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Sistemi in 2D e 3D e Momento angolare

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Riassunto

Un oscillatore armonico piano ha come Hamiltoniano

$$ H = \frac{1} {{2m}}\left( {p_x^2 + p_y^2 } \right) + \frac{1} {2}m\omega ^2 \left( {q_x^2 + q_y^2 } \right). $$
  1. a)

    Si dica quali sono i livelli energetici e la loro degenerazione;

  2. b)

    si scriva l’Hamiltoniano in termini degli operatori

    $$ \eta + = \frac{1} {{\sqrt 2 }}\left( {a_x + ia_y } \right) \eta - = \frac{1} {{\sqrt 2 }}\left( {a_x + ia_y } \right) $$

    con

    $$ a_x = \sqrt {\frac{{m\omega }} {{2\hbar }}} q_x + i\sqrt {\frac{1} {{2m\omega \hbar }}} p_x a_y = \sqrt {\frac{{m\omega }} {{2\hbar }}} q_y + i\sqrt {\frac{1} {{2m\omega \hbar }}} p_y $$

    e dei loro hermitiano coniugati;

  3. c)

    si scriva l’operatore momento angolare per questo problema; cosa si puo dire sul momento angolare a fissato livello di energia?

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© 2008 Springer-Verlag Italia, Milano

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Angelini, L. (2008). Sistemi in 2D e 3D e Momento angolare. In: Meccanica quantistica: problemi scelti. UNITEXT(). Springer, Milano. https://doi.org/10.1007/978-88-470-0745-1_3

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