Science, culture, complexity

Tag: CP-violation

  • Physicists test if they can load antimatter on a truck

    Physicists in Europe have reported that it’s possible to transport charged particles on a truck for four hours without disturbing them in any way. This seemingly run-of-the-mill announcement, reported in Nature on May 14, actually contains within its details the possibility of “a new era of precision antimatter spectroscopy”, in the team’s words.

    This is because of how the world currently studies antimatter, an elusive form of matter with some properties switched. For example, the electron’s antiparticle is the positron: it has the same mass but behaves like the electron’s mirror image. When a particle touches its antiparticle, they annihilate each other in a flash of energy.

    Physicists study antiparticles for what they can reveal about the still-mysterious things about our universe, such as dark matter. They’re also keen to crack the baryon asymmetry problem, which had a breakthrough reported on July 16.

    The problem is that antimatter is hard to produce in a machine made entirely of matter. What little scientists already know is based on studying antiprotons and atoms of hydrogen and helium made of antiprotons and positrons at the Antimatter Factory (AMF) at CERN, the European nuclear physics research facility more famous for hosting the Large Hadron Collider. Specifically, the problem is that AMF has instruments to study antiparticles but have limited sensitivity. Antimatter particles are also very sensitive to magnetic fields and the AMF hall has other instruments that emit such energy.

    In an ideal world, physicists should be able to produce antiparticles at AMF and transport it to a lab that has very good instruments to study them. The new study delivers a proof of concept showing this is now possible.

    At the heart of their effort is a Penning trap, a device that uses a combination of electric and magnetic fields to confine charged particles in a cylindrical tube. The magnetic field is uniform and flows through the cylinder’s central axis, holding the particles together like a string of beads. The electric field is quadrupole, like two positive and two negative charges forming a square shape with alternating charges at the vertices. This field keeps the particles from drifting away.

    In their truck, the physicists used a BASE-STEP Penning trap, a special kind of trap developed by the BASE collaboration at CERN. It’s a “Penning-trap system inside the bore of a superconducting magnet that can withstand transport-related forces.” Among other features, it uses cold beryllium ions to cool the stored particles and includes precision measurement techniques to study them.

    The team first moved a trap containing a cloud of around 100 protons out of the AMF hall using a pair of overhead cranes, then loaded it on a truck and drove 3.7 km through CERN’s Meyrin campus. They hit a maximum speed of 42.2 km/hr in this run.

    The setup included magnetic shielding and a “transport frame to handle acceleration forces apart from gravity of up to 1 g in all directions”, per the paper. On the truck, the apparatus was cooled by an “internal 30-litre liquid helium tank”. The precision voltage supply, frequency generators, and a spectrum analyser were run by a “UPS with two battery units”.

    In all, the device — 2 m long, 1.6 m tall, and 0.85 m wide — weighed about 900 kg.

    “In our future planned antiproton transport experiments,” the team wrote in its paper, “the last step in the transport campaign would be the extraction of a fraction of particles from the trapped antiproton reservoir, followed by the injection of the extracted fraction into a receiver experiment. Although we do not have such a receiver available yet, we have demonstrated particle separation and extraction after returning to the experiment zone.”

    The reason for going to all this trouble with a truck is an idea in physics called CPT symmetry. The material world is made of matter and all matter is made up of subatomic particles. While physicists know a lot about the material universe, there are still many unknowns and lots of room left for physicists to explore and learn. CPT symmetry is one corner of the room.

    Each letter stands for a kind of transformation. C (charge conjugation) means switching a particle with an antiparticle. P (parity) means switching left and right, like looking in a mirror. And T (time reversal) means reversing the flow of time. In quantum field theory (the tool physicists use to understand the physical properties of subatomic particles), CPT theorem states that if you applied all three operations to a particle, physics should be the same.

    That is to say, if you studied for a physics exam and then someone applied CPT to all particles in the universe, the answers to your question paper wouldn’t change.

