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From the paper titled: In Quantum Mechanics, Everything Happens in a Box: The UPC–QM Bridge zenodo.org/records/20572820
A.1 Detectors Are Classical Devices That Amplify Microscopic Events
Primary Citation
Hadfield, R. H. (2009). Single-photon detectors for optical quantum information applications. Nature Photonics, 3(12), 696–705.
Reveals: Single‑photon detectors are classical devices that convert microscopic absorption events into macroscopic electrical pulses via classical amplification.
Secondary Citation
Eisaman, M. D., Fan, J., Migdall, A., & Polyakov, S. V. (2011). Invited Review Article: Single-photon sources and detectors. Review of Scientific Instruments, 82(7), 071101.
Reveals: Avalanche photodiodes and superconducting nanowire detectors operate through classical avalanche processes and thresholded amplification.
A.2 The Source Pulse Is Consumed; Nothing From It Survives
Primary Citation
Loudon, R. (2000). The Quantum Theory of Light (3rd ed.). Oxford University Press.
Reveals: Photodetection is an absorption process; the incident field is destroyed and does not persist.
Secondary Citation
Mandel, L., & Wolf, E. (1995). Optical Coherence and Quantum Optics. Cambridge University Press.
Reveals: Detection corresponds to the annihilation of the incident field mode; no “photon” survives the interaction.
A.3 “Single Photons” Are Prepared States, Not Objects
Primary Citation
Eisaman, M. D., Fan, J., Migdall, A., & Polyakov, S. V. (2011). Invited Review Article: Single-photon sources and detectors. Review of Scientific Instruments, 82(7), 071101.
Reveals: Single photons are created by attenuation, filtering, gating, and heralding — they are prepared states, not emitted pellets.
Secondary Citation
Grangier, P., Roger, G., & Aspect, A. (1986). Experimental evidence for a photon anticorrelation effect on a beam splitter: A new light on single-photon interferences. Europhysics Letters, 1(4), 173–179.
Reveals: “Single photons” are operationally defined by preparation and detection conditions, not by intrinsic objecthood.
A.4 The Device Stores Settings, Not Particles
Primary Citation
Nielsen, M. A., & Chuang, I. L. (2010). Quantum Computation and Quantum Information. Cambridge University Press.
Reveals: Quantum experiments are defined entirely by the choice of observable, basis, and measurement operators — i.e., the settings.
Secondary Citation
Peres, A. (1995). Quantum Theory: Concepts and Methods. Kluwer Academic Publishers.
Reveals: The apparatus implements operators; it does not store or contain particles.
A.5 Measurement Is a Classical, Irreversible Amplification Event
Primary Citation
Zurek, W. H. (2003). Decoherence, einselection, and the quantum origins of the classical. Reviews of Modern Physics, 75(3), 715–775.
Reveals: Measurement is an irreversible classical amplification process that produces stable macroscopic records.
Secondary Citation
Bohr, N. (1935). Can quantum-mechanical description of physical reality be considered complete? Physical Review, 48(8), 696–702.
Reveals: Bohr emphasizes that measurement outcomes are classical and require amplification to become definite.
A.6 The Wavefunction Is a Model, Not a Physical Wave
Primary Citation
Ballentine, L. E. (1970). The statistical interpretation of quantum mechanics. Reviews of Modern Physics, 42(4), 358–381.
Reveals: The wavefunction is a statistical tool describing ensembles, not a physical wave in space.
Secondary Citation
Fuchs, C. A., & Peres, A. (2000). Quantum theory needs no “interpretation”. Physics Today, 53(3), 70–71.
Reveals: The wavefunction is a calculational device, not an ontological entity.
A.7 The “Photon” Is a Quantized Excitation Defined by Measurement Context
Primary Citation
Mandel, L., & Wolf, E. (1995). Optical Coherence and Quantum Optics. Cambridge University Press.
Reveals: The photon is not a localized particle but a quantized excitation defined by the measurement context.
Secondary Citation
Scully, M. O., & Zubairy, M. S. (1997). Quantum Optics. Cambridge University Press.
Reveals: Photon number states are mathematical constructs tied to specific measurement operators.
A.8 The Detector Output Is Classical and Observer‑Interpreted
Primary Citation
Peres, A. (1995). Quantum Theory: Concepts and Methods. Kluwer Academic Publishers.
Reveals: Measurement outcomes are classical records that require an Observer to interpret them.
Secondary Citation
Wheeler, J. A., & Zurek, W. H. (Eds.). (1983). Quantum Theory and Measurement. Princeton University Press.
Reveals: Measurement is a classical event producing macroscopic information accessible to Observers.
The citations collectively prove:
detectors are classical, amplification is classical, the source pulse is consumed, nothing from the source survives, the device stores settings, not particles, “single photons” are prepared states, the wavefunction is a model, measurement is classical and observer‑indexed.
