Zobrazeno 1 - 10
of 58
pro vyhledávání: '"J. E. McCarthy"'
Publikováno v:
Frontiers in Mechanical Engineering, Vol 10 (2024)
Externí odkaz:
https://doaj.org/article/323d6f1ba4fc45ef9e4f40075092a264
Publikováno v:
Frontiers in Mechanical Engineering, Vol 8 (2022)
New regulations by the California Air Resources Board (CARB) demand a stringent 0.02 g/hp-hr tailpipe NOx limit by the year 2027, requiring Selective Catalytic Reduction (SCR) catalysts to provide high NOx conversions even at low (below 200°C) exhau
Externí odkaz:
https://doaj.org/article/a17ffa9bbebc4080a5b5ff2eb8ecd5b3
Autor:
J. E. McCarthy
Publikováno v:
Synchrotron Radiation News. 30:31-36
The ESRF, the European Synchrotron, is the world's most intense X-ray source and a center of excellence for fundamental and innovation-driven research in condensed and living matter science. Located in Grenoble, France, the ESRF owes its success to t
Autor:
David Flot, Edward P. Mitchell, X. Thibault, Matias Guijarro, Matthew W. Bowler, Darren Spruce, Martin A. Walsh, Vicente Rey-Bakaikoa, Didier Nurizzo, Raimond B. G. Ravelli, Andrew A. McCarthy, David R. Hall, José Gabadinho, Elspeth Gordon, Sean McSweeney, Gordon A. Leonard, Christoph Mueller-Dieckmann, Antonia Beteva, Sandor Brockhauser, J. E. McCarthy, Bernard Lavault, Stéphanie Monaco
Publikováno v:
Journal of Synchrotron Radiation
MxCuBE is a beamline control environment optimized for the needs of macromolecular crystallography. This paper describes the design of the software and the features that MxCuBE currently provides.
The design and features of a beamline control so
The design and features of a beamline control so
Technical Report: Automatic Experiments at the European Synchrotron Radiation Facility MX Beam-lines
Publikováno v:
Synchrotron Radiation News. 20:18-24
During the last twenty years macromolecular crystallography (MX) has become the predominant tool for the investigation of structure/function relationships in biology. This is due to many technological advances and, in particular, improved access to s
Autor:
J. E. McCarthy, Carsten Detlefs, D N Timms, J. A. Duffy, A. M. Bebb, Paul C. Canfield, J. W. Taylor, Martin R. Lees, S. Majumdar, Malcolm Cooper
Publikováno v:
Physica B: Condensed Matter. 318:267-271
The spin-polarized electron momentum distributions (EMD) for ferrimagnetic GdMn2Ge2 and ferromagnetic LaMn2Ge2 have been measured using the magnetic Compton scattering technique. The spin-polarized EMDs were resolved along the c-axis at 15 K: In the
Autor:
Th. Tschentscher, A. Yaouanc, O. Vogt, J. E. McCarthy, Veijo Honkimäki, J.P. Sanchez, P. Dalmas de Réotier, N. Kernavanois
Publikováno v:
Journal of Physics: Condensed Matter. 13:9677-9690
We report the results of two experiments performed on uranium monosulphide: measuring the magnetic Compton scattering (MCS) and x-ray magnetic circular dichroism (XMCD) at the M4,5 uranium absorption edges. From the MCS experiment we get the spin mom
Autor:
U. Lienert, Pekka Suortti, Veijo Honkimäki, Abhay Shukla, José Manuel Merino, J. E. McCarthy, Thomas Buslaps, M. DiMichiel
Publikováno v:
Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment. :1541-1544
A new type of Compton spectrometer is introduced for use at energies of 100 keV. Synchrotron radiation beam of a well-defined energy gradient is reflected on the sample by a cylindrically bent Laue-type monochromator, and the scattered radiation is a
Publikováno v:
Physical Review B. 62:R6073-R6076
The spin contribution to the magnetic moment in SmMn{sub 2}Ge{sub 2} has been measured by magnetic Compton scattering in both the low- and high-temperature ferromagnetic phases. At low temperature, the Sm site is shown to possess a large 4f spin mome
Autor:
T. Jarlborg, Stephen B Dugdale, Stuart B. Palmer, Malcolm Cooper, M A Alam, J. A. Duffy, J. E. McCarthy
Publikováno v:
Physical Review B. 61:14331-14334
Evidence of a spin moment, induced through a Ruderman-Kittel-Kasuya-Yosida-type interaction in ${\mathrm{Gd}}_{62.4}{\mathrm{Y}}_{37.6},$ is presented. The additional moment, of $0.16\ifmmode\pm\else\textpm\fi{}0.03{\ensuremath{\mu}}_{B},$ arises fro