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1
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0003641685
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NATO Science Series (Kluwer, Dordrecht)
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2 and Related Dielectrics: Science and Technology, edited by G. Pacchioni, L. Skuja, and D. L. Griscom, NATO Science Series (Kluwer, Dordrecht, 2000).
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(2000)
2 and Related Dielectrics: Science and Technology
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Pacchioni, G.1
Skuja, L.2
Griscom, D.L.3
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2
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0035934795
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H. Hosono, Y. Ikuta, T. Kinoshita, K. Kajihara, and M. Hirano, Phys. Rev. Lett. 87, 175501 (2001).
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(2001)
Phys. Rev. Lett.
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Hosono, H.1
Ikuta, Y.2
Kinoshita, T.3
Kajihara, K.4
Hirano, M.5
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4
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1542394280
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Copyright IBM Corp 1990-2003, Copyright MPI fuer Festkoerperforschung Stuttgart
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CPMD V3.7, Copyright IBM Corp 1990-2003, Copyright MPI fuer Festkoerperforschung Stuttgart 1997-2001.
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(1997)
CPMD V3.7
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12
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0000192206
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M. Benoit, S. Ispas, P. Jund, and R. Jullien, Eur. Phys. J. B 13, 631 (2000).
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(2000)
Eur. Phys. J. B
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Benoit, M.1
Ispas, S.2
Jund, P.3
Jullien, R.4
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14
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15744400687
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note
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In the other two models, the hole is self-trapped on a strongly strained siloxane bond in large rings. Their concentration in our samples is probably overestimated due to the still fast cooling rate and small simulation cell.
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18
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15744405768
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private communication
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A. Laio (private communication).
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Laio, A.1
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21
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15744398005
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note
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In a preliminary simulation, we have chosen a collective variable which allows the breaking of any SiO bond of the ring. As expected, by adding Gaussians, we have seen a large lengthening of the Si(1)-O(2) bond indicating that the bond which traps the hole is weaker and is the most prone to break.
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22
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15744390059
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note
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Constant temperature is enforced by velocity rescaling at the target temperature with a tolerance of 10%.
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23
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0345491105
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1-NBOHC distances below 5 Å for the B3LYP functional and below 5.4 Å for the BLYP functional. The calculations have been performed with the code Gaussian98 [GAUSSIAN98, M. J. Frisch, G. W. Trucks, H. B. Schlegel et al. (Gaussian Inc., Pittsburgh, PA, 1998)] and the 6-311+G* basis set which provides a good description of point defects in silica [G. Pacchioni and M. Vitiello, J. Non-Cryst. Solids 245, 175 (1999)].
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(1988)
Phys. Rev. B
, vol.37
, pp. 785
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Lee, C.1
Yang, W.2
Parr, R.G.3
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24
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0000189651
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1-NBOHC distances below 5 Å for the B3LYP functional and below 5.4 Å for the BLYP functional. The calculations have been performed with the code Gaussian98 [GAUSSIAN98, M. J. Frisch, G. W. Trucks, H. B. Schlegel et al. (Gaussian Inc., Pittsburgh, PA, 1998)] and the 6-311+G* basis set which provides a good description of point defects in silica [G. Pacchioni and M. Vitiello, J. Non-Cryst. Solids 245, 175 (1999)].
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(1993)
J. Chem. Phys.
, vol.98
, pp. 5648
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Becke, A.D.1
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25
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0004133516
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Gaussian Inc., Pittsburgh, PA
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1-NBOHC distances below 5 Å for the B3LYP functional and below 5.4 Å for the BLYP functional. The calculations have been performed with the code Gaussian98 [GAUSSIAN98, M. J. Frisch, G. W. Trucks, H. B. Schlegel et al. (Gaussian Inc., Pittsburgh, PA, 1998)] and the 6-311+G* basis set which provides a good description of point defects in silica [G. Pacchioni and M. Vitiello, J. Non-Cryst. Solids 245, 175 (1999)].
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(1998)
GAUSSIAN98
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Frisch, M.J.1
Trucks, G.W.2
Schlegel, H.B.3
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26
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0032673437
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1-NBOHC distances below 5 Å for the B3LYP functional and below 5.4 Å for the BLYP functional. The calculations have been performed with the code Gaussian98 [GAUSSIAN98, M. J. Frisch, G. W. Trucks, H. B. Schlegel et al. (Gaussian Inc., Pittsburgh, PA, 1998)] and the 6-311+G* basis set which provides a good description of point defects in silica [G. Pacchioni and M. Vitiello, J. Non-Cryst. Solids 245, 175 (1999)].
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(1999)
J. Non-Cryst. Solids
, vol.245
, pp. 175
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Pacchioni, G.1
Vitiello, M.2
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