Electron phonon interaction hamiltonian problem

In summary, the conversation discusses the different notations used for the phonon part of the frohlich electron phonon interaction hamiltonian, specifically the use of a + or - sign. The individual asks for suggestions on why the sign may be different and offers some possibilities, such as a typo or different definitions of operators, as well as the presence of fermion terms in the equation.
  • #1
phdojg
5
0
Hi

In almost every reference I have found the phonon part of the frohlich electron phonon interaction hamiltonian is given by
(b_{q}+b^{\dag}_{-q})

notice the +, where b_{q} is a phonon creation operator and b^{\dag}_{-q})is the destruction operator of a phonon.

however in a paper on colossal magnetoresistance and in the book polarons in advanced materials p69, this + is replaced with a -, I simply cannot understand why this is. There are no real changes to the rest of the hamiltonian simply different constants at the start depending what has been incorperated into the coupling constant. Does anyone have any sugestions as to how or why the sign is different? any sugestions would be really helpful

Many thanks
 
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  • #2
phdojg said:
Hi

In almost every reference I have found the phonon part of the frohlich electron phonon interaction hamiltonian is given by
(b_{q}+b^{\dag}_{-q})

notice the +, where b_{q} is a phonon creation operator and b^{\dag}_{-q})is the destruction operator of a phonon.

however in a paper on colossal magnetoresistance and in the book polarons in advanced materials p69, this + is replaced with a -, I simply cannot understand why this is. There are no real changes to the rest of the hamiltonian simply different constants at the start depending what has been incorperated into the coupling constant. Does anyone have any sugestions as to how or why the sign is different? any sugestions would be really helpful

Many thanks

typo maybe? or different definitions of 'b'. Or maybe in one case they interchange a position operator with a momentum operator--e.g., inside a dipole matrix element?
 
  • #3
Are there any fermion terms? Maybe the minus sign comes from commuting them somewhere in the derivation.
 

1. What is the electron-phonon interaction Hamiltonian problem?

The electron-phonon interaction Hamiltonian problem is a theoretical physics problem that involves studying the interaction between electrons and phonons (quantized lattice vibrations) in a solid material. This interaction is described by a mathematical model known as the electron-phonon Hamiltonian, which is used to understand the behavior of electrons and phonons in materials at the quantum level.

2. Why is the electron-phonon interaction important?

The electron-phonon interaction is crucial for understanding the properties of materials, such as electrical conductivity, thermal conductivity, and superconductivity. It also plays a significant role in the behavior of materials under extreme conditions, such as high pressures and temperatures.

3. How is the electron-phonon interaction Hamiltonian problem solved?

The electron-phonon interaction Hamiltonian problem is typically solved using various theoretical and computational methods, such as perturbation theory, density functional theory, and many-body techniques. These methods allow scientists to calculate the effects of electron-phonon interactions on the properties and behavior of materials.

4. What are the challenges in studying the electron-phonon interaction Hamiltonian problem?

One of the main challenges in studying the electron-phonon interaction Hamiltonian problem is the complexity of the mathematical models involved. These models require advanced mathematical techniques and computational resources, making it a challenging problem to solve. Additionally, the electron-phonon interaction can also be affected by various factors, such as temperature and impurities, which can make the problem more complicated.

5. What are the potential applications of understanding electron-phonon interactions?

Understanding electron-phonon interactions can have various practical applications, such as in the development of new materials with enhanced properties. It can also help in designing more efficient electronic devices, such as transistors and solar cells. Furthermore, a better understanding of these interactions can also lead to advancements in fields like nanotechnology, quantum computing, and renewable energy.

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