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Optimisers in Quantum Computing: VQE Insights

A look into how optimisers enhance Variational Quantum Eigensolver performance.

Benjamin D. M. Jones, Lana Mineh, Ashley Montanaro

― 7 min read


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In the world of quantum computers, one of the big challenges is figuring out how to find the lowest energy state of a system, especially when that system is something as complicated as the Fermi-Hubbard Model. Imagine trying to find the best spot to pitch a tent in a crowded park; some spots are great, but you might have to check out a lot of places before you find the best one. To help with this, scientists use something called the Variational Quantum Eigensolver (VQE) to simulate these complex systems.

What’s the Fermi-Hubbard Model Anyway?

Let’s break this down. The Fermi-Hubbard model is a fancy way of looking at how particles move and interact in a system. It’s a bit like trying to understand how people move around at a concert while bumping into each other, but with particles. In this model, you have particles (think of them like excited concert-goers) that can hop from one place to another (like finding a new spot to dance) and can also push against each other (because, well, nobody likes a crowd). Scientists study this to discover how these interactions lead to different properties, like conductivity.

Enter the Variational Quantum Eigensolver

Now to the superhero of our story: the Variational Quantum Eigensolver (VQE). This tool helps scientists calculate the lowest energy state of quantum systems. It requires a bit of setup, like preparing an initial state and adjusting parameters until things are just right. Think of it as tuning a guitar; you keep fiddling with the knobs until you get that sweet sound.

But there’s a catch: the process can get tricky because of the randomness of quantum measurements. Sometimes you might not get the results you expect, and it can be hard to trust the numbers. That’s where optimisers come in!

Meet the Optimisers

Optimisers are algorithms-think of them as smart calculators-that help find the best solutions. There are many types of optimisers, and each has its strengths and weaknesses, like having a toolbox with different tools for different jobs. In our study, we looked at 30 different optimisers across a whopping 372 scenarios. That’s a lot of tests!

We ranked these optimisers based on how well they performed, looking at things like energy results and how many attempts they needed to get good answers. The standout performers included variations of Gradient Descent, which is like having a GPS that keeps updating its route to guide you to your destination as quickly as possible.

The Results Are In

So, what did we learn from all this testing? First off, some optimisers did a great job when it came to accuracy. The Momentum and ADAM optimisers were like the top athletes of the bunch, consistently bringing in the best energy results with fewer tries. But there were others, like SPSA and CMAES, that were the real champions when it came to efficiency-using the least calls to find answers.

Interestingly, there was a lot of attention paid to the steps taken by these optimisers. Step sizes in gradient calculations had a massive impact on results. If you’ve ever tried to walk a tightrope, you know that the size of your steps can really change the outcome. It’s the same with these algorithms!

Gradient Analysis: The Easiest Way to Visualise

When optimising, it’s crucial to understand how these steps affect performance. We did a gradient analysis and discovered that using finite differences gives more accurate estimates, but at the cost of making more calls. Think of it like checking several maps to ensure you have the right route versus trusting just one map that might be outdated.

Simultaneous perturbation, inspired by SPSA, is another method that can quickly converge but might not always be as precise in the long run. It’s like rushing to a concert without checking the ticket; you might get in, but you might also miss the best seats!

Quantum Natural Gradient Algorithm: A New Challenger

We also tackled the quantum natural gradient algorithm, implemented specifically for one-dimensional Fermi-Hubbard systems. It turned out to have some impressive capabilities, but when we factored in the total function calls needed, the edges in performance often disappeared. It's a bit like finding out that the fastest car also uses twice as much gas!

Hyperparameter Tuning: Fine-tuning the Process

To find the best results, we carefully adjusted Hyperparameters for our tests. This is like making sure you're wearing the right shoes for a hike-too tight, and you're uncomfortable; too loose, and you might trip. For our purposes, a step size of about 0.4 worked well, proving crucial to getting the best results.

