Quantum Computer System and Method for Partial Differential Equation-Constrained Optimization

Abstract

A computer (such as a classical computer, a quantum computer, or a hybrid quantum-classical computer) which performs PDE-constrained optimization of problems in cases in which, for a fixed {right arrow over (w)}, there is an explicit expression for {right arrow over (s)} that is either optimal or an approximation to the optimal solution. This enables embodiments of the present invention to eliminate {right arrow over (s)} from the optimization problem and to formulate the optimization as a polynomial unconstrained binary optimization (PUBO) problem.

Description

BACKGROUND

Quantum computers promise to solve industry-critical problems which are otherwise unsolvable or only very inefficiently addressable using classical computers. Key application areas include chemistry and materials, bioscience and bioinformatics, logistics, and finance. Interest in quantum computing has recently surged, in part due to a wave of advances in the performance of ready-to-use quantum computers.

Many solutions to engineering problems involve optimizing physical systems with respect to an application specific metric, while the evolution of the states of the physical systems is described by a partial differential equation (PDE). This naturally gives rise to PDE-constrained optimization problems involving two sets of variables:

• • Design variables {right arrow over (w)}, which consist of design parameters that specify features of a product (such as the length of the wing of an aircraft, the maximum thickness of the wing, etc.). The vector {right arrow over (w)} may, for example, be a collection of discrete parameters that can be codified into m binary variables:

{right arrow over (w)}={right arrow over (w)} ₀ +W ₁ {right arrow over (b)}  (1)

• • where {right arrow over (b)} is a vector of elements from {−1,1} and W₁ is a matrix representing the binary encoding.
  • State variables {right arrow over (s)}, which represent the physical state of the system (such as temperature, pressure, and velocity distribution over the wing surface), and which evolve as described by a governing PDE (such as the Navier-Stokes equation in the case of fluid dynamics or the heat equation in the case of heat transfer). If the underlying PDE is linear then

D{right arrow over (s)}={right arrow over (ƒ)}({right arrow over (w)})  (2)

• • with D being the discretized PDE operator and {right arrow over (ƒ)}({right arrow over (w)}) being a vector of polynomials in the design variables {right arrow over (w)}. The above equation reflects that the boundary condition of the system is under the influence of design decisions represented by {right arrow over (w)}. If the underlying PDE is non-linear, in the quadratic cases the constraints may, for example, take the form of (for details see Section 3)

{right arrow over (s)} ^† H{right arrow over (s)}+{right arrow over (g)} ^† {right arrow over (s)}+h({right arrow over (w)})=0  (3)

• • where H and {right arrow over (g)} result from discretization of the PDE and h({right arrow over (w)}) is a scalar function which is a polynomial of the design parameters {right arrow over (w)}.

The objective function is then a function of both {right arrow over (w)} and {right arrow over (s)}, with the constraints on {right arrow over (s)} that are either linear (Equation 2) or non-linear (Equation 3).

SUMMARY

Embodiments of the present invention are directed to a computer (such as a classical computer, a quantum computer, or a hybrid quantum-classical computer) which performs PDE-constrained optimization of problems in cases in which, for a fixed {right arrow over (w)}, there is an explicit expression for {right arrow over (s)} that is either optimal or an approximation to the optimal solution. This enables embodiments of the present invention to eliminate {right arrow over (s)} from the optimization problem and to formulate the optimization as a polynomial unconstrained binary optimization (PUBO) problem.

Other features and advantages of various aspects and embodiments of the present invention will become apparent from the following description and from the claims.

BRIEF DESCRIPTION OF THE DRAWINGS

This invention is described with particularity in the appended claims. The above and further aspects of this invention may be better understood by referring to the following description in conjunction with the accompanying drawings, in which like numerals indicate like structural elements and features in various figures. The drawings are not necessarily to scale, emphasis instead being placed upon illustrating the principles of the invention.

FIG. 1 is a diagram of a system implemented according to one embodiment of the present invention.

FIG. 2A is a flow chart of a method performed by the system of FIG. 1 according to one embodiment of the present invention.

FIG. 2B is a diagram illustrating operations typically performed by a computer system which implements quantum annealing.

FIG. 3 is a diagram of a hybrid quantum-classical computer system implemented according to one embodiment of the present invention.

FIG. 4 is a flowchart of a method performed by one embodiment of the present invention.

FIGS. 5A-5D are diagrams of equations used in embodiments of the present invention.

DETAILED DESCRIPTION

Introduction. Embodiments of the present invention are directed to a hybrid quantum-classical computer (which includes both a classical computer and a quantum computer) which solves PDE-constrained optimization problems. The method comprises, on the classical computer, transforming an initial problem description of a PDE-constrained optimization problem into a transformed problem description of a polynomial unconstrained binary optimization problem in the form of an Ising Hamiltonian. The hybrid quantum-classical computer then executes computer program instructions to generate the ground state, or a state approximating the ground state, of the Ising Hamiltonian.

Embodiments of the present invention are directed to cases in which, for a fixed {right arrow over (w)}, there is an explicit expression for {right arrow over (s)} that is either optimal or an approximation to the optimal solution. This enables embodiments of the present invention to eliminate {right arrow over (s)} from the optimization problem and to formulate the optimization as a polynomial unconstrained binary optimization (PUBO) problem:

$\begin{array}{cc}\underset{\overrightarrow{b}\in {\left\{0,1\right\}}^n}{\min }\sum _{i=1}^n{t}_i{b}_i+\sum _{i,j=1}^n{t}_{\mathrm{ij}}{b}_i{b}_j+\sum _{i,j,k=1}^n{t}_{\mathrm{ijk}}{b}_i{b}_j{b}_k+\cdots .& \left(4\right)\end{array}$

Formulating the problem in this way enables embodiments of the present invention to solve the problem using a quantum computer, such as by using either a quantum annealer or a quantum approximate optimization algorithm (QAOA), thereby solving the problem much more efficiently than would be possible with a classical computer alone. Since each b_i∈{−1,1}, embodiments of the present invention may treat the above problem as finding the ground state of a k-local Ising Hamiltonian (by equating each b_i to a spin variable). The general problem is NP-complete and, while its implementation on quantum annealing devices is well studied, issues such as overhead in embedding the k-local Hamiltonian onto the annealing device of limited connectivity remains to pose major obstacles for practical implementation. However, recent efforts based on QAOA have proven a promising alternative, and such efforts may be leveraged by embodiments of the present invention.

The remainder of the document is organized as follows. First, examples of ways in which embodiments of the present invention treat constraints that arise from linear PDEs are described. Next, examples of ways in which embodiments of the present invention may treat quadratic constraints that arise from nonlinear PDEs are described. For simplicity, and without limitation, the description herein focuses on the objective function being quadratic in {right arrow over (w)} and {right arrow over (s)}:

$\begin{array}{cc}\underset{\overrightarrow{v}=\left(\overrightarrow{w},\overrightarrow{s}\right)}{\min }{\overrightarrow{v}}^{†}A\overrightarrow{v}+{\overrightarrow{d}}^{†}\overrightarrow{v}s.t.\left(\mathrm{constraints}\right)& \left(5\right)\end{array}$

where the constraints may be either linear or non-linear. Next, the most general framework that takes into account objective functions of more generic forms is described.

Linear PDE-constrained optimization. Embodiments of the present invention in which the optimization problem has linear constraints, as illustrated by Equation 2, will now be described. For simplicity, and without limitation, assume that the function {right arrow over (ƒ)} is linear in {right arrow over (w)}: {right arrow over (ƒ)}({right arrow over (w)})={right arrow over (ƒ)}₀+F₁{right arrow over (w)}. More general cases will be described below. Since the discretized PDE operator D is commonly invertible:

{right arrow over (s)}=D ⁻¹({right arrow over (ƒ)}₀+F₁{right arrow over (w)}).  (6)

The full constrained optimization problem can then be written as

$\begin{array}{cc}\underset{\overrightarrow{v}}{\min }{\overrightarrow{v}}^{†}A\overrightarrow{v}+{\overrightarrow{d}}^{†}\overrightarrow{v}s.t.M\overrightarrow{v}=\overrightarrow{\ell }& \left(7\right)\end{array}$

A is assumed to be Hermitian. Also, {right arrow over (v)} is an n-dimensional vector that results from concatenating the vector {right arrow over (w)} of n_w discrete design parameters and the vector {right arrow over (s)} of n_s performance parameters (and thus n=n_w+n_s). Let m be the total number of linear constraints. Then the matrix M is of dimension m×n. The block forms of M and are

M=(−D⁻¹F₁I), =D⁻¹{right arrow over (ƒ)}₀.  (8)

