Laser Heating on Beamline I15 at Diamond
Transcription
Laser Heating on Beamline I15 at Diamond
Laser Heating on Beamline I15 at Diamond Dominik Daisenberger, Simone Anzellini, Annette Kleppe, Allan Ross, Jon Thompson, Stuart Gurney, David Hawkins and Heribert Wilhelm Diamond Light Source, Harwell Science and Innovation Campus, Didcot, OX11 0DE, U.K. www.diamond.ac.uk/Beamlines/Engineering-and-Environment/I15 MAIN COMPONENTS OF THE EXTREME CONDITIONS BEAMLINE (I15) BEAMLINE LAYOUT • Insertion device: superconducting multi-pole wiggler • Si(111) Bragg double-crystal monochromator: E = 20-80 keV • Pair of 1 m long KB mirrors: minimum focal spot size ~70 μm Station 1: 6-circle diffractometer • Minimum (collimated) beam size 20 μm • Powder and single-crystal diffraction, pair distribution function measurements • High pressure (DAC), resistive heating, and low-temperature (T > 8 K) experiments Station 2: X-ray micro-focusing and laser heating • Pair of 30 cm long KB mirrors: minimum focal spot size ~8 μm • Double sided YAG laser heating currently being commissioned • DAC powder diffraction Detectors: MAR345, Perkin Elmer flat panel, Atlas CCD, Pilatus 100K SCHEMATIC OF THE ON-LINE LASER HEATING SET-UP DIAMOND ANVIL CELL LASER HEATING • Double-sided (2 x 100 W) laser YAG heating (λ = 1090 nm) in onaxis configuration (see schematic to the right and photos below). • Apochromatic objectives L1 focus the lasers onto the sample and collect thermal emission spectra. • Dichroic mirrors (DM) separate laser and visible light. • L2 focuses the light onto spectrometer entrance (15x magnification). • A mirror with two, vertically separated, pinholes provides the spectrometer entrance pupils. • A CCD camera records the sample image superimposed on the entrance pupil (via beam splitter and Navitar Zoom objective). This allows the spectrometer entrance pupil to be aligned to the laser and X-ray beams. • Thermal-emission spectra of up- and downstream sides of the sample are recorded on different stripe of the spectrometer CCD. • The sample temperature is obtained from a fit of Planck and Wien functions to the emission spectra. ON-LINE LASER HEATING SYSTEM AT BEAMLINE I15 L1 PH TM L1 TM The sample stage of the on-line laser heating system. The laser beams are focussed and directed onto the sample with lenses L1 and mirrors TM, respectively. XRD Detector Carbon fibre strut m-KBs LED Spectrometer L2 DAC HKHKHK On-line laser heating system at I15. Photograph taken at roughly 45° to the upstream X-ray beam direction, showing the breadboard mounted on the station 2 table. The optical system is adjacent to the micro-focussing KB-mirror vessel (left) and the X-ray detector. The location of some components is indicated. The entire optical system is mounted on a motorised breadboard, attached to the table of station 2. The breadboard can move horizontally and vertically with respect to the X-ray path. The objectives L1 and Xray transparent mirrors TM are attached to the breadboard via a carbon fibre strut. The entire optical system can therefore be translated independently of the sample. This simplifies the alignment of the optical system to the sample which is centred to the X-ray beam. For remote control of laser heating experiments objectives L1 are motorised individually. In addition L1 and TM can also travel back along the carbon fibre strut towards the breadboard to facilitate change of DACs on the sample stage. Temperature information will be saved together with the diffraction data in Nexus data format. f Acknowledgements: We thank M. Walter for fruitful discussions and Lee Hudson for technical support. The laser-heating project is supported by NERC grant NE/M000117/1.