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Zigzag Spin Model at F-AF Transition Point

Let us consider the s = spin chain with nearest- and next-nearest interactions given by the Hamiltonian [Pg.771]

We note that the Hamiltonian (2) has a symmetry, its spectrum coincides with the spectrum of H(x) obtained by the following transformation [Pg.772]

This transformation permutes the factors at the first and the second terms in the Hamiltonian (2). Thus, due to the symmetry it is sufficient to consider the range [Pg.772]

we will show that the ground-state energy of (2) is zero. Let us represent the Hamiltonian (2) as a sum of Hamiltonians hn of cells containing three sites [Pg.772]

We will present a singlet wave function which is an exact zero-energy eigenvector to each hn and, therefore, it is the exact ground-state wave function of (2). This function has a form [Pg.773]


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