Difference between revisions of "- The Resonance Condition"
(→The Resonance Condition) |
|||
| Line 10: | Line 10: | ||
| − | The energy of a magnetic dipole moment <math>\mu</math> in a magnetic field <math>H_{_0}</math> is <math>E=-\mu\cdot H_{0}</math>. If the energy in the system is low enough, most, if not all, of the spins will be parallel to the field (lowest energy state). However, if there is enough energy around then some | + | The energy of a magnetic dipole moment <math>\mu</math> in a magnetic field <math>H_{_0}</math> is <math>E=-\mu\cdot H_{0}</math>. If the energy in the system is low enough, most, if not all, of the spins will be parallel to the field (lowest energy state). However, if there is enough energy around then some nucleons will ''absorb'' a bit of energy and will become aligned anti-parallel to the magnetic field. |
A careful study of quantum mechanics reveals that the length of the nuclear angular momentum vector is <math>[I(I+1)]^{1/2}\hbar</math> but that the only measurable components of this vector are given by <math>m\hbar</math> , where <math>m</math>, the magnetic quantum number, may take any of the <math>(2I+1)</math> values in the series <math>I, I-1, I-2, ... , -(I-1), -I</math>. | A careful study of quantum mechanics reveals that the length of the nuclear angular momentum vector is <math>[I(I+1)]^{1/2}\hbar</math> but that the only measurable components of this vector are given by <math>m\hbar</math> , where <math>m</math>, the magnetic quantum number, may take any of the <math>(2I+1)</math> values in the series <math>I, I-1, I-2, ... , -(I-1), -I</math>. | ||
| − | Correspondingly, the nuclear magnetic moment also has <math>(2I+1)</math> components in proportion. We can define <math>\mu</math> as the maximum measurable (observable) component of the magnetic moment. | + | Correspondingly, the nuclear magnetic moment also has <math>(2I+1)</math> components in proportion. This is a consequence of "space quantization" demonstrated so famously by Stern and Gerlach in 1922. |
| + | |||
| + | We can define <math>\mu</math> as the maximum measurable (observable) component of the magnetic moment. Even though the length of the magnetic moment vector is <math>[(I+1)/I]^{1/2}\mu </math>, the quantity of physical interest is <math>\mu</math> and for this reason workers in the field usually refer to <math>\mu</math> as ''the magnetic moment''. As mentioned above, the energy levels of the nuclear magnet in the filed <math>H_{_0}</math> are given by the <math>(2I+1)</math> values of <math>-m\mu H_{_0}/I</math>. In the general case, this results in a set of equally-spaced levels with separation <math>\mu H_{_0}/I</math> between adjacent levels. | ||
| + | |||
| + | This separation is often written as <math>g \mu_{_0} H_{_0}</math>, where <math>g=\frac{\mu}{\mu_{_0}I}</math> is called the ''splitting factor'' of the ''g-factor''. | ||
Revision as of 13:09, 7 February 2019
The Resonance Condition
Consider an isolated nucleus in a steady magnetic field . The magnetic field breaks the symmetry of free space and defines a particular spatial direction. Suppose that the nucleus possesses an intrinsic "spin" with spin number so that it has an intrinsic magnetic moment (moving/spinning electric charge creates a magnetic field). How does this intrinsic "spin" relate to angular momentum? It is necessary to find this relation explicitly.
We know from quantum mechanics that (on small enough scales) energy appears in discrete bits ( shows its face ). It is then reasonable to suppose that "spin" energies are also discrete (or quantized). Physical experiments bear out this supposition.
The nucleus will have different energy states depending on the magnitude and direction of the nucleon's magnetic moment. See the figure below for the allowed spin states of a spin-1/2 particle.
The energy of a magnetic dipole moment in a magnetic field is . If the energy in the system is low enough, most, if not all, of the spins will be parallel to the field (lowest energy state). However, if there is enough energy around then some nucleons will absorb a bit of energy and will become aligned anti-parallel to the magnetic field.
A careful study of quantum mechanics reveals that the length of the nuclear angular momentum vector is but that the only measurable components of this vector are given by , where , the magnetic quantum number, may take any of the values in the series .
![{\displaystyle [I(I+1)]^{1/2}\hbar }](https://wikimedia.org/api/rest_v1/media/math/render/svg/7ab134e30271f2490d101ce9e10aef3314b00c32)
Correspondingly, the nuclear magnetic moment also has components in proportion. This is a consequence of "space quantization" demonstrated so famously by Stern and Gerlach in 1922.
We can define as the maximum measurable (observable) component of the magnetic moment. Even though the length of the magnetic moment vector is , the quantity of physical interest is and for this reason workers in the field usually refer to as the magnetic moment. As mentioned above, the energy levels of the nuclear magnet in the filed are given by the values of . In the general case, this results in a set of equally-spaced levels with separation between adjacent levels.
![{\displaystyle [(I+1)/I]^{1/2}\mu }](https://wikimedia.org/api/rest_v1/media/math/render/svg/66f79a86c4c790dee4dd076f2fa6e4468e92cf88)
This separation is often written as , where is called the splitting factor of the g-factor.