    CPT symmetry has a sobering history. At the dawn of quantum field theory, scientists assumed all subatomic particles conserve C, P, and T symmetries separately. Then they found that wasn’t true, so they moved the goalpost and said all particles conserve CP symmetry. An experiment in 1964 challenged this as well when physicists found particles called kaons violated CP symmetry. Finally physicists moved the goalpost even further, saying that all subatomic particles should be expected to conserve CPT symmetry.

    Since the C part of the symmetry requires swapping a particle with its antiparticle, physicists need both matter and antimatter to check if particles obey or violate CPT symmetry. The more the merrier, too: larger quantities of antimatter will make it easier to tease out any subtle effects that might point to a violation. If all such subtlety can be ruled out, CPT symmetry will hold and physicists might breathe easier.

    In the truck study, of course, the physicists only used ~100 protons. “Although the number of stored particles was not pushed to the limit,” they explained, “the transported number would already be enough for our high-precision experiments to operate for several years. As an example, the non-destructive high-precision measurements performed in BASE … typically consume around six antiprotons per year.”

    So far, researchers have verified CPT symmetry conservation in anti-hydrogen (hydrogen atoms made of an antiproton and a positron) and anti-protonic helium (helium atoms with antiprotons). These are of course anti-atoms and are considered a type of particle called baryons.

    Baryons are the most well-known matter particles: they include protons and neutrons as well as all atoms. Your body, for example, is baryonic matter. Physicists are keen to crack the universe’s baryon asymmetry mystery, too — and the answer is expected to have to do with some particles violating CPT symmetry in a hitherto unknown way.

    The physicists wrote in their paper that their findings indicate the “next generation” of antiproton studies could reduce the uncertainty in measurements by a factor of 10 from the “present state of the art”.

    Featured image: Left: The route for the first transport demonstration through the AMF hall. Point 1 is the experiment zone from which an overhead crane moved the transport frame to point 2. At point 2, the transport frame was loaded onto a trailer and moved to point 3, where it then got picked up by the second overhead crane. Point 4 is the loading bay with the truck. Right: Road map of the Meyrin site of CERN and the GPS position data recorded during transportation. Credit: Nature 641, 871–875 (2025).

  • Found: clue to crack the antimatter mystery

    Imagine you’ve put together a torchlight. You know exactly how each part of the device works. You know exactly how they’re all connected togetger. Yet when you put in fresh batteries and turn it on, the light flickers. You take the torchlight apart, check each component piece by piece. It’s all good. The batteries are fully charged as well. Then you put it back together and turn it — and the light flickers still.

    This torchlight is the Standard Model of particle physics. It’s the main theory of its field: it ties together the various properties of all the subatomic particles scientists have found thus far. It organises them into groups, describes how the groups interact with each other, and makes predictions about particles that have been tested to extraordinary precision. And yet, the Standard Model can’t explain what dark matter is, why the Higgs boson is so light or how neutrinos have mass.

    Physicists are thus looking for ‘new physics’: a hitherto unseen part of the torchlight’s internal apparatus that causes its light to flicker, i.e. some new particle or force that completes the Standard Model, closing the gaps that the current crop of particles and forces haven’t been able to.

    This search for new physics received a boost yesterday when the physicists working with one of the detectors of the Large Hadron Collider reported that they had observed CP violations in baryons. This phenomenon is required to explain why the universe has more matter than antimatter today even though it was assumed to have been born with equal quantities of both. Baryons are particles made up of three quarks, like protons and neutrons.

    CP symmetry is the idea that the laws of physics should be the same if you swap all particles with their antiparticles and flip left and right, like looking in a mirror. Thus CP violation in baryons means if swapped a baryon with the corresponding anti-baryon and swapped left and right, the laws of physics won’t be the same, i.e. the laws treat matter and antimatter differently.

    I wrote about this finding and its implications — including its place in the Sakharov conditions and what the results mean for the Standard Model — for The Hindu. Do read it.

