**The weighty issue of quarks**

Electrons make circular tracks when they move perpendicular to a magnetic field in a particle detector. From the radius of the circle, knowing the electric charge, we can determine the electron mass. Quarks, on the other hand, are never seen as free particles. Instead, all we see in our particle detectors are the bound states of quarks, called hadrons. We can measure hadron masses, but how do we then determine, or even define, the mass of a quark?

The answer is that we must define the mass as the parameter that enters the equations of QCD, the theory of the strong interaction that binds quarks into hadrons. We can solve the equations of QCD using the numerical approach of lattice QCD and hence determine the quark mass parameter that we need to put into the theory to give the correct mass for a calibration hadron containing that quark. Since experimentalists can measure some hadron masses very well, we can do this accurately. For example, to fix the charm quark mass, m_{c}, we use the mass of the η_{c} (pictured in Figure 1).

To be of use to other theorists, however, we must convert the lattice quark mass into that appropriate to QCD defined in continuous space-time. We must do this accurately too, to avoid introducing a sizeable uncertainty into the result.

HPQCD developed one of the main techniques used to determine quark masses (the JJ method) and most recently used this, on DiRAC, to determine m_{c} to 1% in 2014 (arXiv:1408.4169). This year we used a completely different technique (called RI-SMOM) to ‘match’ our lattice quark mass to that of continuum QCD, directly on the lattice (arXiv:1805.06225). We were careful to quantify and remove lattice artefacts, which had been ignored in previous calculations. Our new 1% accurate result agrees very well with our 2014 value and also with a third, MRS, method developed by FNAL/MILC/TUM in 2018. This gives a world-average for m_{c} of 1.2753(65) GeV (1.36 times the mass of the proton). The quark masses need to be accurately known so that we can test whether the newly-discovered Higgs boson is behaving as we expect when it decays to hadrons via quark-antiquark pairs of different flavours.