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| − | ''Quantum numbers'' are sets of parameters that produce physically acceptable solutions to the [[Schrodinger equation]]. They often take [[integer]] or half-integer values. They are used to label the different eigenstates of a quantum system. The number of quantum numbers in a system depends on the system, but there will be equal to or greater than the number of dimensions in the problem. | + | '''Quantum numbers''' are sets of parameters that produce physically acceptable solutions to the [[Schrodinger equation]]. They often take [[integer]] or half-integer values. They are used to label the different eigenstates of a quantum system. The number of quantum numbers in a system depends on the system, but there will be equal to or greater than the number of dimensions in the problem. |
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| | ==Infinite Square well== | | ==Infinite Square well== |
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| | <math>\psi(x) = \sqrt{\frac{2}{L}}\sin{n \pi x}</math> | | <math>\psi(x) = \sqrt{\frac{2}{L}}\sin{n \pi x}</math> |
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| − | Here, <math>n</math> is our quantum number and can take integer values. Notice how in this 1 dimensional problem there is only 1 quantum number. The | + | Here, <math>n</math> is our quantum number and can take integer values. Notice how in this 1 dimensional problem there is only 1 quantum number. The infinite square well problem can be extended to consider a particle trapped inside a 3 dimensional box. This produces a solution of the form: |
| − | infinite square well problem can be extended to consider a particle trapped inside a 3 dimensional box. This produces a solution of the form: | |
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| | <math>\psi(x,y,z) = \sqrt{\frac{8}{L_x L_y L_z}} \sin{(n_x x)} \sin{(n_y y)} \sin{(n_z z)}</math> | | <math>\psi(x,y,z) = \sqrt{\frac{8}{L_x L_y L_z}} \sin{(n_x x)} \sin{(n_y y)} \sin{(n_z z)}</math> |
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| | '''Principle quantum number''' - corresponds to the main [[electron shell]] in which the electron resides. Can have the value n=1, 2, 3..., corresponding to shells with increasing amounts of energy. However, in stable atoms, this tends to be less than or equal to 7 | | '''Principle quantum number''' - corresponds to the main [[electron shell]] in which the electron resides. Can have the value n=1, 2, 3..., corresponding to shells with increasing amounts of energy. However, in stable atoms, this tends to be less than or equal to 7 |
| − | <br>'''Azmuthal quantum number''' - corresponds to the [[electron subshell]] of the electron. Can have the number l=0, 1, 2, 3 up to n-1. It is also sometimes called the "angular momentum quantum number", due to its relationship with [[angular momentum]] | + | <br>'''Azimuthal quantum number''' - corresponds to the [[electron subshell]] of the electron. Can have the number l=0, 1, 2, 3 up to n-1. It is also sometimes called the "angular momentum quantum number", due to its relationship with [[angular momentum]] |
| | <br>'''Magnetic quantum number''' - corresponds to the [[orbital]] of the electron, the orbital is the different orientations of the electron subshell around the atom. It is normally denoted by m and varies from -l to l, taking integer values, i.e. -1, -l + 1,..., -1, 0, 1, ..., l-1, l | | <br>'''Magnetic quantum number''' - corresponds to the [[orbital]] of the electron, the orbital is the different orientations of the electron subshell around the atom. It is normally denoted by m and varies from -l to l, taking integer values, i.e. -1, -l + 1,..., -1, 0, 1, ..., l-1, l |
| | <br>'''Spin quantum number''' - corresponds to the spin of the electron, can have the value 1/2 or -1/2, indicating that each orbital of an atom can only hold 2 electrons. This is an example of a quantum number that takes half-integer values. | | <br>'''Spin quantum number''' - corresponds to the spin of the electron, can have the value 1/2 or -1/2, indicating that each orbital of an atom can only hold 2 electrons. This is an example of a quantum number that takes half-integer values. |