Beam Mode

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OAM / photon2 ℏ
Ring radius0.00
Topological charge ℓ2
Radial index p0
Rings (p+1)1
Cross-section of a Laguerre–Gauss LGp,ℓ beam. Amplitude ∝ (r√2/w₀)|ℓ| · Lp|ℓ|(2r²/w₀²) · e−r²/w₀², phase = ℓθ. The helical phase forces zero amplitude on-axis, giving the doughnut; p adds p concentric extra rings. "Animate propagation" spins the helical phase front, as it would along the beam's optical axis.