# Difference between revisions of "Electron Spin Resonance"

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Generally the magnetic moment of an electron is given by | Generally the magnetic moment of an electron is given by | ||

− | <math> \vec{\mu}=-\mu_B\left(\vec{L}+g_e\vec{S}\right) </math> , | + | <math> \vec{\mu}=-\mu_B\left(\vec{L}+g_e\,\vec{S}\right) </math> , |

where <math> \mu_B </math> is the Bohr's magneton and <math> g_e </math> the magnetogyric ratio, for a free electron it is <math> g_e=2.0023\approx 2 </math>. This formula includes the orbital angular momentum as well. With ESR it is only possible to detect and investigate the spin component of the total magnetic moment. Hence, in the further deviation we will look at the pure magnetic moment originating from the spin <math> \vec{S} </math>. | where <math> \mu_B </math> is the Bohr's magneton and <math> g_e </math> the magnetogyric ratio, for a free electron it is <math> g_e=2.0023\approx 2 </math>. This formula includes the orbital angular momentum as well. With ESR it is only possible to detect and investigate the spin component of the total magnetic moment. Hence, in the further deviation we will look at the pure magnetic moment originating from the spin <math> \vec{S} </math>. | ||

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#Absolute value: <math> |S|=\sqrt{s\left(s+1\right)} </math> | #Absolute value: <math> |S|=\sqrt{s\left(s+1\right)} </math> | ||

− | |||

#Projection onto the z-axis: <math> m_S=\pm\frac{\hbar}{2} </math> | #Projection onto the z-axis: <math> m_S=\pm\frac{\hbar}{2} </math> | ||

Incedentally, those two quantities are the best way to distinguish the state of the electron, because only their operator commute and hence, are mesasurable at the same time. For instance, it is not possible to measure two of the three cartesian components of the spin vector simultaneously. | Incedentally, those two quantities are the best way to distinguish the state of the electron, because only their operator commute and hence, are mesasurable at the same time. For instance, it is not possible to measure two of the three cartesian components of the spin vector simultaneously. | ||

+ | |||

+ | [[File:EPR splitting.jpg|thumb|right|400px|alt=A| The split of one energy state into two, once a magnetic field gets applied.|The split of one energy state into two, once a magnetic field gets applied.]] | ||

The equation for the energy of the electron's spin in an applied magnetic field contains a dot product between the magnetic moment and the B-field: | The equation for the energy of the electron's spin in an applied magnetic field contains a dot product between the magnetic moment and the B-field: | ||

− | <math> E=\mu_B | + | <math> E=\mu_B\,g_e\,\vec{S}\cdot\vec{B_Z} </math> |

− | |||

− | |||

It may seem to complicate the situation, but acutally it simplifies it a lot. We have chosen our magnetic field to point into the <math> z </math> direction. Since the spin is characterized by the projection onto the <math> z </math> axis, depicted by the Quantum number <math> m_S </math>, the dot product cancels to | It may seem to complicate the situation, but acutally it simplifies it a lot. We have chosen our magnetic field to point into the <math> z </math> direction. Since the spin is characterized by the projection onto the <math> z </math> axis, depicted by the Quantum number <math> m_S </math>, the dot product cancels to | ||

− | <math> E=\mu_B | + | <math> E=\mu_B\,g_e\,m_S\,B_Z </math> |

with | with | ||

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<math> m_S=\pm\frac{\hbar}{2} </math> . | <math> m_S=\pm\frac{\hbar}{2} </math> . | ||

− | Bohr's magneton <math> \mu_B </math> and the magnetogyric ratio <math> g_e </math> are both natural constants at this point. If a external magnetic field <math> B_Z </math> is applied (positive value, because we picked the <math> z </math> orientation of our coordinate system in such a way), the electron's energy is reduced or raised, depending whether <math> m_S </math> is negative or positive, respectively. The original single energy state, which we still get out of the equation for <math> B_Z=0 </math>, is split into two different energy states. Moreover, the energy difference is proportional to the strength of the applied magnetic field. Therefore that difference can be tuned very precisely by the experimental setup, which is very important for the latter detection of the ESR signal. | + | Bohr's magneton <math> \mu_B </math> and the magnetogyric ratio <math> g_e </math> are both natural constants at this point. If a external magnetic field <math> B_Z </math> is applied (positive value, because we picked the <math> z </math> orientation of our coordinate system in such a way), the electron's energy is reduced or raised, depending whether <math> m_S </math> is negative or positive, respectively. The original single energy state, which we still get out of the equation for <math> B_Z=0 </math>, is split into two different energy states. Moreover, the energy difference |

+ | |||

+ | <math> \Delta E=E_{+1/2}-E_{-1/2}=+\frac{1}{2}\,\mu_B\,g_e\,B_Z-(-\frac{1}{2}\,\mu_B\,g_e\,B_Z)=\mu_B\,g_e\,B_Z</math> | ||

