Quantum Mechanics: Angular Momentum

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This set of vocabulary flashcards covers the fundamental operators, eigenvalues, commutation relations, and ladder operators associated with Angular Momentum in Quantum Mechanics.

Last updated 8:27 PM on 6/3/26
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14 Terms

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Angular Momentum Components

The operators representing the components of angular momentum defined as Lx=yPzzPyL_x = yP_z - zP_y, Ly=zPxxPzL_y = zP_x - xP_z, and Lz=xPyyPxL_z = xP_y - yP_x.

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Fundamental Commutation Relations

The relationships between angular momentum components, specifically [Lx,Ly]=ih2τLz[L_x, L_y] = i\frac{h}{2\tau} L_z (or iħLzi\text{ħ} L_z) and its cyclic permutations.

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Simultaneous Measurement

The ability to measure L2L^2 and one component of angular momentum (typically LzL_z) at the same time because their commutator [L2,Lz]=0[L^2, L_z] = 0.

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Ladder Operators (L+L_+ and LL_-)

Operators defined as L+=Lx+iLyL_+ = L_x + iL_y and L=LxiLyL_- = L_x - iL_y that raise or lower the eigenvalue of the LzL_z component.

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LzL_z Eigenvalue

The value measured for the zz-component of angular momentum, represented as Lz=mħL_z = m\text{ħ}, where m=0,±1,±2m = 0, \text{±}1, \text{±}2 \text{…}.

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L2L^2 Eigenvalue

The square of the total angular momentum magnitude, given by the relation L2ψ(r,θ,ϕ)=l(l+1)ħ2ψ(r,θ,ϕ)L^2 \text{ψ}(r, \theta, \text{ϕ}) = l(l+1)\text{ħ}^2 \text{ψ}(r, \theta, \text{ϕ}).

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Lz Differential Operator

The representation of the zz-component of angular momentum in spherical coordinates as Lz=iħ∂ϕL_z = -i\text{ħ} \frac{\text{∂}}{\text{∂}\text{ϕ}}.

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Space Quantization

The phenomenon where the angular momentum vector can only take certain orientations relative to a chosen axis, defined by cos(θ)=ml(l+1)\text{cos}(\theta) = \frac{m}{\text{√}l(l+1)}.

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Raising Operator Commutation

The relation between the zz-component and the raising operator, expressed as [Lz,L+]=ħL+[L_z, L_+] = \text{ħ} L_+.

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Lowering Operator Commutation

The relation between the zz-component and the lowering operator, expressed as [Lz,L]=ħL[L_z, L_-] = -\text{ħ} L_-.

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Lowering Operator Action

The mathematical effect of LL_- on an eigenstate, given by Ll,m=l(l+1)m(m1)ħl,m1L_- |l, m\rangle = \text{√}l(l+1) - m(m-1) \text{ħ} |l, m-1\rangle.

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Raising Operator Action

The mathematical effect of L+L_+ on an eigenstate, given by L+l,m=l(l+1)m(m+1)ħl,m+1L_+ |l, m\rangle = \text{√}l(l+1) - m(m+1) \text{ħ} |l, m+1\rangle.

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Angular Momentum Uncertainty (ΔLx\text{Δ}L_x)

The statistical uncertainty in the xx-component, calculated using ΔLx=√〈Lx2Lx2\text{Δ}L_x = \text{√}\text{〈}L_x^2\text{〉} - \text{〈}L_x\text{〉}^2.

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Spherical Harmonics (YlmY_{lm})

The angular part of the wavefunction in spherical coordinates, which are common eigenstates of L2L^2 and LzL_z.