Introduction to Solid State Physics, Lecture 8: Reciprocal Lattice

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  • Опубликовано: 26 дек 2024
  • Upper-level undergraduate course taught at the University of Pittsburgh in the Fall 2015 semester by Sergey Frolov.
    The course is based on Steven Simon's "Oxford Solid State Basics" textbook.
    Lectures recorded using Panopto, to see them in Panopto viewer follow this link: pitt.hosted.pa...
    Syllabus available at: sergeyfrolov.w...
    Video is available in HD, make sure to adjust the youtube settings accordingly.

Комментарии • 12

  • @tekweh
    @tekweh 4 года назад +1

    You explained so well Sir

  • @没有巅峰人生永远是上
    @没有巅峰人生永远是上 8 месяцев назад

    thanks very much. I do not think I understand the proof at 36:17. for me questions i that x1 and x2 may not the projected points for G, so distance may not be |x1|-|x2|. I am not sure where I am wrong.

  • @claramdm6585
    @claramdm6585 8 лет назад +1

    In which lecture does the explanation of the reciprocal lattice start?

  • @Minhnguyen-ny7gq
    @Minhnguyen-ny7gq 8 лет назад

    Thank you very much!

  • @afshinbakhtiari1810
    @afshinbakhtiari1810 4 года назад

    Nice. I enjoyed

  • @shaw8234
    @shaw8234 2 года назад

    24:30

  • @TheBigBanggggg
    @TheBigBanggggg 7 лет назад

    Momentum k???

    • @abhinavgupta3632
      @abhinavgupta3632 7 лет назад

      Marco Polo k = 2pi / lambda
      By de broglie's principle
      Momentum = h/ lambda. So
      K is directly proportional to momentum hence ofter referred to as momentum

    • @Dr.kcMishra
      @Dr.kcMishra 6 лет назад +1

      Still not understand how to convert a real lattice into reciprocal lattice

    • @Aragmatiki
      @Aragmatiki 3 года назад

      @@Dr.kcMishra Fourier Transform the real lattice or just hit it with X-Rays and collect the data

  • @cerenbeyoglu5435
    @cerenbeyoglu5435 2 года назад

    kamerayı çek