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A composite fermion is the topological bound state of an electron and an even number of quantized
vortices In fluid dynamics, a vortex ( : vortices or vortexes) is a region in a fluid in which the flow revolves around an axis line, which may be straight or curved. Vortices form in stirred fluids, and may be observed in smoke rings, whirlpools in th ...
, sometimes visually pictured as the bound state of an electron and, attached, an even number of magnetic flux quanta. Composite fermions were originally envisioned in the context of the
fractional quantum Hall effect The fractional quantum Hall effect (FQHE) is a physical phenomenon in which the Hall conductance of 2-dimensional (2D) electrons shows precisely quantized plateaus at fractional values of e^2/h. It is a property of a collective state in which elec ...
, but subsequently took on a life of their own, exhibiting many other consequences and phenomena. Vortices are an example of
topological defect A topological soliton occurs when two adjoining structures or spaces are in some way "out of phase" with each other in ways that make a seamless transition between them impossible. One of the simplest and most commonplace examples of a topological ...
, and also occur in other situations. Quantized vortices are found in type II superconductors, called
Abrikosov vortices In superconductivity, fluxon (also called a Abrikosov vortex and quantum vortex) is a vortex of supercurrent in a type-II superconductor, used by Alexei Abrikosov to explain magnetic behavior of type-II superconductors. Abrikosov vortices occu ...
. Classical vortices are relevant to the Berezenskii–Kosterlitz–Thouless transition in two-dimensional
XY model The classical XY model (sometimes also called classical rotor (rotator) model or O(2) model) is a lattice model of statistical mechanics. In general, the XY model can be seen as a specialization of Stanley's ''n''-vector model for . Definition G ...
.


Description

When electrons are confined to two dimensions, cooled to very low temperatures, and subjected to a strong magnetic field, their kinetic energy is quenched due to Landau level quantization. Their behavior under such conditions is governed by the
Coulomb repulsion Coulomb's inverse-square law, or simply Coulomb's law, is an experimental law of physics that quantifies the amount of force between two stationary, electrically charged particles. The electric force between charged bodies at rest is conventiona ...
alone, and they produce a strongly correlated quantum liquid. Experiments have shown that electrons minimize their interaction by capturing quantized vortices to become composite fermions. The interaction between composite fermions themselves is often negligible to a good approximation, which makes them the physical
quasiparticle In physics, quasiparticles and collective excitations are closely related emergent phenomena arising when a microscopically complicated system such as a solid behaves as if it contained different weakly interacting particles in vacuum. For exam ...
s of this quantum liquid. The signature quality of composite fermions, which is responsible for the otherwise unexpected behavior of this system, is that they experience a much smaller magnetic field than electrons. The magnetic field seen by composite fermions is given by : B^*=B-2p \rho \phi_0, where B is the external magnetic field, 2p is the number of vortices bound to composite fermion (also called the vorticity or the vortex charge of the composite fermion), \rho is the particle density in two dimensions, and \phi_0=hc/e is called the "flux quantum" (which differs from the superconducting flux quantum by a factor of two). The effective magnetic field is a direct manifestation of the existence of composite fermions, and also embodies a fundamental distinction between electrons and composite fermions. Sometimes it is said that electrons "swallow" 2p flux quanta each to transform into composite fermions, and the composite fermions then experience the residual magnetic field B^*. More accurately, the vortices bound to electrons produce their own
geometric phase In classical and quantum mechanics, geometric phase is a phase difference acquired over the course of a cycle, when a system is subjected to cyclic adiabatic processes, which results from the geometrical properties of the parameter space of the Ha ...
s which partly cancel the Aharonov–Bohm phase due to the external magnetic field to generate a net geometric phase that can be modeled as an Aharonov–Bohm phase in an effective magnetic field B^*. The behavior of composite fermions is similar to that of electrons in an effective magnetic field B^*. Electrons form Landau levels in a magnetic field, and the number of filled Landau levels is called the filling factor, given by the expression \nu=\rho \phi_0/B. Composite fermions form Landau-like levels in the effective magnetic field B^*, which are called composite fermion Landau levels or \Lambda levels. One defines the filling factor for composite fermions as \nu^*=\rho \phi_0/, B^*, . This gives the following relation between the electron and composite fermion filling factors : \nu=\frac. The minus sign occurs when the effective magnetic field is antiparallel to the applied magnetic field, which happens when the geometric phase from the vortices overcompensate the Aharonov–Bohm phase.


