angular ladder operators
The angular ladder operators, written L+ and L−, are clever combinations of Lx and Ly that step a state up or down the angular-momentum ladder. Apply L+ and the magnetic quantum number m increases by one; apply L− and it decreases by one. The total angular momentum ℓ stays put — these operators reorient the angular momentum without changing how much of it there is.
Their power is that they let you build a whole family of states from a single one, by repeated stepping, much as the ladder operators of the harmonic oscillator generate its energy levels. Starting from any state and climbing with L+, you eventually reach a top rung where m = +ℓ and the operator returns nothing — you cannot tilt further toward the axis. The same happens at the bottom, m = −ℓ. These natural stopping points are what force m to run from −ℓ to +ℓ in integer steps.
Beyond their practical use, the ladder operators reveal the structure of angular momentum without any pictures of orbits or cones. Working purely from the commutation relations, they show that the allowed values of ℓ and m, and even the possibility of half-integer spin, are dictated by algebra alone. They turn a problem about rotation in space into clean bookkeeping about raising and lowering a single quantum number.
L+ and L− shift m by one while leaving ℓ unchanged.
L+ and L− are not Hermitian, so they are not themselves observables — you cannot measure them. They are bookkeeping tools for moving between states, related as each other's adjoint.