSN$$a0034-6748 000192786 0247_ $$2ISSN$$a1089-7623 000192786 0247_ $$2WOS$$aWOS:000345646000266 000192786 0247_ $$2pmid$$apmid:25430117 000192786 0247_ $$2altmetric$$aaltmetric:21824448 000192786 0247_ $$2openalex$$aopenalex:W2018773381 000192786 037__ $$aPUBDB-2014-04315 000192786 082__ $$a530 000192786 1001_ $$0P:(DE-H253)PIP1014388$$aPatt, M.$$b0$$eCorresponding Author 000192786 245__ $$aBulk sensitive hard x-ray photoemission electron microscopy 000192786 260__ $$a[S.l.]$$bAmerican Institute of Physics$$c2014 000192786 3367_ $$00$$2EndNote$$aJournal Article 000192786 3367_ $$2DRIVER$$aarticle 000192786 3367_ $$0PUB:(DE-HGF)16$$2PUB:(DE-HGF)$$aJournal Article$$bjournal$$mjournal$$s1447850243_18013 000192786 3367_ $$2BibTeX$$aARTICLE 000192786 500__ $$3POF3_Assignment on 2016-02-15 000192786 500__ $$3POF3_Prefill: G:(DE-HGF)POF3-6214 000192786 500__ $$a(c) AIP Publishing LLC. 000192786 520__ $$aHard x-ray photoelectron spectroscopy (HAXPES) has now matured into a well-established technique as a bulk sensitive probe of the electronic structure due to the larger escape depth of the highly energetic electrons. In order to enable HAXPES studies with high lateral resolution, we have set up a dedicated energy-filtered hard x-ray photoemission electron microscope (HAXPEEM) working with electron kinetic energies up to 10 keV. It is based on the NanoESCA design and also preserves theperformance of the instrument in the low and medium energy range. In this way, spectromicroscopy can be performed from threshold to hard x-ray photoemission. The high potential of the HAXPEEM approach for the investigation of buried layers and structures has been shown already on a layered and structured SrTiO3 sample. Here, we present results of experiments with test structures to elaborate the imaging and spectroscopic performance of the instrument and show the capabilities of the method to image bulk properties. Additionally, we introduce a method to determine the effective attenuation length of photoelectrons in a direct photoemission experiment. 000192786 536__ $$0G:(DE-H253)POF2-P09-20130405$$aPETRA Beamline P09 (POF2-54G14)$$cPOF2-54G14$$fPOF II$$x0 000192786 588__ $$aDataset connected to CrossRef, bib-pubdb1.desy.de 000192786 693__ $$0EXP:(DE-H253)P-P09-20150101$$1EXP:(DE-H253)PETRAIII-20150101$$6EXP:(DE-H253)P-P09-20150101$$aPETRA III$$fPETRA Beamline P09$$x0 000192786 7001_ $$0P:(DE-H253)PIP1012885$$aWiemann, C.$$b1 000192786 7001_ $$0P:(DE-H253)PIP1012892$$aWeber, N.$$b2 000192786 7001_ $$0P:(DE-H253)PIP1012889$$aEscher, M.$$b3 000192786 7001_ $$0P:(DE-H253)PIP1007694$$aGloskovskii, A.$$b4 000192786 7001_ $$0P:(DE-H253)PIP1002684$$aDrube, W.$$b5 000192786 7001_ $$0P:(DE-H253)PIP1014409$$aMerkel, M.$$b6 000192786 7001_ $$0P:(DE-H253)PIP1012053$$aSchneider, C. 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