Rectified voltage induced by a microwave field in a confined two-dimensional electron gas with a mesoscopic static vortex

PMC Physics B20081:14

DOI: 10.1186/1754-0429-1-14

Received: 13 November 2007

Accepted: 21 October 2008

Published: 21 October 2008

Abstract

We investigate the effect of a microwave field on a confined two dimensional electron gas which contains an insulating region comparable to the Fermi wavelength. The insulating region causes the electron wave function to vanish in that region. We describe the insulating region as a static vortex. The vortex carries a flux which is determined by vanishing of the charge density of the electronic fluid due to the insulating region. The sign of the vorticity for a hole is opposite to the vorticity for adding additional electrons. The vorticity gives rise to non-commuting kinetic momenta. The two dimensional electron gas is described as fluid with a density which obeys the Fermi-Dirac statistics. The presence of the confinement potential gives rise to vanishing kinetic momenta in the vicinity of the classical turning points. As a result, the Cartesian coordinate do not commute and gives rise to a Hall current which in the presence of a modified Fermi-Surface caused by the microwave field results in a rectified voltage. Using a Bosonized formulation of the two dimensional gas in the presence of insulating regions allows us to compute the rectified current. The proposed theory may explain the experimental results recently reported by J. Zhang et al.

PACS numbers: 71.10.PM

I. Introduction

The topology of the ground state wave function plays a crucial role in determining the physical properties of a many-particle system. These properties are revealed through the quantization rules. It is known that Fermions and Bosons obey different quantization rules, while the quantized Hall conductance [1] and the value of the spin-Hall conductivity are a result of non-commuting Cartesian coordinates [2]. Similarly the phenomena of quantum pumping observed in one-dimensional electronic systems [35] is a result of a space-time cycle and can be expressed in the language of non-commuting frequency ω = i t and coordinate x = i k as shown in ref[6].

Recently, the phenomena of rectification current I r (V) = [I(V) + I(-V)]/2 has been proposed as a DC response to a low-frequency AC square voltage resulted from a strong 2k F scattering in a one dimensional Luttinger liquid [7].

In a recent experiment [8], a two-dimensional electron gas (2DEG) GaAs with three insulating antidots has been considered. A microwave field has been applied, and a DC voltage has been measured. The experiment has been performed with and without a magnetic field. The major result which occurs in the absence of the magnetic field is a change in sign of the rectified voltage when the microwave frequency varies from 1.46 GHz to 17.41 GHz. This behavior can be understood as being caused by the antidots, which create obstacles for the electrons.

We report in this letter a proposal for rectification. In section II we present a theory which show that rectification can be viewed as a result of non-commuting coordinates. In section III we present a qualitative model for rectification, namely the presence of vanishing wave function is described by a vortex which induces non-commuting kinetic momenta. The sign the vorticity is determined by the vanishing of the electronic density. The electronic fluid can be seen as a hard core boson which carry flux, the removal of charge caused by the insulating region is equivalent to a decrease of flux with respect the flux of the uniform fluid. Including in addition a confining potential we obtain regions where the momentum vanishes. The combined effect non-commuting kinetic momenta and confinement gives rise to non-commuting cartesian coordinates. In section IV we use the Bosonization method to construct a quantitative theory which gives rise to a set of equations of motion. Constructing an iterative solution of this equations reveals the phenomena of rectifications explained in sections II and III.

