Every problem, one list
66 pencil-and-paper problems spanning Quantum Chemistry I, numbered straight through — the way a professor hands out the semester's whole set on day one. This is the target: work them all. Tick each as you solve it; the worked solutions live on each set's page. The reading is a supplement — this is the spine.
Pick a parameterized trial wavefunction, write the energy as a function of the parameters, and minimize — the upper-bound calculation at the root of every electronic-structure method.
- 1workedHelium in one parameter — every integral shown
- 2practiceWhen the trial contains the exact answer
- 3practiceA basis of the wrong shape
- 4practiceA parameter-free trial on a different system
- 5practiceReading a physical constant out of the optimum
- 6practiceLinear variation — the secular equation
- 7checkAn energy below exact
- 8checkWhy the bound is for the ground state only
Evaluate molecular integrals over s-type Gaussians by hand via the Gaussian product theorem.
- 9practicegeometry / weighted averages
- 10practicescreening & sparsity
- 11practicebasis design
- 12practiceoperator limits
- 13practicenormalization
- 14practicespecial functions
- 15checkCheck 1
- 16checkCheck 2
Constrained functional variation: minimize the orbital energy functional under orthonormality and earn the Fock eigenvalue equation.
- 17workedFrom the energy functional to the eigenvalue equation
- 18practiceCalculus of variations — where the 2 comes from
- 19practiceVarying the Coulomb functional
- 20practiceBrillouin as a unit test
- 21practiceThe unitary freedom
- 22practiceWhy “density stopped” equals “energy stationary”
- 23practiceKoopmans from the canonical equations
- 24checkThe FPS − SPF criterion
- 25checkMultipliers vs. energies
Recognize a problem as a fixed-point iteration — an operator that depends on its own eigenvector — and solve by iterative refinement: linearize with a guess, solve, use the result to rebuild the operator, iterate. Diagnose convergence, oscillation, and the use of damping or DIIS-style acceleration.
- 26practicescalar fixed-point analysis
- 27practicecosine fixed-point (Dottie number)
- 28practicepower iteration for eigenvectors
- 29practiceoscillation and damping
- 30practicemean-field self-consistency (Ising)
- 31practiceSCF convergence diagnostics
- 32practicecross-domain self-consistency
- 33checkCheck 1
- 34checkCheck 2
Reduce determinant energies to one- and two-electron integrals; let spin orthogonality kill terms.
- 35practicereal H₂ numbers
- 36practiceorbital energies
- 37practicetriplet spin
- 38practicefour electrons
- 39practiceKoopmans by subtraction
- 40practiceterm bookkeeping
- 41checkCheck 1
- 42checkCheck 2
Evaluate Hamiltonian matrix elements between determinants by counting orbital differences — three rules replace N! terms.
- 43practicediagonal energies
- 44practiceBrillouin numerically
- 45practicethe MP2/FCI coupling
- 46practicethe two-body cutoff
- 47practicepermutation signs
- 48practicespin selection rules
- 49checkCheck 1
- 50checkCheck 2
Evaluate matrix elements with creation/annihilation anticommutators; normal ordering and Wick contractions.
- 51practicenumber operator
- 52practicePauli algebraically
- 53practiceone-body element
- 54practiceordering signs
- 55practicenormal order
- 56practiceWick contractions
- 57checkCheck 1
- 58checkCheck 2
Normalize Slater and Gaussian primitives, read the exponent as an inverse size, and use the Gaussian product theorem — the bookkeeping behind every basis set.
- 59workedNormalize a primitive 1s Gaussian
- 60practiceThe Slater orbital, for contrast
- 61practiceThe cusp a Gaussian can never make
- 62practiceExponent as inverse size
- 63practiceThe product theorem, with numbers
- 64practiceCounting the degrees of freedom
- 65checkDerive the Gaussian product theorem
- 66checkWhy Gaussians win anyway