emanaly said:
I know that the vacuum in Quantum Field theory is not empty, but sometimes I find some people say that the particles are created from nothing because they are created from the vacuum , are those people expression a misleading?
In quantum field theory, the ideas of "vacuum" and "particle" become rather complicated. In the beginning, we define vacuum |0 \rangle as a no-particle state and we define creation operators a^{\dag} which produce 1-particle states by acting on the vacuum
|1 \rangle = a^{\dag} |0 \rangle
So far, everything is nice and easy. Next, we define the Hamiltonian of our theory, which is an operator expressed as a function of creation and annihilation operators H(a^{\dag}, a).
Now, according to physical intuition, we would expect that our vacuum |0 \rangle is an eigenstate of the Hamiltonian with lowest (zero?) energy. We would also expect one-particle states |1 \rangle to be eigenstates of the Hamiltonian. But this is not true in QFT! It appears that (almost) all Hamiltonians used in QFT do not have |0 \rangle and |1 \rangle as their eigenvectors.
The usual answer to this puzzle is to say that vacuum |0 \rangle is not the real physical vacuum state, and |1 \rangle are not states of real physical particles. It is said that |0 \rangle is a so-called "bare" vacuum, and |1 \rangle are states of "bare" particles. The vacuum and particles we see in reality are called "physical". These physical vacuum |vac \rangle and one-particle |one \rangle states are true eigenvectors of the Hamiltonian, and they are expressed as some complex linear combinations of "bare" particle states. This is the reason why one often hears that vacuum if full of (bare and virtual) particles, and that physical particles are "dressed" by the cloud of (virtual bare) particles.
This situation is a bit paradoxical. In QFT nobody cares about properties of bare particles and states. We want to study physical particles and states. However, our Hamiltonian H(a^{\dag}, a) is expressed through bare particle operators. This makes all calculations and their interpretation very cumbersome.
A great new idea arrived in 1958:
O. W. Greenberg, S. S. Schweber, "Clothed particle operators in simple models of quantum field theory", Nuovo Cim., 8 (1958) 378.
They said (rephrased): "since we don't care about bare particles, there is no reason to keep their creation and annihilation operators in the theory. Let's express our Hamiltonian directly in terms of creation and annihilation operators of "physical " or "dressed" particles. Let's work directly with the full physical vacuum state |vac \rangle." Greenberg and Schweber were able to show that "bare" particles can be eliminated and quantum field theories can be reformulated in this "dressed particle" picture without losing anything of importance. In this picture, vacuum |vac \rangle is a no-particle state (there are no "physical" particles in vacuum). One-particle states |one \rangle have just one (physical) particle in them. So, our physical intuition should not be offended.
So, in answering you question about vacuum filled with virtual particles, I should say that this (unfortunately widespread) idea is an artefact of using unphysical (bare) states as our basis in QFT. In fact, there are no "physical" particles in the "physical" vacuum.
Eugene.