As of July 30, 2011 |
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for international journal X-Ray Spectrometry (John Wiley & Sons Ltd.) |
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Sciences | |||
Absolute K-shell photoionization for gas-phase atomic nitrogen (July 11, 2011) |
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So far, because of the difficulty of creating a target of neutral atomic
nitrogen, there have been no reports on the details of high-resolution K-edge
spectra. Recently, scientists at Lawrence Berkeley National Laboratory have
performed both experimental and theoretical studies on the strong 1s→np
resonance features throughout the threshold region. The absolute value of the
K-shell binding energy was experimentally obtained for the first time, and it
was 409.64±0.02
eV. For more information, see the paper,
"K-Shell X-Ray Spectroscopy of Atomic Nitrogen", M. M. Sant’Anna et al., Phys.
Rev. Lett. 107, 033001 (2011). |
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Real-time analysis of martensitic phase transition of cobalt (June 30, 2011) |
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Professor
K. F. Ludwig (Boston University, USA) and his colleagues have recently reported
their
real-time X-ray scattering
studies on
heterogeneous microscale dynamics in the martensitic phase transition of
cobalt. During the transformation of the high-temperature fcc phase to the
low-temperature hcp phase, first, a rapid local transformation happens, and
then, strains are relaxed slowly. The research group employed coherent X-ray
scattering measurements to see the latter part of the transformation. It was
found that the kinetics is dominated by discontinuous sudden changes -
avalanches. The spatial size of observed avalanches varies widely, from 100 nm
to 10μm, the size of the X-ray beam. For more information, see the paper,
"Direct Measurement of Microstructural Avalanches during the Martensitic
Transition of Cobalt Using Coherent X-Ray Scattering", C. Sanborn et al., Phys.
Rev. Lett. 107, 015702 (2011). |
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3D micro analysis of the Dead Sea Scrolls (June 29, 2011) |
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The Dead Sea Scrolls are a collection of 972 texts from the Hebrew Bible and
extra-biblical documents found between 1947 and 1956 at Khirbet Qumran on the
northwest shore of the Dead Sea from which it derives its name, in the British
Mandate for Palestine, in what is now named the West Bank. Recently, a research
group led by Professor B. Kanngiesser (Technische Universität Berlin, Germany)
has investigated the feasibility of merging two X-ray techniques, ordinary micro
XRF and confocal 3D micro XRF for optimized analysis of highly inhomogeneous
samples such as the Dead Sea Scrolls. Ordinary micro XRF lacks information on
the depth, but the measurement is efficient and rather quick. On the other
hand, confocal 3D micro XRF has depth resolution, but the measurement takes very
long. The authors found that the reliability of the analysis of highly
heterogeneous samples can be improved by quantitatively combining both data.
For more information, see the paper,
"3D Micro-XRF for Cultural Heritage Objects: New Analysis Strategies for the
Investigation of the Dead Sea Scrolls", I. Mantouvalou et al., Anal. Chem.,
Article ASAP (DOI: 10.1021/ac2011262 Publication Date (Web): June 29, 2011). |
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3D micro X-ray spectroscopic analysis of natural diamond formed in ultra-deep underground (June 27, 2011) |
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A research group led by Professor L. Vincze (Ghent University, Belgium) has
recently reported the interesting analysis of 1-20 μm sized inclusions in
natural diamond crystals from Rio Soriso (Juina area, Mato Grosso State,
Brazil). The crystals are called ultra-deep diamond, because they were formed
in the astenospheric upper mantle, the transition zone (410-670 km), and even
the lower mantle (>670 km) of the Earth. The experiment is basically 3D imaging
by confocal X-ray fluorescence suing synchrotron radiation. By scanning X-ray
energy near the Mn and Fe K absorption edges, the authors obtained chemical
information on the inclusion cloud in the crystal. It was found that the
observed Fe-rich inclusions were ferropericlase (Fe,Mg)O, hematite and a mixture
of these two minerals. Another finding was that significant overprint of
inclusions along pre-existing planar features is possible without changing their
outer shape. For more information, see the paper,
"Three-Dimensional Fe Speciation of an Inclusion Cloud within an Ultradeep
Diamond by Confocal μ-X-ray Absorption Near Edge Structure: Evidence for Late
