
ASK them to name their heartâs truest desire, and many a science nut might say the answer to life, the universe and everything â or, failing that, a fully functioning lightsaber.
Odd, then, that one field of scientific enquiry that could conceivably provide both gets so little press. After all the hoopla of the past few years, you could be forgiven for believing that understanding matterâs fundamentals is all about the Higgs boson â the âGod particleâ that explains where mass comes from.
The Higgs is undoubtedly important. But it is actually pretty insignificant for real stuff like you and me, accounting for just 1 or 2 per cent of normal matterâs mass. And the huge energy needed to make a Higgs means weâre unlikely to see technology exploiting it any time soon.
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Two more familiar, though less glamorous, particles might offer more. Get to grips with their complexities, and we can begin to explain how the material universe came to exist and persist, and explore mind-boggling technologies: not just lightsabers, but new sorts of lasers and materials to store energy, too. Thatâs easier said than done, granted â but with a lot of computing muscle, it is what we are starting to do.
Chances are you know about protons and neutrons. Collectively known as nucleons, these two particles make up the nucleus, the meaty heart of the atom. (In terms of mass, the weedy electrons that orbit the nucleus are insignificant contributors to the atom.)
The headline difference between protons and neutrons is that protons have a positive electrical charge, whereas neutrons are neutral. But they also differ ever so slightly in mass: in the units that particle physicists use, the neutron weighs in at 939.6 megaelectronvolts (MeV) and the proton at 938.3 MeV.
Thatâs a difference of just 0.14 per cent, but boy does it matter. The neutronsâ extra mass means they decay into protons, not the other way around. Protons team up with negatively charged electrons to form robust, structured, electrically neutral atoms, rather than the world being a featureless neutron gloop.
âThe whole universe would be very different if the proton were heavier than the neutron,â says particle theorist of the University of Southampton in the UK. âThe proton is stable, so atoms are stable and weâre stable.â Our current best guess is that the protonâs half-life, a measure of its stability over time, is at least 1032 years. Given that the universe only has 1010 or so years behind it, that is a convoluted way of saying no one has ever seen a proton decay.
The exact amount of the neutronâs excess baggage matters, too. The simplest atom is hydrogen, which is a single proton plus an orbiting electron. Hydrogen was made in the big bang, before becoming fuel for nuclear fusion in the first stars, which forged most of the other chemical elements. Had the proton-neutron mass difference been just a little bigger, adding more neutrons to make more complex elements would have encountered energy barriers that were âdifficult or impossibleâ to overcome, says of the Massachusetts Institute of Technology. The universe would be stuck at hydrogen.
But had the mass difference been subtly less, hydrogen would have spontaneously changed to the more inert, innocuous helium before stars could form â and the cosmos would have been an equally limp disappointment. Narrow the gap further, and hydrogen atoms would have transformed via a process called inverse beta decay into neutrons and another sort of neutral particle, the neutrino. Bingo, no atoms whatsoever.
All of that leads to an unavoidable conclusion about the proton and neutron masses. âWithout these numbers, people wouldnât exist,â says ZoltĂĄn Fodor of the University of Wuppertal, Germany.
But where do they come from?
The question is fiendishly difficult to answer. Weâve known for half a century that protons and neutrons are not fundamental particles, but made of smaller constituents called quarks. There are six types of quark: up, down, strange, charm, bottom and top. The proton has a composition of up-up-down, while the neutron is up-down-down.
Down quarks are slightly heavier than up quarks, but donât expect that to explain the neutronâs sliver of extra mass: both quark masses are tiny. Itâs hard to tell exactly how tiny, because quarks are never seen singly (see âQuark quirksâ), but the up quark has a mass of something like 2 or 3 MeV, and the down quark maybe double that â just a tiny fraction of the total proton or neutron mass.
Like all fundamental particles, quarks acquire these masses through interactions with the sticky, all-pervasive Higgs field, the thing that makes the Higgs boson. But explaining the mass of matter made of multiple quarks clearly needs something else.
