Superposition of wave functions

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SUMMARY

The discussion centers on the superposition of wave functions in quantum mechanics, specifically addressing the scenario where two particles have wave functions w1 and w2. The resultant wave function W, defined as W = w1 + w2, indeed corresponds to the probability density of locating both particles within a specified spatial interval. This conclusion aligns with the postulates of quantum mechanics, which state that any superposition of state vectors remains a valid state vector. The probability of measuring a specific eigenvalue from an operator is mathematically expressed using the formula P_n(a_n)=\frac{|\langle \psi_n | \psi \rangle|^2}{\langle \psi | \psi \rangle}.

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If 2 particles have wave functions w1 and w2, in which W = w1 + w2 is a superposition of the wave functions, then would the probability density of W correspond to the probability of finding both particles at the same position within some interval of space?
 
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The short answer is yes. One of the postulates of quantum mechanics is

"The state of any physical system is specified, at each time t, by a state vector [itex]|\psi(t) \rangle[/tex] in a Hilbert space, [itex]|\psi(t) \rangle[/tex] contains all the needed information about the system. Any superposition of state vectors is also a state vector."<br /> <br /> In fact, even further, that is exactly how finding the probability of a state works for discrete spectra. For nondegenerate discrete eigenvalues the probability of obtaining one of the eigenvalues [itex]a_n[/itex] of an operator [itex]\hat{A}[/itex] is given by<br /> <br /> [tex]P_n(a_n)=\frac{|\langle \psi_n | \psi \rangle|^2}{\langle \psi | \psi \rangle}[/tex]<br /> <br /> where [itex]\psi_n[/itex] is the eigenstate of [itex]\hat{A}[/itex] with eigenvalue a_n.[/itex][/itex]
 

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