(adsbygoogle = window.adsbygoogle || []).push({}); I don't understand what the eigenvalue of a translation operator means physically. The eigenvalues of other operators like momentum and hamiltonian give us the physically measurable values I suppose. Then what exactly do we obtain by the translation eigenvalues?

I am new to the field of quantum mechanics and as far as what I understand up until now the eigenvalue of an operator give us the physically measurable value of that operator.(Please correct me if I am wrong.)

So I was reading about the eigenfunctions of translation operator(the Bloch functions I mean) for a simple 1D chain of atoms extended upto infinity by the Born von Karman boundary condition(φ(0)=φ(l)) where L is the length of the chain. The author says that the eigenvalue equation of translation operator can be written as follows:

λ being a constant eigenvalue I presume.Rφ(x) = λφ(x)

After a little trial and error he defines:

where k is some number and u(k) is another function with the same periodicity as the lattice(also known as cell function in solid state physics)φ(x) = exp(2πikx)u(x)

(The details in the exponential are for mathematical convenience in further operations and is fairly elastic)

He then goes on to verify the solution

and since it is of the form as the first the formulated eigenfunction seems valid.Rφ(x) = exp(2πikR)φ(x)

I cannot visualise the translational operator properly. I mean I am confused as to what this eigenvalue means. I know I still need to normalise it using the identity translation but I am still confused. In fact I don't even know what's getting me so worked up. Any sort of help or advice will be welcomed.

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# I Regarding the eigenvalues of the translation operator

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