The Importance of Optimiser Selection

Choosing the right optimiser can dramatically change the outcomes. In our study, we noted that the best-performing optimisers varied from those that delivered excellent energy accuracy to those that worked well with fewer calls. For final accuracy, we found that Momentum or ADAM with finite differences really shone. But when it came to using fewer calls, SPSA, CMAES, or BayesMGD proved to be champions.

In short, it’s important to weigh the trade-offs between getting precise results versus using fewer calls when implementing these algorithms.

Future Directions and Extensions

There’s a ton of potential for expanding this work. Other models, like the Transverse Field Ising model, are waiting in the wings for exploration. We know that the performance of optimisers could vary between different systems, so it’ll be exciting to see which ones rise to the occasion.

Different ansätze (a fancy term for templates or forms in mathematical optimization) also hold promise. The Hamiltonian variational ansatz we used is neat because it doesn’t require a lot of parameters. However, we could try more expressive ansätze that might yield better results but come with a trade-off of increased complexity.

Multi-stage Approaches: Taking it to the Next Level

One creative strategy would be to adopt multi-stage approaches where we start with simpler problems and gradually increase complexity. It’s a bit like climbing a mountain: you wouldn’t start at the peak! By beginning with a few parameters and gradually adding more, or switching up the optimiser halfway through, we could potentially get the best of both worlds.

Wrapping Up

So what's the takeaway from our deep dive into the optimisation world? Selecting the right optimiser can make a big difference in the effectiveness of the variational quantum eigensolver. The performance of different algorithms varies widely, just like how people each have their preferred tactics at a buffet line-some zoom right to the desserts, while others carefully pick healthy options first.

In the complex universe of quantum computing, exploring these optimisers is like finding the right tools for a home renovation. With the right optimisers in hand, we can better understand quantum systems and unlock even deeper insights into their behavior (without losing our sanity along the way).

And while we’ve made strides in comparing these optimisers, the journey is far from over. There’s plenty more to investigate, and as research continues, we’re bound to uncover even better approaches to tackle the challenges posed by quantum mechanics.

Let’s Keep the Momentum Going

Our exploration of VQE and the Fermi-Hubbard model shows not just the power of quantum computing but the endless possibilities that lie ahead. Like a concert that keeps going with more surprises (and maybe a surprise guest), the world of quantum algorithms has plenty in store for those willing to tackle its complexities. Who knows? Perhaps the next optimiser will just be around the corner, waiting to steal the show!

Original Source

Title: Benchmarking a wide range of optimisers for solving the Fermi-Hubbard model using the variational quantum eigensolver

Abstract: We numerically benchmark 30 optimisers on 372 instances of the variational quantum eigensolver for solving the Fermi-Hubbard system with the Hamiltonian variational ansatz. We rank the optimisers with respect to metrics such as final energy achieved and function calls needed to get within a certain tolerance level, and find that the best performing optimisers are variants of gradient descent such as Momentum and ADAM (using finite difference), SPSA, CMAES, and BayesMGD. We also perform gradient analysis and observe that the step size for finite difference has a very significant impact. We also consider using simultaneous perturbation (inspired by SPSA) as a gradient subroutine: here finite difference can lead to a more precise estimate of the ground state but uses more calls, whereas simultaneous perturbation can converge quicker but may be less precise in the later stages. Finally, we also study the quantum natural gradient algorithm: we implement this method for 1-dimensional Fermi-Hubbard systems, and find that whilst it can reach a lower energy with fewer iterations, this improvement is typically lost when taking total function calls into account. Our method involves performing careful hyperparameter sweeping on 4 instances. We present a variety of analysis and figures, detailed optimiser notes, and discuss future directions.

Authors: Benjamin D. M. Jones, Lana Mineh, Ashley Montanaro

Last Update: 2024-11-20 00:00:00

Language: English

Source URL: https://arxiv.org/abs/2411.13742

Source PDF: https://arxiv.org/pdf/2411.13742

Licence: https://creativecommons.org/licenses/by/4.0/

Changes: This summary was created with assistance from AI and may have inaccuracies. For accurate information, please refer to the original source documents linked here.

Thank you to arxiv for use of its open access interoperability.

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