With the explicit expression of {right arrow over (s)} in Equation 6, embodiments of the present invention may eliminate {right arrow over (s)} from the optimization problem and obtain an unconstrained optimization problem over {right arrow over (w)} only:

$\begin{array}{cc}\underset{\overrightarrow{w}}{\min }{\overrightarrow{w}}^{†}\hat{A}\overrightarrow{w}+{\overrightarrow{\hat{d}}}^{†}\overrightarrow{w}+\hat{c}& \left(9\right)\end{array}$

where the new matrix Â, vector {circumflex over ({right arrow over (d)})} and scalar ĉ may be written as

Â=A _ww +F ₁ ^† D ⁻¹ A _SW +F ₁ ^† D ⁻¹ A _ss PD ⁻¹ F ₁

{circumflex over ({right arrow over (d)})}={right arrow over (d)}_x+2A_sw^†D⁻¹{right arrow over (ƒ)}₀+2F₁^†D⁻¹A_ssPD⁻¹{right arrow over (ƒ)}₀+F₁^†D⁻¹{right arrow over (d)}_s

ĉ={right arrow over (ƒ)} ₀ \D ⁻¹ A _ss PD ⁻¹{right arrow over (ƒ)}₀+{right arrow over (d)}_s^†D⁻¹{right arrow over (ƒ)}₀.  (10)

A and {right arrow over (d)} in Equation 7 may be partitioned into blocks

$\begin{array}{cc}A=\left(\begin{array}{cc}{A}_{\mathrm{ww}}& A_{\mathrm{ws}}\\ A_{\mathrm{sw}}& A_{\mathrm{ss}}\end{array}\right),\overrightarrow{d}=\left(\begin{array}{c}{\overrightarrow{d}}_w\\ {\overrightarrow{d}}_s\end{array}\right),& \left(11\right)\end{array}$

the same way {right arrow over (v)} is parititioned into n_w and n_s subblocks. Furthermore, embodiments of the present invention also assume that D is Hermitian, which should be the case in most linear PDE operators.

Further applying Equation 1 to Equation 9 produces an unconstrained binary optimization problem over strings {right arrow over (b)} of elements from {−1,1}. Ignoring the scalar term, the problem may be expressed as

$\begin{array}{cc}{\underset{\overrightarrow{b}}{\min }{\overrightarrow{b}}^{T}Q\overrightarrow{b},Q_{\mathrm{ij}}={\left(W_1^{†}\hat{A}{W}_1\right)}_{\mathrm{ij}}+\left(2{\overrightarrow{x}}_0^{†}\hat{A}{W}_1+{\overrightarrow{\hat{d}}}^{†}{W}_1\right)\overrightarrow{b})}_i{\delta }_{\mathrm{ij}}.& \left(12\right)\end{array}$

The binary optimization problem as stated in Equation 12 is NP-complete for general Q. Although there are classical heuristics for solving the problem, its solution using noisy intermediate scale quantum devices has been studied intensely in recent efforts.

An example of an application of embodiments of the present invention to a heat equation will now be described. Consider, for example, a one-dimensional bounded physical system whose temperature distribution s(x) over time is governed by the heat equation:

$\begin{array}{cc}\frac{\partial s}{\partial t}=\alpha \frac{{\partial }^{2}s}{\partial x^2},t\in \left[0,T\right],x\in \left[0,1\right].& \left(13\right)\end{array}$

The goal is to have a specific temperature distribution s_ideal(x) at time T. To accomplish this, in embodiments of the present invention the initial temperature distribution s(x,0) may be designed such that the difference between s(x,T) and s_ideal(x) is minimized.

Space and time may be discretized using a grid as the following:

{right arrow over (t)}=(t₀,t₀, . . . ,t_N), with t₀=0, t_N=T

{right arrow over (x)}=(x₀,x₁, . . . ,x_M), with x₀=0, x_M=1.  (14)

The following scheme may then be used to approximate the partial derivatives:

$\begin{array}{cc}\frac{\partial s\left(x_k,t_k\right)}{\partial t}\approx \frac{s\left(x_k,t_{k+1}\right)-s\left(x_k,t_k\right)}{\Delta t}\frac{\partial s\left(x_k,t_k\right)}{\partial x}\approx \frac{s\left(x_{k+1},t_k\right)-s\left(x_k,t_k\right)}{\Delta x}\frac{{\partial }^{2}s\left(x_k,t_k\right)}{\partial x^2}\approx \frac{s\left(x_{k+1},t_k\right)-2s\left(x_k,t_k\right)+s\left(x_{k-1},t_k\right)}{\Delta x^2}.& \left(15\right)\end{array}$

Then Equation 13 for a point (x_k,t_k) to in the middle of the (x,t) domain may be rearranged to obtain

$\begin{array}{cc}s\left(x_k,t_{k+1}\right)=\frac{\alpha }{\Delta x^2}s\left(x_{k+1},t_k\right)+\left(\frac{1}{\Delta t}-\frac{2\alpha }{\Delta x^2}\right)s\left(x_k,t_k\right)+\frac{\alpha }{\Delta x^2}s\left(x_{k-1},t_k\right).& \left(16\right)\end{array}$

Denote {right arrow over (s)}({right arrow over (x)},t)=(s(x₁,t),s(x₂,t), . . . ,s(x_m,t)). Then a matrix L may be constructed according to Equation 16 such that {right arrow over (s)}({right arrow over (x)},t_k+1)=L{right arrow over (s)}({right arrow over (x)},t_k). Then the state variables {right arrow over (s)}={right arrow over (s)}({right arrow over (x)},T) may be related to the initial state by

{right arrow over (s)}=L ⁿ {right arrow over (s)}({right arrow over (x)},0)  (17)

Let the PDE operator D=L⁻ⁿ and the initial state {right arrow over (s)}({right arrow over (x)},0) be some polynomial function {right arrow over (ƒ)}({right arrow over (x)}) of the design parameters {right arrow over (x)}. Then the linear constraint in Equation 2 may be recovered. For the purpose of illustration assume {right arrow over (ƒ)}({right arrow over (w)})={right arrow over (ƒ)}₀+F₁{right arrow over (w)}. Let {right arrow over (s)}_ideal=(s_ideal(x₁), s_ideal(x₂) . . . , s_ideal(x_m)). Then we can formulate the design optimization problem as

$\begin{array}{cc}\underset{\overrightarrow{w}}{\min }{\overrightarrow{s}-{\overrightarrow{s}}_{\mathrm{ideal}}}_2^2={\overrightarrow{s}}^T\overrightarrow{s}=2{\overrightarrow{s}}_{\mathrm{ideal}}^T\overrightarrow{s}+{\overrightarrow{s}}_{\mathrm{ideal}}^T{\overrightarrow{s}}_{\mathrm{ideal}}s.t.D\overrightarrow{s}={\overrightarrow{f}}_0+F_1\overrightarrow{w}.& \left(18\right)\end{array}$

The previously described general technique may then be used to convert the above problem to an unconstrained binary optimization problem over variables {right arrow over (b)} where each b_i∈{−1,1}. Assume that {right arrow over (b)} can be linearly related to {right arrow over (w)} by an encoding of the form described in Equation 1.

Non-linear PDE-constrained optimization. Embodiments of the present invention which are directed to non-linear PDE-constrained optimization will now be described. Unlike linear PDE constraints, which, as was described above, can be removed rather elegantly by linear algebra, non-linear PDE constraints have their own distinct challenges that need to be addressed. Instead of attempting to derive a general theory, the following description focuses on a specific example solely for the purpose of illustration and without limitation. Consider the following one-dimensional bounded physical system whose velocity u obeys Burger's equation:

$\begin{array}{cc}\frac{\partial u}{\partial t}+u\frac{\partial u}{\partial x}=0,t\in \left[0,T\right],x\in \left[0,1\right].& \left(19\right)\end{array}$

As a simplified form of Navier-Stokes equation for general fluid dynamics problems, Burger's equation is used for describing specific fluid dynamical phenomena such as the formation of shock waves. In spite of its simple form, its quadratic nonlinearity (due to the term

$u\frac{\partial u}{\partial x})$

is also a core feature of Navier-Stokes equation. Therefore, the following description on solving Burger's equation may be used as a building block for solving general Navier-Stokes equation-based problems.

