Quantum Nonlinear Oscillator Annealing for Combinatorial Optimization
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Solution Overview
Problem
Current quantum annealing methods for solving combinatorial optimization problems require lengthy execution times, especially when first-order phase transitions occur, leading to exponential increases in required time with problem size.
Innovation Solution
A calculation device and method utilizing quantum nonlinear oscillators coupled by first and second couplers, with a control unit adjusting control parameters and coupling strengths over time to avoid first-order phase transitions, enabling non-stoquastic quantum annealing and reducing the minimum energy gap, thereby shortening execution time.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Loss of time
If quantum annealing is executed using conventional methods, then the quantum state evolves according to standard quantum mechanics, but the execution time becomes excessively long due to first-order phase transitions
Solution Approach 1:
The patent modifies the quantum annealing Hamiltonian by introducing a non-stoquastic term with parameter γ (gamma) that changes the nature of phase transitions. By adjusting the parameter γ in the Hamiltonian H(s) = H₀(s) + γH₁(s), the system transforms first-order phase transitions into second-order phase transitions, thereby reducing execution time while maintaining solution accuracy through controlled parameter evolution
2Measurement precision
If the coupling strength between quantum nonlinear oscillators is increased to improve solution quality, then the minimum energy gap decreases, but the execution time increases exponentially
Solution Approach 1:
The patent employs dynamic control of coupling strengths through time-dependent functions f(s) and g(s) that modulate the interaction between oscillators. The coupling term γg(s)(a_i†a_j + a_i a_j†) allows the system to adapt coupling strength during annealing, maintaining strong coupling when needed for solution quality while reducing it during critical phases to avoid exponential time increases
3Loss of time
If quantum nonlinear oscillators are used to enable non-stoquastic quantum annealing, then first-order phase transitions can be avoided, but the device complexity increases due to additional couplers and control mechanisms
Solution Approach 1:
The patent designs the second coupler to serve multiple functions: it provides non-stoquastic coupling to prevent first-order phase transitions, enables dynamic control of energy gaps, and facilitates adaptive parameter adjustment throughout the annealing process. This multi-functionality reduces the need for separate dedicated components for each control aspect
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
This approach reduces the execution time of quantum annealing by potentially transforming first-order phase transitions into second-order phase transitions, decreasing the time required to solve combinatorial optimization problems from exponential to power function growth.
Implementation Method 1
Quantum annealing using quantum mechanical phenomena has been proposed as one method of solving combinatorial optimization problems
Implementation Method 2
a first coupler that couples the quantum nonlinear oscillators to one another at a coupling strength corresponding to a combinatorial optimization problem
Implementation Method 3
a second coupler that couples the quantum nonlinear oscillators to one another separately from the first coupler
Implementation Method 4
a control means that, in response to a passage of time, controls the control parameter value of the quantum nonlinear oscillators and the coupling strength between the quantum nonlinear oscillators by the second coupler
Implementation Method 5
a measurement device that measures the quantum state represented by the quantum nonlinear oscillators
Data Source
AI summary
A calculation device includes: a plurality of quantum nonlinear oscillators that change a quantum state from one quantum state to one of two quantum states, which differ from the one quantum state, or to a combined state of the two quantum states, according to a change in a control parameter value; a first coupler that couples the quantum nonlinear oscillators to one another at a coupling strength corresponding to a combinatorial optimization problem; a second coupler that couples the quantum nonlinear oscillators to one another separately from the first coupler; a controller that, in response to a passage of time, controls the control parameter value of the quantum nonlinear oscillators and the coupling strength between the quantum nonlinear oscillators by the second coupler; and a measurement device that measures the quantum state represented by the quantum nonlinear oscillators.


