scholarly journals Interaction of Hydrogen with Actinide Dioxide (011) Surfaces

2020 ◽  
Author(s):  
James Pegg ◽  
Ashley E. Shields ◽  
Mark T. Storr ◽  
David Scanlon ◽  
Nora De Leeuw

<p>The hydrogen catalysed oxidation of nuclear materials has led to containment vessel failure. The interaction of hydrogen with actinide dioxide (AnO<sub>2</sub>, An = U, Np, Pu) (011) surfaces has been completed by DFT+U; where, spin-orbit interactions and noncollinear 3k antiferromagnetic behaviour have been included. The energy of atomic hydrogen adsorption for UO<sub>2</sub> (0.44 eV), NpO<sub>2</sub> (-0.47 eV), and PuO<sub>2</sub> (-1.71 eV) has been calculated, where the subsequent formation of an OH group is shown to distort the surface structure. The dissociation of hydrogen on the PuO<sub>2</sub> (011) surfaces has been found; however, UO<sub>2</sub> (011) and NpO<sub>2</sub> (011) surfaces are relatively inert. The recombination of hydrogen ions on the UO<sub>2</sub> (011) and NpO<sub>2</sub> (011) surfaces is highly-probable; whereas, hydroxide formation on the PuO<sub>2</sub> (011) surface has been shown. The results have consequences for fuel storage management.</p>

2020 ◽  
Author(s):  
James Pegg ◽  
Ashley E. Shields ◽  
Mark T. Storr ◽  
David Scanlon ◽  
Nora De Leeuw

<p>The hydrogen catalysed oxidation of nuclear materials has led to containment vessel failure. The interaction of hydrogen with actinide dioxide (AnO<sub>2</sub>, An = U, Np, Pu) (011) surfaces has been completed by DFT+U; where, spin-orbit interactions and noncollinear 3k antiferromagnetic behaviour have been included. The energy of atomic hydrogen adsorption for UO<sub>2</sub> (0.44 eV), NpO<sub>2</sub> (-0.47 eV), and PuO<sub>2</sub> (-1.71 eV) has been calculated, where the subsequent formation of an OH group is shown to distort the surface structure. The dissociation of hydrogen on the PuO<sub>2</sub> (011) surfaces has been found; however, UO<sub>2</sub> (011) and NpO<sub>2</sub> (011) surfaces are relatively inert. The recombination of hydrogen ions on the UO<sub>2</sub> (011) and NpO<sub>2</sub> (011) surfaces is highly-probable; whereas, hydroxide formation on the PuO<sub>2</sub> (011) surface has been shown. The results have consequences for fuel storage management.</p>


2019 ◽  
Author(s):  
James Pegg ◽  
Ashley E. Shields ◽  
Mark T. Storr ◽  
David Scanlon ◽  
Nora De Leeuw

<p>The hydrogen catalysed oxidation of nuclear materials has led to containment vessel failure. The interaction of hydrogen with actinide dioxide (AnO<sub>2</sub>, An = U, Np, Pu) (011) surfaces has been completed by DFT+U; where, spin-orbit interactions and noncollinear 3k antiferromagnetic behaviour have been included. The energy of atomic hydrogen adsorption for UO<sub>2</sub> (0.44 eV), NpO<sub>2</sub> (-0.47 eV), and PuO<sub>2</sub> (-1.71 eV) has been calculated, where the subsequent formation of an OH group is shown to distort the surface structure. The dissociation of hydrogen on the PuO<sub>2</sub> (011) surfaces has been found; however, UO<sub>2</sub> (011) and NpO<sub>2</sub> (011) surfaces are relatively inert. The recombination of hydrogen ions on the UO<sub>2</sub> (011) and NpO<sub>2</sub> (011) surfaces is highly-probable; whereas, hydroxide formation on the PuO<sub>2</sub> (011) surface has been shown. The results have consequences for fuel storage management.</p>


2019 ◽  
Author(s):  
James Pegg ◽  
Ashley E. Shields ◽  
Mark T. Storr ◽  
David Scanlon ◽  
Nora De Leeuw

The interaction of atomic and molecular hydrogen with the actinide dioxide (AnO<sub>2</sub>, An = U, Np, Pu) (111) surfaces has been investigated by DFT+U, where noncollinear 3k antiferromagnetic (AFM) behaviour and spin-orbit interactions (SOI) are considered. The adsorption of atomic hydrogen forms a hydroxide group, and is coupled to the reduction of an actinide ion. The energy of atomic hydrogen adsorption on the UO<sub>2</sub> (0.82 eV), NpO<sub>2</sub> (-0.10 eV), and PuO<sub>2</sub> (-1.25 eV) surfaces has been calculated. The dissociation of molecular hydrogen is not observed, and shown to be due to kinetic rather than thermodynamic factors. As a barrier in the formation of a second hydroxyl group, an unusual charge distribution has been shown. This is possibly a limitation of a (1·1) unit cell method. The recombination of hydrogen ions on the AnO<sub>2</sub> (111) surfaces is favoured over hydroxide formation.


