The scientific aim at ISISS is to study the electronic surface/near surface structure of functional materials in the presence of a reactive environment. This includes both gas/solid interfaces (e.g. heterogeneous catalysis) and liquid/solid interfaces (e.g. catalytic water splitting).

Fig. 1: Optical beamline layout <br>

Fig. 1: Optical beamline layout

Station data
Temperature range room temperature up to 1000 K
Pressure range Maximum pressure: 20 mbar
Minimum pressure: 10-8 mbar
Typical pressure: 1 mbar

For more details contact the instrument scientist.
More details ISISS station
Beamline data
Segment L04
Location (Pillar) 6.1
Source D41 (Dipole)
Monochromator PGM
Energy range 80 - 2000 eV
Energy resolution >15,000 at 400eV
Flux 6x1e10 photons/s/0.1A with 111µm exit slit
Polarisation linear horizontal
Divergence horizontal 2 mrad
Divergence vertical 2.4 mrad
Focus size (hor. x vert.) 100x80 µm2
User endstation not possible
Distance Focus/last valve 870 mm
Height Focus/floor level 1405 mm
Beam availability 24h/d, operation in TRIBS mode possible
Phone +49 30 8062 14905 / 14906
Fig. 2: Scheme of ISISS approach <br><br><br>

Fig. 2: Scheme of ISISS approach

Fig. 3: Typical photon flux at sample position (with 50nm SiNx pressure resistant membrane) <br><br><br>

Fig. 3: Typical photon flux at sample position (with 50nm SiNx pressure resistant membrane)

Fig. 4: Impact of higher diffraction orders at varying c-value (simulation) <br><br><br>

Fig. 4: Impact of higher diffraction orders at varying c-value (simulation)

ISISS (Innovative Station for In Situ Spectroscopy) is a project of the Inorganic Chemistry department of the Fritz-Haber-Institut der Max-Planck-Gesellschaft (FHI), Max Planck Institute for Chemical Energy Conversion (MPI-CEC), and HZB/BESSY II in Berlin. The purpose of the ISISS facility is to provide access for a large community to surface sensitive gas/solid interface characterisation methodologies in the presence of a reactive gas, i.e. in situ under conditions equal to or close to reality. The working area of the facility is material science in general and catalysis in particular. Our approach includes 3 units that have to complement on another: a state of the art soft X-ray beamline, an endstation for ambient pressure X-ray photoelectron (NAP-XPS) and X-ray absorption spectroscopy (XAS), and an infrastructure on site to perform experiments with a chemical background. In contrast to standard vacuum surface science experiments, in situ experiments require the installation of a complex gas feed and an elaborated gas analytic to follow the conversion of the gas phase during the reaction.


 The beamline has to accommodate for a variety of user requirements resulting from the scientific approach as outlined above. The basic design considerations are as follows: 

  • A variety of materials with a large diversity in composition should be characterised and diverse scientific problems should be tackled. This requires a beamline that is adaptable to the needs of the users. This comprises a high flexibility concerning the provided photon energy range and spectral resolution.
  • Due to the compounds usually studied in catalyst research, the available photon flux at energies between 400 eV and 1200 eV is the main concern covering e.g. the C1s, N1s, O1s and transition metal 2p core levels.
  • The X-ray spot size at the sample position is optimised for a best fit to the electrostatic lens system of the in situ apparatus and the electron analyser.
  • The beamline should be easy to handle to allow for multi-user operation without elaborated knowledge of technical details.
  • An accurate and reliable energy calibration should be feasible as an essential part of high quality XPS studies.

The design considerations resulted in the selection of a plane grating monochromator (PGM). This PGM design is a development based on the Petersen type monochromator at BESSY at which the light is colliminated in the dispersive plane in front of the grating by the mirror M1. In this design, the fix focus constant c = (cos β / cos α) (α: angle of incidence, β: angle of diffraction relative to the grating normal, respectively) is kept constant during the scanning of the photon energy. This allows the free adjustment of the fix-focus constant without movement of the exit slit which can be used to easily optimise the monochromator to the requirements of the users.