From the paper titled: In Quantum Mechanics, Everything Happens in a Box: The UPC–QM Bridge zenodo.org/records/20572820
A.1 Detectors Are Classical Devices That Amplify Microscopic Events
Primary Citation
Hadfield, R. H. (2009). Single-photon detectors for optical quantum information applications. Nature Photonics, 3(12), 696–705.
Reveals: Single‑photon detectors are classical devices that convert microscopic absorption events into macroscopic electrical pulses via classical amplification.
Secondary Citation
Eisaman, M. D., Fan, J., Migdall, A., & Polyakov, S. V. (2011). Invited Review Article: Single-photon sources and detectors. Review of Scientific Instruments, 82(7), 071101.
Reveals: Avalanche photodiodes and superconducting nanowire detectors operate through classical avalanche processes and thresholded amplification.
A.2 The Source Pulse Is Consumed; Nothing From It Survives
Primary Citation
Loudon, R. (2000). The Quantum Theory of Light (3rd ed.). Oxford University Press.
Reveals: Photodetection is an absorption process; the incident field is destroyed and does not persist.
Secondary Citation
Mandel, L., & Wolf, E. (1995). Optical Coherence and Quantum Optics. Cambridge University Press.
Reveals: Detection corresponds to the annihilation of the incident field mode; no “photon” survives the interaction.
A.3 “Single Photons” Are Prepared States, Not Objects
Primary Citation
Eisaman, M. D., Fan, J., Migdall, A., & Polyakov, S. V. (2011). Invited Review Article: Single-photon sources and detectors. Review of Scientific Instruments, 82(7), 071101.
Reveals: Single photons are created by attenuation, filtering, gating, and heralding — they are prepared states, not emitted pellets.
Secondary Citation
Grangier, P., Roger, G., & Aspect, A. (1986). Experimental evidence for a photon anticorrelation effect on a beam splitter: A new light on single-photon interferences. Europhysics Letters, 1(4), 173–179.
Reveals: “Single photons” are operationally defined by preparation and detection conditions, not by intrinsic objecthood.
A.4 The Device Stores Settings, Not Particles
Primary Citation
Nielsen, M. A., & Chuang, I. L. (2010). Quantum Computation and Quantum Information. Cambridge University Press.
Reveals: Quantum experiments are defined entirely by the choice of observable, basis, and measurement operators — i.e., the settings.
Secondary Citation
Peres, A. (1995). Quantum Theory: Concepts and Methods. Kluwer Academic Publishers.
Reveals: The apparatus implements operators; it does not store or contain particles.
A.5 Measurement Is a Classical, Irreversible Amplification Event
Primary Citation
Zurek, W. H. (2003). Decoherence, einselection, and the quantum origins of the classical. Reviews of Modern Physics, 75(3), 715–775.
Reveals: Measurement is an irreversible classical amplification process that produces stable macroscopic records.
Secondary Citation
Bohr, N. (1935). Can quantum-mechanical description of physical reality be considered complete? Physical Review, 48(8), 696–702.
Reveals: Bohr emphasizes that measurement outcomes are classical and require amplification to become definite.
A.6 The Wavefunction Is a Model, Not a Physical Wave
Primary Citation
Ballentine, L. E. (1970). The statistical interpretation of quantum mechanics. Reviews of Modern Physics, 42(4), 358–381.
Reveals: The wavefunction is a statistical tool describing ensembles, not a physical wave in space.
Secondary Citation
Fuchs, C. A., & Peres, A. (2000). Quantum theory needs no “interpretation”. Physics Today, 53(3), 70–71.
Reveals: The wavefunction is a calculational device, not an ontological entity.
A.7 The “Photon” Is a Quantized Excitation Defined by Measurement Context
Primary Citation
Mandel, L., & Wolf, E. (1995). Optical Coherence and Quantum Optics. Cambridge University Press.
Reveals: The photon is not a localized particle but a quantized excitation defined by the measurement context.
Secondary Citation
Scully, M. O., & Zubairy, M. S. (1997). Quantum Optics. Cambridge University Press.
Reveals: Photon number states are mathematical constructs tied to specific measurement operators.
A.8 The Detector Output Is Classical and Observer‑Interpreted
Primary Citation
Peres, A. (1995). Quantum Theory: Concepts and Methods. Kluwer Academic Publishers.
Reveals: Measurement outcomes are classical records that require an Observer to interpret them.
Secondary Citation
Wheeler, J. A., & Zurek, W. H. (Eds.). (1983). Quantum Theory and Measurement. Princeton University Press.
Reveals: Measurement is a classical event producing macroscopic information accessible to Observers.
The citations collectively prove:
detectors are classical, amplification is classical, the source pulse is consumed, nothing from the source survives, the device stores settings, not particles, “single photons” are prepared states, the wavefunction is a model, measurement is classical and observer‑indexed.
