Unpicking the Links Between Knots and Quantum Theory

BLOG: Heidelberg Laureate Forum

Laureates of mathematics and computer science meet the next generation
Heidelberg Laureate Forum

When a researcher collects a Nobel Prize in Physics, Chemistry, or Physiology/Medicine it is often a reward for one astonishing breakthrough or a series of breakthroughs many years before that have had a lasting impact on a field or society. With no Nobel Prize for mathematics, the Fields Medal is one of two awards (alongside the Abel Prize) that carry a similar level of prestige. Yet this award is not given just for outstanding achievements that have already been made. Given that Fields Medals are only handed out to mathematicians under the age of 40, its other purpose is to highlight mathematicians’ potential for making significant contributions in the future.

Undergraduate Promise in Knot Theory

John Pardon, of Stony Brook University in New York, is one of four recipients of this year’s Fields Medal (alongside Yu Deng, Jacob Tsimerman and Hong Wang). The unassuming American already has significant achievements to his name. For instance, his first original contribution to mathematics came when he was a Princeton University undergraduate, where he disproved a 1983 conjecture by renowned geometer Mikhael Gromov (2009 Abel Prize).

John Pardon
2026 Fields Medallist John Pardon. Image: HLFF / Badge

Gromov’s conjecture was to do with knots, a mathematical topic that includes real-world rope knots that we all know; described in three-dimensional (3D) space mathematically as smooth closed curves. Gromov’s work related to a specific property of knots known as a distortion, otherwise known as how tangled a knot is geometrically. He surmised that there must be some universal upper bound on distortion for a class of knots known as torus knots. In other words, there must be a limit to how tangled a torus knot can be, even for the most complex of knots. In work published in 2011, Pardon proved this was not true, finding certain infinitely repeating knot families whose geometric tangling was inherently limitless.

In the intervening years, Pardon has made significant achievements in many highly technical areas. His advances across symplectic geometry particularly have been groundbreaking. However, instead of providing a superficial glimpse into a number of different areas that have piqued Pardon’s interest and his subsequent achievements in them, what is perhaps more insightful is to focus on just one of these interests – knots – and how he is now and might in the future apply his mathematical talents to vexing unsolved problems in this area.

Picking Apart One of Pardon’s Research Interests

Though by all accounts a quiet and reserved mathematician who rarely makes his thoughts known, a strong hint of Pardon’s focus in this area was given in a rare interview for SCGP News shortly after he joined the Simons Center for Geometry and Physics (SCGP) at Stony Brook in 2022. “I’ve always been fascinated by quantum invariants of 3-manifolds arising from Witten’s path integral reformulation of the Jones polynomial based on the Chern–Simons functional,” he said.

Now, that sentence contains a litany of terms – none of which are ‘knot ’ – that need some unpacking. A ‘3-manifold’ is the 3D analogue of a 2D surface of a sphere, torus, or any other surface with more holes. Continuing the 2D analogy, the number of holes of a surface is an example of an invariant: a property of a shape or space that remains the same even when other properties change. A ‘quantum invariant’ can be loosely thought of as invariants constructed using ideas originating in quantum theory.

Digging deeper into the weeds, the ‘Jones polynomial’ is an example of a knot and link (a disjoint union of several knots) invariant. Invented in the 1980s by Sir Vaughan Jones (1990 Fields Medal), it is an algebraic rule that assigns a polynomial equation to any knot/link, acting as a mathematical fingerprint, often distinguishing different knots, although distinct knots can sometimes share the same Jones polynomial.

Vaughan Jones
Sir Vaughan Jones (1990 Fields Medallist), who passed away in 2020. Image: HLFF / Badge

How the ‘Chern–Simons functional’ relates to the Jones polynomial in Pardon’s sentence is far from obvious on face value. This is because Chern–Simons theories are now often regarded as physical quantum field theories that describe how forces and fields behave in a given space; even though they were introduced as mathematical concepts by Shiing-Shen Chern and James Simons (latterly of Simons Foundation fame) in 1974. To make sense of this, a little history might help.

In the late 1980s, theoretical physicist Edward Witten (1990 Fields Medal; the first physicist to receive this honour) started thinking about a problem posed to quantum field theorists by mathematician Sir Michael Atiyah (1966 Fields Medal, 2004 Abel Prize): Why did definitions of the Jones polynomial and its generalizations always involve looking in some way at a 2D projection or slicing of a knot when these objects were inherently 3D invariants? In other words, it didn’t feel right that defining a fundamental property of a 3D object should rely on drawing it in 2D.

Edward Witten
1990 Fields Medallist Edward Witten. Image: HLFF / Badge

Detailed in his seminal 1989 paper, Witten took a unique approach to the problem. Rather than studying knots directly, he considered special observables – known as Wilson loops – associated with knots in Chern–Simons quantum field theory. Using the path integral formalism introduced by Richard Feynman (1965 Nobel Prize in Physics) – a way of averaging together every possible quantum state the field could take – he argued that their expectation values reproduce the Jones polynomial. What Witten had shown was that the Jones polynomial from knot theory was a natural outcome of 3D quantum field theory, where the physical observables are topological invariants of the spacetime in which the theory lives.

The Intersection of Abstract Mathematics and Fundamental Theoretical Physics

So, when Pardon said he was interested in “quantum invariants of 3-manifolds arising from Witten’s path integral reformulation of the Jones polynomial based on the Chern–Simons functional,” one interpretation of this is that he was going to explore how the intrinsic topology of 3D (and higher-dimensional) spaces can be understood through invariants derived from physical theories.

