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target="_blank" rel="nofollow" href="#fb3_img_img_d4bd1e75-5ae0-5f44-a06e-84e18a8dba52.png" alt="i StartFraction partial-differential psi Over partial-differential t EndFraction equals upper H psi where upper H equals minus StartFraction partial-differential squared Over partial-differential x squared EndFraction plus upper V left-parenthesis x right-parenthesis period"/>

      while the implicit Euler BTCS scheme is given by:

i StartFraction psi Superscript n plus 1 Baseline minus psi Superscript n Baseline Over k EndFraction equals upper H psi Superscript n plus 1

      or

      or

left-parenthesis 1 plus italic i upper H k right-parenthesis psi Superscript n plus 1 Baseline equals psi Superscript n Baseline period

      (5.27)integral Subscript negative infinity Superscript infinity Baseline StartAbsoluteValue psi left-parenthesis x right-parenthesis EndAbsoluteValue squared italic d x equals 1 period

      A remedy for this is to use the Cayley form (this is essentially the Crank–Nicolson scheme):

i StartFraction psi Superscript n plus 1 Baseline minus psi Superscript n Baseline Over k EndFraction equals StartFraction upper H Over 2 EndFraction left-parenthesis psi Superscript n plus 1 Baseline plus psi Superscript n Baseline right-parenthesis

      or

      This scheme is unitary; you can check this by a bit of arithmetic using complex arithmetic.

      The solution of (5.24) is:

      (5.29)psi left-parenthesis x comma t right-parenthesis equals e Superscript negative italic i upper H t Baseline psi left-parenthesis x comma 0 right-parenthesis

      Matrix theory is too important to be ignored or given short shrift in any book on numerical analysis and its applications. For this reason, we gave a reasonably detailed exposition of matrix theory as a companion to the other chapters in this book (and it could possibly be a companion to other books).

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