With the same discretization scheme as Equation 14, the solution u(x,t) may, for example, be represented in a vector form. Specifically, assume that

$\begin{array}{cc}\overrightarrow{u}\left(\overrightarrow{x},\overrightarrow{t}\right)=\left(\begin{array}{c}\overrightarrow{u}\left(\overrightarrow{x},t_0\right)\\ \overrightarrow{u}\left(\overrightarrow{x},t_1\right)\\ ⋮\\ \overrightarrow{u}\left(\overrightarrow{x},t_n\right)\end{array}\right)=\left(\begin{array}{c}{\overrightarrow{u}}_0\\ {\overrightarrow{u}}_{+}\end{array}\right)& \left(20\right)\end{array}$

where {right arrow over (e)}₀={right arrow over (u)}({right arrow over (x)},t₀) and {right arrow over (u)}₊ is the remaining entries of {right arrow over (u)}({right arrow over (x)},{right arrow over (t)}). In the framework defined in the “Introduction” section above, the state variables {right arrow over (s)}={right arrow over (u)}₊. However, for notational transparency the following description will use {right arrow over (u)}₊ instead of {right arrow over (s)}. Adopting the same approximation scheme as Equation 15 allows Burger's equation to be rewritten as

D _t {right arrow over (u)}+{right arrow over (u)}⊙D _x {right arrow over (u)}=0  (21)

where D_t and D_x are discretized derivative operators and ⊙ is the Hadamard product (elementwise product). More specifically, with mesh size Δt and Δx for time and space, D_t may be given as

$\begin{array}{cc}{D}_t=\frac{1}{\Delta t}{D}_1\otimes I,D_x=\frac{1}{\Delta x}I\otimes D_1,D_1=\left(\begin{array}{ccccc}-1& 1& & & \\ & -1& 1& & \\ & & \ddots & \ddots & \\ & & & -1& 1\end{array}\right)& \left(22\right)\end{array}$

where D₁ is the discrete first-order derivative operator. Using the same partitioning as in Equation 20, D_t and D_x may be partitioned accordingly

$\begin{array}{cc}{D}_t=\left(\begin{array}{cc}{D}_{t0}& D_{t,0+}\\ 0& D_{t+}\end{array}\right),D_x=\left(\begin{array}{cc}{D}_{x0}& 0\\ 0& D_{x+}\end{array}\right).& \left(23\right)\end{array}$

For any vector {right arrow over (v)}, left multiplying Equation 21 by {right arrow over (v)}^T gives the following:

{right arrow over (v)} ^T D _t {right arrow over (u)}+{right arrow over (u)} ^TΛ_vD_x{right arrow over (u)}=0  (24)

where Λ_v=diag({right arrow over (v)}) is a diagonal matrix whose diagonal elements correspond to elements of {right arrow over (v)}. Using the same partitioning on {right arrow over (v)} such that {right arrow over (v)}=({right arrow over (v)}₀^T,{right arrow over (v)}₊^T), Equation 23 can be written as

{right arrow over (u)} ₊ ^T A _v {right arrow over (u)} ₊ +{right arrow over (d)} _v ^T {right arrow over (u)} ₊ +c _v+=0  (25)

where

A _v=Λ_v+D_x+

{right arrow over (d)} _v ^T ={right arrow over (v)} ₀ ^T D _t,0 +{right arrow over (v)} ₊ ^T D _t+

c _v ={right arrow over (v)} ₀ ^T D _t0 {right arrow over (u)} ₀ +{right arrow over (u)} ₀ ^TΛ_v0D_x0{right arrow over (u)}₀.  (26)

Suppose a set of m vectors {right arrow over (v)}₁, {right arrow over (v)}₂, . . . , {right arrow over (v)}_m is introduced. Then m quadratic constraints may be formed, as in Equation 25 for each

${\overrightarrow{v}}_i=\left(\begin{array}{c}{\overrightarrow{v}}_{i0}\\ {\overrightarrow{v}}_{i+}\end{array}\right):$

$\begin{array}{cc}{\overrightarrow{u}}_{+}^T{A}_{v_1}{\overrightarrow{u}}_{+}+{\overrightarrow{d}}_{v_1}^T{\overrightarrow{u}}_{+}+c_{v_1}=0{\overrightarrow{u}}_{+}^T{A}_{v_2}{\overrightarrow{u}}_{+}+{\overrightarrow{d}}_{v_2}^T{\overrightarrow{u}}_{+}+c_{v_2}=0⋮{\overrightarrow{u}}_{+}^T{A}_{v_m}{\overrightarrow{u}}_{+}+{\overrightarrow{d}}_{v_m}^T{\overrightarrow{u}}_{+}+c_{v_m}=0.& \left(27\right)\end{array}$

Assume that the optimization target is a quadratic function of the solution vector {right arrow over (u)}:

{right arrow over (u)} ^T A{right arrow over (u)}+{right arrow over (d)} ^T {right arrow over (u)}  (28)

where A is Hermitian and {right arrow over (d)} is some vector which is given. The objective function may, for example, be the norm distance between the final state and some ideal state, just as it is the case with the heat equation example in the previous section. However, for ease of explanation and without limitation, assume that the objective function has a general quadratic form. With the partition

$\begin{array}{cc}A=\left(\begin{array}{cc}{A}_0& A_{0+}\\ A_{+0}& A_{+}\end{array}\right),\overrightarrow{d}=\left(\begin{array}{c}{\overrightarrow{d}}_0\\ {\overrightarrow{d}}_{+}\end{array}\right)& \left(29\right)\end{array}$

the objective function may be rewritten as

{right arrow over (u)} ₀ ^T A ₀ {right arrow over (u)} ₀+2{right arrow over (u)}₊^TA₊₀{right arrow over (u)}₀+{right arrow over (u)}₊^TA₊{right arrow over (u)}₊+{right arrow over (b)}₀^T{right arrow over (u)}₀+{right arrow over (b)}₊^T{right arrow over (u)}₊.  (30)

Taking into account the constraints in Equation 27, assuming that the initial state {right arrow over (u)}₀ depends on the design parameters {right arrow over (w)} linearly:

{right arrow over (u)} ₀={right arrow over (ƒ)}({right arrow over (w)})={right arrow over (ƒ)}₀+F₁{right arrow over (w)},  (31)

the full design optimization problem may be stated as

$\begin{array}{cc}\underset{\overrightarrow{w}}{\min }{\overrightarrow{u}}^{T}A\overrightarrow{u}+{\overrightarrow{d}}^T\overrightarrow{u}s.t.{\overrightarrow{u}}_{+}^T{A}_{v_1}{\overrightarrow{u}}_{+}+{\overrightarrow{d}}_{v_1}^T{\overrightarrow{u}}_{+}+c_{v_1}=0{\overrightarrow{u}}_{+}^T{A}_{v_2}{\overrightarrow{u}}_{+}+{\overrightarrow{d}}_{v_2}^T{\overrightarrow{u}}_{+}+c_{v_2}=0⋮{\overrightarrow{u}}_{+}^T{A}_{v_m}{\overrightarrow{u}}_{+}+{\overrightarrow{d}}_{v_m}^T{\overrightarrow{u}}_{+}+c_{v_m}=0.& \left(32\right)\end{array}$

The dependence between {right arrow over (u)}, {right arrow over (u)}₀ and {right arrow over (u)}₊ is implicit in the above specification. As a next step, embodiments of the present invention may remove the m constraints and transform the problem into an unconstrained optimization over {right arrow over (u)}₀ and therefore {right arrow over (w)} by Equation 31. Embodiments of the present invention may accomplish this by the Lagrangian function

$\begin{array}{cc}L\left({\overrightarrow{u}}_{+},\overrightarrow{\lambda }\right)={\overrightarrow{u}}_0^T{A}_0{\overrightarrow{u}}_0+2{\overrightarrow{u}}_{+}^T{A}_{+0}{\overrightarrow{u}}_0+{\overrightarrow{u}}_{+}^T{A}_{+}{\overrightarrow{u}}_{+}+{\overrightarrow{b}}_0^T{\overrightarrow{u}}_0+{\overrightarrow{b}}_{+}^T{\overrightarrow{u}}_{+}-\sum _{i=1}^m{\lambda }_i\left({\overrightarrow{u}}_i^T{A}_{v_i}{\overrightarrow{u}}_{+}+{\overrightarrow{d}}_{v_i}^T{\overrightarrow{u}}_{+}+c_{v_i}\right).& \left(33\right)\end{array}$

A necessary condition for global optimum is

$\frac{\partial L\left({\overrightarrow{u}}_{+},\overrightarrow{\lambda }\right)}{\partial {\overrightarrow{u}}_{+}}=0,$

which gives rise to solution

$\begin{array}{cc}{\overrightarrow{u}}_{+}^{*}\left(\overrightarrow{\lambda }\right)=\frac{1}{2}{\left(A_{+}-\sum _{i=1}^m{\lambda }_i{A}_{v_i}\right)}^{-1}\left(-{\overrightarrow{b}}_{+}-2A_{+0}{\overrightarrow{u}}_0+\sum _{i=1}^m{\lambda }_i{\overrightarrow{d}}_{v_i}\right).& \left(34\right)\end{array}$