II. Rectifications due to non-commuting coordinates

Due to the existence of the obstacles, the wave function of the electron vanishes in the domain of the obstacles. This will give rise to a change in the wave function, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq89_HTML.gif where http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq90_HTML.gif is the unitary transformation (induced by the obstacle) and the coordinate coordinate representation becomes, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq2_HTML.gif [1, 2, 9]. An interesting situation occurs when the wave function |Φ > has zero's [1, 2, 9] or points of degeneracy [10] in the momentum space. This gives rise to non -commuting coordinates [1, 2, 11]. As a result we will have a situation where the the commutator [r 1, r 2] of the coordinates is non zero.
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ1_HTML.gif
(1)
Using the one particle hamiltonian http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq3_HTML.gif in the presence of an external electric field with the commutators http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq4_HTML.gif one obtains [2] the Heisenberg equations of motions,
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ2_HTML.gif
(2)
This equations are identical with the one obtained in ref.[11] where http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq5_HTML.gif is the single particle energy being in the semi-classical approximation and E 2(t) the external electric field. As a result of the external electric field E 2(t) changes the velocity changes according to eq.2. Using the interaction picture we find,
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ3_HTML.gif
(3)
V 2(t) is the voltage caused by the external field E 2(t). The Fermi Dirac occupation function http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq6_HTML.gif in the presence of the electric field is used to sum over all the single particle states. We obtain the current density J 1(r) in the i = 1,
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ4_HTML.gif
(4)
The result obtained in the last equation follows directly from the non-commuting coordinates given by http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq91_HTML.gif . The current in eq. 1 depends on http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq6_HTML.gif , the Fermi- Dirac occupation function in the presence of the external voltage V 2(t) ≃ E 2(t)L. We expand the non equilibrium density http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq7_HTML.gif to first order in V 2(t) we obtain the final form of the rectified current. http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq92_HTML.gif has dimensions of a frequency and can be replaced with the help of the Larmor's theorem, by an effective magnetic field http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq8_HTML.gif . This allows us to replace eq. 4 by the formula.
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equa_HTML.gif

III. A model for non-commuting coordinates

We consider a two dimensional electron gas (2DEG) in the presence of a parabolic confining potential http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq93_HTML.gif . The 2DEG contains an insulting region of radius D caused by an infinite potential U I (r) (in the experiment the insulating region this is caused by three antidots) see figure 1a. The effect of the insulating region of radius D causes the electronic wave function http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq10_HTML.gif to vanish for http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq97_HTML.gif . The spin of the electrons seems not to play any significant role, therefore we approximate the 2DEG by a spinless charge system. Such a charged electronic system is equivalent to a hard core charged Boson. For Bosonic wave function has zero's which can be described as a vortex centered at http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq12_HTML.gif .
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Fig1_HTML.jpg
Figure 1

(a)A confined 2DEG of size L × L with a classical turning point length L F which contains an insulating region of radius D centered at R (the location of the vanishing wave function). (b) Particles close to the classical turning point L F , represented by the shaded area which satisfy the constraint Π1 = Π2 = 0.

We will show that the following properties are essential in order to have non-commuting coordinates.
  1. (1)

    The vanishing of the wave function for http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq97_HTML.gif is described by a vortex localized at http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq13_HTML.gif .

     
  2. (2)

    The many particles will be described in term of a continuous Lagrange formulation [12] http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq14_HTML.gif . Here, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq14_HTML.gif is the continuous form of http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq15_HTML.gif , where "α" denotes the particular particle, α = 1, 2, ..., N with a density function http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq94_HTML.gif , which satisfies http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq100_HTML.gif in two dimensions (L 2 is the two dimensional area). The coordinate http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq17_HTML.gif and the momentum http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq18_HTML.gif obey canonical commutation rules, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq19_HTML.gif .

     
  3. (3)

    The parabolic confining parabolic potential http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq20_HTML.gif provides the confining length L F , see figures 1a and 1b.

     

Using the conditions (1)–(3), we will show that the non-commuting coordinates emerge.

A. The vanishing of the wave function

In the literature it was established that the vanishing of the Bosonic wave function gives rise to a multivalued phase and vorticity. See in particular the derivation given in ref. [13]. The vortex (the insulating region) gives rise to non-commuting kinetic momenta, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq21_HTML.gif where, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq22_HTML.gif and the phase http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq23_HTML.gif is caused by the localized vortex [1315]. This result is obtained in the following way:

In the presence of a vortex the single particle operator is parametrize as follows: http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq24_HTML.gif for http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq98_HTML.gif , and http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq25_HTML.gif for http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq99_HTML.gif . The field http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq95_HTML.gif is a regular hard core boson field and http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq26_HTML.gif is a multivalued phase. As a result, the Hamiltonian http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq27_HTML.gif and the field http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq28_HTML.gif are replaced by the transformed Hamiltonian:
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ5_HTML.gif
(5)
The momentum http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq1_HTML.gif is replaced by the kinetic momentum, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq22_HTML.gif . The derivative of the multivalued phase http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq26_HTML.gif determines the vector potential http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq29_HTML.gif . [Π1, Π2] ≠ 0.
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ6_HTML.gif
(6)

where http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq30_HTML.gif is an effective magnetic field due to the insulation region, which is defined as http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq31_HTML.gif . The sign of the magnetic field http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq32_HTML.gif is determined by the vorticity. Following the theory presented in ref. [8] (see pages 94–99 and 222–227) http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq32_HTML.gif has positive vorticity since the electronic density vanishes for the region http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq99_HTML.gif creating a hole on background density (see figure 13.1 page 227 in ref.[8]).

For the remaining part of this paper we will replace the delta function by a step function http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq33_HTML.gif which takes the value of one for http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq98_HTML.gif and zero otherwise.

B. The many particle representation

In the presence of hard core Bosons (spinless Fermions) the momenta is replaced by http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq34_HTML.gif . The static vortex describes the insulating region and modifies the momentum operator, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq35_HTML.gif . Making use of this continuous formulation, we find a similar result as we have for the single particles [13], i.e.,
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ7_HTML.gif
(7)

where http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq104_HTML.gif for http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq105_HTML.gif and zero otherwise.

C. The confining potential

The last ingredient of our theory is provided by the confining potential and the Fermi energy. Due to the confining potential the kinetic momentum has to vanishes for particles which have the coordinate close to the classical turning point (see figure 1b) http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq96_HTML.gif . This lead to the following constraint problem for the kinetic momentum,
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ8_HTML.gif
(8)
and
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ9_HTML.gif
(9)

The kinetic momentum http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq101_HTML.gif and http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq102_HTML.gif form a second class constraints (according to Dirac's definition [9] the commutator of the constraints has to be non-zero) [Π1(| http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq16_HTML.gif | ≈ L F ), Π2(| http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq16_HTML.gif | ≈ L F )] ≠ 0 if the region http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq9_HTML.gif overlaps with the vortex region http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq97_HTML.gif . For http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq37_HTML.gif D the commutator of the kinetic momenta is given by http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq38_HTML.gif given by eq.7.

We define the matrix http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq39_HTML.gif . Using the function http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq36_HTML.gif (which replaces the delta function) and the eqs.8,9 we obtain
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ10_HTML.gif
(10)
The overlapping conditions are given by the conditions: http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq36_HTML.gif is equal to one for http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq37_HTML.gif <D and zero otherwise and http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq40_HTML.gif describes the condition of the classical turning points. Using eq.10 we find according to Dirac's second class constraints [9] the following new commutator http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq41_HTML.gif ,
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ11_HTML.gif
(11)
For http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq98_HTML.gif we define a field http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq42_HTML.gif trough the equation,
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equb_HTML.gif

This means that http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq106_HTML.gif is approximated by Ω ∝ D 2 for http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq98_HTML.gif .

Eq. 11 shows that the presence of the momentum, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq35_HTML.gif with the constraints given by eqs. 8 and 9 gives rise to non-commuting coordinates http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq43_HTML.gif .

Once we have the result that the coordinate do not commute we can use the analysis given in eq 4 (and the result for the current I 1 derived with the help of equation 4) to compute the rectified current, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq44_HTML.gif .

This result can be derived by directly using a modified Bosonization method with a non-commuting Kac-Moody algebra [10, 16].

IV. Continuous formulation for the 2deg – a bosonization approach

A. Bosonization for the 2DEG

We introduce a continuous formulation for the 2DEG many particles system. We replace the single particle Hamiltonian http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq45_HTML.gif by a many electron formulation [12]. We introduce a continuous representation, namely http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq14_HTML.gif . Here, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq14_HTML.gif is the continuous form of http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq15_HTML.gif . The coordinate and the momentum obey http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq46_HTML.gif and http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq47_HTML.gif The equilibrium Fermi-Dirac density is given by http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq48_HTML.gif

One of the useful description for many electrons in two dimensions is the Bosonization method. We will modify this method [10] in order to introduce the effect of the vortex field and the confining potential http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq49_HTML.gif .

