In Quantum Computation we define a map that takes on density matrix to another. It is represented by some kraus matrices. I do not know why it has to be completely positive.
I'm not active in this area, so take my remarks with a grain of salt.
A positive map \Phi takes a density matrix to another density matrix. The difference between positive and completely positive maps is important for entangled states in combined systems, where the map acts only on one of the systems.
For a seperable state \rho = \rho_1 \otimes \rho_2, a new state (\Phi \otimes I_2)\rho is always positive (I_2 is the identity in the second system). Counterintuitively, non-seperable states can yield negative eigenvalues when acted upon with a positive but not completely positive map.
Since we want our map to yield a valid density matrix in all cases, we require it to be completely positive, that is to say that (\Phi \otimes I_2)\rho has to be positive for arbitrary systems 2 and states \rho.
Insights auto threads is broken atm, so I'm manually creating these for new Insight articles.
Towards the end of the first lecture for the Qiskit Global Summer School 2025, Foundations of Quantum Mechanics, Olivia Lanes (Global Lead, Content and Education IBM) stated...
Source: https://www.physicsforums.com/insights/quantum-entanglement-is-a-kinematic-fact-not-a-dynamical-effect/
by @RUTA
If we release an electron around a positively charged sphere, the initial state of electron is a linear combination of Hydrogen-like states. According to quantum mechanics, evolution of time would not change this initial state because the potential is time independent. However, classically we expect the electron to collide with the sphere. So, it seems that the quantum and classics predict different behaviours!
The wavefunction of an atomic orbital like ##p_x##-orbital is generally in the form ##f(\theta)e^{i\phi}## so the probability of the presence of particle is identical at all the directional angles ##\phi##. However, it is dumbbell-shape along the x direction which shows ##\phi##-dependence!