A problem in Quantum
Control:
Solving an Instance of the Schrödinger Equation
Brown University
Under the Guidance of:
Professor Avy Soffer and
Pieter Blue,
Rutgers University
Department of Mathematics
The
physical question:
Given
a particular initial quantum state of a several particle system, can we
introduce perturbations into the system to bring the system into a quantum
state of our choosing?
-In practice, the perturbations take the form of laser pulses acting on the particles.
-This
problem has applications in quantum computing.
The
Schrödinger equation is used to model the behavior of a quantum system :
i(da/dt)=Ha(t)
-H is a (possibly time
dependent) linear operator whose specific form is a manifestation of the
particular physical situation we are modeling.
-a(t) is a vector-valued function.
(It represents the quantum state of our system as a function of time)
My problem concerns the behavior of a quantum system
whose particles are acted on by lasers with intensities in time of form ce-lt, where c is a constant and l is a positive valued constant.

For large l, this function approximates a short laser pulse.
This system can be modeled
using the following instance of the Schrödinger equation:
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i(da/dt) = (H0+ ce-ltM0) a(t)
where
-a(t) is finite-dimensional
vector-valued function
-H0 is a
hermitian matrix
-M0 is a block
diagonal matrix whose blocks are rotation matrices
-a(0), the
initial state of the system, is known.
My task for this summer has been to solve this
equation for the vector a(t).
Once the equation is solved we can specify a desired quantum state and
use the solution to algebraically determine physical parameters that will yield
this desired state over large time.
i(da/dt) = (H0+ ce-ltM0) a(t)
-This matrix differential equation represents a
“non-autonomous” system of ordinary differential equations.
-it cannot be solved by the methods used to easily
solve non-linear problems (such as decoupling by diagonalization of the
operator)
NOTE:The imaginary constant can be absorbed into the
operator to make the computation simpler.
Henceforth, all H0, M0 used here will be
understood to be the matrices specified above, each multiplied by the scalar
constant –i.
My
approach to solving the problem:
-I take the Laplace transform, denoted
L{f(t)} for a function f(t), of both sides of the equation to
turn the differential equation into a difference equation of a complex variable
s.

-I solve this difference equation explicitly for the
(vector valued) Laplace transform F(s) of a(t). This solution takes the form of an infinite
sum.
-I use the theory of complex variables to:
1)Show that taking inverse Laplace
transform, or Bromwich integral, of
F(s) recovers a(t).
2)Demonstrate certain algebraic equalities that we would like to employ to bring the integrand in the Bromwich integral into a more easily calculable form.
3)Calculate the value of the
inverse Laplace transform of F(s) using the theory of residues
from complex analysis.
The difference equation obtained by taking the
Laplace transform of both sides of the matrix equation is:
F(s)=(sI-H0)-1a(0)+M0F(s+l)
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In
the special case where H0 and M0 commute, this reduces to
the neater sum:

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If
certain conditions on either F(s) or the unknown function a(t)
are satisfied, a(t) is equal to the inverse Laplace transform
of F(s), denoted
L-1{F(s)}:

for
(t>0) and for some real g sufficiently large.
So,
in summary, to find a(t) we must first show that L-1{F(s)}=a(t),
and then calculate L-1{F(s)}
using residue theory.
Results:
For
the case where M0 and H0 commute, I have a tentative
solution:

Work
in progress:
-meticulous
verification of this result
-solving
the general case
References/Recommended
Reading:
-Churchill, Operational Mathematics-Laplace
transforms
-Brown, Churchill, Complex Variables and
Applications-calculating residues
-http://www.qubit.com –web resource
for
information on applications of quantum control to quantum computing
-Schirmer,
Greentree, Ramakrishna, Rabitz, Quantum
Control Using
Sequences of Simple Control Pulses, arXiv:quant-ph/0105155 v1, May 31
2001. A paper that tackles the problem
of quantum control using sinusoidal laser pulses.