This interest has already borne fruit. Calabi–Yau 3-folds (named after Eugenio Calabi and 1983 Fields Medallist Shing-Tung Yau) are manifolds that crop up in superstring theory as candidates for extra dimensions proposed to be curled up in our universe. Associated with them are slightly more complicated invariants than numbers of holes. This set of ‘curve-counting’ invariants can be thought of as answering how many distinct geometric curves of a given type can fit inside the 6D Calabi–Yau space (though they do not literally count embedded curves).

Shing-Tung Yau
1983 Fields Medallist Shing-Tung Yau. Image: HLFF / Badge

Gromov and Witten proposed a way of counting these curves dynamically derived from string theory using certain invariants, whereas Simon Donaldson (1986 Fields Medal) and Richard Thomas proposed a static method derived from gauge theory using different invariants. In 2023, Pardon established the longstanding MNOP correspondence – proposed by Davesh MaulikNikita NekrasovAndrei Okounkov (2006 Fields Medal), and Rahul Pandharipande in the 2000s – that the two methods are actually equivalent.

Given how the MNOP correspondence is inspired by gauge/string duality, and how long the correspondence remained unproven, it is no surprise then that, as his citation states, Pardon’s MNOP conjecture proof was a key achievement being recognized with the Fields Medal.

What Pardon will do next in this area could have even greater consequences. Expanding curve-counting techniques beyond standard Calabi–Yau spaces to broader classes of manifolds and developing these methods even further to make them highly generalizable would be significant advances. These could deepen mathematical understanding of enumerative geometry, symplectic topology, and quantum field theory, while potentially providing new tools for studying conjectural links between geometry and theoretical physics. With Pardon still only 37, there will hopefully be many years to see what exciting contributions he will make from his unwavering interest in knots and the hidden topology of space.

Avatar photo

Posted by

Benjamin Skuse is a professional freelance writer of all things science. In a previous life, he was an academic, earning a PhD in Applied Mathematics from the University of Edinburgh and MSc in Science Communication. Now based in the West Country, UK, he aims to craft understandable, absorbing and persuasive narratives for all audiences – no matter how complex the subject matter. His work has appeared in New Scientist, Sky & Telescope, BBC Sky at Night Magazine, Physics World and many more.

1 comment

  1. Science is nearing the end of 100 years of „throw Einstein a bone and hope he stays away“.

    Nope. Relativity is everywhere. Dimensions are relative.

    We have one primary dimension, time, where you can only move and can’t help moving in just one direction (how do you call it, a half-dimension?). We have three secondary dimensions spreading at a right angle from the time axis and from each other. We have an infinity of tertiary dimensions, where you can rotate the coordinate cross around the 0 point where the time axis perforates space, painting a sphere in 3D and a hypertube in 4D.

    Make it explode and implode, and you have a common wave. How do I know it does? Gravity: some objects expand faster when the universe explodes and are harder to squeeze when it implodes, giving us the impression of a constant.

    A point has infinite parallel dimensions prolonged into a line. A line has infinite parallel dimensions if you rotate it within a circle. A circle has infinite parallel dimensions within a sphere. You still keep the dots, lines, circles, no matter how many dimensions you add. What does a dot know of spheres?

    Imagine you’re a 2D-being living within a piece of paper. No matter how crumpled the paper is, you perceive it as perfectly flat. You see light as falling frontally into your 2D-eye, no matter if it’s following the wrinkles of the paper or going diagonally right through it like through transparent foil. If someone jams a pencil through it, you only see a circle. But you still need to push all of it if you want to move it.

    Which means, we probably see objects with more than 3 dimensions as mass and measure extra dimensions in kg.

    If you flatten a sphere into a circle, you increase density. Again, you see foreshortening turning dimensions into mass.

    If you move fast enough, two dimensions can collapse into one. You are about to hit a tree with your car, is the tree in your future or is it ahead of you? That’s an Einstein light speed phenomenon far below light speed. How many other dimensions are lumped together in our time-dimension? Is the number of dimensions you live in just dependent on how often you brake? Explosion-implosion, stop and go, braking is part of it.

    If you see two spaceships at the end of rays coming from a common origin but diverging, you can make them appear parallel by increasing the communication speed between both. If you needed 1 second to get from A to B yesterday and 1 second today, the distance between A and B hasn’t changed.

    You can turn parallel courses of two objects into full-fledged secondary dimensions by reducing the travel speed. If you keep slowing down the speed of light between them at exactly the right rate, their radio conversation will tell them, they move apart at 90 degrees.

    We are 2D-beings living within 2D-space, if you look at Earth from space. However, there is a small area where life can exist in 3D. It seems to be a matter of energy – pressure squeezing us and the pressure we build up while we are being squeezed create an equilibrium. We are living within a Goldilocks zone for 3D life.

    We cannot leave it. Either we’ll get crushed (test it with any scrap press, but on scrap, not on yourself), or we explode. Do you have a skin keeping your organs within your body in the 2765th dimension? Do your atoms have one? Almighty Pressure keeps the Universe together.

    If objects get smaller with distance, it’s more than an optical illusion – an archer still has to shoot through a keyhole. What exactly is keeping his arrow from dispersing into many rays to cover the whole area he’s shooting at? Why don’t objects just seem to get bigger and blurred when they move away, as they should in theory – if light would move along straight lines?

    Obviously, it’s not. It’s moving in zigzags, going through invisible lenses. Quantum foam is everywhere, bubbles made of bubbles made of bubbles, it’s around you, around every star, every galaxy.

    Imagine a world where all objects are more or less the same size and the same distance apart. What exactly would be the difference between a star and an atom? The finger you put to your nose and the Andromeda galaxy?

    There are many ways of describing it all. And they might all be true at the same time.

    And we’re still far from dealing with knots. But I need to go now. Due to obligations in a parallel dimension.

Leave a Reply


E-Mail-Benachrichtigung bei weiteren Kommentaren.
-- Auch möglich: Abo ohne Kommentar. +