Maximum chemical and physical hardness

[1] [Anonymous], 1987, Statistical Thermodynamics of Nonequilibrium Processes

[2] Chandler D., 1987, INTRO MODERN STAT ME

[3] THE MAXIMUM HARDNESS PRINCIPLE IN THE GYFTOPOULOS-HATSOPOULOS 3-LEVEL MODEL FOR AN ATOMIC OR MOLECULAR-SPECIES AND ITS POSITIVE AND NEGATIVE-IONS [J]. CHEMICAL PHYSICS LETTERS, 1995, 237 (1-2) : 171 - 176

[4] HARDNESS PROFILE OF A REACTION-PATH [J]. JOURNAL OF PHYSICAL CHEMISTRY, 1992, 96 (06) : 2409 - 2410

[5] GAZQUEZ JL, 1989, J PHYS CHEM, V93, P3068

[6] WHY SILICON IS HARD [J]. SCIENCE, 1993, 261 (5127) : 1436 - 1439

[7] GILMAN JJ, IN PRESS MAT RES INN

[8] GOBLE RJ, 1985, CAN MINERAL, V23, P273

[9] QUANTUM-THERMODYNAMIC DEFINITION OF ELECTRONEGATIVITY [J]. PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 1968, 60 (03) : 786 - +

[10] HARRISON WA, 1980, ELECTRONIC STRUCTURE, P193

[1] [Anonymous], 1987, Statistical Thermodynamics of Nonequilibrium Processes

[2] Chandler D., 1987, INTRO MODERN STAT ME

[3] THE MAXIMUM HARDNESS PRINCIPLE IN THE GYFTOPOULOS-HATSOPOULOS 3-LEVEL MODEL FOR AN ATOMIC OR MOLECULAR-SPECIES AND ITS POSITIVE AND NEGATIVE-IONS [J]. CHEMICAL PHYSICS LETTERS, 1995, 237 (1-2) : 171 - 176

[4] HARDNESS PROFILE OF A REACTION-PATH [J]. JOURNAL OF PHYSICAL CHEMISTRY, 1992, 96 (06) : 2409 - 2410

[5] GAZQUEZ JL, 1989, J PHYS CHEM, V93, P3068

[6] WHY SILICON IS HARD [J]. SCIENCE, 1993, 261 (5127) : 1436 - 1439

[7] GILMAN JJ, IN PRESS MAT RES INN

[8] GOBLE RJ, 1985, CAN MINERAL, V23, P273

[9] QUANTUM-THERMODYNAMIC DEFINITION OF ELECTRONEGATIVITY [J]. PROCEEDINGS OF THE NATIONAL ACADEMY OF SCIENCES OF THE UNITED STATES OF AMERICA, 1968, 60 (03) : 786 - +

[10] HARRISON WA, 1980, ELECTRONIC STRUCTURE, P193