Stage Overprint", G. Silversmit et al., Anal. Chem., Article ASAP (DOI:
10.1021/ac201073s Publication Date (Web): June 27, 2011). |
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Resolution enhancement in ptychographic X-ray diffraction microscopy (June 13, 2011) |
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Ptychographic X-ray diffraction microscopy is known as an extension of so-called
X-ray diffraction microscopy, which is a lensless X-ray imaging technique based
on coherent diffraction measurements and iterative phasing methods. The
technique employs sample scanning to see a large viewing area, but so far, the
spatial resolution has been rather limited mainly because of positioning errors
due to the drift between the sample and illumination optics. Recently,
Professor Y. Takahashi (Osaka University, Japan) and his colleagues have
published an experimental way to resolve the problem. The research group has
developed a method of correcting positioning errors, and made it possible to
illuminate a highly focused hard X-ray beam at the exact position on the
samples. The spatial resolution achieved is as good as 10 nm or even better in
a viewing area of larger than 5 μm. For more information, see the paper,
"Towards high-resolution ptychographic X-ray diffraction microscopy", Y.
Takahashi et al., Phys. Rev. B83, 214109 (2011). |
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Theory of Kα emission efficiency under the irradiation of ultra short pulse laser (June 6, 2011) |
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When laser light hits thin solid foil, one can obtain soft X-rays, and this is
sometimes called a laser plasma X-ray source. When the peak power of the laser
becomes extremely high by shortening the pulse duration, it is also possible to
observe hard X-ray spectra including Kα and Kβ emission. A team at Sandia
National Laboratory has recently reported some calculations on the efficiency of
Kα emission. The conversion efficiency of laser energy into Kα X-ray energy is
clearly a critical parameter for designing an X-ray source. Basically the value
is fairly small, but the team’s simulations indicate that an enhancement of
efficiency greater than tenfold over conventional single targets may be possible
by introducing a two-phase target concept. For more information, see the paper,
"Efficiency Enhancement for Kα X-Ray Yields from Laser-Driven Relativistic
Electrons in Solids", A. B. Sefkow et al., Phys. Rev. Lett. 106, 235002
(2011). |
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Quantitative chemical imaging of trace elements using advanced synchrotron X-rays (May 31, 2011) |
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A Swiss group has recently published many interesting chemical images of trace
elements in heterogeneous media. The authors combined several techniques; laser
ablation inductively coupled plasma mass spectrometry (LA-ICPMS), synchrotron
radiation based micro-X-ray fluorescence and extended X-ray absorption fine
structure spectroscopy. The analysis was done for Opalinus clay, which has been
proposed as the host rock for high-level radioactive waste repositories. 2D
images were shown for the matrix elements Ca, Fe, and Ti, as well as for the
trace element, Cs. The synchrotron experiments were performed at Sector 20
(PNC-CAT), Advanced Photon Source (APS), and microXAS beamline at the Swiss
Light Source (SLS). The beam size was 4×3 μm2 and 3×3 μm2,
respectively. For more information, see the paper,
"Quantitative Chemical Imaging of Element Diffusion into Heterogeneous Media
Using Laser Ablation Inductively Coupled Plasma Mass Spectrometry, Synchrotron
Micro-X-ray Fluorescence, and Extended X-ray Absorption Fine Structure
Spectroscopy", H. A. O. Wang et al., Anal. Chem., Article ASAP (DOI:
10.1021/ac200899x Publication Date (Web): May 31, 2011). |
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Tissue imaging with X-ray excited optical luminescence (May 27, 2011) |
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Professor J. N. Anker (Clemson University, South Carolina, United States) and
his colleagues have recently reported an interesting application of optical
luminescence excited by X-rays. So far, the spatial resolution of conventional
florescence microscopy for tissue has been fairly limited. This is mainly due
to the spread of the excitation light, which is scattered by the sample itself,
particularly in the case of thick tissue. The novel idea is to use X-ray
excited optical luminescent light from the scintillator plate placed at the back
of the tissue. X-rays are not scattered very much even in thick tissue, and
such a small spread leads to high-resolution chemical imaging of the tissue.
