Of Particular Significance

Tag: bottom quarks

At a conference like LHCP12, covering all of Large Hadron Collider [LHC] physics and beyond, there’s far too much to summarize: hundreds of talks, with thousands of incremental experimental results and theoretical insights. So instead, today I’ll draw attention to one of the longest-running puzzles of the LHC era, and to a significant step that’s been made toward resolving it. The puzzle in question involves a rare decay of bottom quarks.

[All figures in this post are taken from LHCP12 talks by Zhangqier Wang and Eluned Smith.]

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Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON June 5, 2024

For the general reader:

Last week I showed you, without any technicalities, how to recognize the elementary forces of nature in the pattern of particle masses and lifetimes. This week we’ll start seeing what we can extract just from the particles’ masses alone… and what we cannot. Today we’ll focus on quarks and the strong nuclear force.

A key factor in nature, which plays an enormous role in everyday life, is the mass of a typical atom. [Note: on this website, “mass” always means “rest mass”, which does not increase with a particle’s speed.] This in turn arises mainly from the masses of protons and neutrons, which are about equal, and tiny: about 0.00000000000000000000000000167 kg (or 0.00000000000000000000000000368 pounds). Since those numbers are crazy-small, physicists use a different measure; we say the mass is about 1 GeV/c2, and more precisely, 0.938 GeV/c2. In any case, it’s tiny on human scales, but it’s some definite quantity, the same for every proton in nature. Where does this mass come from; what natural processes determine it?

You may have heard the simplistic remark that “a proton is made of three quarks” (two up quarks and a down quark), which would suggest these quarks have mass of about 1/3 of a proton, or about 0.313 GeV/c2. But something’s clearly amiss. If you look at websites and other sources about particle physics, they all agree that up and down quark masses are less than 0.01 GeV/c2; these days they usually say the up quark has mass of 0.002 GeV/c2 and the down quark has 0.005 GeV/c2. So if the proton were simply made of three quarks, it would naively have a mass of less than 1% of its actual mass.

What’s going on? A first little clue is that different sources sometimes quote different numbers for the quark masses. There are six types of quarks; from smallest mass to largest, they are up, down, strange (u,d,s, the three light quarks), charm, bottom (c,b, the two somewhat heavy quarks) and top (t, the super-heavy quark.) [Their names, by the way, are historical accidents and don’t mean anything.] But some websites say the up quark mass is 0.003 instead of 0.002 GeV/c2, a 50% discrepancy; the bottom quark’s mass is variously listed as 4.1 GeV/c2, 4.5 GeV/c2, and so forth. This is in contrast to, say, the electron’s mass; you’ll never see websites that disagree about that.

The origin of all these discrepancies is that quarks (and anti-quarks and gluons) are affected by the strong nuclear force, unlike electrons, Higgs bosons, and all the other known elementary particles. The strong forces that quarks undergo make everything about them less clear and certain. Among numerous manifestations, the most dramatic is that quarks (and anti-quarks and gluons) are never observed in isolation. Instead they’re always found in special combinations, called “hadrons“. A proton is an example, but there are many more. And the strong nuclear force can have a big effect on their masses.

The Modern Proton and the Masses of Quarks

A proton, in fact, is not simply made from three quarks, the way a hydrogen atom is simply made from a proton and an electron. As I described in this article, it’s vastly more complex; it’s made from three quarks plus lots of gluons plus lots of pairs of other quarks and anti-quarks. So the simple intuition we get from atoms does not apply to hadrons like the proton.

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Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON July 14, 2022

The HCP [Hadron Collider Physics] 2012 conference in Kyoto is underway.  After opening talks laying out the field’s future, the main topics today have been

  • Collisions of heavy ions (specifically of lead or gold nuclei) and generic proton-proton collisions
  • Processes involving “heavy flavor” (meaning in this case the properties of hadrons containing bottom and charm quarks.)

Although there were a number of interesting new results from several experiments, today’s highlight so far has been a presentation on a new measurement by the LHCb experiment, one of the special-purpose experiments at the Large Hadron Collider [LHC], of a rare decay of a B_s meson to a muon and an antimuon.  I described this process in some detail, and claims and counterclaims about it, in the first portion of an article last year; the details of the measurements are out of date, but the physics process is, of course, the same.

Today the LHCb experiment, for the first time, announced evidence for the existence of this process, using their data collected in both 2011 and 2012.  In the Standard Model (the equations that describe the known particles and forces), it is predicted that about one in about 300,000,000 B_s mesons (hadrons containing a bottom quark and a strange anti-quark, or vice versa) should decay in this fashion.  The measurement that LHCb has made is completely consistent with this prediction.

[In detail, the Standard Model predicts (3.54 ± 0.30) × 10-9 {including mixing effects} and LHCb measures (3.2 +1.5[−1.2])× 10-9.]  The measurement is at the level of 3.5 standard deviations — evidence, but not yet a convincing observation.  LHCb excludes a rate of zero at much better than 95% confidence; their 95% confidence lower bound on the process is 1.1 × 10-9.]

The detailed implications of this result will take a while to work through, but the general implication is easy to state: the Standard Model has survived another test.  And the constraints from LHC data on speculative ideas that predict particles and forces beyond those of the Standard Model have become tighter.  Many variants of these speculative ideas would have affected this process, and the more precisely the data matches the Standard Model prediction, the more of these variants are excluded by the data.

Note Added: CMS says they a very good chance of being able to confirm LHCb’s result using the full 2012 data; not sure what ATLAS says about their chances.

2nd Note Added: Gino Isidori, in his talk on the theoretical perspective on heavy flavor physics, emphasized that a future high-precision measurement of this process will be very important; it can be predicted with high precision, and interesting variants of speculative ideas often have effects on its rate that are between 10% and 100%.

Picture of POSTED BY Matt Strassler

POSTED BY Matt Strassler

ON November 12, 2012

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