| Ideal Level of Achievement (Very Good) | Standard Level of Achievement (Good) | Unacceptable Level of Achievement (Fail) |
| Evaluation 1 | One can calculate energy, wave function and existence probability of particles confined in potential wells by solving Schrödinger's equation when the well walls have finite height. | One can calculate energy, wave function and existence probability of particles confined in potential wells by solving Schrödinger's equation when the well walls have infinite height. | One cannot calculate energy, wave function and existence probability of particles confined in potential wells by solving Schrödinger's equation. |
| Evaluation 2 | One can calculate transmission and reflection probability of particle incident to potential barriers of finite width by solving Schrödinger's equation. | One can calculate transmission and reflection probability of particle incident to step-wise potential barriers by solving Schrödinger's equation. | One cannot calculate transmission and reflection probability of particle incident to step-wise potential barriers by solving Schrödinger's equation. |
| Evaluation 3 | One can caluculate entropy, temperature and pressure by using microcanonical ensemble in various cases. | One can caluculate entropy, temperature and pressure by using microcanonical ensemble in the cases of free particles and harmonic oscillators. | One cannot caluculate entropy, temperature and pressure by using microcanonical ensemble. |
| Evaluation 4 | One can caluculate energy and pressure by using canonical ensemble in various cases. | One can caluculate energy and pressure by using canonical ensemble in the cases of free particles and harmonic oscillators. | One cannot caluculate energy and pressure by using canonical ensemble. |