Importance of choosing a convenient form of the state (normalized state).
Photons and States of Light
Light states can be represented by polarization states.
Example: Two types of photons -
Polarized along the x-axis (state X).
Polarized along the y-axis (state Y).
General photon state:
Expressed as: |ψ⟩ = α|X⟩ + β|Y⟩
Parameters: Has 2 complex parameters (α, β), equating to 4 real parameters.
The overall coefficient doesn’t matter, allowing simplification to:
|ψ⟩ = (β/α)|Y⟩
Results in 1 complex parameter (γ = β/α), thus the most general state is characterized by just 2 real parameters (shape of ellipse).
Elliptical Polarization
The most general state of polarization of a wave is elliptical polarization.
Key characteristics:
Two Parameters:
Ratio of semi-major axes (a/b).
Angle θ of the ellipse.
Size is not a parameter; it depends on the magnitude of the electric field.
Spin in Quantum Mechanics
Spin: Intrinsic angular momentum of elementary particles.
Measured in specific directions, e.g., z-direction yielding:
Spin Up: |↑⟩
Spin Down: |↓⟩
Superposition of spin states:
Example: |↑⟩ + |↓⟩.
Normalization factor may apply when calculating probabilities.
Measurement and Probability in Spin States
Measuring spin in z-direction on 1000 particles results in:
Approximately 50% up and 50% down when measured multiple times.
Einstein’s critique of quantum superposition:
Suggests realism: If spin is measured as up, it was up before measurement.
Distinguishing Ensembles of States
Quantum state ensemble vs. classical ensemble (50% up, 50% down):
When measuring along x-direction:
Quantum state ensemble: All pointing up along x.
Classical ensemble: 50% up, 50% down along x.
The ability to distinguish these states can indicate the existence of quantum states.
Conclusion
The discussion of superpositions and spins emphasizes the non-classical nature of quantum mechanics, the roles of assumptions, and implications for measurement and observation.