+ | |||

+ | is proportional to the strength of the applied magnetic field. Therefore that difference can be tuned very precisely by the experimental setup, which is very important for the latter detection of the ESR signal. | ||

+ | For typical laboratory B-fields the energy difference <math> \Delta E </math> ranges in the microwave photon band, if you convert the energy to wavelength or rather frequency. This is the point, where the name of the entire phenomenon originates. Namely, if one irradiates the unpaired spin, which normally sits in the lower energy state (due to general energy minimization of nature), with the correct frequency, the energy gets absorbed, combined with a transition to the upper level. In this case, the energy of the photons match exactly the energy difference between both states. Physicist call this situation '''Electron Spin Resonance'''. | ||

+ | In formula language the fowolling becomes true; | ||

+ | <math> h\,\nu=\mu_B\,g_e\,B_Z </math> , | ||

+ | where <math> h </math> is Planck's constant and <math> \nu </math> the frequency of the incident light. | ||

+ | Other than the magnetogyric ration <math> g_e </math> are all quantities either natural constants or measured values. Above I claimed that this value is a natural constant, too. Well, technically it is one, however, depends on the material and its compounds and especially spin stucture. Taking the previous equation as well as transferring it to an expression for <math> g_e </math> yields material properties with regard to the spin configuration. For example, the comparison to the definite value of a free electron is a indicator for various substances' features. | ||

## Revision as of 21:28, 9 November 2014

**Electron Spin Resonance (ESR)** is a phenomenon, usefull for the investigation of materials which contain unpaired spins. Those are caused by various sources. One are not completely filled atomic shells, however, the more interesting ESR signals arise from different circumstances combined in the term defect. For instance, a important one is impurities of semiconductors or isolators which can trap electron or holes. Therefore this measuring technique is very powerfull evaluation of material properties and is used in lots of research fields in physics, chemistry and biology.

## Physical background

As the term Electron Spin Resonance already implies, the most essential part of the entire topic is the Spin, an intrinsic angular momentum of the electron. In an atom most of the electron are paired regarding spin. That is, each electron has a partner with an opposite spin, creating a zero net spin. Depending on the electron configuration of an atom or one step above in molecules and solids respectively, it is possible that there are a few or even many single electrons, being up to material.

Generally the magnetic moment of an electron is given by

,

where is the Bohr's magneton and the magnetogyric ratio, for a free electron it is . This formula includes the orbital angular momentum as well. With ESR it is only possible to detect and investigate the spin component of the total magnetic moment. Hence, in the further deviation we will look at the pure magnetic moment originating from the spin .

If the spin and its magnetic moment is placed in a externally applied magnetic field, the magnetic moment of the spin starts to precess around the axis of the magnetic field due to the torque

.

As always in Quantum Physics the chosen axis of the magnetic field points in direction.

In generell, the energy of a magnetic moment is defined as

.

The magnetic moment is related to the spin , which is a so called Quantum Vector with special properties:

- Absolute value:
- Projection onto the z-axis:

Incedentally, those two quantities are the best way to distinguish the state of the electron, because only their operator commute and hence, are mesasurable at the same time. For instance, it is not possible to measure two of the three cartesian components of the spin vector simultaneously.

The equation for the energy of the electron's spin in an applied magnetic field contains a dot product between the magnetic moment and the B-field:

It may seem to complicate the situation, but acutally it simplifies it a lot. We have chosen our magnetic field to point into the direction. Since the spin is characterized by the projection onto the axis, depicted by the Quantum number , the dot product cancels to

with

.

Bohr's magneton and the magnetogyric ratio are both natural constants at this point. If a external magnetic field is applied (positive value, because we picked the orientation of our coordinate system in such a way), the electron's energy is reduced or raised, depending whether is negative or positive, respectively. The original single energy state, which we still get out of the equation for , is split into two different energy states. Moreover, the energy difference

is proportional to the strength of the applied magnetic field. Therefore that difference can be tuned very precisely by the experimental setup, which is very important for the latter detection of the ESR signal.

For typical laboratory B-fields the energy difference ranges in the microwave photon band, if you convert the energy to wavelength or rather frequency. This is the point, where the name of the entire phenomenon originates. Namely, if one irradiates the unpaired spin, which normally sits in the lower energy state (due to general energy minimization of nature), with the correct frequency, the energy gets absorbed, combined with a transition to the upper level. In this case, the energy of the photons match exactly the energy difference between both states. Physicist call this situation **Electron Spin Resonance**.

In formula language the fowolling becomes true;

,

where is Planck's constant and the frequency of the incident light.

Other than the magnetogyric ration are all quantities either natural constants or measured values. Above I claimed that this value is a natural constant, too. Well, technically it is one, however, depends on the material and its compounds and especially spin stucture. Taking the previous equation as well as transferring it to an expression for yields material properties with regard to the spin configuration. For example, the comparison to the definite value of a free electron is a indicator for various substances' features.

.

.

.

**TO BE CONTINUED**

.

.

.