    I’ve found it’s one of those things you don’t read because it has anything to say about saving money or living longer. By reminding you that there’s a natural universe out there worth exploring and discovering and that it contains no sign or imprint of the false justifications humans have advanced for their crimes, perhaps it can help you live better. As I’ve said before, if you’re not interested in particle physics, that’s fine. But remember that you can be.

    Featured image: A view of the LHCb detector at the LHC as seen through a fisheye lens. Credit: CERN.

  • Where’s all the antimatter? New CERN results show the way.

    If you look outside your window at the clouds, the stars, the planets, all that you will see is made of matter. However, when the universe was born, there were equal amounts of matter and antimatter. So where has all the antimatter gone?

    The answer, if one is found, will be at the Large Hadron Collider (LHC), the world’s most powerful particle physics experiment, now taking a breather while engineers refit it to make it even more powerful by 2015. Then, it will be able to spot tinier, much more shortlived particles than the Higgs boson, which itself is notoriously shortlived.

    While it ran from 2008 to early 2013, the LHC was incredibly prolific. It smashed together billions of protons in each experiment at speeds close to light’s, breaking them open. Physicists hoped the things that’d tumble out might show why the universe has come to prefer matter over antimatter.

    In fact, from 2013 to 2015, physicists will be occupied gleaning meaningful results from each of these experiments because they simply didn’t have enough time to sift through all of them while the machine was running.

    They will present their results as papers in scientific journals. Each paper will will be the product of analysis conducted on experimental data corresponding to some experiment, each with some energy, some luminosity, and other such experimental parameters central to experimental physics.

    One such paper was submitted to a journal on April 23, 2013, titled ‘First observation of CP violation in the decays of B_s mesons‘. According to this paper, its corresponding experiment was conducted in 2011, when the LHC was smashing away at 7 TeV centre-of-mass (c.o.m) collision energy. This is the energy at the point inside the LHC circuit where two bunches of protons collide.

    The paper also notes that the LHCb detector was used to track the results of the collision. The LHCb is one of seven detectors situated on the LHC’s ring. It has been engineered to study a particle known as the beauty quark, which is more than 4.2 times heavier than a proton, and lasts for about one-hundred-trillionth of a second before breaking down into lighter particles, a process mediated by some of nature’s four fundamental forces.

    The beauty is one of six kinds of quarks, and together with other equally minuscule particles called bosons and leptons, they all make up everything in the universe: from entire galaxies to individual atoms.

    For example, for as long as it lives, the beauty quark can team up with another quark or antiquark, the antimatter counterpart, to form particles called mesons. Generally, mesons are particles composed of one quark and one antiquark.

    Why don’t the quark and antiquark meet and annihilate each other in a flash of energy? Because they’re not of the same type. If a quark of one type and an antiquark of another type meet, they don’t annihilate.

    The B_s meson that the April 23 paper talks about is a meson composed of one beauty antiquark and one strange quark. Thus the notation ‘B_s’: A B-meson with an s component. This meson violates a law of the universe physicists long though unbreakable, called the charge-conjugation/parity (CP) invariance. It states that if you took a particle, inverted its charge (‘+’ to ‘-‘ or ‘-‘ to ‘+’), and then interchanged its left and right, its behaviour shouldn’t change in a universe that conserved charge and parity.

    Physicists, however, found in the 2011 LHCb data that the B_s meson was flouting the CP invariance rule. Because of the beauty antiquark’s and strange quark’s short lifetimes, the B_s meson only lasted for so long before breaking down into lighter particles, in this case called kaons and pions.

    When physicists calculated the kaons‘s and pions‘s charges and compared it to the B_s meson’s, they added up. However, when they calculated the kaons‘s and pions‘s left- and right-handednesses, i.e. parities, in terms of which direction they were spinning in, they found an imbalance.

