2002
DOI: 10.1023/a:1021211206564
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Cited by 7 publications
(6 citation statements)
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“…Starting from these inequalities and whithin this Gramian approach, a bounds for expectation values of quantum observables have been derived for pure states [12,[20][21][22][23][24][25][26] and in the context of classical methods for quantum chemistry. While certainly useful, this leaves a gap for these bounds to be applied in the NISQ era where noise is prevalent and quantum states and their evolutions are described by density operators.…”
Section: Review Of the Gramian Methodsmentioning
confidence: 99%
“…Starting from these inequalities and whithin this Gramian approach, a bounds for expectation values of quantum observables have been derived for pure states [12,[20][21][22][23][24][25][26] and in the context of classical methods for quantum chemistry. While certainly useful, this leaves a gap for these bounds to be applied in the NISQ era where noise is prevalent and quantum states and their evolutions are described by density operators.…”
Section: Review Of the Gramian Methodsmentioning
confidence: 99%
“…The three fundamental inequalities governing this class are due to Temple, Weinstein, and Stevenson, all involving the computation of the mean value of the square of the Hamiltonian, 〈〉trueH^2. An interesting review on these methods can be found in the work of Marmorino . The lower bound E W , to the true energy E 0 defined by the Weinstein inequality, e .…”
Section: Calculating Upper and Lower Bounds To The Energymentioning
confidence: 99%
“…An interesting review on these methods can be found in the work of Marmorino. 16 The lower bound E W , to the true energy E 0 defined by the Weinstein inequality, e.g., is:…”
Section: Calculating Upper and Lower Bounds To The Energymentioning
confidence: 99%
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“…Recently, Taseli [22] studied the squared tangent potential V (x) = ν(ν − 1)tan 2 (x), x ∈ ( −π 2 , π 2 ) also known as the symmetric Pöschl-Teller potential [23,24]. It was noted that the energy eigenvalues, but not the eigenfunctions, of the Hamiltonian with the squared tangent potential on the symmetric interval ( −π 2 , π 2 ) are precisely the same as those of the Hamiltonian with the squared cotangent potential V (x) = ν(ν − 1)cot 2 (x) on the asymmetric interval (0, π) considered by Marmorino in [25] (see also [26]). This observation can be easily verified using the identity…”
Section: Trigonometric Tangent-squared Potentialmentioning
confidence: 99%