This eliminates the {right arrow over (u)}₊ variables. If {right arrow over (u)}₊* is substituted into the Lagrangian function, then {right arrow over (λ)}* may be obtained by solving

$\begin{array}{cc}\underset{\overrightarrow{\lambda }}{\min }L\left({\overrightarrow{u}}_{+}^{*}\left(\overrightarrow{\lambda }\right),\overrightarrow{\lambda }\right).& \left(35\right)\end{array}$

Note that for solving this it is assumed, solely for the sake of example and without limitation, that {right arrow over (u)}₀ is fixed. As will be explained below, {right arrow over (u)}₀ in fact comes from a previous iteration of the solver. Once {right arrow over (u)}₀ is fixed, depending on m, the solution {right arrow over (λ)}* may be obtained by a variety of heuristic solvers. This leads to the expression

{right arrow over (u)} ₊ ={right arrow over (u)} ₊*({right arrow over (λ)}*)=K{right arrow over (u)}₀+{right arrow over (y)}  (36)

for some matrix K and vector {right arrow over (y)} determined from Equation 34 and the optimization in (35). Substituting Equation 36 into the objective function 30 gives an unconstrained optimization over ěcu₀, which can be related to design parameters {right arrow over (w)} through, for example, Equation 31 and ultimately to binary variables {right arrow over (b)} through the encoding representation of the form in Equation 1. Putting these together, the final unconstrained binary optimization may be given as

$\begin{array}{cc}{\underset{\overrightarrow{b}}{\min }{\overrightarrow{b}}^{T}Q\overrightarrow{b},Q_{\mathrm{ij}}={\left(W_1^T{F}_1^T\left(A_0+2A_{0+}K+K^T{A}_{+}K\right)F_1{W}_1\right)}_{\mathrm{ij}}+\left\{\left[2\left({\overrightarrow{w}}_0^T{F}_1^T+{\overrightarrow{f}}_0^T\right)\left(A_0+2A_{0+}K+K^T{A}_{+}K\right)\right)+\left(2{\overrightarrow{y}}^T{A}_{0+}^T+2{\overrightarrow{y}}^T{A}_{0+}^T+2{\overrightarrow{y}}^T{A}_{+}K+{\overrightarrow{b}}_0^T+{\overrightarrow{b}}_{+}^T\right)\right]F_1{W}_1\}}_{\mathrm{ii}}{\delta }_{\mathrm{ij}}.& \left(37\right)\end{array}$

From the remark after Equation 35, it follows that the Q matrix in Equation 37 itself also depends on {right arrow over (b)}, making the solution to this problem a self-consistent procedure. More explicitly, the algorithm may be as follows:

• • 1. Start from an initial guess {right arrow over (b)}⁽⁰⁾;
  • 2. Compute Q⁽⁰⁾ based on {right arrow over (b)}⁽⁰⁾ according to Equation 37;
  • 3. For k=1, 2, . . .
    • (a) Compute {right arrow over (b)}^(k) by minimizing Equation 37 with the matrix Q computed from {right arrow over (b)}^(k-1);
    • (b) Compute Q from {right arrow over (b)}^(k).

In case m has the same dimension as {right arrow over (u)} and all vectors {right arrow over (v)}_i are independent, the constraints in Equation 27 are equivalent to Equation 21. However, in practice the dimension of {right arrow over (u)} may be high, causing many constraints which need to be satisfied. Embodiments of the present invention instead adopt a sampling approach, namely generating {right arrow over (v)}_i vectors by sampling from a specific distribution . The explicit notation Q(V) is used herein to denote the dependence of Q on the samples V=({right arrow over (v)}₁, {right arrow over (v)}₂, . . . , {right arrow over (v)}_m). Then, in the algorithm, Q is replaced with Q(V). In practice, embodiments of the present invention may sample many batches of V's and average over the results.

Generalization to higher-order problems. The discussions so far have yielded only unconstrained quadratic binary optimization problems. This is due to the linearity assumptions made in various locations for simplicity of argument. However, these linear assumptions are merely examples and do not constitute limitations of the present invention. The following description describes some examples of which in which the schemes described in the previous sections may be generalized to account for more involved scenarios in practice.

In the section above entitled, “Linear PDE-Constrained Optimization,” it is assumed that the dependence of the boundary condition on the design parameters {right arrow over (w)} is linear. This is merely an example and does not constitute a limitation of the present invention. Alternatively, for example, the function {right arrow over (ƒ)}({right arrow over (w)}) may be any bounded degree polynomial in {right arrow over (w)}. This yields a vector of polynomials {right arrow over (q)}({right arrow over (b)})={right arrow over (ƒ)}({right arrow over (w)}), where {right arrow over (b)} is a vector of {−1,1} variables. For convenience, the language of tensor networks may be used to represent the polynomials. As a start, {right arrow over (w)}({right arrow over (b)}) may be described as shown in FIG. 5A. In a similar fashion, the scalar objective function in (4) may also be described using tensor networks.

In general, no matter how complicated the dependence of the objective function, and no matter how complicated the boundary condition of the PDE constraints on the design parameters {right arrow over (w)} or equivalently their binary encoding {right arrow over (b)}, as long as for a fixed {right arrow over (w)} the constraints and the objective function are linear or quadratic in state variables {right arrow over (s)}, the PDE-constrained optimization problem may always be converted into one or more unconstrained binary optimization problems of the form in (4). The following description will cover the linear and quadratic cases separately.

General scheme for linear PDE constraints. The section above entitled, “Linear PDE-Constrained Optimization,” discussed a special case where the objective function is quadratic in both design variables {right arrow over (w)} and state variable {right arrow over (s)}, and {right arrow over (w)} contributes linearly to the boundary condition (namely {right arrow over (ƒ)}({right arrow over (w)}) is linear in {right arrow over (w)}). The following description considers general scenarios where {right arrow over (w)} contributes arbitrary polynomial dependence to both the objective function and the boundary condition of the linear PDE constraints. The resulting binary optimization problem then corresponds to finding the ground state of a k-local Ising Hamiltonian.

More explicitly, a general objective function may be written (as shown in FIG. 5B) as a degree-d polynomial in {right arrow over (w)} and {right arrow over (s)} assuming elements of {right arrow over (w)} and {right arrow over (s)} are both real, where {right arrow over (w)} and {right arrow over (s)} can be expressed as shown in FIGS. 5C and 5D.

Substituting the equations represented in FIGS. 5C and 5D into the objective function into the equation represented in FIG. 5B yields an unconstrained PUBO problem in the form of Equation 4.

General scheme for nonlinear PDE constraints. The case of nonlinear PDE constraints is more involved and restrictive than the linear case. Because it is necessary to be able to solve explicitly for the dependence between the state variables and the design variables (see for example Equation 34, where {right arrow over (u)}₊ is the state variable and {right arrow over (u)}₀ is dependent on the design variables), the objective function cannot be a too high-degree polynomial in the state variables. In such a case, embodiments of the present invention restrict to objective functions that are quadratic in state variables (but unrestricted in design variables). This allows for explicit expression connecting state variables to design variables (Equation 34). (In principle higher order dependence of the objective function on the state variables is also possible. For cubic and quartic polynomial equations, explicit solutions are still possible in some cases. Higher order equations than quartic do not admit analytical solution due to Galois theory. Therefore in order for

$\frac{\partial L}{\partial \overrightarrow{s}}=0$

to be analytically tractable there is an upper limit for the degree of the objective function on the state variables to not exceed 5.)

The scheme may then proceed as described in the section above entitled, “Non-Linear PDE-Constrained Optimization.” The only differences lie in the objective function that may possibly contain high order terms in the design variables {right arrow over (w)}, and the initial state being a high degree polynomial in the design variables {right arrow over (w)}. One may also explicitly write down the details using the language of tensor networks as in the section above entitled, “Introduction.”

Referring to FIG. 4, a flowchart is shown of a method 400 that is performed by one embodiment of the present invention. The method 400 may, for example, be performed by a hybrid quantum-classical computer 414 including a classical computer and a quantum computer, which may be implemented in any of the ways disclosed herein, such as in any of the ways shown and described in connection with FIGS. 1 and 3. Although FIG. 4 shows a hybrid quantum-classical computer 414 as distinct from the classical computer 412, the classical computer 412 may be within the hybrid quantum-classical computer. More generally, the classical computer 412 and the hybrid quantum-classical computer 414 are shown in FIG. 4 merely to illustrate the elements that may be used to perform the method steps 402, 404, 406, 408, and 410.