The authors demonstrated an interesting application as a pH imager using
methyl-red dyed paper. For more information, see the paper,
"High-Resolution Chemical Imaging through Tissue with an X-ray Scintillator
Sensor", H. Chen et al., Anal. Chem., 83, 5045 (2011). |
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Pump-probe X-ray reflectivity (March 10, 2011) |
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A research team led by Professor J. Larsson (Lund University, Sweden) has
recently performed time-resolved X-ray reflectivity measurements with 100
picosecond resolution at ID09B, at the European Synchrotron Radiation Facility (ESRF).
The experiment is a so-called pump-probe measurement, i.e., the repetition of
the measurement with systematic change of the delay time of the pump (laser
light) and probe (X-ray) pulses. In their research, amorphous carbon films with
a thickness of 46 nm were excited with laser pulses (100 fs duration, 800 nm
wavelength, and 70 mJ/cm2 fluence). Here, the laser-induced stress
caused a rapid expansion of the thin film followed by a relaxation of the film
thickness as heat diffused into the silicon substrate. The researchers
succeeded in measuring changes in film thickness by X-ray reflectivity with a
short X-ray pulse (100 ps duration). It was observed that thermal stress
generated by laser excitation causes the film to rapidly expand and increases
the surface roughness substantially. The subsequent relaxation of film
thickness is governed by heat diffusion into the substrate. For more
information, see the paper,
"Picosecond time-resolved x-ray reflectivity of a laser-heated amorphous carbon
film", R. Nuske et al., Appl. Phys. Lett. 98, 101909 (2011). |
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Professional | |||
Ultra fast X-ray camera designed for European XFEL (July 27, 2011) |
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JEOL has developed a new generation of energy-dispersive X-ray spectrometer,
Centurio, for the element analysis and mapping of electron microscope samples.
The detector is a silicon drift detector that collects X-rays from samples at
an unprecedented large solid angle of up to 0.98 steradians from a detection
area of 100mm2. For further information, visit the web page,
http://www.jeolusa.com/ |
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Amptek’s new detector for low energy X-ray spectra (March 7, 2011) |
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Amptek Inc has introduced a new series of low energy X-ray windows. The new "C
Series" represents a new technology that extends the low energy response of the
Amptek Super SDD down to carbon. These windows can be used in SEMs, benchtops,
or hand-held analyzers. For further information, visit the web page,
http://www.amptek.com/press.html |
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New Products | |||
JEOL’s new large angle SDD for TEM samples (July 7, 2011) |
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PANalytical has released new hardware and software for small-angle X-ray
scattering (SAXS) measurements on their range of X-ray diffraction (XRD)
systems. For existing users, the SAXS capability is a straightforward addition
to the instrument. With the release of software, EasySAXS v2.0, nanoparticle
analysis could become easier. For further information, visit the web page,
http://www.panalytical.com/ |
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Corporate | |||
GE moves X-ray business to China (July 25, 2011) |
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General Electric Healthcare has announced the transition of the 115-year-old
X-ray business from Waukesha, Wisconsin to Beijing, China. This is the first GE
business to be headquartered there. For further information,
visit the web page,
http://www.genewscenter.com/Press-Releases/GE-Healthcare-Global-X-ray-Business-Announces-Leadership-Move-to-China-324f.aspx |
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For additional news about X-ray analysis and other spectroscopy sciences, browse the Wiley website. http://www.SpectroscopyNow.com |
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Kenji
Sakurai |
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Back Issue
(Vol.40, No.4) Previous News Vol. 34 No.1-6 (pdf) Vol. 35 No.1-6 (pdf) Vol. 36 No.1-6 (pdf) Vol. 37 No.1-6 (pdf) Vol. 38 No.1-6 (pdf) Vol. 39 No.1-6 (pdf) |
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