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Transcript
Part I, Section 2, Chapter 3. Quantum Circuit Theory
Chapter 3.
Quantum Circuit Theory for Mesoscoptic Devices
Academic and Research Staff
Professor Xiao-Gang Wen
Graduate Students
Sven Heemeyer
3.1 Goals and Objectives
Sponsor
U.S. Army Research Office
Contract DAAG55-98-1-0080
Project Staff
Professor Xiao-Gang Wen, Sven Heemeyer
The goal of this research is to create realistic theoretical models for electronic circuits (or components of a
circuit) at scales so small that quantum effects are
important. More generally, the goal is to understand
the fundamental behavior of systems at the border of
the classical and quantum regimes. We propose to
create theoretical models of quantum dots and quantum wires, for these are the fundamental building
blocks of quantum electronic circuits. We will use
these models to study the nonlinear quantum dynamics of coupled dots and wires. We believe that these
theoretical models will allow us to design quantum
electronic circuits with prescribed properties. Beyond
this, we hope to discover phenomena not present in
classical electronic circuits, and to find applications
for them in new generations of nano-electronic
devices.
3.2 Dynamics of Quantum Dots Coupled
to Environment
The first step in achieving our goal is to find the fundamental theory that describes the systems between
the classical and quantum world, that is to find the
equation of motion that governs the behaviors of
those systems. We use equation of motion for the
density matrix to formulate the fundamental theory.The density matrix can describe both pure coherent quantum states and incoherent classical states.
Thus it can reach both the classical and the quantum
worlds. For an isolated system such as an isolated
quantum dot, the density-matrix equation is linear as
expected for a pure quantum system. However, for a
dot that couples to the outside world, the dot influences its own environment, and the change in its
environment in turn affects the dot. We include this
feedback effect to the equation of motion for the density matrix, using techniques developed in the theory
of many-body physics. This approach allows us to
incorporate both quantum phase coherent effects of
the dots and the dissipative/nonlinear effects of the
environment.
In the on-going study, graduate student Sven Heemeyer and I derived the equation of motion for the density matrix with the feedback effects mentioned
above using a perturbation theory. We found that the
density-matrix equation is indeed nonlinear, even in
the leading order perturbative calculation. More nonlinear terms may appear in higher order perturbative
expansions.
A preliminary study demonstrates that the coupling to
the environment can generate large off-diagonal elements in the density matrix. Since classical systems
are always described by diagonal density matrices,
the appearance of the off-diagonal elements indicate
the importance of the quantum effects. The values of
those off-diagonal matrix elements depend on various parameters, such as the bias/gate voltage. As a
consequence of the large off-diagonal elements, the
impedance of a dot has sharp peaks at frequencies
corresponding to the energy-level spacing in the dot,
and current through the dot displays narrow band
noise at these frequencies. This preliminary example
demonstrates how one can manipulate the density
matrix of the dot by tuning bias or gate voltages,
which in turn changes the properties of the dot.
Currently, we are using our density-matrix equation
to model the quantum dots studied in experiments, to
understand how well the density-matrix equation can
describe the real dots. Recently, Professors Raymond C. Ashoori’s and Marc A. Kastner's groups at
MIT have generated data on the transport properties
of quantum dots. Systematic experimental studies
have been carried out for different gate voltages,
magnetic fields, and temperatures. Our theoretical
model for quantum dots will be closely checked
against the experimental results.
77
Part I, Section 2, Chapter 3. Quantum Circuit Theory
We are also exploring different design of the dot and
the coupling to the environment to see when the nonlinear effects are important and the dot can have
some interesting and useful behaviors. For example,
a dot can serve as a memory element if the equation
has two stable fixed points. It may behave like an
oscillator if the equation has a limiting cycle. We
hope these studies1 will help guide experiments in
creating real quantum dots that exhibit these novel
properties.
3.3 Journal Article
Heemeyer, S., and X.-G. Wen, “Integral Equation of
Motion of Quantum Dot.” Bull. APS 43(1): 872
(1998).
1 S. Heemeyer and X.-G. Wen, “High Frequency Dynamics of Quantum Dot,” Bull. APS 42(1): 129 (1997).
78 RLE Progress Report Number 141
Part I, Section 2, Chapter 3. Quantum Circuit Theory
Chapter 3.