Experimental manifestations

The central statement of composite fermion theory is that the strongly correlated electrons at a magnetic field B (or filling factor \nu) turn into weakly interacting composite fermions at a magnetic field B^* (or composite fermion filling factor \nu^*). This allows an effectively single-particle explanation of the otherwise complex many-body behavior, with the interaction between electrons manifesting as an effective kinetic energy of composite fermions. Here are some of the phenomena arising from composite fermions:


Fermi sea

The effective magnetic field for composite fermions vanishes for B=2p\rho\phi_0, where the filling factor for electrons is \nu=1/2p. Here, composite fermions make a Fermi sea. This Fermi sea has been observed at half filled Landau level in a number of experiments, which also measure the Fermi wave vector.


Cyclotron orbits

As the magnetic field is moved slightly away from B^*=0, composite fermions execute semiclassical cyclotron orbits. These have been observed by coupling to surface acoustic waves, resonance peaks in antidot superlattice, and magnetic focusing. The radius of the cyclotron orbits is consistent with the effective magnetic field B^*=0 and is sometimes an order of magnitude or more larger than the radius of the cyclotron orbit of an electron at the externally applied magnetic field B. Also, the observed direction of trajectory is opposite to that of electrons when B^* is anti-parallel to B.


Cyclotron resonance

In addition to the cyclotron orbits, cyclotron resonance of composite fermions has also been observed by photoluminescence.


Shubnikov de Haas oscillations

As the magnetic field is moved further away from B^*=0,
quantum oscillations In condensed matter physics, quantum oscillations describes a series of related experimental techniques used to map the Fermi surface of a metal in the presence of a strong magnetic field. These techniques are based on the principle of Landau qua ...
are observed that are periodic in 1/B^*. These are Shubnikov–de Haas oscillations of composite fermions. These oscillations arise from the quantization of the semiclassical cyclotron orbits of composite fermions into composite fermion Landau levels. From the analysis of the Shubnikov–de Haas experiments, one can deduce the effective mass and the quantum lifetime of composite fermions.


Integer quantum Hall effect

With further increase in , B^*, or decrease in temperature and disorder, composite fermions exhibit integer quantum Hall effect. The integer fillings of composite fermions, \nu^*=n, correspond to the electrons fillings : \nu=\frac. Combined with : \nu=1-\frac, which are obtained by attaching vortices to holes in the lowest Landau level, these constitute the prominently observed sequences of fractions. Examples are :=,\, ,\, ,\, ,\,,\cdots :=,\, ,\, ,\, ,\,,\cdots :=,\, ,\, ,\, ,\cdots The
fractional quantum Hall effect The fractional quantum Hall effect (FQHE) is a physical phenomenon in which the Hall conductance of 2-dimensional (2D) electrons shows precisely quantized plateaus at fractional values of e^2/h. It is a property of a collective state in which elec ...
of electrons is thus explained as the integer quantum Hall effect of composite fermions. It results in fractionally quantized Hall plateaus at : R_H=, with \nu given by above quantized values. These sequences terminate at the composite fermion Fermi sea. Note that the fractions have odd denominators, which follows from the even vorticity of composite fermions.


Fractional quantum Hall effect

The above sequences account for most, but not all, observed fractions. Other fractions have been observed, which arise from a weak residual interaction between composite fermions, and are thus more delicate. A number of these are understood as fractional quantum Hall effect of composite fermions. For example, the fractional quantum Hall effect of composite fermions at \nu^*=4/3 produces the fraction 4/11, which does not belong to the primary sequences.


Superconductivity

An even denominator fraction, \nu=5/2, has been observed. Here the second Landau level is half full, but the state cannot be a Fermi sea of composite fermions, because the Fermi sea is gapless and does not show quantum Hall effect. This state is viewed as a "superconductor" of composite fermion, arising from a weak attractive interaction between composite fermions at this filling factor. The pairing of composite fermions opens a gap and produces a fractional quantum Hall effect.


Excitons

The neutral excitations of various fractional quantum Hall states are
exciton An exciton is a bound state of an electron and an electron hole which are attracted to each other by the electrostatic Coulomb force. It is an electrically neutral quasiparticle that exists in insulators, semiconductors and some liquids. The ...
s of composite fermions, that is, particle hole pairs of composite fermions. The energy dispersion of these excitons has been measured by light scattering and phonon scattering.


Spin

At high magnetic fields the spin of composite fermions is frozen, but it is observable at relatively low magnetic fields. The fan diagram of the composite fermion Landau levels has been determined by transport, and shows both spin-up and spin-down composite fermion Landau levels. The fractional quantum Hall states as well as composite fermion Fermi sea are also partially spin polarized for relatively low magnetic fields.


