|
gptkbp:instance_of
|
gptkb:Physics
|
|
gptkbp:can_detect
|
particle detectors
|
|
gptkbp:charging_time
|
+1 or -1
|
|
gptkbp:components
|
the weak nuclear force
|
|
gptkbp:discovered_by
|
gptkb:1983
|
|
gptkbp:has_a_focus_on
|
particle physics research
|
|
gptkbp:has_a_lifetime
|
3 × 10⁻²⁴ seconds
|
|
gptkbp:has_role
|
electroweak interaction
|
|
https://www.w3.org/2000/01/rdf-schema#label
|
W bosons
|
|
gptkbp:influence
|
weak nuclear force
|
|
gptkbp:interacts_with
|
gptkb:Z_bosons
|
|
gptkbp:is_a_carrier_of
|
weak force interactions
|
|
gptkbp:is_a_fundamental_particle
|
gptkb:true
|
|
gptkbp:is_a_gauge_boson
|
gptkb:true
|
|
gptkbp:is_a_key_component_of
|
the Higgs mechanism
|
|
gptkbp:is_a_subject_of
|
gptkb:quantum_field_theory
|
|
gptkbp:is_a_vector_boson
|
gptkb:true
|
|
gptkbp:is_associated_with
|
weak isospin
|
|
gptkbp:is_characterized_by
|
spin-1
|
|
gptkbp:is_essential_for
|
understanding particle interactions
|
|
gptkbp:is_involved_in
|
gptkb:beta_decay
matter-antimatter asymmetry
neutrino interactions
quark flavor changing processes
|
|
gptkbp:is_part_of
|
gptkb:the_Standard_Model_of_particle_physics
the electroweak force
|
|
gptkbp:is_produced_alongside
|
gptkb:Z_bosons
|
|
gptkbp:is_related_to
|
the weak force coupling constant
|
|
gptkbp:is_studied_for
|
their role in the universe
|
|
gptkbp:is_studied_in
|
high-energy physics
|
|
gptkbp:isotopes
|
carries weak charge
can be detected via decay products
is essential for the Standard Model
is studied in astrophysics
mediates weak interactions
plays a role in particle decay processes
|
|
gptkbp:mass
|
80.379 Ge V/c²
|
|
gptkbp:mode
|
gptkb:Nexon
gptkb:leptons
gptkb:Quark
charged leptons
|
|
gptkbp:named_after
|
gptkb:Wilhelm_Wien
|
|
gptkbp:produced_by
|
LHC experiments
supernova explosions
high-energy particle collisions
electron-positron collisions
collider experiments
|
|
gptkbp:type_of
|
gptkb:quantum_field_theory
|
|
gptkbp:bfsParent
|
gptkb:Higgs_boson
gptkb:top_quark
|
|
gptkbp:bfsLayer
|
5
|