Mod-01 Lec-21 Quenching of Orbital Angular Momentum; Ferromagnetism

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  • Опубликовано: 18 окт 2024

Комментарии • 11

  • @jitendramisra722
    @jitendramisra722 4 года назад +1

    Excellent man of knowledge and kind human being.

  • @nabeel123ful
    @nabeel123ful Год назад

    at the very beginning, he had typos to say 4f electrons protected by 5s and 5p electrons for rare earth element, but I think they should be 6s and 5d electrons.

  • @vishnuunni.c9802
    @vishnuunni.c9802 6 лет назад +2

    At 10.50,. Its stated that... An imaginary operator acting on a real function gives eigen value equal to zero ?
    How ?

    • @moglibora
      @moglibora 5 лет назад

      It's not the eigenvalue, the expectation value would be zero

    • @sairamithineni2588
      @sairamithineni2588 3 года назад

      @@moglibora why would that vanish again

    • @shaikwasef6974
      @shaikwasef6974 3 года назад

      The angular momentum Lz operator acts on a wave function ( say f ) as the following :
      -i.hbar.(dow.f/dowphi) = m.hbar.f
      if f is a real function, we would not get a real eigenvalue ( m is the magnetic quantum number and is real , hbar is real , hence m.hbar is real ) since the i term on the left cannot vanish.
      The only way this equation is satisfied is if the eigenvalue is zero.

    • @nabeel123ful
      @nabeel123ful Год назад

      @@shaikwasef6974 Thanks for your explanation, but why would we force the eigenvalue to vanish instead of questioning the validity of the assumption of a real wavefunction? Of course, this goes back to why would a nondegenerate eigenvector of an operator must be real, which I don't quite get.

  • @ishanandwani6113
    @ishanandwani6113 6 лет назад

    T and theta are different ?? at 22:21

    • @majjisiva6710
      @majjisiva6710 8 месяцев назад

      Theta is nothing but Curie temperature here