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0042560071
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note
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Strictly speaking, the action is the integral over time of the Lagrangian; however, it is convenient to label the present time-independent integral as the action, and call the variational minimization as an application of the principle of stationary action.
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McGraw-Hill, New York
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O. C. Zienkiewicz and R. L. Taylor, The Finite Element Method, 4th ed. (McGraw-Hill, New York, 1994); T. J. R. Hughes, The Finite Element Method (Prentice-Hall, Englewood Cliffs, NJ, 1987). L. R. Ram-Mohan, Finite Element and Boundary Element Applications to Quantum Mechanics (Oxford University Press, Oxford, U.K., 2002).
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O. C. Zienkiewicz and R. L. Taylor, The Finite Element Method, 4th ed. (McGraw-Hill, New York, 1994); T. J. R. Hughes, The Finite Element Method (Prentice-Hall, Englewood Cliffs, NJ, 1987). L. R. Ram-Mohan, Finite Element and Boundary Element Applications to Quantum Mechanics (Oxford University Press, Oxford, U.K., 2002).
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O. C. Zienkiewicz and R. L. Taylor, The Finite Element Method, 4th ed. (McGraw-Hill, New York, 1994); T. J. R. Hughes, The Finite Element Method (Prentice-Hall, Englewood Cliffs, NJ, 1987). L. R. Ram-Mohan, Finite Element and Boundary Element Applications to Quantum Mechanics (Oxford University Press, Oxford, U.K., 2002).
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0004161838
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to be published
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S. A. Solin, D. R. Hines, A. C. H. Rowe, J. S. Tsai, Yu. A. Pashkin, N. Goel, and M. B. Santos, Mater. Res. Soc. Symp. Proc. (to be published).
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Mater. Res. Soc. Symp. Proc.
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0043060897
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