2012
DOI: 10.1088/0253-6102/57/2/09
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Three-Body Problem of H + 2 Ion

Abstract: The Feshbach-Rubinow approximation and its improved versions have been applied to the H + 2 ion system. The ground-state energies are calculated with these different methods. The best ground-state energy obtained is only 2% higher than the experimental result. Given the simplicity of the method, this accuracy is quite remarkable. It is shown that the screening effect plays a less significant role and the effective potential between the two protons is probably of most importance in this problem.

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Cited by 3 publications
(5 citation statements)
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“…Then the parameter b qe expresses the effect of "quantum entanglement". This quantum fluctuation appears only in quantum systems, and it is used as an order parameter of quantum systems at zero temperature in many cases [17][18][19][20][21][22]. The temperature dependences of b d1 , b cf , b qe and b d2 are shown in Fig.2.…”
Section: Equilibrium Systems Without External Fields (Hmentioning
confidence: 99%
See 3 more Smart Citations
“…Then the parameter b qe expresses the effect of "quantum entanglement". This quantum fluctuation appears only in quantum systems, and it is used as an order parameter of quantum systems at zero temperature in many cases [17][18][19][20][21][22]. The temperature dependences of b d1 , b cf , b qe and b d2 are shown in Fig.2.…”
Section: Equilibrium Systems Without External Fields (Hmentioning
confidence: 99%
“…From the definition of the entanglement entropy (6), it is easily understood that S A includes the original fluctuation of the partial system A. The above studies [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23][24] do not separate the fluctuations, namely the original fluctuations and the entanglement fluctuations. In addition, the entanglement entropy is not a physical parameter defined by eigenvalues of unitary operators, such as magnetization, but a status of states.…”
Section: Quantum Entanglementmentioning
confidence: 99%
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“…A quench scenario is considered thereafter, where we couple our model to a spin half system, and compute the LE. Thereafter, using the density matrix renormalisation group methods [2,[30][31][32], we compute the entanglement entropy, and find sharp jumps across both first order and second order phase transitions, a result that is in contradiction to the ones known in the literature, namely that the EE shows discontinuity at a first-order QPT, while a cusp or a kink in the EE indicates the second-order QPT [33,34]. Finally, we also consider multiple global quench scenarios in the model and contrast this with such quenches in the transverse XY model.…”
Section: Introductionmentioning
confidence: 99%