Abstract
The energy (E) versus number of electrons (N) and external potential (v) functional E = E[N, v], which has proved to be of fundamental importance in conceptual density functional theory through the response functions it generates, has been examined concentrating on the concavity of the E = E[v] functional as opposed to the convexity of the E = E(N) function. The concavity of the E = E[v] functional is reflected in negative values of the diagonal elements of the linear response function \(\chi ({\mathbf{r}},{\mathbf{r}}')\) comprising the second functional derivative of E with respect to \(v({\mathbf{r}})\), whereas no sign can be retrieved for the off-diagonal elements. These findings are in agreement with recent computational studies in extracting the chemical content of the linear response function. The results for the diagonal elements can easily be interpreted in terms of electron depletion from regions where the potential is increased and are easily retrieved via the independent particle model expression and in agreement with the diagonal elements of the most general expression for the linear response function. These concavity-related issues are put in contrast with the positive \((\partial ^2E/\partial N^2)_v\) derivative, resulting from the convexity of the E(N) function, in line with the positivity of the chemical hardness as resulting from the I versus A (ionization vs. electron affinity) ratio. The first-order derivative \((\delta E/\delta v({\mathbf{r}}))_N\) is discussed within an iso-electronic atom series for which it is shown in detail that the potentials can be ordered univocally, through their Z-dependence. The sign of the slope of the E = E[v] curve is in agreement with the positivity of \(\rho ({\mathbf{r}})\). The result for the E = E[v] functional is put in contrast with the negative \((\partial E/\partial N)_v\) derivative (identified as minus the electronegativity) for the E = E(N) function retrieved on the basis of experimental and theoretical data on ionization energies and electron affinities.
Similar content being viewed by others
References
Hohenberg P, Kohn W (1964) Phys Rev 136:B864
Parr RG, Yang W (1989) Density-functional theory of atoms and molecules. International series of monographs on chemistryOxford University Press, New York
Kohn W, Sham LJ (1965) Phys Rev 140:A1133
Becke AD (1993) J Chem Phys 98(7):5648
Perdew JP, Ernzerhof M, Burke K (1996) J Chem Phys 105(22):9982
Lee C, Yang W, Parr RG (1988) Phys Rev B 37:785
Koch W, Holthausen M (2001) A chemists guide to density functional theory, 2nd edn. Wiley, London
Yang W (2014) J Chem Phys 140(18):18A101
Parr RG, Yang W (1995) Ann Rev Phys Chem 46:701
Geerlings P, De Proft F, Langenaeker W (2003) Chem Rev 103(5):1793
De Proft F, Geerlings P (2001) Chem Rev 101:1451
Chermette H (1999) J Comput Chem 20(1):129
Ayers PW, Anderson JSM, Bartolotti LJ (2005) Int J Quantum Chem 101(5):520
Gázquez JL (2008) J Mex Chem Soc 52:3
Chattaraj PK (ed) (2009) Chemical reactivity theory. A density functional view. CRC Press, Boca Raton
Liu SB (2009) Acta Phys Chim Sin 25(3):590
Geerlings P, Ayers PW, Toro-Labbé A, Chattaraj PK, De Proft F (2012) Acc Chem Res 45(5):683
Parr RG, Szentply LV, Liu S (1999) J Am Chem Soc 121(9):1922
Chattaraj PK, Sarkar U, Roy DR (2006) Chem Rev 106(6):2065
Parr R, Donnelly RA, Levy M, Palke WE (1978) J Chem Phys 68:3801
Parr RG, Yang W (1984) J Am Chem Soc 106(14):4049
Geerlings P, De Proft F (2008) Phys Chem Chem Phys 10:3028
Morell C, Grand A, Toro-Labbé A (2005) J Phys Chem A 109(1):205
Savin A, Colonna F, Allavena M (2001) J Chem Phys 115(15):6827
Runge E, Gross EKU (1984) Phys Rev Lett 52:997
Gross E, Kohn W (1990) Density functional theory of many-fermion systems. Advances in quantum chemistry. Academic Press, London
Casida ME (1995) Recent advances in density functional methods. World Scientific Pub. Co. Inc., Singapore
Ayers PW, De Proft F, Borgoo A, Geerlings P (2007) J Chem Phys 126(22):224107
Sablon N, De Proft F, Ayers PW, Geerlings P (2007) J Chem Phys 126(22):224108
Yang W, Cohen AJ, De Proft F, Geerlings P (2012) J Chem Phys 136(14):144110
Fias S, Boisdenghien Z, De Proft F, Geerlings P (2014) J Chem Phys 141(18):184107
Boisdenghien Z, Fias S, Pieve FD, De Proft F, Geerlings P (2015) Mol. Phys. 113(13–14):1890
Boisdenghien Z, Van Alsenoy C, De Proft F, Geerlings P (2013) J Chem Theory Comput 9(2):1007
Boisdenghien Z, Fias S, Van Alsenoy C, De Proft F, Geerlings P (2014) Phys Chem Chem Phys 16:14614
Sablon N, De Proft F, Geerlings P (2010) Chem Phys Lett 498(1–3):192
Sablon N, De Proft F, Geerlings P (2010) J Phys Chem Lett 1(8):1228
