In 1 Dim harmonie oscillator $, $2.13 are the ground, Ist, Ind excited state respectively. There....
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In 1 Dim harmonie oscillator $, $2.13 are the ground, Ist, Ind excited state respectively. There. three states are normalised & orthogonal to one another. Y₁ & 4₂' are 2 states defined by 14₁ = -24, +34₂ $-$17, 2+₂ where x is car stant. 2 (1) The value of & for which 1/₂ is orthogonal to 4,, (a): 2 - (b) 1 (ec) (c) -1 (d) -2- ****** ("" for the value of x. determined in (1) pant, the expectation value of energy of oscillator in state 1/2 25. 9₁. = 中。2中,+342 2二中。一中+中之 In 1 Dim harmonie oscillator $, $2.13 are the ground, Ist, Ind excited state respectively. There. three states are normalised & orthogonal to one another. Y₁ & 4₂' are 2 states defined by 14₁ = -24, +34₂ $-$17, 2+₂ where x is car stant. 2 (1) The value of & for which 1/₂ is orthogonal to 4,, (a): 2 - (b) 1 (ec) (c) -1 (d) -2- ****** ("" for the value of x. determined in (1) pant, the expectation value of energy of oscillator in state 1/2 25. 9₁. = 中。2中,+342 2二中。一中+中之
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Applied Regression Analysis and Other Multivariable Methods
ISBN: 978-1285051086
5th edition
Authors: David G. Kleinbaum, Lawrence L. Kupper, Azhar Nizam, Eli S. Rosenberg
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