The method includes: (A) on the classical computer 412, transforming 404 an initial problem description 402 of an initial PDE-constrained optimization problem into a transformed problem description 406 of a polynomial unconstrained binary optimization problem in the form of an Ising Hamiltonian 408; and (B) on the hybrid quantum-classical computer 414, executing 410 computer program instructions to generate an approximate ground state of the Ising Hamiltonian. The method 400 may further include, after (A) and before (B): (C) on the classical computer 412, producing the computer program instructions for finding the approximate ground state of the Ising Hamiltonian representing the transformed problem. In other words, the computer program instructions produced in (C) may be the computer program instructions that are executed in (B).

The initial problem description may be or include a tensor network. The transformed problem description may be or include a tensor network.

Producing the computer program instructions may include producing computer program instructions for applying the quantum approximate optimization algorithm. Producing the computer program instructions may include producing computer program instructions for performing quantum annealing.

The initial PDE-constrained optimization problem may be governed by the heat equation. The initial PDE-constrained optimization problem may be governed by Burger's equation.

Executing the computer program instructions may include applying the quantum approximate optimization algorithm. Executing the computer program instructions may include performing quantum annealing.

The approximate ground state of the Ising Hamiltonian may be the ground state of the Ising Hamiltonian.

Another embodiment of the present invention is directed to a system for use with a hybrid quantum-classical computer. The hybrid quantum-classical computer may include a classical computer and a quantum computer. The classical computer may include at least one processor and at least one non-transitory computer-readable medium having computer program instructed stored thereon. The computer program instructions may be executable by the at least one processor in the classical computer to perform a method. The method may be any of the methods disclosed herein. For example, the method may include: (A) on the classical computer, transforming an initial problem description of an initial PDE-constrained optimization problem into a transformed problem description of a polynomial unconstrained binary optimization problem in the form of an Ising Hamiltonian; (B) on the hybrid quantum-classical computer, executing computer program instructions to generate an approximate ground state of the Ising Hamiltonian.

It is to be understood that although the invention has been described above in terms of particular embodiments, the foregoing embodiments are provided as illustrative only, and do not limit or define the scope of the invention. Various other embodiments, including but not limited to the following, are also within the scope of the claims. For example, elements and components described herein may be further divided into additional components or joined together to form fewer components for performing the same functions.

Various physical embodiments of a quantum computer are suitable for use according to the present disclosure. In general, the fundamental data storage unit in quantum computing is the quantum bit, or qubit. The qubit is a quantum-computing analog of a classical digital computer system bit. A classical bit is considered to occupy, at any given point in time, one of two possible states corresponding to the binary digits (bits) 0 or 1. By contrast, a qubit is implemented in hardware by a physical medium with quantum-mechanical characteristics. Such a medium, which physically instantiates a qubit, may be referred to herein as a “physical instantiation of a qubit,” a “physical embodiment of a qubit,” a “medium embodying a qubit,” or similar terms, or simply as a “qubit,” for ease of explanation. It should be understood, therefore, that references herein to “qubits” within descriptions of embodiments of the present invention refer to physical media which embody qubits.

Each qubit has an infinite number of different potential quantum-mechanical states. When the state of a qubit is physically measured, the measurement produces one of two different basis states resolved from the state of the qubit. Thus, a single qubit can represent a one, a zero, or any quantum superposition of those two qubit states; a pair of qubits can be in any quantum superposition of 4 orthogonal basis states; and three qubits can be in any superposition of 8 orthogonal basis states. The function that defines the quantum-mechanical states of a qubit is known as its wavefunction. The wavefunction also specifies the probability distribution of outcomes for a given measurement. A qubit, which has a quantum state of dimension two (i.e., has two orthogonal basis states), may be generalized to a d-dimensional “qudit,” where d may be any integral value, such as 2, 3, 4, or higher. In the general case of a qudit, measurement of the qudit produces one of d different basis states resolved from the state of the qudit. Any reference herein to a qubit should be understood to refer more generally to an d-dimensional qudit with any value of d.

Although certain descriptions of qubits herein may describe such qubits in terms of their mathematical properties, each such qubit may be implemented in a physical medium in any of a variety of different ways. Examples of such physical media include superconducting material, trapped ions, photons, optical cavities, individual electrons trapped within quantum dots, point defects in solids (e.g., phosphorus donors in silicon or nitrogen-vacancy centers in diamond), molecules (e.g., alanine, vanadium complexes), or aggregations of any of the foregoing that exhibit qubit behavior, that is, comprising quantum states and transitions therebetween that can be controllably induced or detected.

For any given medium that implements a qubit, any of a variety of properties of that medium may be chosen to implement the qubit. For example, if electrons are chosen to implement qubits, then the x component of its spin degree of freedom may be chosen as the property of such electrons to represent the states of such qubits. Alternatively, the y component, or the z component of the spin degree of freedom may be chosen as the property of such electrons to represent the state of such qubits. This is merely a specific example of the general feature that for any physical medium that is chosen to implement qubits, there may be multiple physical degrees of freedom (e.g., the x, y, and z components in the electron spin example) that may be chosen to represent 0 and 1. For any particular degree of freedom, the physical medium may controllably be put in a state of superposition, and measurements may then be taken in the chosen degree of freedom to obtain readouts of qubit values.

Certain implementations of quantum computers, referred as gate model quantum computers, comprise quantum gates. In contrast to classical gates, there is an infinite number of possible single-qubit quantum gates that change the state vector of a qubit. Changing the state of a qubit state vector typically is referred to as a single-qubit rotation, and may also be referred to herein as a state change or a single-qubit quantum-gate operation. A rotation, state change, or single-qubit quantum-gate operation may be represented mathematically by a unitary 2×2 matrix with complex elements. A rotation corresponds to a rotation of a qubit state within its Hilbert space, which may be conceptualized as a rotation of the Bloch sphere. (As is well-known to those having ordinary skill in the art, the Bloch sphere is a geometrical representation of the space of pure states of a qubit.) Multi-qubit gates alter the quantum state of a set of qubits. For example, two-qubit gates rotate the state of two qubits as a rotation in the four-dimensional Hilbert space of the two qubits. (As is well-known to those having ordinary skill in the art, a Hilbert space is an abstract vector space possessing the structure of an inner product that allows length and angle to be measured. Furthermore, Hilbert spaces are complete: there are enough limits in the space to allow the techniques of calculus to be used.)

A quantum circuit may be specified as a sequence of quantum gates. As described in more detail below, the term “quantum gate,” as used herein, refers to the application of a gate control signal (defined below) to one or more qubits to cause those qubits to undergo certain physical transformations and thereby to implement a logical gate operation. To conceptualize a quantum circuit, the matrices corresponding to the component quantum gates may be multiplied together in the order specified by the gate sequence to produce a 2n×2n complex matrix representing the same overall state change on n qubits. A quantum circuit may thus be expressed as a single resultant operator. However, designing a quantum circuit in terms of constituent gates allows the design to conform to a standard set of gates, and thus enable greater ease of deployment. A quantum circuit thus corresponds to a design for actions taken upon the physical components of a quantum computer.

A given variational quantum circuit may be parameterized in a suitable device-specific manner. More generally, the quantum gates making up a quantum circuit may have an associated plurality of tuning parameters. For example, in embodiments based on optical switching, tuning parameters may correspond to the angles of individual optical elements.

In certain embodiments of quantum circuits, the quantum circuit includes both one or more gates and one or more measurement operations. Quantum computers implemented using such quantum circuits are referred to herein as implementing “measurement feedback.” For example, a quantum computer implementing measurement feedback may execute the gates in a quantum circuit and then measure only a subset (i.e., fewer than all) of the qubits in the quantum computer, and then decide which gate(s) to execute next based on the outcome(s) of the measurement(s). In particular, the measurement(s) may indicate a degree of error in the gate operation(s), and the quantum computer may decide which gate(s) to execute next based on the degree of error. The quantum computer may then execute the gate(s) indicated by the decision. This process of executing gates, measuring a subset of the qubits, and then deciding which gate(s) to execute next may be repeated any number of times. Measurement feedback may be useful for performing quantum error correction, but is not limited to use in performing quantum error correction. For every quantum circuit, there is an error-corrected implementation of the circuit with or without measurement feedback.

