LINXS Christmas Open House
…neutron science. Take the chance to meet with colleagues in the LINXS community! For those of you who are not familiar with how LINXS work, this is an excellent opportunity…
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Beamline optics
…coherent part of the beam, generating a new virtual source for the experimental stations. NanoMAX beamline optics layout The optical beamline components for the beam shaping and beam transport up…
Beamline optics
FemtoMAX performance2024 Energy range 1.8 -15 keV (0.8 – 6.8 Å) Photon source 2 x in-vacuum undulators U15 Monochromator Double Crystal Monochromator with InSb(111) crystals. 3 x Multi-Layer Mirror Photons…
Merry Christmas and a happy New Year!
…it would have been possible without your support and engagement. Despite our financial difficulties, we have committed to remain open for business 2024. Looking forward to a new year of…
Accelerators
…an operator. We are responsible for delivering a stable high-quality beam to the users. This means operating and controlling the accelerator complex consisting of the 3 GeV linac, the 1.5…
Solid-state end station
The solid-state end station (SSES) is designed for studying solid-state material via advanced experimental techniques in an ultra-high vacuum (UHV) environment. The end station is composed of four UHV chambers…
Atomic Force Microscope
…in late 1990-ies. Despite seemingly old, it is still competitive with the brand-new AFMs in terms of high-resolution topography determination. It is capable of both contact and tapping modes, allowing…
Sample holders
…OMNY pin sample holders for the NanoMAX Imaging Station. Left: sample pins compatible usable at the NanoMAX imaging station. Sample preparation and mounting is essential for a successful beamtime. Discuss…
Access modes
…of fast access proposals can be found here. Proprietary access chevron_right The complete beamline setup is available for Proprietary users, please contact the MAX IV Industrial Relations Office for further…
Technical Notes
R3 beam dynamics High-Chromaticity_Optics_for_the_MAX_IV_3_GeV_Storage_Ring.pdf Internal_Note_20090902_Updated_Lattice_120614.pdf Internal_Note_20100318_Updated_Lattice_120614.pdf Internal_Note_20100512_Pulsed_Magnet_Injection_120612.pdf Internal_Note_20101101_Updated_Lattice_120614.pdf Internal_Note_20101203_Magnet_Synchronization_120612.pdf Internal_Note_20110117_Updated_Lattice_120612.pdf Internal_Note_20111124_Updated_Lattice_120611.pdf Internal_Note_20121107_Updated_Lattice_140129.pdf Internal_Note_20130724_OCO_Modeling_141009.pdf Internal_Note_20150129_MIK_Analysis_150130.pdf Internal_Note_20150930_MW_Threshold.pdf insertion devices Internal_Note_20090922_Insertion_Devices_for_the_MAX_IV_3_GeV_Storage_Ring.pdf Internal_Note_20100215_Insertion_Devices_for_the_MAX_IV_3_GeV_Ring.pdf Internal_Note_20101209_Elliptically_Polarising_Undulators_with_11_mm_Magnetic_Gap_at_the_MAX_IV_3_GeV_Ring.pdf Internal_Note_20111110_Comparison_Brilliance_MAX_IV_NSLS-II.pdf Internal_Note_20111220_Elliptically_polarizing_undulators_for_the_Arpes_beamline_at_the_Solaris_Light_Source.pdf RF cavities Internal_Note_20240410 Harmonic Cavity Parameters for Flat…