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various interprettaion Of Qm focusing on pilot wave theory and Many world
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Prashant Bisht
TIFR-Hyderabad
24 April 2025
Quantum mechanics is a theory: The standard model for matter and energy at small scales (photons, atoms, nuclei, quarks, gluons, leptons,... ). Like all theories: Mathematical formalism + interpretation. Unlike other theories: Formalism accepted for 80 years, but interpretation debated. Rival QM interpretations exist, like the 6 blind men’s views.
An interpretation of a formalism should: An interpretation of quantum mechanics is a statement which attempts to explain how QM informs our understanding of nature. Link mathematical symbols to the physical world. Neutralize all paradoxes. Provide tools for visualization or speculation/extension. Not have its own sub-formalism. Not make testable predictions (but may be falsifiable if inconsistent with formalism and experiment).
Experiment : Source emits one photon; wave function passes slits 1 and 2, making interference. Observer’s Choice (after photon passes slits): (a) Measure interference at plane σ 1 (photon travels both slits). (b) Measure at plane σ 2 which slit (photon passes slit 2 only). Paradox : Photon decides wave/particle after passing slits (particle: one slit; wave: both slits). Key Issue : Measurement choice retroactively determines wave/particle nature!
EPR Experiment : Measures correlated polarizations of entangled photons, obeying Malus’ Law: P ( θ rel) = cos^2 θ rel. Result : Same as if photons were in the same state. Furry’s Proposal : Photons in the same random polarization state—gives a weaker correlation. Paradox : Measurement on one photon causes the other’s state to change, even light years apart. FTL Issue : EPR “influence across space-time”—no FTL signaling possible.
Heisenberg’s Uncertainty : Wave-particle duality, conjugate variables (e.g., x and p , E and t ); impossible to measure simultaneously. Born’s Statistical Interpretation : Wave function ψ as probability: P = ψψ ∗; QM predicts only averages. Bohr’s Complementarity : System and apparatus as a whole; wave-particle duality: particle or wave. Heisenberg’s “Knowledge” Interpretation : ψ reflects observer’s knowledge; collapse is non-local knowledge change. Heisenberg’s Positivism : “Don’t-ask/Don’t-tell” on meaning/reality; focus on observables and measurements.
Key Principles There is no “classical realm.” Everything is quantum, including you, the observer. Wave functions never “collapse.” Only smooth, deterministic evolution. Apparent collapse due to entanglement/decoherence. Unobserved possibilities – other “worlds” – still exist.
The cat is in a superposition of |awake⟩ and |asleep⟩, then observed. (Hilbert space = all such superpositions.)
Initial State |cat⟩|observer⟩ = (|awake⟩ + |asleep⟩) |observer⟩
observation/collapse
Final State |cat⟩|observer⟩ = |awake⟩|observer sees awake⟩
|cat⟩|observer⟩ = |asleep⟩|observer sees asleep⟩
Now the cat and the observer are both quantum.Consider environment also. Initial State |cat⟩|observer⟩|env.⟩ = (|awake⟩ + |asleep⟩) |observer⟩|env⟩
Measurement
Decoherence
Everettian QM: Overview, Objections, Questions
Bottom Line: Everettian QM Everettian QM: Wave functions evolve smoothly. No collapse, no measurement, fully deterministic. Entanglement with a messy environment means outcomes never interfere, don’t affect each other—like separate worlds.
Misguided Objections (^1) Too many universes? Hilbert space size is fixed; all QM includes many worlds—you just let them happen. (^2) Untestable? EQM follows Schrödinger; falsifiable via collapse or extra variables (e.g., dynamical collapse, hidden variables).
Open Questions 1 Why probabilities from | ψ |^2? Why probabilities at all in a deterministic theory? 2 Classical world emergence? Why quasiclassical branching? Why spacetime?
Key Idea Subsystems S 1 and S 2 do not have definite states independently due to entanglement in the composite system. There does not exist a single state for one subsystem:
ψS^ ̸= ψS^1 ⊗ ψS^2 (in general)
One can only ask the state relative to a given state of the remainder:
State of S 1 is relative to S 2 , and vice versa
Definition For a chosen state ξk of S 1 , the relative state of S 2 is:
ψ ( S 2 ; rel ξk, S 1 ) = Nk
∑
j
ak,j ηS j^2
where Nk is a normalization constant. The total state can be represented as:
ψS^ =
∑
i
Ni ξi ⊗ ψ ( S 2 ; rel ξi, S 1 )
This relative state uniquely describes S 2 ’s state given S 1 = ξi.