Some embodiments described herein generate, measure, or utilize quantum states that approximate a target quantum state (e.g., a ground state of a Hamiltonian). As will be appreciated by those trained in the art, there are many ways to quantify how well a first quantum state “approximates” a second quantum state. In the following description, any concept or definition of approximation known in the art may be used without departing from the scope hereof. For example, when the first and second quantum states are represented as first and second vectors, respectively, the first quantum state approximates the second quantum state when an inner product between the first and second vectors (called the “fidelity” between the two quantum states) is greater than a predefined amount (typically labeled E). In this example, the fidelity quantifies how “close” or “similar” the first and second quantum states are to each other. The fidelity represents a probability that a measurement of the first quantum state will give the same result as if the measurement were performed on the second quantum state. Proximity between quantum states can also be quantified with a distance measure, such as a Euclidean norm, a Hamming distance, or another type of norm known in the art. Proximity between quantum states can also be defined in computational terms. For example, the first quantum state approximates the second quantum state when a polynomial time-sampling of the first quantum state gives some desired information or property that it shares with the second quantum state.

Not all quantum computers are gate model quantum computers. Embodiments of the present invention are not limited to being implemented using gate model quantum computers. As an alternative example, embodiments of the present invention may be implemented, in whole or in part, using a quantum computer that is implemented using a quantum annealing architecture, which is an alternative to the gate model quantum computing architecture. More specifically, quantum annealing (QA) is a metaheuristic for finding the global minimum of a given objective function over a given set of candidate solutions (candidate states), by a process using quantum fluctuations.

FIG. 2B shows a diagram illustrating operations typically performed by a computer system 250 which implements quantum annealing. The system 250 includes both a quantum computer 252 and a classical computer 254. Operations shown on the left of the dashed vertical line 256 typically are performed by the quantum computer 252, while operations shown on the right of the dashed vertical line 256 typically are performed by the classical computer 254.

Quantum annealing starts with the classical computer 254 generating an initial Hamiltonian 260 and a final Hamiltonian 262 based on a computational problem 258 to be solved, and providing the initial Hamiltonian 260, the final Hamiltonian 262 and an annealing schedule 270 as input to the quantum computer 252. The quantum computer 252 prepares a well-known initial state 266 (FIG. 2B, operation 264), such as a quantum-mechanical superposition of all possible states (candidate states) with equal weights, based on the initial Hamiltonian 260. The classical computer 254 provides the initial Hamiltonian 260, a final Hamiltonian 262, and an annealing schedule 270 to the quantum computer 252. The quantum computer 252 starts in the initial state 266, and evolves its state according to the annealing schedule 270 following the time-dependent Schrödinger equation, a natural quantum-mechanical evolution of physical systems (FIG. 2B, operation 268). More specifically, the state of the quantum computer 252 undergoes time evolution under a time-dependent Hamiltonian, which starts from the initial Hamiltonian 260 and terminates at the final Hamiltonian 262. If the rate of change of the system Hamiltonian is slow enough, the system stays close to the ground state of the instantaneous Hamiltonian. If the rate of change of the system Hamiltonian is accelerated, the system may leave the ground state temporarily but produce a higher likelihood of concluding in the ground state of the final problem Hamiltonian, i.e., diabatic quantum computation. At the end of the time evolution, the set of qubits on the quantum annealer is in a final state 272, which is expected to be close to the ground state of the classical Ising model that corresponds to the solution to the original optimization problem 258. An experimental demonstration of the success of quantum annealing for random magnets was reported immediately after the initial theoretical proposal.

The final state 272 of the quantum computer 254 is measured, thereby producing results 276 (i.e., measurements) (FIG. 2B, operation 274). The measurement operation 274 may be performed, for example, in any of the ways disclosed herein, such as in any of the ways disclosed herein in connection with the measurement unit 110 in FIG. 1. The classical computer 254 performs postprocessing on the measurement results 276 to produce output 280 representing a solution to the original computational problem 258 (FIG. 2B, operation 278).

As yet another alternative example, embodiments of the present invention may be implemented, in whole or in part, using a quantum computer that is implemented using a one-way quantum computing architecture, also referred to as a measurement-based quantum computing architecture, which is another alternative to the gate model quantum computing architecture. More specifically, the one-way or measurement based quantum computer (MBQC) is a method of quantum computing that first prepares an entangled resource state, usually a cluster state or graph state, then performs single qubit measurements on it. It is “one-way” because the resource state is destroyed by the measurements.

The outcome of each individual measurement is random, but they are related in such a way that the computation always succeeds. In general the choices of basis for later measurements need to depend on the results of earlier measurements, and hence the measurements cannot all be performed at the same time.

Any of the functions disclosed herein may be implemented using means for performing those functions. Such means include, but are not limited to, any of the components disclosed herein, such as the computer-related components described below.

Referring to FIG. 1, a diagram is shown of a system 100 implemented according to one embodiment of the present invention. Referring to FIG. 2A, a flowchart is shown of a method 200 performed by the system 100 of FIG. 1 according to one embodiment of the present invention. The system 100 includes a quantum computer 102. The quantum computer 102 includes a plurality of qubits 104, which may be implemented in any of the ways disclosed herein. There may be any number of qubits 104 in the quantum computer 104. For example, the qubits 104 may include or consist of no more than 2 qubits, no more than 4 qubits, no more than 8 qubits, no more than 16 qubits, no more than 32 qubits, no more than 64 qubits, no more than 128 qubits, no more than 256 qubits, no more than 512 qubits, no more than 1024 qubits, no more than 2048 qubits, no more than 4096 qubits, or no more than 8192 qubits. These are merely examples, in practice there may be any number of qubits 104 in the quantum computer 102.

There may be any number of gates in a quantum circuit. However, in some embodiments the number of gates may be at least proportional to the number of qubits 104 in the quantum computer 102. In some embodiments the gate depth may be no greater than the number of qubits 104 in the quantum computer 102, or no greater than some linear multiple of the number of qubits 104 in the quantum computer 102 (e.g., 2, 3, 4, 5, 6, or 7).

The qubits 104 may be interconnected in any graph pattern. For example, they be connected in a linear chain, a two-dimensional grid, an all-to-all connection, any combination thereof, or any subgraph of any of the preceding.

As will become clear from the description below, although element 102 is referred to herein as a “quantum computer,” this does not imply that all components of the quantum computer 102 leverage quantum phenomena. One or more components of the quantum computer 102 may, for example, be classical (i.e., non-quantum components) components which do not leverage quantum phenomena.

The quantum computer 102 includes a control unit 106, which may include any of a variety of circuitry and/or other machinery for performing the functions disclosed herein. The control unit 106 may, for example, consist entirely of classical components. The control unit 106 generates and provides as output one or more control signals 108 to the qubits 104. The control signals 108 may take any of a variety of forms, such as any kind of electromagnetic signals, such as electrical signals, magnetic signals, optical signals (e.g., laser pulses), or any combination thereof.

For example:

• • In embodiments in which some or all of the qubits 104 are implemented as photons (also referred to as a “quantum optical” implementation) that travel along waveguides, the control unit 106 may be a beam splitter (e.g., a heater or a mirror), the control signals 108 may be signals that control the heater or the rotation of the mirror, the measurement unit 110 may be a photodetector, and the measurement signals 112 may be photons.
  • In embodiments in which some or all of the qubits 104 are implemented as charge type qubits (e.g., transmon, X-mon, G-mon) or flux-type qubits (e.g., flux qubits, capacitively shunted flux qubits) (also referred to as a “circuit quantum electrodynamic” (circuit QED) implementation), the control unit 106 may be a bus resonator activated by a drive, the control signals 108 may be cavity modes, the measurement unit 110 may be a second resonator (e.g., a low-Q resonator), and the measurement signals 112 may be voltages measured from the second resonator using dispersive readout techniques.
  • In embodiments in which some or all of the qubits 104 are implemented as superconducting circuits, the control unit 106 may be a circuit QED-assisted control unit or a direct capacitive coupling control unit or an inductive capacitive coupling control unit, the control signals 108 may be cavity modes, the measurement unit 110 may be a second resonator (e.g., a low-Q resonator), and the measurement signals 112 may be voltages measured from the second resonator using dispersive readout techniques.
  • In embodiments in which some or all of the qubits 104 are implemented as trapped ions (e.g., electronic states of, e.g., magnesium ions), the control unit 106 may be a laser, the control signals 108 may be laser pulses, the measurement unit 110 may be a laser and either a CCD or a photodetector (e.g., a photomultiplier tube), and the measurement signals 112 may be photons.
  • In embodiments in which some or all of the qubits 104 are implemented using nuclear magnetic resonance (NMR) (in which case the qubits may be molecules, e.g., in liquid or solid form), the control unit 106 may be a radio frequency (RF) antenna, the control signals 108 may be RF fields emitted by the RF antenna, the measurement unit 110 may be another RF antenna, and the measurement signals 112 may be RF fields measured by the second RF antenna.
  • In embodiments in which some or all of the qubits 104 are implemented as nitrogen-vacancy centers (NV centers), the control unit 106 may, for example, be a laser, a microwave antenna, or a coil, the control signals 108 may be visible light, a microwave signal, or a constant electromagnetic field, the measurement unit 110 may be a photodetector, and the measurement signals 112 may be photons.
  • In embodiments in which some or all of the qubits 104 are implemented as two-dimensional quasiparticles called “anyons” (also referred to as a “topological quantum computer” implementation), the control unit 106 may be nanowires, the control signals 108 may be local electrical fields or microwave pulses, the measurement unit 110 may be superconducting circuits, and the measurement signals 112 may be voltages.
  • In embodiments in which some or all of the qubits 104 are implemented as semiconducting material (e.g., nanowires), the control unit 106 may be microfabricated gates, the control signals 108 may be RF or microwave signals, the measurement unit 110 may be microfabricated gates, and the measurement signals 112 may be RF or microwave signals.

