- #1
Philipsmett
- 78
- 4
What does it mean that an electron in a material can split into a spinon or an orbiton? Does QFT have a spinon or orbiton field?
Philipsmett said:Does QFT have a spinon or orbiton field?
But how do electrons repel each other if they are divided into quasi-particles and only the holon repels because it carries a charge?king vitamin said:It's not correct to think of the microscopic electrons literally splitting when you have fractionalized quantum numbers in a material. The resulting excitations (call them spinons and orbitons if you like) are really many-body composites of the degrees of freedom in the system. The electrons in a system form some sort of strongly-interacting "liquid" in the ground state, and the exact excitations above this very nontrivial state can contain delocalized quasiparticles which separately carry fractions of the electron charge/spin/etc. I think of the total charge/spin being shared among all of the electrons, so that locally fractions can be made, but this is pretty heuristic.
But you must create enough quasiparticles that their total charges add up to the electron charge. For example, in the ##\nu = 1/3## fractional quantum Hall effect, you must create multiples of three quasiparticles at once, since each quasiparticle carries a third of the electron charge.
It can, in the sense that you can consider an effective QFT at low energies, and in the QFT the "fundamental" fields are the spinon/orbiton fields. Note that when you have fractionalization, you necessarily have some dynamic gauge fields at low-energy too (which are usually emergent from the original microscopic Hamiltonian you started with). In certain cases and approximations you can actually derive the low-energy QFT from the microscopic model of electrons, and see these fields emerge.
Now I realized. thanksking vitamin said:Once again, you should not view the orbitons/halons as split up versions of the original electrons. They are extremely complicated superpositions of a large number of the original electrons.
As an example, let's look at the ##\nu = 1/3## fractional quantum Hall effect (FQHE) again. I claimed that the quasiparticles carry a third of an electron charge. What does the wave function of this quasiparticle look like in terms of the original electrons? For realistic materials, there is no exact solution, but the "Laughlin wavefunctions" are known to provide very accurate approximations to the actual ones (and they are exact if one considers simplified models of electron-electron interactions). Up to a normalization constant, the Laughlin wave function describing the ground state of the ##\nu = 1/3## FQHE is
$$
\psi_0(z_1,z_2,...,z_N) = \prod_{j<k}^N (z_j - z_k)^3 \exp\left( - \frac{1}{4 l_B^2} \sum_{m=1}^N |z_m|^2 \right)
$$
Here, ##z_m = x_m + i y_m## is the position of the ##m##th electron, where we write the positions as complex numbers for convenience, and we have a total of ##N## electrons. We also have a length scale ##l_B## (related to the applied magnetic field for the FQHE, ##l_B = \sqrt{\hbar c/eB}##).
Now, what does the fundamental excitation (the "Laughlin quasihole"), which has charge ##+e/3##, look like? A single excitation at position ##z_0## has wave function
$$
\psi_{\mathrm{qh}} = \left[\prod_{j=1}^N (z_j - z_0) \right] \psi_0(z_1,z_2,...,z_N)
$$
As you can see, although this describes a localized excitation above the ground state, it is described by an enormously complicated function of all of the electrons in the system. Even in describing its difference from the ground state wave function ##\psi_0##, it involves a product over all of the electron positions. It is certainly not some sort of "fraction" of the original electrons!
I apologize.king vitamin said:It's not correct to think of the microscopic electrons literally splitting when you have fractionalized quantum numbers in a material. The resulting excitations (call them spinons and orbitons if you like) are really many-body composites of the degrees of freedom in the system. The electrons in a system form some sort of strongly-interacting "liquid" in the ground state, and the exact excitations above this very nontrivial state can contain delocalized quasiparticles which separately carry fractions of the electron charge/spin/etc. I think of the total charge/spin being shared among all of the electrons, so that locally fractions can be made, but this is pretty heuristic.
But you must create enough quasiparticles that their total charges add up to the electron charge. For example, in the ##\nu = 1/3## fractional quantum Hall effect, you must create multiples of three quasiparticles at once, since each quasiparticle carries a third of the electron charge.
It can, in the sense that you can consider an effective QFT at low energies, and in the QFT the "fundamental" fields are the spinon/orbiton fields. Note that when you have fractionalization, you necessarily have some dynamic gauge fields at low-energy too (which are usually emergent from the original microscopic Hamiltonian you started with). In certain cases and approximations you can actually derive the low-energy QFT from the microscopic model of electrons, and see these fields emerge.
Philipsmett said:charge fractionation means that the electron must be divided for example into three parts
This is the best explanation! Thanksking vitamin said:Electrons do not split. This has already been explained to you, and it is getting frustrating for you to repeat this incorrect statement repeatedly in spite of our earnestly trying to help you.
The quasiparticles in a material are collective excitations of a large number of (non-"split") electrons. Whenever you have many particles interacting, like electrons in a material, your low-energy states are better described by quasiparticles rather than electrons. These quasiparticles may have fractions of the quantum numbers held by an individual electron, or more commonly they have the same charge and spin but have some different effective mass.
QFT stands for Quantum Field Theory, which is a theoretical framework used to describe the behavior of subatomic particles and their interactions.
Spinons and orbitons are theoretical particles that arise in QFT when studying the behavior of electrons in materials. Spinons are particles associated with the spin of electrons, while orbitons are particles associated with the orbital motion of electrons.
In QFT, electron splitting is explored by studying the behavior of spinons and orbitons in materials. This involves using mathematical equations and models to understand how these particles interact with each other and with other particles in the material.
Exploring electron splitting in materials can provide valuable insights into the properties and behavior of materials at a subatomic level. This can help scientists understand and potentially manipulate the electronic properties of materials, which can have practical applications in fields such as electronics and materials science.
The research on spinons and orbitons has the potential to contribute to the development of new materials with unique electronic properties, as well as advancements in technologies such as quantum computing and spintronics. It can also deepen our understanding of fundamental physics principles and potentially lead to new discoveries and theories.