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  • 00:00

    The standard model of particle physics,  with its quarks, leptons, and bosons,  

  • 00:04

    has served scientists incredibly well since it was  first put forward in 1967. For the most part, it  

  • 00:11

    has correctly predicted the existence of particles  with such precision that it’s often hailed as the  

  • 00:16

    most successful scientific theory of all time.  

  • 00:21

    And yet scientists are not done with it, and they’re 

  • 00:24

    constantly probing around its edges hunting  for new particles. In fact several teams of  

  • 00:29

    scientists are racing to discover what’s known as  a Majorana fermion, which could be a major key to  

  • 00:35

    settling some of the universe’s biggest mysteries.  

  • 00:40

    Fermions are matter particles like the quarks 

  • 00:42

    that make up protons and neutrons, as well as  electrons and neutrinos. Fermions also include  

  • 00:48

    corresponding antiparticles with very similar  properties except they have opposite charge, so  

  • 00:54

    the antiparticle of a negatively charged electron  has a positive charge and is known as a positron.  

  • 01:00

    Should a particle and its antiparticle meet,  the two will annihilate each other, leaving behind

  • 01:05

    only energy. But a Majorana fermion would  play by its own rules that could totally upend  

  • 01:11

    our understanding of the Standard Model. In theory  a Majorana particle doesn’t have a corresponding  

  • 01:16

    antiparticle; it is its own antiparticle! That  means when two of the same particles meet,  

  • 01:23

    they could wipe each other out. So where would we even begin to look  

  • 01:28

    for a Majorana particle? As it happens  scientists have already identified a candidate  

  • 01:34

    from the Standard Model; the neutrino. Neutrinos  are bizarre little things for more reasons than  

  • 01:39

    just their famous ability to pass right through  whole planets. Unlike electrons and positrons  

  • 01:45

    which both can have right or left-handed  spins, neutrinos all have left-handed spins  

  • 01:51

    while antineutrinos are all right-handed.  To explain this, one idea is that maybe  

  • 01:57

    antineutrinos aren’t antimatter after all, they’re  just all the missing right-handed neutrinos. 

  • 02:04

    Speaking of missing matter, if neutrinos  are Majorana particles they could account  

  • 02:09

    for that too. One of the great mysteries of  the universe is why there’s… well, anything. 

  • 02:15

    There’s no reason we can solidly point to that  explains why there’s more matter than antimatter  

  • 02:20

    today. There’s nothing inherently special  about matter, and it probably formed in equal  

  • 02:25

    amounts with antimatter after the Big Bang. That means by now everything should have been  

  • 02:32

    annihilated, and yet here we are, made up  of and surrounded by regular matter, not  

  • 02:36

    getting spontaneously annihilated all the time.  It’s possible the imbalance is the result of a  

  • 02:43

    particular way some atoms decay. Beta minus decay  is when a neutron in an unstable nucleus decays  

  • 02:50

    into a proton and emits an electron and  antineutrino. An extremely rare event  

  • 02:55

    known as double beta decay occurs when certain  nuclei have two neutrons decay simultaneously. 

  • 03:03

    You see where I’m going with this right? If  a neutrino and an antineutrino are actually  

  • 03:08

    the same particle capable of annihilating  itself, then sometimes double beta  

  • 03:13

    decays will emit only electrons. This net gain of particles could help  

  • 03:19

    account for the imbalance between matter  and antimatter. Of course theorizing about  

  • 03:24

    Majorana particles is one thing, actually  finding evidence of them is quite another. 

  • 03:30

    While neutrinos are notoriously hard  to spot, neutrinoless double beta decay  

  • 03:35

    should be detectable just by adding up the energy  of the resulting two electrons and isotope. 

  • 03:41

    Really the problem lies with luck and timing.  Remember I said double beta decay is rare? Well  

  • 03:47

    a double beta decay where the neutrinos annihilate  each other should be at least 100 times rarer. 

  • 03:54

    That doesn’t mean scientists  aren’t still trying to spot it. 

  • 03:57

    The preferred approach involves getting a huge  amount of an isotope capable of double beta decay  

  • 04:02

    and just… waiting. There are multiple experiments  active and planned using elements like germanium

  • 04:09

    and xenon. They need to keep background  radiation and the energetic movement of atoms  

  • 04:14

    from ruining the data so many of them are shielded  and kept cold, like the CUORE experiment in Italy  

  • 04:20

    which is just 0.01 kelvin above absolute zero. What’s cooler than that? Maybe the fact that  

  • 04:28

    it’s protected by 4 metric tonnes of lead  recovered from a 2,000-year-old Roman shipwreck.  

  • 04:35

    Seriously, the scientists borrowed it from a  museum. If these experiments don’t see signs  

  • 04:40

    of neutrinoless double beta decay, then  maybe it’s even rarer than predicted, and  

  • 04:45

    even bigger tanks of decaying isotopes will be  necessary. Maybe it’s not possible at all and  

  • 04:51

    the Majorana particle is a dead-end. Or, if luck  is on our side, maybe we’ll see the telltale sign  

  • 04:58

    of two neutrinos erasing each other, and the  standard model and our understanding of the  

  • 05:03

    universe will get a little bit more complete.  

  • 05:06

    Fun fact: Majorana Fermions are named for Ettore 

  • 05:09

    Majorana, a physicist who mysteriously disappeared  without a trace in 1938. So about that  

  • 05:17

    whole Standard Model being “The Most Successful  Scientific Theory of All Time”. Turns out a recent  

  • 05:23

    discovery has thrown a wrench in that. Amanda  has muon that here.

  • 05:27

    So, what major mysteries about our universe do you want to see us cover next?

  • 05:31

    Let us know down in the comments. Be sure to subscribe, and I'll see you

  • 05:34

    next time on Seeker.

All

The example sentences of FERMION in videos (4 in total of 5)

scientists noun, plural are verb, non-3rd person singular present racing verb, gerund or present participle to to discover verb, base form what wh-pronoun s proper noun, singular known verb, past participle as preposition or subordinating conjunction a determiner majorana proper noun, singular fermion noun, singular or mass , which wh-determiner could modal be verb, base form a determiner major adjective key adjective to to
either determiner a determiner fermion noun, singular or mass , which wh-determiner is verb, 3rd person singular present a determiner matter noun, singular or mass particle noun, singular or mass , or coordinating conjunction a determiner boson noun, singular or mass , which wh-determiner is verb, 3rd person singular present a determiner force noun, singular or mass particle noun, singular or mass .
we personal pronoun can modal interpret verb, base form fermion verb, base form arrows noun, plural going verb, gerund or present participle forwards adverb in preposition or subordinating conjunction time noun, singular or mass as preposition or subordinating conjunction matter noun, singular or mass particles noun, plural , and coordinating conjunction fermion noun, singular or mass arrows noun, plural
each determiner mirror noun, singular or mass particle noun, singular or mass is verb, 3rd person singular present of preposition or subordinating conjunction the determiner opposite adjective type noun, singular or mass , so preposition or subordinating conjunction each determiner fermion noun, singular or mass has verb, 3rd person singular present a determiner supersymmetric proper noun, singular counterpart noun, singular or mass

Definition and meaning of FERMION

What does "fermion mean?"

/ˈfermēän/

noun
subatomic particle, such as nucleon, which has half-integral spin and follows statistical description given.