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Range criterion
Encyclopedia
In quantum mechanics
, in particular quantum information
, the Range criterion is a necessary condition that a state must satisfy in order to be separable
. In other words, it is a separability criterion.
.
For simplicity we will assume throughout that all relevant state spaces are finite dimensional.
The criterion reads as follows: If ρ is a separable mixed state acting on H, then the range of ρ is spanned by a set of product vectors.
, it is obvious that the range of M, Ran(M), is contained in the linear span of
. On the other hand, we can also show
lies in Ran(M), for all i. Assume without loss of generality i = 1. We can write
, where T is Hermitian and positive semidefinite. There are two possibilities:
1) span
Ker(T). Clearly, in this case,
Ran(M).
2) Notice 1) is true if and only if Ker(T)
span
, where
denotes orthogonal compliment. By Hermiticity of T, this is the same as Ran(T)
span
. So if 1) does not hold, the intersection Ran(T)
span
is nonempty, i.e. there exists some complex number α such that
. So
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-16.gif)
Therefore
lies in Ran(M).
Thus Ran(M) coincides with the linear span of
. The range criterion is a special case of this fact.
A density matrix ρ acting on H is separable if and only if it can be written as
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-19.gif)
where
is a (un-normalized) pure state on the j-th subsystem. This is also
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-21.gif)
But this is exactly the same form as M from above, with the vectorial product state
replacing
. It then immediately follows that the range of ρ is the linear span of these product states. This proves the criterion.
Quantum mechanics
Quantum mechanics, also known as quantum physics or quantum theory, is a branch of physics providing a mathematical description of much of the dual particle-like and wave-like behavior and interactions of energy and matter. It departs from classical mechanics primarily at the atomic and subatomic...
, in particular quantum information
Quantum information
In quantum mechanics, quantum information is physical information that is held in the "state" of a quantum system. The most popular unit of quantum information is the qubit, a two-level quantum system...
, the Range criterion is a necessary condition that a state must satisfy in order to be separable
Separable states
In quantum mechanics, separable quantum states are states without quantum entanglement.- Separable pure states :For simplicity, the following assumes all relevant state spaces are finite dimensional...
. In other words, it is a separability criterion.
The result
Consider a quantum mechanical system composed of n subsystems. The state space H of such a system is the tensor product of those of the subsystems, i.e.![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-1.gif)
For simplicity we will assume throughout that all relevant state spaces are finite dimensional.
The criterion reads as follows: If ρ is a separable mixed state acting on H, then the range of ρ is spanned by a set of product vectors.
Proof
In general, if a matrix M is of the form![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-2.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-3.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-4.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-5.gif)
1) span
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-6.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-7.gif)
2) Notice 1) is true if and only if Ker(T)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-8.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-9.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-10.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-11.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-12.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-13.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-14.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-15.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-16.gif)
Therefore
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-17.gif)
Thus Ran(M) coincides with the linear span of
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-18.gif)
A density matrix ρ acting on H is separable if and only if it can be written as
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-19.gif)
where
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-20.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-21.gif)
But this is exactly the same form as M from above, with the vectorial product state
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-22.gif)
![](http://image.absoluteastronomy.com/images/formulas/8/2/2826760-23.gif)