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Australian Synchrotron

The authors thank the National Health and Medical Research Council (NHMRC) of Australia for financial support, and their many collaborators who made this work possible, in particular Michael Quinn, Corey Evans and Max Diem. Mr Finlay Shanks is thanked for instrumental support and Mr Clyde Riley and Dr Virginia Billson (Royal Women s Hospital, Melbourne) for sectioning and histopathology advice, respectively. Ian Boundy (Department of Anatomy and Cell Biology, Monash University) is thanked for the tissue sectioning. Dr Wood is funded by an Australian Synchrotron Research Program Fellowship Grant and a Monash Synchrotron Research Fellowship. [Pg.220]

We want to acknowledge all the people who kindly provided material, especially about the early phase of SR IR and the most recent progresses in the field we tried to summarize. A special thanks to helpful friends and colleagues from ex-LURE and Daresbury facilities, as well as from SOLEIL, ANKA, BESSY, MAX, Elettra, ESRF, the Hefei and Australian Synchrotrons, CLS, ALS, NSLS and SRC. One of the Authors (GC) wants also to thank Paul Dumas and Oleg Chubar at Soleil for the SRW code and the help with simulations. [Pg.100]

Principal Scientist, Infrared Beamline, Australian Synchrotron, Clayton, Victoria 3168, Clayton, Australia School of Chemistry, University of Nottingham, University Park, Nottingham NG7 2RD, UK CR-UK Research Fellow. Faculty of Medicine and Health, University of Leeds, UK Senior Lecturer/Hon. Consultant in Maxillofacial Surgery, Faculty of Medicine and Health, University of Leeds, UK Faculty of Medicine and Health, Floor 6, Worsley Building, Clarendon Way, Leeds, West Yorkshire, UK, LS2 9LU... [Pg.291]

We are grateful to the Australian Research Council (ARC) for Discovery grants an ARC Postdoctoral Fellowship (CPM) an ARC Professorial Fellowship (PAL) and ARC LIEF grants for the FTIR instrumentation and for National Health and Medical Research Council project grants 211040 and 352354 (TCS). This work was supported by the Australian Synchrotron Research Program, which is funded by the Commonwealth of Australia under the Major National Research Facilities Program. [Pg.82]

Figure 15.7 Comparison of RS and WF spectromicroscopy for Cicada Wing. Chemical intensity maps of amide II and CHj absorbance bands obtained by integration of the respective bands (amide II 1588-1483 cm-, v,5 CHj 2931 2913 cm- ), (a), (b), and (c) represent the images obtained from the IR scans performed at the RS spectromicroscopy beamline at the Australian Synchrotron while (d) to (i) are the respective images obtained from the WF spectromi-crscopy IRENI beamline. The intensities of the integrated area of the amide II band (a, d, and g) and CHj antisymmetric stretching (b, e, and h) are shown in consistent color... Figure 15.7 Comparison of RS and WF spectromicroscopy for Cicada Wing. Chemical intensity maps of amide II and CHj absorbance bands obtained by integration of the respective bands (amide II 1588-1483 cm-, v,5 CHj 2931 2913 cm- ), (a), (b), and (c) represent the images obtained from the IR scans performed at the RS spectromicroscopy beamline at the Australian Synchrotron while (d) to (i) are the respective images obtained from the WF spectromi-crscopy IRENI beamline. The intensities of the integrated area of the amide II band (a, d, and g) and CHj antisymmetric stretching (b, e, and h) are shown in consistent color...
Chapter 7, Australian Synchrotron, 800 Blackburn Rd, Clayton, Australia Elena P. Ivanova... [Pg.174]

The discovery of a prompt radio burst is related to the epoch of shock break-out was an important Australian contribution to the studies of SN1987A. The burst lasted for only about a week, (Turtle et al. ), and can be understood in terms of free-free absorption of synchrotron emission (Storey and Manchester). The location of this radio emission was probably in the shocked stellar wind region of the star, with the free-free absorption arising from within this layer. The thickness of the emitting layer was estimated at only 4.8% of the radius, which would be consistent with a power law density distribution of matter with an index of 11.8. Since the first week, the radio emission continued to fade (despite some other reports to the contrary), becoming effectively unobservable at 843MHz after about 50 days. [Pg.268]

Monash Centre for Synchrotron Science, The Australian Centre for Electromateriafs Science and School of Chemistry, Monash University, Melbourne 3800, Australia... [Pg.155]

Figure 3.10 Schematic of the Australian Infrared beamline showing (from right) synchrotron beam entering front end optics (Ml, M2, M3, M3a mirrors), diamond exit window, beamsplitter optics vessel and matching optics boxes for the two end station instruments. (Courtesy of Mark Tobin.)... Figure 3.10 Schematic of the Australian Infrared beamline showing (from right) synchrotron beam entering front end optics (Ml, M2, M3, M3a mirrors), diamond exit window, beamsplitter optics vessel and matching optics boxes for the two end station instruments. (Courtesy of Mark Tobin.)...

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See also in sourсe #XX -- [ Pg.33 ]




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