Effective magnetic field

The effective magnetic field of composite fermions has been confirmed by the similarity of the fractional and the integer quantum Hall effects, observation of Fermi sea at half filled Landau level, and measurements of the cyclotron radius.


Mass

The mass of composite fermions has been determined from the measurements of: the effective cyclotron energy of composite fermions; the temperature dependence of Shubnikov–de Haas oscillations; energy of the cyclotron resonance; spin polarization of the Fermi sea; and quantum phase transitions between states with different spin polarizations. Its typical value in GaAs systems is on the order of the electron mass in vacuum. (It is unrelated to the electron band mass in GaAs, which is 0.07 of the electron mass in vacuum.)


Theoretical formulations

Much of the experimental phenomenology can be understood from the qualitative picture of composite fermions in an effective magnetic field. In addition, composite fermions also lead to a detailed and accurate microscopic theory of this quantum liquid. Two approaches have proved useful.


Trial wave functions

The following trial wave functions embody the composite fermion physics: \Psi^_=P\;\; \Psi^_ \prod_(z_j-z_k)^ Here \Psi^_ is the wave function of interacting electrons at filling factor \nu; \Psi^_ is the wave function for weakly interacting electrons at \nu^*; N is the number of electrons or composite fermions; z_j=x_j+iy_j is the coordinate of the jth particle; and P is an operator that projects the wave function into the lowest Landau level. This provides an explicit mapping between the integer and the fractional quantum Hall effects. Multiplication by \prod_^N(z_j-z_k)^ attaches 2p vortices to each electron to convert it into a composite fermion. The right hand side is thus interpreted as describing composite fermions at filling factor \nu^*. The above mapping gives wave functions for both the ground and excited states of the fractional quantum Hall states in terms of the corresponding known wave functions for the integral quantum Hall states. The latter do not contain any adjustable parameters for \nu^*=n, so the FQHE wave functions do not contain any adjustable parameters at \nu=n/(2pn\pm 1) . Comparisons with exact results show that these wave functions are quantitatively accurate. They can be used to compute a number of measurable quantities, such as the excitation gaps and exciton dispersions, the phase diagram of composite fermions with spin, the composite fermion mass, etc. For \nu^*=1 they reduce to the
Laughlin wavefunction In condensed matter physics, the Laughlin wavefunction pp. 210-213 is an ansatz, proposed by Robert Laughlin for the ground state of a two-dimensional electron gas placed in a uniform background magnetic field in the presence of a uniform jellium ...
at fillings \nu=1/(2p+1).


Chern–Simons field theory

Another formulation of the composite fermion physics is through a Chern–Simons field theory, wherein flux quanta are attached to electrons by a singular gauge transformation. At the mean field approximation the physics of free fermions in an effective field is recovered. Perturbation theory at the level of the random phase approximation captures many of the properties of composite fermions.


See also

*
Composite boson A composite boson is a bound state of fermions such that the combination gives a boson.Monique Combescot and Shiue-Yuan Shiau, "Excitons and Cooper Pairs: Two Composite Bosons in Many-Body Physics", Oxford University Press (). Examples include Coop ...
* Integer quantum Hall effect *
Fractional quantum Hall effect The fractional quantum Hall effect (FQHE) is a physical phenomenon in which the Hall conductance of 2-dimensional (2D) electrons shows precisely quantized plateaus at fractional values of e^2/h. It is a property of a collective state in which elec ...


References

{{Reflist


External links


Nobel Lecture: "The fractional quantum Hall effect"
by H. L. Stormer * "Composite Fermions: New particles in the fractional quantum Hall effect", by H. Störmer and D. Tsui, ''Physics News'' in 1994, American Institute of Physics, 1995, p. 33.
Composite Fermion
at the
Pennsylvania State University The Pennsylvania State University (Penn State or PSU) is a Public university, public Commonwealth System of Higher Education, state-related Land-grant university, land-grant research university with campuses and facilities throughout Pennsylvan ...

Composite Fermions - von Klitzing's department
at the
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"Composite fermions are real"
at the Physics News Update,
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"Half filled Landau level yields intriguing data and theory"
in ''
Physics Today ''Physics Today'' is the membership magazine of the American Institute of Physics. First published in May 1948, it is issued on a monthly schedule, and is provided to the members of ten physics societies, including the American Physical Society. I ...
''
"The composite fermion: A quantum particle and its quantum fluids"
in ''
Physics Today ''Physics Today'' is the membership magazine of the American Institute of Physics. First published in May 1948, it is issued on a monthly schedule, and is provided to the members of ten physics societies, including the American Physical Society. I ...
'' Hall effect Quasiparticles Quantum phases