Connections among the papers · Modern synthesis

One pulse, three questions.

What is its quantum energy? What does another observer measure? What changes when a body emits light?

The light-quanta paper does not establish relativity. The September mass–energy argument does not require quanta. This laboratory connects their consequences without turning one paper’s conclusion into another’s hidden premise.

Explore the connections among the papers →

One pulse · Three distinct questions

Follow the energy without confusing the claims

Ideal model, host calculation

This is a modern comparison using the exact modern SI definitions of h and c, not a reconstruction of what was measured in 1905. A programmed consequence is not experimental confirmation.

Predict before changing the observer

Keep the source frequency and pulse energy fixed. Will a receding observer report less energy per quantum, fewer quanta, or both? Compare E/(hν) in the two frames after changing β. No answer is required to continue.

Keep the pulse fixed, or change what was emitted

Accepted settings: ν = 500000000000000 Hz; E = 1 J per pulse; β = 0.6; source-frame angle = 0°. Changing only β changes the observer, not the emitted pulse.

Bookmark these accepted settings

1. Light quanta: an energy scale, not a proof of relativity

In modern notation the quantum energy is hν. Total pulse energy E and frequency ν are independent settings. E/(hν) is shown without rounding: an energy ratio is not an independently measured integer photon count.

Source pulse and quantum-energy comparison
QuantityValueUnit
Frequency in the source frame500000000000000Hz
Pulse energy in the source frame1J
hν in the source frame3.313e-19J
E/(hν) in the source frame3.0184e181

Read the light-quanta argument, §6 · Compare the entropy coefficients

2. Relativity: energy and frequency change together

For the same pulse, the wave owners evaluate ν′/ν and E′/E. Both follow q = γ(1 − β cos θ), so the modern comparison E′/(hν′) equals E/(hν), apart from numerical rounding. This equality compares two computed consequences; it does not independently establish light quanta.

The same pulse in the moving frame
QuantityValueUnit
Frequency transformation factor0.51
Energy transformation factor0.51
Frequency in the moving frame250000000000000Hz
Pulse energy in the moving frame0.5J
hν in the moving frame1.6565e-19J
E′/(hν′) in the moving frame3.0184e181

Read relativity, §8 · Explore the finite light complex

3. Mass–energy: first specify the system

A unidirectional light pulse has zero invariant mass. Its energy divided by c² is not its rest mass. To connect to the September argument, now add a distinct, equal pulse traveling in the opposite direction. Their total source-frame energy is 2E and their momenta cancel.

A pulse versus an equal, opposite two-pulse system
QuantityValueUnit
Pulse energy divided by c² (not its rest mass)1.1127e-17kg
Invariant mass of a unidirectional light pulse0kg
Opposite equal pulse: moving-frame energy2J
Balanced pair: source-frame energy2J
Balanced pair: moving-frame energy2.5J
Balanced pair: invariant mass2.2253e-17kg
Body's mass decrease for balanced emission2.2253e-17kg

For a body initially at rest that emits this balanced pair without recoil, the mass decrease is 2E/c². The displayed system invariant mass is a later interpretation. The historical argument instead compares two energy ledgers and uses the low-speed kinetic-energy premise. It does not require quanta, and we have not assigned the unknown initial body energy E₀ = Mc².

Read the September paper · Follow the two ledgers · Inspect the low-speed coefficient

Model limits and the code behind the numbers

The idealization is a unidirectional, monochromatic vacuum pulse between inertial frames. This does not model finite spectral bandwidth, diffraction, media, gravitational shifts, detector response, or the recoil caused by unbalanced single-pulse emission. The control bounds are numerical admission limits, not claims of physical impossibility.

The frequency and energy factors come from the existing relativistic wave owners. One accepted, instance-scoped snapshot supplies every displayed quantity. No FrankenSim/WASM execution is claimed.

Wave owners · Cross-paper calculation · Snapshot publication