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- Aad, G., et al.
(författare)
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The ATLAS Simulation Infrastructure
- 2010
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Ingår i: European Physical Journal C. Particles and Fields. - : Springer Science and Business Media LLC. - 1434-6044 .- 1434-6052. ; 70:3, s. 823-874
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Tidskriftsartikel (refereegranskat)abstract
- The simulation software for the ATLAS Experiment at the Large Hadron Collider is being used for large-scale production of events on the LHC Computing Grid. This simulation requires many components, from the generators that simulate particle collisions, through packages simulating the response of the various detectors and triggers. All of these components come together under the ATLAS simulation infrastructure. In this paper, that infrastructure is discussed, including that supporting the detector description, interfacing the event generation, and combining the GEANT4 simulation of the response of the individual detectors. Also described are the tools allowing the software validation, performance testing, and the validation of the simulated output against known physics processes.
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- Li, Wen, et al.
(författare)
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Understanding from First-Principles Why LiNH2BH3 · NH3BH3 Shows Improved Dehydrogenation over LiNH2BH3 and NH3BH3
- 2010
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Ingår i: The Journal of Physical Chemistry C. - : American Chemical Society (ACS). - 1932-7447 .- 1932-7455. ; 114:44, s. 19089-19095
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Tidskriftsartikel (refereegranskat)abstract
- Lithium amidoborane-ammonia borane (LiNH2BH3 center dot NH3BH3, LiAB center dot AB for short) was synthesized recently. Compared with lithium amidoborane (LiNH2BH3, LiAB for short) and ammonia borane (NH3BH3, AB for short), this new ammonia borane derivative has better dehydrogenation kinetics and releases 14.8 wt % hydrogen with peak temperatures at ca. 80 and 140 degrees C, respectively. In this report, first-principles calculations were employed to reveal the differences in dehydrogenation properties of AB, LiAB, and LiAB center dot AB. Furthermore, we attempted to correlate the crystal structure and electronic properties with dehydrogenation performance. The results show that Li+ cations play similar roles in LiAB center dot AB as in LiAB in destabilizing the B-H and N-H bonds, and the mechanism of the first-step dehydrogenation of LiAB center dot AB is likely via the dissociation and combination of hydridic H delta-(B) from LiAB molecule and protonic H delta+(N) from the adjacent AB molecule, rather than from the [LiAB] or [AB] layer alone, resulting in the desorption of H-2 at lower temperatures.
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| 5. |
- Aad, G., et al.
(författare)
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- 2010
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swepub:Mat__t
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| 6. |
- Aad, G., et al.
(författare)
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- 2010
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swepub:Mat__t
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| 7. |
- Aad, G., et al.
(författare)
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- 2010
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swepub:Mat__t
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| 8. |
- Aad, G., et al.
(författare)
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- 2010
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swepub:Mat__t (refereegranskat)
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| 9. |
- Aad, G., et al.
(författare)
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- 2010
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swepub:Mat__t
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| 10. |
- Li, Wen, et al.
(författare)
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Li+ ion conductivity and diffusion mechanism in α-Li3N and β-Li3N
- 2010
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Ingår i: Energy & environmental science. - : Royal Society of Chemistry (RSC). - 1754-5692 .- 1754-5706. ; 3:10, s. 1524-1530
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Tidskriftsartikel (refereegranskat)abstract
- beta-Li3N of hexagonal D-6h(4) (P6(3)/mmc) structure was synthesized by high-energy ball milling commercial Li3N (composed of both alpha and beta phases). Ionic conductivities of alpha-Li3N and beta-Li3N were tested by direct current (D. C.) and alternating current (A. C.) impedance methods. beta-Li3N exhibited the same order of magnitude of Li+ ion conductivity (2.085 x 10(-4) S cm(-1)) as that of alpha-Li3N (5.767 x 10(-4) S cm(-1)) at room temperature. First-principles calculations were employed to simulate the diffusion mechanism of Li+ ion in alpha-Li3N and beta-Li3N. Our results indicate that the diffusion of Li+ ion in beta-Li3N likely occurs between pure Li-beta(1) planes, which is different from that in alpha-Li3N, where the diffusion of Li+ ion occurs within Li2N plane. The Li+ ion migration energy barriers (E-m) for alpha-Li3N and beta-Li3N are 0.007 eV and 0.038 eV, respectively.
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