    A force, called the weak force, was pushing a particle to spin one way instead of the other about 27 per cent of the time. According to the physicists’ paper, this result has been reached with a confidence-level of more than 5-sigma. This means that some reading in the data would disagree with their conclusion not more than 0.00001 per cent of the time, sufficient to claim direct evidence.

    Of course, this wouldn’t be the first time evidence of CP violation in B-mesons had been spotted. On 17 May, 2010B-mesons composed of a beauty antiquark and a down quark were shown shown to decay at a much slower rate than B-antimesons of the same composition, in the process outlasting them. However, this is the first time evidence of this violation has been found in B_s mesons, a particle that has been called “bizarre”.

    While this flies in the face of a natural, intuitive understanding of our universe, it is a happy conclusion because it could explain the aberration that is antimatter’s absence, one that isn’t explained by a theory in physics called the Standard Model.

    Here was something in the universe that was showing some sort of a preference, ready to break the symmetry and uniformity of laws that pervade the space-time continuum.

    Physicists know that the weak force, one of the fundamental forces of nature like gravity is, is the culprit. It has a preference for acting on left-handed particles and right-handed antiparticles. When such a particle shows itself, the weak force offers to mediate its breakdown into lighter particles, in the process resulting in a preference for one set of products over another.

    But in order to fully establish the link between matter’s domination and the weak force’s role in it, physicists have to first figure out why the weak force has such biased preferences.

    This post originally appeared in The Copernican science blog at The Hindu on April 25, 2013.

  • The strong CP problem: We’re just lost

    Unsolved problems in particle physics are just mind-boggling. They usually concern nature at either the smallest or the largest scales, and the smaller the particle whose properties you’re trying to decipher, the closer you are to nature’s most fundamental principles, principles that, in their multitudes, father civilisations, galaxies, and all other kinds of things.

    One of the most intriguing such problems is called the ‘strong CP problem’. It has to do with the strong force, one of nature’s four fundamental forces, and what’s called the CP-violation phenomenon.

    The strong force is responsible for most of the mass of the human body, most of the mass of the chair you’re sitting on, even most of the mass of our Sun and the moon.

    Yes, the Higgs mechanism is the mass-giving mechanism, but it gives mass only to the fundamental particles, and if we were to be weighed by that alone, we’d weigh orders of magnitude lesser. More than 90 per cent of our mass actually comes from the strong nuclear force.

    The relationship between the strong nuclear force and our mass is unclear (this isn’t the problem I’m talking about). It’s the force that holds together quarks, a brand of fundamental particles, to form protons and neutrons. As with all other forces in particle physics, its push-and-pull is understood in terms of a force-carrier particle – a messenger of the force’s will, as it were.

    This messenger is called a gluon, and the behaviour of all gluons is governed by a set of laws that fall under the subject of quantum chromodynamics (QCD).


    Dr. Murray Gell-Mann is an American scientist who contributed significantly to the development of theories of fundamental particles, including QCD

    According to QCD, the farther two gluons get away from each other, the stronger the force between them will get. This is counterintuitive to those who’ve grown up working with Newton’s inverse-square laws, etc. An extension of this principle is that gluons can emit gluons, which is also counter-intuitive and sort of like the weird Banach-Tarski paradox.

    Protons and neutrons belong to a category called hadrons, which are basically heavy particles that are made up of three quarks. When, instead, a quark and an antiquark are held together, another type of hadron called the meson comes into existence. You’d think the particle and its antiparticle would immediately annihilate each other. However, it doesn’t happen so quickly if the quark and antiquark are of different types (also called flavours).

    One kind of meson is the kaon. A kaon comprises one strange quark (or antiquark) and one upantiquark (or quark). Among kaons, there are two kinds, K-short and K-long, whose properties were studied by Orreste Piccioni in 1964. They’re called so because K-long lasts longer than K-short before it decays into a shower of lighter particles, as shown:

    Strange antiquark –> up antiquark + W-plus boson (1)

    W-plus boson –> down antiquark + up quark

    Up quark –> gluon + down quark + down antiquark (2)

    The original other up quark remains as an up quark.