B. The bosonization method in the absence of the insulating region and confining potential

In this section we will present the known [2, 10] results for a two dimensional interacting metal in the absence of the vortex field and confining potential http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq49_HTML.gif . Our starting point is the Bosonized form of the 2DEG given in ref. [10, 16].
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equc_HTML.gif

where http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq50_HTML.gif is the Landau function for the two body interaction [10] and the notation :: represents the normal order with respect the Fermi Surface. [10]. According to ref.[10, 16], the F.S. is described by, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq51_HTML.gif . The "normal" deformation to the F.S. is given by, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq52_HTML.gif . "s" is the polar angle on the F.S. http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq53_HTML.gif , and http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq107_HTML.gif is the normal to the F.S. The commutation relations for the F.S. are, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq55_HTML.gif

C. The modification of the bosonization method in the presence of a confining potential

Following ref. [17] (see the last term of eq.10 in ref. [17]), we incorporate into the Bosonic hamiltonian the effect of the confining and external potentials. We parametrize the Fermi surface in terms of the polar angle s = [0 - 2π] and the coordinate http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq16_HTML.gif . The Fermi surface momentum http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq56_HTML.gif given by the solution, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq57_HTML.gif . As a result the the FERMI SURFACE (F.S.) excitations is given by, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq58_HTML.gif . The "normal" deformation to the F.S. is given by, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq59_HTML.gif and http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq60_HTML.gif is the normal to the F.S. as a function of the polar angle s and real space coordinate http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq16_HTML.gif .

Following refs. [11, 17], we obtain the Bosonized hamiltonian for the many particles system in the presence of the potentials, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq49_HTML.gif and time dependent external potential http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq61_HTML.gif .
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ12_HTML.gif
(12)
The new part of in the Bosonic hamiltonian is the presence of the confining http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq62_HTML.gif and external potential http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq61_HTML.gif . http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq61_HTML.gif is the external microwave radiation field,
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equd_HTML.gif
The commutation relations for the FERMI SURFACE in are given by the Kack Moody commutation relation [11, 17]
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ13_HTML.gif
(13)

D. The bosonization method in the presence of the insulating region and confining potential

This problem can be investigated using the hamiltonian given in eq.12 supplemented by the constraints conditions imposed by the vanishing density. described by a vortex. Using the results given in eq.11 one modifies the commutation relations. This modification can be viewed as Dirac's bracket due to second class constraints [9]. The commutator [,] is replaced by Dirac 's commutators http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq41_HTML.gif . The region of vanishing density is described by the function http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq63_HTML.gif for http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq37_HTML.gif <D and zero otherwise. Using http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq64_HTML.gif we find that the Dirac commutator http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq65_HTML.gif replaces the commutator given in equation 13
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ14_HTML.gif
(14)

The result given by eq. 14 due to non-commuting coordinates http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq64_HTML.gif . We will compare this result with the one for a magnetic field B, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq66_HTML.gif given in ref. [17]. The commutator for the two dimensional densities in the presence of a magnetic field http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq103_HTML.gif perpendicular to the 2DEG has been obtained in ref. [10].

The modified commutator caused by the magnetic field (see eq. 27 in ref. [10]) is:
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ15_HTML.gif
(15)

Where http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq103_HTML.gif is the magnetic field and http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq67_HTML.gif is the derivative in the tangential direction perpendicular to the vector http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq107_HTML.gif (the normal to the Fermi surface), http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq68_HTML.gif .

Using the analogy between the vortex field an the external magnetic field (eq. 15) we can represent equation 14 in terms of the parameters given in eq. 11.
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ16_HTML.gif
(16)

where http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq67_HTML.gif is the derivative according to the tangential direction which is perpendicular to the vector http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq107_HTML.gif with, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq68_HTML.gif .

The commutator given in equation 16 allows to investigate the physics given in the hamiltonian 12. Using this formulation we will compute the rectified current.

