In the nearly-free electron model, the first band gap size is mainly proportional to A Lattice temperature only B Electron
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Chapter 23: Band Theory, Semiconductors and Superconductivity (Set-4)
In Kronig–Penney, band width mainly increases when adjacent wells have A Higher tunneling B Lower tunneling C No periodicity D
Continue readingChapter 23: Band Theory, Semiconductors and Superconductivity (Set-3)
In Kronig–Penney, increasing barrier height mainly tends to A Shrink band gaps B Remove periodicity C Fix Fermi level D
Continue readingChapter 23: Band Theory, Semiconductors and Superconductivity (Set-2)
In a crystal, allowed energy ranges are mainly called A Forbidden gaps B Lattice nodes C Energy bands D Photon
Continue readingChapter 23: Band Theory, Semiconductors and Superconductivity (Set-1)
In the Kronig–Penney picture, why do energy bands form in a crystal A Random atomic collisions B Single isolated atoms
Continue readingChapter 22: Specific Heat of Solids and Electron Gas (Set-5)
In classical harmonic solid, why does equipartition give molar heat capacity 3R rather than 3R/2 A Only kinetic terms B
Continue readingChapter 22: Specific Heat of Solids and Electron Gas (Set-4)
In classical theory, why does a vibrating atom contribute kB per direction to internal energy A Only kinetic part B
Continue readingChapter 22: Specific Heat of Solids and Electron Gas (Set-3)
For a monoatomic solid, why does Dulong–Petit give 3R at high temperature for one mole A Two rotational modes B
Continue readingChapter 22: Specific Heat of Solids and Electron Gas (Set-2)
For one mole of a solid, what does “3R” represent in Dulong–Petit law A B. Fermi energy value B A.
Continue readingChapter 22: Specific Heat of Solids and Electron Gas (Set-1)
What does Dulong–Petit law predict for molar heat capacity at high temperature A 3R value B R/2 value C 2R
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