2019 ◽  
Author(s):  
James Pegg ◽  
Ashley E. Shields ◽  
Mark T. Storr ◽  
David Scanlon ◽  
Nora De Leeuw

The interaction of atomic and molecular hydrogen with the actinide dioxide (AnO<sub>2</sub>, An = U, Np, Pu) (111) surfaces has been investigated by DFT+U, where noncollinear 3k antiferromagnetic (AFM) behaviour and spin-orbit interactions (SOI) are considered. The adsorption of atomic hydrogen forms a hydroxide group, and is coupled to the reduction of an actinide ion. The energy of atomic hydrogen adsorption on the UO<sub>2</sub> (0.82 eV), NpO<sub>2</sub> (-0.10 eV), and PuO<sub>2</sub> (-1.25 eV) surfaces has been calculated. The dissociation of molecular hydrogen is not observed, and shown to be due to kinetic rather than thermodynamic factors. As a barrier in the formation of a second hydroxyl group, an unusual charge distribution has been shown. This is possibly a limitation of a (1·1) unit cell method. The recombination of hydrogen ions on the AnO<sub>2</sub> (111) surfaces is favoured over hydroxide formation.


2019 ◽  
Author(s):  
James Pegg ◽  
Ashley E. Shields ◽  
Mark T. Storr ◽  
David Scanlon ◽  
Nora De Leeuw

The interaction of atomic and molecular hydrogen with the actinide dioxide (AnO<sub>2</sub>, An = U, Np, Pu) (111) surfaces has been investigated by DFT+U, where noncollinear 3k antiferromagnetic (AFM) behaviour and spin-orbit interactions (SOI) are considered. The adsorption of atomic hydrogen forms a hydroxide group, and is coupled to the reduction of an actinide ion. The energy of atomic hydrogen adsorption on the UO<sub>2</sub> (0.82 eV), NpO<sub>2</sub> (-0.10 eV), and PuO<sub>2</sub> (-1.25 eV) surfaces has been calculated. The dissociation of molecular hydrogen is not observed, and shown to be due to kinetic rather than thermodynamic factors. As a barrier in the formation of a second hydroxyl group, an unusual charge distribution has been shown. This is possibly a limitation of a (1·1) unit cell method. The recombination of hydrogen ions on the AnO<sub>2</sub> (111) surfaces is favoured over hydroxide formation.


Author(s):  
J. Nitta

This chapter focuses on the electron spin degree of freedom in semiconductor spintronics. In particular, the electrostatic control of the spin degree of freedom is an advantageous technology over metal-based spintronics. Spin–orbit interaction (SOI), which gives rise to an effective magnetic field. The essence of SOI is that the moving electrons in an electric field feel an effective magnetic field even without any external magnetic field. Rashba spin–orbit interaction is important since the strength is controlled by the gate voltage on top of the semiconductor’s two-dimensional electron gas. By utilizing the effective magnetic field induced by the SOI, spin generation and manipulation are possible by electrostatic ways. The origin of spin-orbit interactions in semiconductors and the electrical generation and manipulation of spins by electrical means are discussed. Long spin coherence is achieved by special spin helix state where both strengths of Rashba and Dresselhaus SOI are equal.


2019 ◽  
Vol 123 (43) ◽  
pp. 26662-26672 ◽  
Author(s):  
Björn Arndt ◽  
Marcus Creutzburg ◽  
Elin Grånäs ◽  
Sergey Volkov ◽  
Konstantin Krausert ◽  
...  

2021 ◽  
Vol 23 (5) ◽  
pp. 3668-3678
Author(s):  
Angela Rodriguez-Serrano ◽  
Fabian Dinkelbach ◽  
Christel M. Marian

Multireference quantum chemical calculations were performed in order to investigate the (reverse) intersystem crossing ((R)ISC) mechanisms of 4,5-di(9H-carbazol-9-yl)-phthalonitrile (2CzPN).


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