jslides 19 3 7 1 2 2 3 3 4 4 5 5 6 5.1................................... 6 5.2................................... 8 5.3..................................... 8 5.4........................... 8 5.5...................................... 9 6 9 6.1.................................. 9 6.2.................................. 10 6.3..................................... 10 6.4..................................... 11 6.5................................... 13 6.6.................................. 13 6.7..................................... 13 7 14 7.1...................................... 14 7.2............................. 15 7.2.1............................... 16 7.2.2.............................. 16 7.3..................................... 19 7.4 2..................................... 19 1
7.5.................................. 21 7.6................................... 21 7.7 Zapf Dingbats............................... 21 7.8.......................... 23 7.9................................... 23 7.10............................ 24 7.11................................. 24 7.12..................................... 25 7.13..................................... 26 8 Q&A 26 1 jslides.cls OHP DVIOUT OHP LATEX slides 2
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7.2 dviout version 3.17.4 Study the solution u(x) of the Shrödinger equation ¼ 1 2 ½ 2 x 2 + U(x) u(x) =λu(x) 1 j n j Study the solution u(x) of the Shrödinger equation ¼ 1 2 ½ 2 x 2 + U(x) u(x) =λu(x) 1 j n j with the potential function with the potential function U(x) = 1 i<j n C (x i x j ) 2. Study the solution u(x) of the Shrödinger equation ¼ 1 2 ½ 2 x 2 + U(x) u(x) =λu(x) 1 j n j with the potential function U(x) = 1 i<j n C (x i x j ) 2. Study the solution u(x) of the Shrödinger equation ¼ 1 2 ½ 2 x 2 + U(x) u(x) =λu(x) 1 j n j with the potential function C U(x) = sinh 2 (x 1 i<j n i x j ) It can be written by Bessel function when n =1. It can be written by Gauss hypergeometric function when n =1. Space 4 Off 4 dviout jslides 15
7.2.1 dviout 0 Space Space 1 0 1 0 Space 1 0 1 TEX jslides 7.2.2 Space Y=begin{slide} Study the solution $u(x)$ of the ShrY="odinger equation Y=[ Y=left(-Y=frac12Y=sum_{1Y=le jy=le n}y=frac{y=partial^2}{y=partial x_j^2} + U(x) Y=right)u(x) = Y=lambda u(x) Y=] with the potential function Y=[ U(x) = Y=sum_{1Y=le i < jy=le n} Y=frac{C}{(x_i - x_j)^2.} Y=] It can be written by Bessel function when $n=1$. Y=end{slide} Space 16
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