Statements (92)
| Predicate | Object |
|---|---|
| gptkbp:instance_of |
gptkb:weapon
gptkb:physicist |
| gptkbp:bfsLayer |
3
|
| gptkbp:bfsParent |
gptkb:ATLAS
gptkb:Higgs_boson gptkb:CMS |
| gptkbp:charging_time |
+1
positive or negative ±1 ±1 e +1 or -1 |
| gptkbp:contributed_to |
gptkb:beta_decay
|
| gptkbp:discovered_by |
gptkb:1983
gptkb:CERN U A1 and U A2 collaborations confirmation of electroweak unification |
| gptkbp:features_character |
gptkb:theorem
nan |
| gptkbp:first_appearance |
gptkb:1983
|
| gptkbp:game_components |
the electroweak interaction
|
| gptkbp:has_spin_off |
gptkb:musical
|
| gptkbp:has_weakness |
gptkb:theorem
|
| https://www.w3.org/2000/01/rdf-schema#label |
W boson
|
| gptkbp:influence |
weak nuclear force
weak force |
| gptkbp:instrumentation |
gptkb:theorem
|
| gptkbp:interacts_with |
quarks and leptons
left-handed fermions |
| gptkbp:involved_forces |
weak force
the weak force |
| gptkbp:is_a_facilitator_of |
weak force interactions
|
| gptkbp:is_associated_with |
the weak interaction
the weak isospin |
| gptkbp:is_fundamental_to |
gptkb:theorem
nan |
| gptkbp:is_involved_in |
gptkb:beta_decay
neutrino interactions charged current interactions change quark flavors |
| gptkbp:is_part_of |
gptkb:Standard_Model
gptkb:the_Standard_Model_of_particle_physics |
| gptkbp:is_recognized_by |
its decay products
|
| gptkbp:is_related_to |
gptkb:Z_boson
the Higgs mechanism |
| gptkbp:is_studied_in |
high-energy physics
|
| gptkbp:isotopes |
is studied in theoretical physics
is essential for understanding fundamental forces is involved in the generation of mass for particles is involved in the creation of matter-antimatter pairs is essential for the understanding of the universe's structure can be absorbed by other particles can be created in high-energy environments can be emitted during particle interactions carries weak charge is a focus of research in particle astrophysics is a key to understanding the Big Bang is detected in neutrino experiments is important for the unification of forces is part of the weak isospin symmetry is produced in the decay of heavy particles is studied in collider experiments mediates interactions between leptons and quarks plays a role in the universe's evolution |
| gptkbp:key |
the electroweak theory
the electroweak unification |
| gptkbp:lifespan |
leptonic and hadronic channels
about 3 x 10^-25 seconds approximately 3 x 10^-25 seconds |
| gptkbp:mass |
80.4 Ge V/c²
80.379 Ge V/c² approximately 80.4 Ge V/c² |
| gptkbp:mode |
gptkb:leptons
gptkb:nebula W+ and W-bosons leptons and quarks |
| gptkbp:named_after |
the weak force
C. N. Yang and R. L. Mills |
| gptkbp:produced_by |
gptkb:beta_decay
high-energy collisions particle accelerators high-energy particle collisions collider experiments the Large Hadron Collider Z bosons in collisions |
| gptkbp:recognizes |
its decay products
|
| gptkbp:related_to |
electroweak theory
|
| gptkbp:responsible_for |
the violation of parity symmetry
|
| gptkbp:roll_rate |
gptkb:musical
|
| gptkbp:symbol |
W⁺ or W⁻
|
| gptkbp:theory |
1970s
|
| gptkbp:type |
gptkb:weapon
|
| gptkbp:year_created |
gptkb:1983
|