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Superposition Principle


The superposition principle for ordinary differential equations states that for a linear homogeneous ordinary differential equation, if y_1(x) and y_2(x) are solutions, then so is y_1(x)+y_2(x).

More generally, for any linear operator L, solutions of Lu=f and Lv=g satisfy L(au+bv)=af+bg. Thus responses to different sources can be combined by taking the same linear combination of the responses as of the sources. Examples include the addition of gravitational fields in Newton's shell theorem and velocity fields in Stokes flow.

In quantum mechanics, superposition means forming a linear combination of state vectors in a complex Hilbert space. For orthonormal vectors psi and phi, a normalized superposition is

 chi=apsi+bphi,

where a and b are complex numbers satisfying |a|^2+|b|^2=1. The corresponding pure-state density matrix chichi^| generally differs from the probabilistic mixture |a|^2psipsi^|+|b|^2phiphi^|. The former includes cross terms that describe coherence between the two components. A qubit provides the simplest example. Solutions of the Schrödinger equation for the same Hamiltonian also obey the superposition principle because the equation is linear (Nielsen and Chuang 2000).


See also

Fourier Series, Harmonic Analysis, Linear Operator, Ordinary Differential Equation, Snark Superposition

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References

Nielsen, M. and Chuang, I. Quantum Computation and Quantum Information. Cambridge, England: Cambridge University Press, 2000.Trott, M. "The Mathematica Guidebooks Additional Material: Wave Propagation on a Torus." https://www.mathematicaguidebooks.org/additions.shtml#N_1_13.

Referenced on Wolfram|Alpha

Superposition Principle

Cite this as:

Weisstein, Eric W. "Superposition Principle." From MathWorld--A Wolfram Resource. https://mathworld.wolfram.com/SuperpositionPrinciple.html

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