|
gptkbp:instanceOf
|
Quantum Mechanics Formulation
|
|
gptkbp:alternativeTo
|
gptkb:Wave_Mechanics
|
|
gptkbp:appliesTo
|
Subatomic Particles
Atomic Systems
Quantum Harmonic Oscillator
Spin Systems
|
|
gptkbp:basisFor
|
gptkb:Modern_Quantum_Mechanics
Heisenberg Picture
Operator Formalism
|
|
gptkbp:countryOfPublication
|
gptkb:German
|
|
gptkbp:describes
|
Quantum Systems
|
|
gptkbp:developedBy
|
gptkb:Max_Born
gptkb:Pascual_Jordan
gptkb:Werner_Heisenberg
1925
|
|
gptkbp:equivalentTo
|
gptkb:Wave_Mechanics
|
|
gptkbp:features
|
Discrete Energy Levels
Matrix Representation of Observables
Non-commutative Algebra
Observable Quantities as Operators
Spectral Lines Explanation
Time Evolution via Matrices
Transition Probabilities
|
|
gptkbp:firstFormulationOf
|
Quantum Theory
|
|
gptkbp:form
|
gptkb:Hilbert_Space
gptkb:Linear_Algebra
|
|
gptkbp:hasConcept
|
gptkb:C*-algebra
Non-commuting Observables
Quantization Rules
|
|
gptkbp:historicalName
|
Quantum Revolution
|
|
gptkbp:historicalSignificance
|
First Complete Quantum Theory
|
|
https://www.w3.org/2000/01/rdf-schema#label
|
Matrix Mechanics
|
|
gptkbp:influenced
|
gptkb:quantum_field_theory
gptkb:Modern_Physics
Dirac Notation
|
|
gptkbp:influencedBy
|
Classical Hamiltonian Mechanics
|
|
gptkbp:key
|
"Über quantentheoretische Umdeutung kinematischer und mechanischer Beziehungen"
|
|
gptkbp:mergedInto
|
gptkb:Wave_Mechanics
|
|
gptkbp:notable_for
|
Canonical Quantization
Commutation Relations
Heisenberg Equation of Motion
|
|
gptkbp:notablePublication
|
1925
|
|
gptkbp:publishedIn
|
gptkb:Zeitschrift_für_Physik
|
|
gptkbp:relatedTo
|
gptkb:Heisenberg_Uncertainty_Principle
gptkb:Schrödinger_Equation
|
|
gptkbp:replacedBy
|
Classical Mechanics (at quantum scale)
|
|
gptkbp:uses
|
Matrices
|
|
gptkbp:bfsParent
|
gptkb:Wave_Mechanics
|
|
gptkbp:bfsLayer
|
7
|