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In solid state physics, a particle's effective mass (often denoted m ∗ {\textstyle m^{*}} ) is the mass that it seems to have when responding to forces, or the mass that it seems to have when interacting with other identical particles in a thermal distribution. One of the results from the band theory of solids is that the movement of particles in a…
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effective mass band materials masses used density electron states electrons different general magnetic particle depends parabolic semiconductors energy force carrier
| Subject | Predicate | Object | Confidence | Src |
|---|---|---|---|---|
| the Drude model must be replaced with the effective mass.One remarkable property is that the effective mass can become negative | instance of | the electron mass in models | 0.80 | text |
| when the band curves downwards away from a maximum | instance of | the electron mass in models | 0.80 | text |
| conductivity appear to be isotropic | instance of | in crystals such as silicon the overall properties | 0.80 | text |
| angle-resolved photoemission spectroscopy | instance of | In recent years effective masses have more commonly been determined through measurement of band structures using techniques | 0.80 | text |
| gallium arsenide | instance of | V compounds | 0.80 | text |
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