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Why this simple scaling appears in so many devices has no accepted explanation.","posed_since":"1949","precise":"Cross-field diffusion in many magnetized low-temperature plasmas follows the Bohm form $D_{B} = c T_{e}/(16 e B)$ ($T_{e}$ in erg), scaling as $1/B$ rather than the classical $1/B^{2}$. Determine whether a common mechanism (E x B drift-wave turbulence, sheath-coupled instabilities, gradient-drift or Simon-Hoh modes) produces this scaling, the origin of the coefficient near 1/16, and the conditions where it fails. An answer is a theory predicting $D_{\\mathrm{perp}}$ versus $B, T_{e}$ and geometry, validated across at least two device classes.","problem_ref":null,"references":"","settled_by":"Kinetic simulations and measurements in two device classes (e.g. Penning discharges and Hall thrusters) agreeing on $D_{\\mathrm{perp}}(B, T_{\\mathrm{e}})$ and its departures from Bohm scaling.","status_note":"","title":"Why magnetized discharges often show Bohm-scaled cross-field 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