Vengono dedotte le equazioni per i momenti idrodinamici di un sistema quantistico descritto da un'Hamiltoniana $k \cdot p$ a due bande. Nel caso di stati puri si dimostra che le equazioni dei momenti di ordine 0 e di ordine 1 forniscono un sistema chiuso che costituisce l'analogo a due bande delle equazioni del fluido di Madelung.
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