âExplaining the mass of normal matter needs more than the Higgs bosonâ
The answer comes by scaling the sheer cliff face that is quantum chromodynamics, or QCD. Just as particles have an electrical charge that determines their response to the electromagnetic force, quarks carry one of three âcolour chargesâ that explain their interactions via another fundamental force, the strong nuclear force. QCD is the theory behind the strong force, and it is devilishly complex.
Electrically charged particles can bind together by exchanging massless photons. Similarly, colour-charged quarks bind together to form matter such as protons and neutrons by exchanging particles known as gluons. Although gluons have no mass, they do have energy. Whatâs more, thanks to Einsteinâs famous E = mc2, that energy can be converted into a froth of quarks (and their antimatter equivalents) beyond the three normally said to reside in a proton or neutron. According to the uncertainty principle of quantum physics, these extra particles are constantly popping up and disappearing again (see animation below).
To try and make sense of this quantum froth, over the past four decades particle theorists have invented and refined a technique known as lattice QCD. In much the same way that meteorologists and climate scientists attempt to simulate the swirling complexities of Earthâs atmosphere by reducing it to a three-dimensional grid of points spaced kilometres apart, lattice QCD reduces a nucleonâs interior to a lattice of points in a simulated space-time tens of femtometres across. Quarks sit at the vertices of this lattice, while gluons propagate along the edges. By summing up the interactions along all these edges, and seeing how they evolve step-wise in time, you begin to build up a picture of how the nucleon works as a whole.
Trouble is, even with a modest number of lattice points â say 100 by 100 by 100 separated by one-tenth of a femtometre â thatâs an awful lot of interactions, and lattice QCD simulations require a screaming amount of computing power. Complicating things still further, because quantum physics offers no certain outcomes, these simulations must be run thousands of times to arrive at an âaverageâ answer. To work out where the proton and neutron masses come from, Fodor and his colleagues had to harness two IBM Blue Gene supercomputers and two suites of cluster-computing processors.
The breakthrough came in 2008, when they finally arrived at a mass for both nucleons of 936 MeV, give or take 25 MeV â pretty much on the nose (). This confirmed that the interaction energies of quarks and gluons make up the lionâs share of the mass of stuff as we know it. You might feel solid, but in fact youâre 99 per cent energy.
But the calculations were nowhere near precise enough to pin down that all-important difference between the proton and neutron masses, which was still 40 times smaller than the uncertainty in the result. Whatâs more, the calculation suffered from a glaring omission: the effects of electrical charge, which is another source of energy, and therefore mass. All the transient quarks and antiquarks inside the nucleon are electrically charged, giving them a âself-energyâ that makes an additional contribution to their mass. Without taking into account this effect, all bets about quark masses are off. Talk about one compound particle being more massive than another because of a difference in quark masses is a âcrude caricatureâ, says Wilczek, who won a for his part in developing QCD.
The subtle roots of the proton-neutron mass difference lie in solving not just the equations of QCD, but those of quantum electrodynamics (QED), which governs electromagnetic interactions. And that is a theoristâs worst nightmare. âItâs awfully difficult to have QED and QCD in the same framework,â says Fodor. The electromagnetic self-energy canât even be calculated directly. In a limited lattice simulation, its interactions create an infinity â a mathematical effect rather like a never-ending reverberation inside a cathedral.
Fodor and his colleaguesâ new workaround involves solving the QED equations for various combinations of quarks inside different subatomic particles. The resulting subtle differences are used to replace the results of calculations that would invoke infinities, and so grind out a value for the proton-neutron mass difference ().
The figure the team came up with is in agreement with the measured value, although the error on it is still about 20 per cent. It is nonetheless âa milestoneâ, says Sachrajda. Wilczek feels similarly. âI think itâs exciting,â he says. âItâs a demonstration of strength.â
You might be forgiven for wondering what we gain by calculating from first principles numbers we already knew. But quite apart from this particular numberâs existential interest, for Wilczek the excitement lies in our ability now to calculate very basic things about how the universe ticks that we couldnât before.