    Whenever a decay results in the formation of a W-plus/W-minus/Z boson, the weak force is said to be involved. Whenever a gluon is seen mediating, the strong nuclear force is said to be involved.

    In the decay shown above, there is one weak-decay (1) and one strong-decay (2). And whenever a weak-decay happens, a strange attitude of nature is revealed: bias.


    Handed spin (the up-down arrows indicate the particle’s momentum)

    The universe may not have a top or a bottom, but it definitely has a left and a right. At the smallest level, these directions are characterised by spinning particles. If a particle is spinning one way, then another particle with the same properties but spinning the other way is said to be the original’s mirror-image. This way, a right and a left orientation are chosen.

    As a conglomeration of such spinning particles, some toward the right and some toward the left, comes together to birth stuff, the stuff will also acquire a handedness with respect to the rest of the universe.

    And where the weak-decay is involved, left and right become swapped; parity gets violated.

    Consider the K-long decay depicted above (1). Because of the energy conservation law, there must be a way to account for all the properties going into and coming out of the decay. This means if something went in left-handed, it must come out left-handed, too. However, the strange antiquark emerges as anup antiquark with its spin mirrored.


    Physicists Tsung-Dao Lee and Chen Ning Yang (Image from the University of Chicago archive)

    As Chen Nin Yang and Tsung-Dao Lee investigated in the 1950s, they found that the weak-decay results in particles whose summed up properties were exactly the same as that of the decaying particle, but in a universe in which left and right had been swapped! In addition, the weak-decay also forced any intervening quarks to change their flavour.


    In the Feynman diagram shown above, a neutron decays into a proton because a down quark is turned into an up quark (The mediating W-minus decays into an electron and an electron antineutrino).

    This is curious behaviour, especially for a force that is considered fundamental, an innate attribute of nature itself. Whatever happened to symmetry, why couldn’t nature maintain the order of things without putting in a twist? Sure, we’re now able to explain how the weak-interaction swaps orientations, but there’s no clue about why it has to happen like that. I mean… why?!

    And now, we come to the strong CP problem(!): The laws governing the weak-interaction, brought under electroweak theory (EWT), are very, very similar to QCD. Why then doesn’t the strong nuclear force violate parity?

    This is also fascinating because of the similarities it bears to nature’s increasing degree of prejudices. Why an asymmetric force like the weak-interaction was born in an otherwise symmetric universe, no one knows, and why only the weak-interaction gets to violate parity, no one knows. Pfft.

    More so, even on the road leading up to this problem, we chanced upon three other problems, and altogether, this provides a good idea of how much humans are lost when it comes to particle physics. It’s evident that we’re only playing catching up, building simulations and then comparing the results to real-life occurrences to prove ourselves right. And just when you ask “Why?”, we’re lost for words.

    Even the Large Hadron Collider (LHC), a multi-billion dollar particle sledgehammer in France-Switzerland, is mostly a “How” machine. It smashes together billions of particles and then, using seven detectors positioned along its length, analyses the debris spewn out.


    An indicative diagram of the layout of detectors on the LHC

    Incidentally, one of the detectors, the LHCb, sifts through the particulate mess to find out how really the weak-interaction affects particle-decay. Specifically, it studies the properties of the B-meson, a kind of meson that has a bottom quark/antiquark (b-quark) as one of its two constituents.

    The b-quark has a tendency to weak-decay into its antiparticle, the b*-quark, in the process getting its left and right switched. Moreover, it has been observed the b*-quark is more likely to decay into the b-quark than it is for the b-quark to decay into the b*-quark. This phenomenon, involved in a process called baryogenesis, was responsible for today’s universe being composed of matter and not antimatter, and the LHCb is tasked with finding out… well, why?

    (This blog post first appeared at The Copernican on December 14, 2012.)