trial wavefunction
A trial wavefunction is an educated guess at a system's state, built with a few adjustable parameters that we are free to tune. It is the raw material of the variational method: rather than solve for the true state directly, we propose a flexible form, calculate its average energy, and then dial the parameters to make that energy as small as the form allows. The result is our best approximation within the family we chose.
Good trial wavefunctions are not pulled from thin air; they are shaped by physical insight. We give them the right symmetry, the right behaviour far away (decaying to zero for a bound state), and the right qualitative shape near important features of the potential. A single width parameter for a smooth well, or a screening parameter for an atom's electron cloud, can already capture the essence while leaving room to optimize.
The art lies in balancing flexibility against effort. A trial form with more parameters can hug the true state more closely and yield a lower, better energy, but it also costs more to compute. Because the variational principle guarantees the energy is always an upper bound, comparing different trial forms is fair and simple: whichever gives the lower energy is the better guess, with no risk of being misled into something too good to be true.
A Gaussian guess with one tunable width: vary the parameter until the average energy is smallest.
A trial wavefunction must respect the system's symmetry and statistics to be meaningful — for instance, a guess for several identical fermions must be antisymmetric, or the energy estimate is physically wrong, not merely poor.