Take the processes inside huge stars that go supernova â the events that first seeded the universe with elements heavier than hydrogen and helium. Our inability to marry QED and QCD meant we couldnât do much more than wave our hands at questions such as the timescale over which heavy elements first formed â and we couldnât make a star to test our ideas. âConditions are so extreme we canât reproduce them in the laboratory,â says Wilczek. âNow we will be able to calculate them with confidence.â
The advance might help clear up some of the funk surrounding fundamental physics. The Large Hadron Colliderâs discovery in 2012 of the Higgs boson, and nothing else so far, leaves many open questions. Why did matter win out over antimatter just after the big bang (New ĐÓ°ÉÔ´´, 23 May, p 28)? Why do the proton and electron charges mirror each other so perfectly when they are such different particles? âWe need new physics, and simulations like ours can help,â says KĂĄlmĂĄn SzabĂł, one of Fodorâs Wuppertal collaborators. âWe can compare experiment and our precise theory and look for processes that tell us what lies beyond standard physics.â
An open road
For Sachrajda, this kind of computational capability comes at just the right time, as the LHC fires up again to explore particle interactions at even higher energies. âWe all hope it will give an unambiguous signal of something new,â he says. âBut youâre still going to have to understand what the underlying theory is, and for that you will need this kind of precision.â
If that still sounds a little highfalutin, itâs also worth considering how modern technologies have sprung from an ever deeper understanding of matterâs workings. A century or so ago, we were just getting to grips with the atom â an understanding on which innovations such as computers and lasers were built. Then came insights into the atomic nucleus, with all the technological positives and negatives â power stations, cancer therapies, nuclear bombs â those have brought.
Digging down into protons and neutrons means taking things to the next level, and a potentially rich seam to mine. Gluons are far more excitable in their interactions with colour charge than are photons in electromagnetic interactions, so it could be that manipulating colour-charged particles yields vastly more energy than fiddling with things on the atomic scale. âI think the possibility of powerful X-ray or gamma-ray sources exploiting sophisticated nuclear physics is speculative, but not outrageously so,â says Wilczek.

Gluons, unlike photons, also interact with themselves, and this could conceivably see them confining each other into a writhing pillar of energy â hence Wilczekâs tongue-in-cheek suggestion they might make a Star Wars-style lightsaber. More immediate, perhaps, is the prospect of better ways to harness and store energy. âNuclei can pack a lot of energy into a small space,â says Wilczek. âIf we can do really accurate nuclear chemistry by calculation as opposed to having hit-and-miss experiments, it could very well lead to dense energy storage.â
For Fodor, thatâs still a long way off â but with the accuracy that calculations are now reaching, the road is at last open. âThese are mostly dreams today, but now we can accommodate the dreams, at least,â he says. âYouâve reached a level where these technological ideas might be feasible.â
Welcome, indeed, to the quark ages.
Quark quirks
Quarks interact principally by the strong nuclear force. On the subatomic scale, this force is around 100 times stronger than the electromagnetic force that acts on particles with electrical charge â but it is insignificant on larger scales.
Whereas electromagnetism gets weaker when electrically charged particles are further apart, try and pull âcolour chargedâ particles that interact via the strong force apart, and the force between them becomes stronger.
Consequently neither quarks nor gluons â the particles responsible for the interactions of the strong force â can have a stand-alone existence. They only ever appear as part of larger composite particles such as protons and neutrons.
The photon, which transmits the electromagnetic force, has no electrical charge, whereas gluons do have colour charge â so gluons can interact with themselves.
Thereâs only one type of electrical charge, but three types of colour charge: red, green and blue. The quarks within particles can change colour as long as they conserve the overall balance between colours.
Quarks also carry electrical charge â the up quark has a charge of +2/3, the down quark â1/3. But oddly they only ever make up larger particles with zero or whole-number electric charge.
This article appeared in print under the headline âDawn of the quark agesâ
