trivalent$85288$ - significado y definición. Qué es trivalent$85288$
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Qué (quién) es trivalent$85288$ - definición

DOPANT ATOM THAT, WHEN ADDED TO A SEMICONDUCTOR, CAN FORM A P-TYPE REGION
Acceptor atom; Acceptor impurity; Trivalent impurity

Trivalent group 14 radicals         
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CLASS OF CHEMICAL COMPOUNDS
A trivalent group 14 radical (also known as a trivalent tetrel radical) is a molecule that contains a group 14 element (E = C, Si, Ge, Sn, Pb) with three bonds and a free radical, having the general formula of R3E•. Such compounds can be categorized into three different types, depending on the structure (or equivalently the orbital in which the unpaired electron resides) and the energetic barrier to inversion.
Acceptor (semiconductors)         
In semiconductor physics, an acceptor is a dopant atom that when substituted into a semiconductor lattice forms a p-type region.
Cubic graph         
  • The [[complete bipartite graph]] <math>K_{3,3}</math> is an example of a bicubic graph
  • Representation of a planar embedding as a graph-encoded map
NODE-LINK GRAPHS IN WHICH EVERY VERTEX IS INCIDENT TO EXACTLY THREE EDGES
Trivalent graph; Bicubic graph; Cubic graphs
In the mathematical field of graph theory, a cubic graph is a graph in which all vertices have degree three. In other words, a cubic graph is a 3-regular graph.

Wikipedia

Acceptor (semiconductors)

In semiconductor physics, an acceptor is a dopant atom that when substituted into a semiconductor lattice forms a p-type region.

When silicon (Si), having four valence electrons, is doped with elements from group III of the periodic table, such as boron (B) and aluminium (Al), both having three valence electrons, a p-type semiconductor is formed. These dopant elements represent trivalent impurities. Other trivalent dopants include indium (In) and gallium (Ga).

When substituting for a silicon atom in the crystal lattice, the three valence electrons of boron form covalent bonds with three of the Si neighbours but the bond with the fourth remains unsatisfied. The initially electro-neutral acceptor becomes negatively charged (ionised). The unsatisfied bond attracts electrons from the neighbouring bonds. At room temperature, an electron from a neighbouring bond can jump to repair the unsatisfied bond thus leaving an electron hole, which is a place where an electron is deficient. The hole, being positively charged, attracts another electron from a neighbouring bond to repair this unsatisfied bond. This chain-like process results in the hole moving around the crystal as a charge carrier. This process can sustain in an electric current useful in electronic circuits.