Although not shown explicitly in FIG. 1 and not required, the measurement unit 110 may provide one or more feedback signals 114 to the control unit 106 based on the measurement signals 112. For example, quantum computers referred to as “one-way quantum computers” or “measurement-based quantum computers” utilize such feedback 114 from the measurement unit 110 to the control unit 106. Such feedback 114 is also necessary for the operation of fault-tolerant quantum computing and error correction.

The control signals 108 may, for example, include one or more state preparation signals which, when received by the qubits 104, cause some or all of the qubits 104 to change their states. Such state preparation signals constitute a quantum circuit also referred to as an “ansatz circuit.” The resulting state of the qubits 104 is referred to herein as an “initial state” or an “ansatz state.” The process of outputting the state preparation signal(s) to cause the qubits 104 to be in their initial state is referred to herein as “state preparation” (FIG. 2A, section 206). A special case of state preparation is “initialization,” also referred to as a “reset operation,” in which the initial state is one in which some or all of the qubits 104 are in the “zero” state i.e. the default single-qubit state. More generally, state preparation may involve using the state preparation signals to cause some or all of the qubits 104 to be in any distribution of desired states. In some embodiments, the control unit 106 may first perform initialization on the qubits 104 and then perform preparation on the qubits 104, by first outputting a first set of state preparation signals to initialize the qubits 104, and by then outputting a second set of state preparation signals to put the qubits 104 partially or entirely into non-zero states.

Another example of control signals 108 that may be output by the control unit 106 and received by the qubits 104 are gate control signals. The control unit 106 may output such gate control signals, thereby applying one or more gates to the qubits 104. Applying a gate to one or more qubits causes the set of qubits to undergo a physical state change which embodies a corresponding logical gate operation (e.g., single-qubit rotation, two-qubit entangling gate or multi-qubit operation) specified by the received gate control signal. As this implies, in response to receiving the gate control signals, the qubits 104 undergo physical transformations which cause the qubits 104 to change state in such a way that the states of the qubits 104, when measured (see below), represent the results of performing logical gate operations specified by the gate control signals. The term “quantum gate,” as used herein, refers to the application of a gate control signal to one or more qubits to cause those qubits to undergo the physical transformations described above and thereby to implement a logical gate operation.

It should be understood that the dividing line between state preparation (and the corresponding state preparation signals) and the application of gates (and the corresponding gate control signals) may be chosen arbitrarily. For example, some or all the components and operations that are illustrated in FIGS. 1 and 2A-2B as elements of “state preparation” may instead be characterized as elements of gate application. Conversely, for example, some or all of the components and operations that are illustrated in FIGS. 1 and 2A-2B as elements of “gate application” may instead be characterized as elements of state preparation. As one particular example, the system and method of FIGS. 1 and 2A-2B may be characterized as solely performing state preparation followed by measurement, without any gate application, where the elements that are described herein as being part of gate application are instead considered to be part of state preparation. Conversely, for example, the system and method of FIGS. 1 and 2A-2B may be characterized as solely performing gate application followed by measurement, without any state preparation, and where the elements that are described herein as being part of state preparation are instead considered to be part of gate application.

The quantum computer 102 also includes a measurement unit 110, which performs one or more measurement operations on the qubits 104 to read out measurement signals 112 (also referred to herein as “measurement results”) from the qubits 104, where the measurement results 112 are signals representing the states of some or all of the qubits 104. In practice, the control unit 106 and the measurement unit 110 may be entirely distinct from each other, or contain some components in common with each other, or be implemented using a single unit (i.e., a single unit may implement both the control unit 106 and the measurement unit 110). For example, a laser unit may be used both to generate the control signals 108 and to provide stimulus (e.g., one or more laser beams) to the qubits 104 to cause the measurement signals 112 to be generated.

In general, the quantum computer 102 may perform various operations described above any number of times. For example, the control unit 106 may generate one or more control signals 108, thereby causing the qubits 104 to perform one or more quantum gate operations. The measurement unit 110 may then perform one or more measurement operations on the qubits 104 to read out a set of one or more measurement signals 112. The measurement unit 110 may repeat such measurement operations on the qubits 104 before the control unit 106 generates additional control signals 108, thereby causing the measurement unit 110 to read out additional measurement signals 112 resulting from the same gate operations that were performed before reading out the previous measurement signals 112. The measurement unit 110 may repeat this process any number of times to generate any number of measurement signals 112 corresponding to the same gate operations. The quantum computer 102 may then aggregate such multiple measurements of the same gate operations in any of a variety of ways.

After the measurement unit 110 has performed one or more measurement operations on the qubits 104 after they have performed one set of gate operations, the control unit 106 may generate one or more additional control signals 108, which may differ from the previous control signals 108, thereby causing the qubits 104 to perform one or more additional quantum gate operations, which may differ from the previous set of quantum gate operations. The process described above may then be repeated, with the measurement unit 110 performing one or more measurement operations on the qubits 104 in their new states (resulting from the most recently-performed gate operations).

In general, the system 100 may implement a plurality of quantum circuits as follows. For each quantum circuit C in the plurality of quantum circuits (FIG. 2A, operation 202), the system 100 performs a plurality of “shots” on the qubits 104. The meaning of a shot will become clear from the description that follows. For each shot S in the plurality of shots (FIG. 2A, operation 204), the system 100 prepares the state of the qubits 104 (FIG. 2A, section 206). More specifically, for each quantum gate G in quantum circuit C (FIG. 2A, operation 210), the system 100 applies quantum gate G to the qubits 104 (FIG. 2A, operations 212 and 214).

Then, for each of the qubits Q 104 (FIG. 2A, operation 216), the system 100 measures the qubit Q to produce measurement output representing a current state of qubit Q (FIG. 2A, operations 218 and 220).

The operations described above are repeated for each shot S (FIG. 2A, operation 222), and circuit C (FIG. 2A, operation 224). As the description above implies, a single “shot” involves preparing the state of the qubits 104 and applying all of the quantum gates in a circuit to the qubits 104 and then measuring the states of the qubits 104; and the system 100 may perform multiple shots for one or more circuits.

Referring to FIG. 3, a diagram is shown of a hybrid classical quantum computer (HQC) 300 implemented according to one embodiment of the present invention. The HQC 300 includes a quantum computer component 102 (which may, for example, be implemented in the manner shown and described in connection with FIG. 1) and a classical computer component 306. The classical computer component may be a machine implemented according to the general computing model established by John Von Neumann, in which programs are written in the form of ordered lists of instructions and stored within a classical (e.g., digital) memory 310 and executed by a classical (e.g., digital) processor 308 of the classical computer. The memory 310 is classical in the sense that it stores data in a storage medium in the form of bits, which have a single definite binary state at any point in time. The bits stored in the memory 310 may, for example, represent a computer program. The classical computer component 304 typically includes a bus 314. The processor 308 may read bits from and write bits to the memory 310 over the bus 314. For example, the processor 308 may read instructions from the computer program in the memory 310, and may optionally receive input data 316 from a source external to the computer 302, such as from a user input device such as a mouse, keyboard, or any other input device. The processor 308 may use instructions that have been read from the memory 310 to perform computations on data read from the memory 310 and/or the input 316, and generate output from those instructions. The processor 308 may store that output back into the memory 310 and/or provide the output externally as output data 318 via an output device, such as a monitor, speaker, or network device.

The quantum computer component 102 may include a plurality of qubits 104, as described above in connection with FIG. 1. A single qubit may represent a one, a zero, or any quantum superposition of those two qubit states. The classical computer component 304 may provide classical state preparation signals Y32 to the quantum computer 102, in response to which the quantum computer 102 may prepare the states of the qubits 104 in any of the ways disclosed herein, such as in any of the ways disclosed in connection with FIGS. 1 and 2A-2B.