We observe that the Dirac commutator, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq65_HTML.gif ≠ 0 is non-zero for ss'! The Heisenberg equation of motion will be given by the Dirac bracket. Due to the fact that different channels ss' do not commute, the application of an external electric field in the http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq69_HTML.gif direction will generate a deformation for the F.S. with http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq54_HTML.gif , http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq70_HTML.gif .

Using this commutation relations given in equation 16 and the hamiltonian given in equation 12, we obtain the equation of motion,
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ17_HTML.gif
(17)

We have included in the equation of motion a phenomenological relaxation time τ for the kinetic momentum. This equation shows that the direct effect caused by the electric field is proportional to sin(s) with the maximum contribution at the polar angles, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq71_HTML.gif and http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq72_HTML.gif where V F (s, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq16_HTML.gif ) is the Fermi velocity. The effect of the vortex is to generates a change in the kinetic momentum perpendicular to the external electric field. This part is given by the last term. The last term is restricted to http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq105_HTML.gif and represents the vortex contribution. This term is maximum for the polar angles s = 0 and s = π. The maximum effect will be obtained in the region close to the classical turning point where the Fermi velocity obeys, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq73_HTML.gif .

The current density in the i = 1 direction is given by the polar integration of s, [0 - 2π].
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Equ18_HTML.gif
(18)

We introduce the dimensionless parameter http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq74_HTML.gif which is a function of http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq75_HTML.gif and D the radius of the insulating region. For values of γ < 1 we can solve iteratively the equation of motion and compute the current.

In the equation for the kinetic momentum we have included a phenomenological relaxation time τ. This relaxation time will allow to perform times averages. We only keep single harmonics and neglect higher harmonics of the microwave field.

The iterative solution is given as a series in γ and the microwave amplitude E c i.e. http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq76_HTML.gif .

Solving the equation of motion we determines the evolution of the Fermi surface deformation in the presence of the microwave field. We substitute the iterative solution http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq77_HTML.gif obtained from eq. 17 into the current density formula given by eq. 18.

V. Application of the theory to the experiment

In order to provide a physical interpretation of our theory we will use physical parameters determined by the experiment. In the experiment the electronic density is n ≃ 1015 m -2 this corresponds to a Fermi energy of E F ≃ 0.01eV, equivalent to a temperature of T F ≃ 120K and a Fermi wavelength of λ F ≃ 0.5 × 10-7 m. For high mobility GaAs, the typical scattering time is τ ≃ 10-11 sec, which corresponds to the mean free path l = ν F τ. The ratio between the mean free path and the Fermi wave length obeys the condition, http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq78_HTML.gif . Therefore, we can neglect multiple scattering effects. When the thermal length is comparable with the size of the system http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq79_HTML.gif , one obtains a ballistic system with negligible multiple scattering.

We describe the confined 2DEG of size L as a system with a parabolic confining potential http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq80_HTML.gif which has a "classical turning point" L F determined by the condition http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq81_HTML.gif . This condition describes the effective physics of a free electron gas of size L = L F . Demanding that L F is of the order of the thermal wave length L F λ thermal determines the confining frequency http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq82_HTML.gif . For this condition, we obtain a ballistic regime where L <L F ~ 10-7 – 10-6 m, T ~ 1 – 10K, ω 0 ≃ 1010 – 1011 Hz and τ ≃ 10-11 sec. In order to be able to observe quantum scattering effects caused by the insulating region of radius "D", we require that the wavelength λ F obeys the condition D > λ F ≃ 0.5 × 10-7 m.

To leading order in γ < 1 and in second order in the microwave amplitude E c we compute the rectified D.C. voltage V 1,D.C . in the i = 1 direction. This rectified voltage is defined as V 1, D.C.= I 1/σ (σ is conductance in the semi classical approximation determined by the transport time which is proportional to the scattering time). The current I 1 given by http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq83_HTML.gif with LL F . The microwave field is expressed in terms of an R.M.S. (effective) voltage http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq84_HTML.gif which allows to define a dimensionless voltage in the i = 1 direction http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq85_HTML.gif , where http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq86_HTML.gif with the function G(φ) given in figure 2.
http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_Fig2_HTML.jpg
Figure 2

The dimensionless voltage G(ϕ, α), as a function of x = ω/ω 0 with the parameters α = II, tan(ϕ) = ω/τ/(ω2 - http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq87_HTML.gif ), γ = 0.7. The solid line represents the theory and the crosses "x" represent the experiment in ref. [8].

