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  2. Bibliography

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper13/node11.html
    28 Oct 2002: Springborg M 2001 Chem. Phys. Lett. 339, 389. 24. ... Paine RT and Sneddon LG 1994 CHEMTECH 24 29. 35.
  3. Bibliography

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper8/node7.html
    31 Oct 2002: Johns Hopkins University Press, Baltimore, 1996). 24.
  4. Bibliography

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper10/node20.html
    29 Oct 2002: Next: About this document. Up: Total-energy calculations on a Previous: Basis for the fine. Bibliography. Payne, M. C., Teter, M. P., Allan, D. C., Arias, T. A., and Joannopolous, J. D.,. Rev. Mod. Phys. 64 (1992) 1045. Kohn, W. and Sham, L. J.,.
  5. Total energy optimisation

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper10/node11.html
    29 Oct 2002: Our implementation follows the simplified version of Millam and Scuseria [24].
  6. Energetics

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper13/node5.html
    28 Oct 2002: BN systems. Benzene. 2.24. 1.99. Borazine. PPV. 2.22. 1.98. PVB. PPP.
  7. Projection operators

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper10/node6.html
    29 Oct 2002: 24). where. Similarly, we define a supplementary operator,. , that performs the same task, but for the fine grid representation:.
  8. The FFT box technique

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper11/node4.html
    31 Oct 2002: In the same way, the calculation of the total energy gradient with respect to the NGWF expansion coefficients of equation (24) can be calculated in the FFT box provided we use ... Therefore all we have to do is to substitute. of equation (24) by.
  9. Introduction

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper13/node1.html
    28 Oct 2002: Next: Why boron nitride polymers? Up: Material design from first Previous: Material design from first. Introduction. Recent advances in synthesis and nanofabrication technologies have dramatically broadened the range of materials that can be
  10. The NGWF pseudopotential plane-wave method in practice

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper11/node5.html
    31 Oct 2002: The equilibrium bond length for this case differs by 3.34% from CASTEP, as compared to -1.24% for the.
  11. Introduction

    www.tcm.phy.cam.ac.uk/~pdh1001/papers/paper11/node1.html
    31 Oct 2002: Next: Charge density and total Up: Nonorthogonal generalized Wannier function Previous: Nonorthogonal generalized Wannier function. Introduction. The pseudopotential plane-wave method for density-functional theory (DFT) calculations has been

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