Once the qubits 104 have been prepared, the classical processor 308 may provide classical control signals Y34 to the quantum computer 102, in response to which the quantum computer 102 may apply the gate operations specified by the control signals Y32 to the qubits 104, as a result of which the qubits 104 arrive at a final state. The measurement unit 110 in the quantum computer 102 (which may be implemented as described above in connection with FIGS. 1 and 2A-2B) may measure the states of the qubits 104 and produce measurement output Y38 representing the collapse of the states of the qubits 104 into one of their eigenstates. As a result, the measurement output Y38 includes or consists of bits and therefore represents a classical state. The quantum computer 102 provides the measurement output Y38 to the classical processor 308. The classical processor 308 may store data representing the measurement output Y38 and/or data derived therefrom in the classical memory 310.

The steps described above may be repeated any number of times, with what is described above as the final state of the qubits 104 serving as the initial state of the next iteration. In this way, the classical computer 304 and the quantum computer 102 may cooperate as co-processors to perform joint computations as a single computer system.

Although certain functions may be described herein as being performed by a classical computer and other functions may be described herein as being performed by a quantum computer, these are merely examples and do not constitute limitations of the present invention. A subset of the functions which are disclosed herein as being performed by a quantum computer may instead be performed by a classical computer. For example, a classical computer may execute functionality for emulating a quantum computer and provide a subset of the functionality described herein, albeit with functionality limited by the exponential scaling of the simulation. Functions which are disclosed herein as being performed by a classical computer may instead be performed by a quantum computer.

The techniques described above may be implemented, for example, in hardware, in one or more computer programs tangibly stored on one or more computer-readable media, firmware, or any combination thereof, such as solely on a quantum computer, solely on a classical computer, or on a hybrid classical quantum (HQC) computer. The techniques disclosed herein may, for example, be implemented solely on a classical computer, in which the classical computer emulates the quantum computer functions disclosed herein.

The techniques described above may be implemented in one or more computer programs executing on (or executable by) a programmable computer (such as a classical computer, a quantum computer, or an HQC) including any combination of any number of the following: a processor, a storage medium readable and/or writable by the processor (including, for example, volatile and non-volatile memory and/or storage elements), an input device, and an output device. Program code may be applied to input entered using the input device to perform the functions described and to generate output using the output device.

Embodiments of the present invention include features which are only possible and/or feasible to implement with the use of one or more computers, computer processors, and/or other elements of a computer system. Such features are either impossible or impractical to implement mentally and/or manually. For example, embodiments of the present invention use a quantum computer to perform operations on qubits which would be impossible for a human to perform or emulate mentally or manually.

Any claims herein which affirmatively require a computer, a processor, a memory, or similar computer-related elements, are intended to require such elements, and should not be interpreted as if such elements are not present in or required by such claims. Such claims are not intended, and should not be interpreted, to cover methods and/or systems which lack the recited computer-related elements. For example, any method claim herein which recites that the claimed method is performed by a computer, a processor, a memory, and/or similar computer-related element, is intended to, and should only be interpreted to, encompass methods which are performed by the recited computer-related element(s). Such a method claim should not be interpreted, for example, to encompass a method that is performed mentally or by hand (e.g., using pencil and paper). Similarly, any product claim herein which recites that the claimed product includes a computer, a processor, a memory, and/or similar computer-related element, is intended to, and should only be interpreted to, encompass products which include the recited computer-related element(s). Such a product claim should not be interpreted, for example, to encompass a product that does not include the recited computer-related element(s).

In embodiments in which a classical computing component executes a computer program providing any subset of the functionality within the scope of the claims below, the computer program may be implemented in any programming language, such as assembly language, machine language, a high-level procedural programming language, or an object-oriented programming language. The programming language may, for example, be a compiled or interpreted programming language.

Each such computer program may be implemented in a computer program product tangibly embodied in a machine-readable storage device for execution by a computer processor, which may be either a classical processor or a quantum processor. Method steps of the invention may be performed by one or more computer processors executing a program tangibly embodied on a computer-readable medium to perform functions of the invention by operating on input and generating output. Suitable processors include, by way of example, both general and special purpose microprocessors. Generally, the processor receives (reads) instructions and data from a memory (such as a read-only memory and/or a random access memory) and writes (stores) instructions and data to the memory. Storage devices suitable for tangibly embodying computer program instructions and data include, for example, all forms of non-volatile memory, such as semiconductor memory devices, including EPROM, EEPROM, and flash memory devices; magnetic disks such as internal hard disks and removable disks; magneto-optical disks; and CD-ROMs. Any of the foregoing may be supplemented by, or incorporated in, specially-designed ASICs (application-specific integrated circuits) or FPGAs (Field-Programmable Gate Arrays). A classical computer can generally also receive (read) programs and data from, and write (store) programs and data to, a non-transitory computer-readable storage medium such as an internal disk (not shown) or a removable disk. These elements will also be found in a conventional desktop or workstation computer as well as other computers suitable for executing computer programs implementing the methods described herein, which may be used in conjunction with any digital print engine or marking engine, display monitor, or other raster output device capable of producing color or gray scale pixels on paper, film, display screen, or other output medium.

Any data disclosed herein may be implemented, for example, in one or more data structures tangibly stored on a non-transitory computer-readable medium (such as a classical computer-readable medium, a quantum computer-readable medium, or an HQC computer-readable medium). Embodiments of the invention may store such data in such data structure(s) and read such data from such data structure(s).

Claims

1. A method performed by a hybrid quantum-classical computer, the hybrid quantum-classical computer comprising a classical computer and a quantum computer, the method comprising: (A) on the classical computer, transforming an initial problem description of an initial PDE-constrained optimization problem into a transformed problem description of a polynomial unconstrained binary optimization problem in the form of an Ising Hamiltonian;(B) on the hybrid quantum-classical computer, executing computer program instructions to generate an approximate ground state of the Ising Hamiltonian.

2. The method of claim 1, further comprising, after (A) and before (B): (C) on the classical computer, producing the computer program instructions for finding the approximate ground state of the Ising Hamiltonian representing the transformed problem.

3. The method of claim 1, wherein the initial problem description comprises a tensor network.

4. The method of claim 1, wherein the transformed problem description comprises a tensor network.

5. The method of claim 2, wherein producing the computer program instructions comprises producing computer program instructions for applying the quantum approximate optimization algorithm.

6. The method of claim 2, wherein producing the computer program instructions comprises producing computer program instructions for performing quantum annealing.

7. The method of claim 1, wherein the initial PDE-constrained optimization problem is governed by the heat equation.

8. The method of claim 1, wherein the initial PDE-constrained optimization problem is governed by Burger's equation.

9. The method of claim 1, wherein executing the computer program instructions comprises applying the quantum approximate optimization algorithm.

10. The method of claim 1, wherein executing the computer program instructions comprises performing quantum annealing.

11. The method of claim 1, wherein the approximate ground state of the Ising Hamiltonian is the ground state of the Ising Hamiltonian.

12. A system for use with a hybrid quantum-classical computer, the hybrid quantum-classical computer comprising a classical computer and a quantum computer, the classical computer comprising at least one processor and at least one non-transitory computer-readable medium having computer program instructed stored thereon, the computer program instructions being executable by the at least one processor in the classical computer to perform a method, the method comprising: (A) on the classical computer, transforming an initial problem description of an initial PDE-constrained optimization problem into a transformed problem description of a polynomial unconstrained binary optimization problem in the form of an Ising Hamiltonian;(B) on the hybrid quantum-classical computer, executing computer program instructions to generate an approximate ground state of the Ising Hamiltonian.

13. The system of claim 12, wherein the method further comprises, after (A) and before (B): (C) on the classical computer, producing the computer program instructions for finding the approximate ground state of the Ising Hamiltonian representing the transformed problem.

14. The system of claim 12, wherein the initial problem description comprises a tensor network.

15. The system of claim 12, wherein the transformed problem description comprises a tensor network.

16. The system of claim 13, wherein producing the computer program instructions comprises producing computer program instructions for applying the quantum approximate optimization algorithm.

17. The system of claim 13, wherein producing the computer program instructions comprises producing computer program instructions for performing quantum annealing.

18. The system of claim 12, wherein the initial PDE-constrained optimization problem is governed by the heat equation.

19. The system of claim 12, wherein the initial PDE-constrained optimization problem is governed by Burger's equation.

20. The system of claim 12, wherein executing the computer program instructions comprises applying the quantum approximate optimization algorithm.

21. The system of claim 12, wherein executing the computer program instructions comprises performing quantum annealing.

22. The system of claim 12, wherein the approximate ground state of the Ising Hamiltonian is the ground state of the Ising Hamiltonian.