The nonlinear coefficient β in the JMGT equation is uniquely determined from boundary measurements, while α, q, and F are recovered up to gauge symmetry.
Numerical reconstruction of Schrödinger equa- tions with quadratic nonlinearities
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Gauge symmetry and uniqueness in inverse problems for the JMGT equation
The nonlinear coefficient β in the JMGT equation is uniquely determined from boundary measurements, while α, q, and F are recovered up to gauge symmetry.