For 2DEG, we use typical parameters used in the experiment [8], i.e. electronic density n ≈ 1015 m -2 with a Fermi energy E F ≈ 0.01ev, ω 0 ≈ 1010 – 1011 Hz, momentum relaxation time τ ≈ 10-11 sec. and radius of the insulating region D > λ F ≈ 0.5 × 10-7 m, with γ ≈ 0.7. We make a single harmonic approximations (neglect terms which oscillate with frequencies 2ω 0, 3ω 0 ...) We have used figure 3 in ref. [8] to extract the voltage changes as a function of the microwave field for a zero magnetic field. Figure 3 in ref. [8] shows clearly a change of sign when the microwave varies between 1.46 GHz to 34 GHz and vanishes at 17.41 GHz. In figure 2, we have plotted our results given by the formula G(φ) as a function of the microwave frequency with the rescaled experimental points (see the three points on our theory graph). As shown we find a good agreement of our theory with the experimental results once we choose ω 0 = 17.41 GHz. For frequencies which obeys http://static-content.springer.com/image/art%3A10.1186%2F1754-0429-1-14/MediaObjects/13067_2007_Article_14_IEq88_HTML.gif , we find good agreement with the experimental results. However, for low frequencies, our theory is inadequate and does not fit the experiment.

VI. Conclusion

In conclusion, we can say that the origin of the rectification is the emergence of the non-commuting Cartesian coordinates and the non-commuting density excitations are a result of the vortex field accompanied the classical turning caused by the confining potential. Using the modified KacK Moody commutations rule for the density excitations we find that excitations with different polar angles s become coupled.

Using this theory we have explained the results of the experiment [8] in a region where the magnetic field was zero.

Declarations

VII. Acknowledgements

The authors acknowledge discussion with Dr. J Zhang about the experiment results in the reference [8]. The authors acknowledge the finance support from CUNY FRAP program.

Authors’ Affiliations

(1)
Department of Physics, City College of the City University of New York

References

  1. Kohmoto : Annals of Physics. 1985, 160:343.View ArticleMathSciNetADS
  2. Schmeltzer D: Phys Rev B. 2006, 73:1655301.View Article
  3. Schmeltzer D: Phys Rev Lett. 2000, 85:4132.View ArticleADS
  4. Brouwer PW: Phys Rev B. 1998, 58:R10135.View ArticleADS
  5. Feldman DE, Scheidl S, Vinokur VM: Phys Rev Lett. 2005, 94:186809.View ArticleADS
  6. Thouless DJ: Phys Rev B. 1983, 27:6083.View ArticleMathSciNetADS
  7. Braunecker B, Feldman DE, Marston JB: Phys Rev B. 2005, 72:125311.View ArticleADS
  8. Zhang J, Vitkalov S, Kvon ZD, Portal JC, Wieck A: Phys rev Lett. 2006, 97:226807.View ArticleADS
  9. Dirac PAM: "Lectures on Quantum Mechanics". Dover Publications Inc; 2001.
  10. Haldane FDM: Cond-Mat 050529v1.
  11. Haldane FDM: Phys Rev Lett. 2004, 93:206602.View ArticleADS
  12. Yourgrau W, Mandelstam S: "Variational principles in dynamics and quantum mechanics". Dover Publications Inc; 1979:142–147.
  13. Kuratsuji H: Phys Rev Lett. 1992, 68:1746.MATHView ArticleMathSciNetADS
  14. Ezawa ZyunF: "Quantum Hall Effect". World Scientific; 2000:94–99.
  15. Nelson David: "Defects and Geometry in Condensed Matter Physics". Cambridge University Press; 2002.
  16. Schmeltzer D: Phys Rev B. 1996, 10269.
  17. Polchinsky J: Nuclear Physics B. 1991, 362:125–140.View ArticleMathSciNetADS

Copyright

© Schmeltzer and Chang 2008

This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://​creativecommons.​org/​licenses/​by/​2.​0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.