In quantum mechanics, the inverse square potential is a form of a central force potential which has the unusual property of the eigenstates of the corresponding Hamiltonian operator remaining eigenstates in a scaling of all cartesian coordinates by the same constant. Apart from this curious feature, it's by far less important central force problem than that of the Keplerian inverse square force system.
Description The potential energy function of an inverse square potential is
V ( r ) = − C r 2 {\displaystyle V(r)=-{\frac {C}{r^{2}}}} , where C {\displaystyle C} is some constant and r {\displaystyle r} is the Euclidean distance from some central point. If C {\displaystyle C} is positive, the potential is attractive and if C {\displaystyle C} is negative, the potential is repulsive. The corresponding Hamiltonian operator H ^ ( p ^ , r ^ ) {\displaystyle {\hat {H}}({\hat {\mathbf {p} }},{\hat {r}})} is
H ^ = p ^ 2 2 m − C r ^ 2 {\displaystyle {\hat {H}}={\frac {{\hat {\mathbf {p} }}^{2}}{2m}}-{\frac {C}{{\hat {r}}^{2}}}} , where m {\displaystyle m} is the mass of the particle moving in the potential.
Properties The canonical commutation relation of quantum mechanics, [ x ^ i , p ^ i ] = i ℏ {\displaystyle [{\hat {x}}_{i},{\hat {p}}_{i}]=i\hbar } , has the property of being invariant in a scaling
p ^ i ′ = p ^ i / λ {\displaystyle {\hat {p}}_{i}'={\hat {p}}_{i}/\lambda } , and
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