Quantum Circuit Theory for Mesoscoptic Devices
Academic and Research Staff
Professor Xiao-Gang Wen
Graduate Students
Sven Heemeyer
3.1 Goals and Objectives
Sponsor
U.S. Army Research Office
Contract DAAG55-98-1-0080
Project Staff
Professor Xiao-Gang Wen, Sven Heemeyer
The goal of this research is to create realistic theoretical models for electronic circuits (or components of a
circuit) at scales so small that quantum effects are
important. More generally, the goal is to understand
the fundamental behavior of systems at the border of
the classical and quantum regimes. We propose to
create theoretical models of quantum dots and quantum wires, for these are the fundamental building
blocks of quantum electronic circuits. We will use
these models to study the nonlinear quantum dynamics of coupled dots and wires. We believe that these
theoretical models will allow us to design quantum
electronic circuits with prescribed properties. Beyond
this, we hope to discover phenomena not present in
classical electronic circuits, and to find applications
for them in new generations of nano-electronic
devices.
3.2 Dynamics of Quantum Dots Coupled
to Environment
The first step in achieving our goal is to find the fundamental theory that describes the systems between
the classical and quantum world, that is to find the
equation of motion that governs the behaviors of
those systems. We use equation of motion for the
density matrix to formulate the fundamental theory.The density matrix can describe both pure coherent quantum states and incoherent classical states.
Thus it can reach both the classical and the quantum
worlds. For an isolated system such as an isolated
quantum dot, the density-matrix equation is linear as
expected for a pure quantum system. However, for a
dot that couples to the outside world, the dot influences its own environment, and the change in its
environment in turn affects the dot. We include this
feedback effect to the equation of motion for the density matrix, using techniques developed in the theory
of many-body physics. This approach allows us to
incorporate both quantum phase coherent effects of
the dots and the dissipative/nonlinear effects of the
environment.
In the on-going study, graduate student Sven Heemeyer and I derived the equation of motion for the density matrix with the feedback effects mentioned
above using a perturbation theory. We found that the
density-matrix equation is indeed nonlinear, even in
the leading order perturbative calculation. More nonlinear terms may appear in higher order perturbative
expansions.
A preliminary study demonstrates that the coupling to
the environment can generate large off-diagonal elements in the density matrix. Since classical systems
are always described by diagonal density matrices,
the appearance of the off-diagonal elements indicate
the importance of the quantum effects. The values of
those off-diagonal matrix elements depend on various parameters, such as the bias/gate voltage. As a
consequence of the large off-diagonal elements, the
impedance of a dot has sharp peaks at frequencies
corresponding to the energy-level spacing in the dot,
and current through the dot displays narrow band
noise at these frequencies. This preliminary example
demonstrates how one can manipulate the density
matrix of the dot by tuning bias or gate voltages,
which in turn changes the properties of the dot.
Currently, we are using our density-matrix equation
to model the quantum dots studied in experiments, to
understand how well the density-matrix equation can
describe the real dots. Recently, Professors Raymond C. Ashoori’s and Marc A. Kastner's groups at
MIT have generated data on the transport properties
of quantum dots. Systematic experimental studies
have been carried out for different gate voltages,
magnetic fields, and temperatures. Our theoretical
model for quantum dots will be closely checked
against the experimental results.
77
Part I, Section 2, Chapter 3. Quantum Circuit Theory
We are also exploring different design of the dot and
the coupling to the environment to see when the nonlinear effects are important and the dot can have
some interesting and useful behaviors. For example,
a dot can serve as a memory element if the equation
has two stable fixed points. It may behave like an
oscillator if the equation has a limiting cycle. We
hope these studies1 will help guide experiments in
creating real quantum dots that exhibit these novel
properties.
3.3 Journal Article
Heemeyer, S., and X.-G. Wen, “Integral Equation of
Motion of Quantum Dot.” Bull. APS 43(1): 872
(1998).
1 S. Heemeyer and X.-G. Wen, “High Frequency Dynamics of Quantum Dot,” Bull. APS 42(1): 129 (1997).
78 RLE Progress Report Number 141