Generation of Spin 1 System

In this paper, we shall establish the connection between the group theory and quantum mechanics by showing how the group theory helps us to construct the spin operators. We look to the group generators SU(3). From these generators, new spin 1 operators will be constructed. These operators , x y S S − − and z S − satisfy all the properties of Pauli spin operators , x y S S and z S . We shall discuss the notion of spin squeezing and correlations for pure spin 1 system using our spin operators , x y S S − − and z S − .


Introduction
The fundamental problem in quantum physics is to investigate the Hamiltonian operator H which is a Hermitian operator.
The operator H may correspond to physical observables such as spin operators… The number of eigen-functions of H in the most quantum systems is in the fact infinite and the set of all eigen-functions of a Hermitian operator is a complete set. These eigen-functions define a Hilbert space on which the operator acts.
The group theory becomes almost inevitable when the system contains a large number of particles. The operator representation can be better understood in the light of the group theoretical interpretation such as spin or Isospin.
The spin operators possess a wide range of applications which plays a key role in both foundation of quantum physics and quantum information [1]- [6], and also makes the atomic clocks more precise [7] [8].
The concept of spin is fascinating in quantum theory which is defined through the commutation relations ( 1 =  ) [9], i × = j j j (1)  On the other hand, the concept of spin is understood through the introduction of a spin operator s consisting of three Hermitian components S x , S y and S z which is called Pauli matrices. The square of the spin operators s defined as: (2) and , is again a Hermitian operator. One can now construct simultaneous eigen-states of 2 S and z S . These eigen-states labeled by sm satisfy: which are well known as S x , S y and S z . Our aim in this paper is to construct a new spin operator which will give equivalent results to the Pauli spin operator by using the group generator.
The spin operators S x , S y and S z possess a wide range of applications such as spin squeezing for sharp as well as for non-sharp spin value [10] [11] [12] [13]. This paper is organized as follows.
In Section 2, we deal with the definition of the group SU(2) and SU(3); from these groups, we will generate new spin operators. We shall show that new spin operators will be acting on a physical system with respect to a new frame. These operators will be satisfying all the physical properties such as commutation relations.
In Section 3, we shall look to the squeezing spin system using a new spin operator with respect to the new frame.
In Section 4, the spin-spin correlations will be discussed and we will show that the new operators give an equivalent result of squeezing and correlation which had been calculated with respect to Pauli-operators [12].

Spin Operators and Group Generators
The group of all unitary matrices of ordered n is known as U(n), whereas the group of all unitary matrices of ordered n with determinant +1 is denoted by SU(n). It is clear that SU(n) is a subgroup of U(n), since a unitary matrix of order n has n 2 − 1 independent parameters.

M. Kh. Srour et al. Journal of Applied Mathematics and Physics
The unitary unimodular group SU (2) in two complex dimensions is the simplest non-trivial example for a non-Abelian group which describe the two level quantum system, at the same time SU(2) is hemimorphic of SU(3).
Thus the Lie algebra of SU(2) in three dimensional representation can be chosen as the set of all real linear combination of , x y σ σ and z σ , such that: The next group after SU(2) is SU(3) which possesses eight-dimensional unimodular matrices in three complex dimension [14].
It is clear from Equation (2) It is clear from Equations (10), (11) and (12) (14) from Equation (13), it is clear that the two groups of spin operators coincide with the z-axis.
To illustrate this situation as shown in Figure 1, let us consider in the simplest case of s = 1. The spin (s = 1) state ψ makes an angle γ with respect to z-axis in the frame xyz and the corresponding operators are Pauli operators , x y S S and z S . Now, in the second frame x'y'z' coincides with the z-axis in frame xyz. We see from Figure 1, that the polar angle with respect to xyz frame is γ, while with respect to x'y'z' it will be π + γ. The operator corresponding to the frame x'y'z' will be

Squeezing Criterion for Pure Spin State
In the last section, we construct left-handed spin operators. In this section we deal with the squeezing aspects for pure spin 1-system by using the left-handed operators. The notion of squeezing had been discussed for spin system with arbitrary sharp spin value by several authors [10] [11] [12] [13].
In order to discuss the squeezing condition, we restrict ourselves to Heisenberg's relationship that a spins-state is squeezed in the spin component normal to the mean spin direction of  The study in this section shows that the left-handed operators give the equivalent result done by Mallesh with respect to the frame xyz and Pauli operators [12].

Spin-Spin Correlations
In the last section, we have looked into squeezing aspect using left-handed operators of pure spin 1 system with respect to the frame x'y'z' as shown in Figure 1.
The squeezing of a spin system arises from the existence of quantum correlations between the spin components.
This can be done by assuming the model in which the spin 1 state is constructed by 2s spin 1 2 system, this work had been done by Mallesh [12] with respect to the frame xyz. In this section we will calculate the correlations with respect to the frame x'y'z' as shown in Figure 3 using left-handed operators.
Here the basis state is referred to the z-axis in frame x'y'z'. The state ψ expressed in terms of the spinor state with respect to z in frame x'y'z' has a form: In terms of the constituent spinor states It is clear from the above equations that: which happen to be a Lakin frame in x'y'z' frame.
For such state, the relevant quantities: The matrix element of correlation D 12 is defined through its elements: In addition, the maximum value of correlations as shown in Figure 5 is 0.25.
Thus, the trace condition Equation (36) is the necessary and sufficient condition for pure spin 1 state to be squeezed.
At the end of this section, we have shown that by using the left-handed operator in a calculation for squeezing or correlations we have got the same result which is done by Mallesh [12].