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Volumn 77, Issue 5, 2008, Pages

Multiparticle entanglement in the Lipkin-Meshkov-Glick model

Author keywords

[No Author keywords available]

Indexed keywords

ANTIFERROMAGNETIC MATERIALS; ELEMENTARY PARTICLES; MAGNETIC ANISOTROPY; MATHEMATICAL MODELS; PARAMETER ESTIMATION; PHASE TRANSITIONS;

EID: 43249130120     PISSN: 10502947     EISSN: 10941622     Source Type: Journal    
DOI: 10.1103/PhysRevA.77.052105     Document Type: Article
Times cited : (39)

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    • note
    • The continuity of function f (x) is defined as limx→ x0 f (x) -f (x0) =0. First suppose that f (x) is a linear function of the subfunctions gk (x) (k=1,2,...,n), i.e., f (x) = k=1 n ck gk (x) in which ck is the coefficient. Without loss of generality any gk (x) is not supposed to be the linear combination of the other gk (x). Then the continuity of f (x) requires k=0 n ck limx→ x0 gk (x) - gk (x0) =0, limx→ x0 gk (x) - gk (x0) =0. The conclusion above means that the continuity of gk (x) is a sufficient and necessary condition for the continuity of f (x). With respect to the nonlinear case, let us consider the function f [g (x)] for simplicity. From the definition of the continuity and supposing δx=x- x0, it requires limx→ x0 f [g (x)] -f [g (x0)] =0, | limδx→0 (f [g (x)] / x) | x= x0 δx=0, | limδx→0 { f [g (x)] / g (x) } | x= x0 [g (x) -g (x0)] =0. The prefactor | f [g (x)] / g (x) | x= x0 has a nontrivial effect. Even if limδx→0 g (x) -g (x0) 0, the condition of continuity may still be satisfied only if this prefactor vanishes and limδx→0 g (x) -g (x0) keeps finite.
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