Sablon N, De Proft F, Sola M, Geerlings P (2012) Phys Chem Chem Phys 14:3960
Fias S, Geerlings P, Ayers P, De Proft F (2013) Phys Chem Chem Phys 15:2882
Geerlings P, Fias S, Boisdenghien Z, De Proft F (2014) Chem Soc Rev 43:4989
Coulson CA, Longuet-Higgins HC (1947) Proc R Soc Lond 191:39
Coulson CA, Longuet-Higgins HC (1947) Proc R Soc Lond 192:16
Stuyver T, Fias S, De Proft F, Fowler PW, Geerlings P (2015) J Chem Phys 142(9):094103
Stuyver T, Fias S, De Proft F, Geerlings P (2015) Chem Phys Lett 630:51
Stuyver T, Fias S, De Proft F, Geerlings P (2015) J Phys Chem C 119(47):26390
Eschrig H (1996) The fundamentals of density functional theory. Vieweg+Teubner Verlag, Stuttgart, TEUBNER-TEXTE zur Physik
Perdew J, Parr R, Levy M, Balduz J Jr (1982) Phys Rev Lett 49:1691
Franco-Pérez M, Gázquez JL, Ayers PW, Vela A (2015) J Chem Phys 143(15):154103
Lieb EH (1983) Int J Quantum Chem 24(3):243
Helgaker T (2014) Density-functional theory. Presentation (2014). In: The 13th sostrup summer school on quantum chemistry and molecular properties
Helgaker T (2015) Differentiable but exact formulation of density-functional theory. Presentation (2015). Formal and practical aspects of electronic structure simulations with density functional theory, Vrije Universiteit, Amsterdam
Kvaal S, Ekström U, Teale AM, Helgaker T (2014) J Chem Phys 140(18):18A518
Atkins P, Friedman R (1997) Molecular quantum mechanics. Oxford University Press, London
Liu S, Li T, Ayers PW (2009) J Chem Phys 131(11):114106
Sablon N, De Proft F, Ayers PW, Geerlings P (2010) J Chem Theory Comput 6(12):3671
Cardenas C, Ayers P, De Proft F, Tozer DJ, Geerlings P (2011) Phys Chem Chem Phys 13:2285
Hellmann H (1937) Einführung in die Quantenchemie (Leipzig F. Deuticke)
Feynman RP (1939) Phys Rev 56:340
Foldy LL (1951) Phys Rev 83:397
Politzer P, Parr RG (1974) J Chem Phys 61(10):4258
Levy M (1978) J Chem Phys 68(11):5298
Pyykkö P (2011) Phys Chem Chem Phys 13:161
Pyykkö P (2012) Chem Rev 112(1):371
Wilson EB (1962) J Chem Phys 36(8):2232
Acknowledgments
Stijn Fias acknowledges the Research Foundation Flanders(FWO) for financial support for his postdoctoral research in the General Chemistry Group (Algemene Chemie, ALGC). P.G. and F.D.P. wish to acknowledge the VUB for a Strategic Research Program from which a research position to Zino Boisenghien could be financed. The authors want to thank an anonymous reviewer for her/his constructive remarks. The authors want to dedicate this account to Professor Alberto Vela at the occasion of his 60th birthday. Alberto has been a fine colleague and friend for many years, a true companion in the search for what DFT has to offer to chemists.
Author information
Authors and Affiliations
Corresponding author
Additional information
Published as part of the special collection of articles “Festschrift in honour of A. Vela”.
Appendix: The energy of iso-electronic atoms
Appendix: The energy of iso-electronic atoms
Consider a neutral many electron atom, with nuclear charge Z and number of electrons N (\(Z=N\)). By virtue of the Hellman–Feynman theorem [56, 57], the derivative of the energy as a function of Z can be written as
which reduces in the case of an atom to
As compared to a reference state \(E(0)=0\) an atom with nuclear charge zero, implying that all electrons are at infinity [63], the energy \(E=E(Z)\) can be written as
retrieving Foldy’s result for the exact non-relativistic energy of a ground-state atom with atomic number Z and N electrons [58]. (In fact, this zero value as Z-reference could be replaced by the \(Z_{{\text {min}}}\) in Fig. 3. This choice, however, does not alter the remaining part and the conclusion of the discussion.)
Consider now two iso-electronic systems with \(Z=Z_1\) and \(Z=Z_2\) where we choose \(Z_2>Z_1\). One then has
Due to the spherical nature of the electron distribution assumed throughout, one gets
Denoting the integral over \({\text {d}}Z\) as \(f(r;Z_1,Z_2)\), we obtain
As it cannot be that for all r values the density \(\rho (r,Z)=0\), \(f(r;Z_1,Z_2)\) will be positive for a number of r values so that the integrand of the integral is positive. Denoting this integral as \(F(Z_1,Z_2)\), we obtain
or \(E(Z_2)<E(Z_1)\), yielding the result that upon increasing Z, the energy E decreases (i.e. becomes more negative).
Rights and permissions
About this article
Cite this article
Geerlings, P., Boisdenghien, Z., Proft, F.D. et al. The E = E[N, v] functional and the linear response function: a conceptual DFT viewpoint. Theor Chem Acc 135, 213 (2016). https://doi.org/10.1007/s00214-016-1967-9
Received:
Accepted:
Published:
DOI: https://doi.org/10.1007/s00214-016-1967-9