The Lab / Alien Math

Alien Math · Proving Ground · PG-018 to PG-021

Every loophole sends a bill

Black holes made of moving water. A cloak that hides a hard cylinder. A wormhole printed on a flat plate. A mirror that plays sound backwards onto its source. A demon that turns information into work. Each one really does bend a rule. The point of this lab is to find exactly where, and exactly who pays.

0.6917simulated cost of wiping one bit, in kT (Landauer's floor is ln 2 = 0.6931)
−17 dBscattering cut by a 20-layer two-fluid cloak
6×10−6radians between the plate's ray bending and the exact wormhole formula
0.58 λtime-reversal focus through clutter, 3× tighter than clear space

How these were run. Every prediction was written into the card and the script before the run. Misses stay on the page as misses, with the reason. Verdicts are one of three words: supports, undercuts, or inconclusive. Each card has a weak, a medium and a strong form of its claim, and the verdict says which form it is about. Nothing here was built in hardware yet; the home builds are designed and waiting.

PG-018 · break thermodynamics

The demon gets paid, then pays more

A Szilard demon that measures which side a particle is on can extract work from a single heat bath. Information really is fuel. The question is what it costs to forget.

reset time τmean work (kT)÷ ln 2reset success
32.282 ± 0.0333.2999.97%
101.164 ± 0.0181.68100%
300.854 ± 0.0101.23100%
1000.740 ± 0.0061.0799.97%

A 3,000-trajectory Langevin simulation of a bit being reset in a double well. Fitting W = W∞ + B/τ gives W∞ = 0.6917 kT, against Landauer's ln 2 = 0.6931. It approaches the floor from above and never goes under it. A noisy demon extracts exactly ln 2 − H(ε), and after paying for the reset its net is zero at best.

A ratchet at one temperature does not move: drift −0.0003 ± 0.0008. Flash it on and off and it moves, but only while something spends 0.3 to 7.6 kT per unit time doing the flashing.

The trap worth knowing about. The same static test on a sharp sawtooth potential produced a fake drift of 98 standard errors. That was the integrator, not physics: the step-size error alone builds a perpetual motion machine, and it shrinks as the step shrinks. Any "free energy from noise" simulation needs this control. As Seen on TV hit the same bug in its first episode.

supports

Weak form

Information can be turned into work, and noise can be rectified.

undercuts

Medium form

No net cycle from one bath, in either device. 4 of 4 predictions held.

PG-019 · pinch and zoom spacetime

A black hole, a cloak, and a wormhole you can print

Sound that can't get out

Where water flows faster than sound travels in it, sound can't swim upstream. That surface is a horizon, and Unruh showed in 1981 it obeys the same wave equation as a black hole's. Our 1-D simulation reproduces the one-way surface and the redshift.

Simulated sound packets near an acoustic horizon: one escapes slowly while its wavelength stretches, the other drifts inward and never reaches the outside.
Two packets launched just outside and just inside the horizon. The inside one never gets out.

Two of three predictions missed numerically. The redshift rate came out 9.5% low because by the end of the fit window the packet had left the region where the flow is linear; refitting near the horizon (labelled post hoc) gives 2% low. The centroid missed its 0.05 tolerance by 0.01. The bill: the analog Hawking temperature at a surface gravity of 100 per second is 1.2×10−10 K. A bathtub can show the horizon, not the glow. That needs a Bose–Einstein condensate at nanokelvin.

A cloak made of two liquids

A cylindrical cloak built from 20 thin layers of two ordinary fluids cuts the scattering from a hard cylinder by 17 dB at kR = 2, and gets better with more layers (−6.3, −11.4, −17.0, −22.8 dB for 5, 10, 20, 40 layers). All 4 predictions held.

Scattering versus frequency for the bare cylinder and the layered cloak with different numbers of layers.
Scattering cross-section against frequency. The cloak works up to about kR = 8.

The bill comes in materials. The two fluids in the innermost layer must differ in density by 6,722 to 1 at 20 layers, and that ratio grows with the square of the layer count. It is the perfect cloak's impossible inner surface coming back as a shopping list.

The wormhole lens

The Ellis wormhole, a throat joining two universes, bends light the same way a flat plate does if the plate's refractive index is n = 1 + (a/2ρ)2. The ray deflections through that plate match the exact wormhole formula 2K(a/b) − π to 6×10−6 radians, and rays aimed inside the throat vanish into a dark disc of radius exactly a. The derivation is short and is probably already in the transformation-optics literature; we don't claim it.

Ray paths through the wormhole plate: wide rays bend around, rays inside the throat fall toward the centre.
Rays through the index profile. Inside b = a they cross the throat into the other side.

The bill: n goes to infinity at the centre. A 3-D printed pillar plate reaches about n = 1.34, which keeps the lensing for rays with b ≥ 1.15a and loses the throat. One prediction missed: the threshold was estimated by hand at 1.1a, and that estimate was wrong. The site's Wormhole Physics Playground shows the same geometry in 3-D.

supports

Black hole, medium form

Horizon and redshift reproduced; 1 of 3 predictions held, misses explained.

supports

Cloak, medium form

4 of 4 held, with the density contrast as the dominant caveat.

supports

Wormhole lens

3 of 4 held. Lensing yes; the throat is out of reach of simple prints.

PG-020 · the looking glass

Play it backwards and it comes home

Record a pulse on a row of 61 microphones, reverse the recording, and play it back out of the same row. The wave un-scatters and refocuses on the spot where it started. The surprise is what clutter does: through a slab of 170 random scatterers the focus is 3× tighter than through clear space, 7 cells or 0.58 wavelengths, close to the half-wavelength floor. The mess acts as a lens.

Refocused pressure maps for clear space, a cluttered slab, and a lossy cluttered slab.
Refocusing in clear space (left), through clutter (middle), and through lossy clutter (right).

2 of 4 predictions held. Without clutter the focus is a long cigar along the axis, so its brightest point sat 5 cells off the source; the prediction should have been about the transverse position only. And the chosen loss was too weak to cut the contrast by the predicted 30% (it cut 15%). The bill is loss, which is never played back, and the recording itself: only what the 61 elements caught comes home. As Seen on TV asks the related question of whether a Kozyrev mirror focuses anything.

supports

Medium form

Clutter sharpens the refocus beyond the mirror's own aperture. Strong form untested.

PG-021 · phase-shift matter

Teleportation, and the two bits it can't skip

Quantum teleportation moves a qubit's state from one qubit to another with no quantum channel between them at that moment. In a noise-free simulation the fidelity is 1.000; with realistic noise, 0.94 to 0.96, well above the classical limit of 2/3.

The bill is the part people skip. If Bob never hears Alice's two ordinary bits, he holds noise: fidelity 0.496, and none of his measurement statistics depend on the input at all (worst case 1.9 standard errors over 18 probes, against 90.5 for the positive control). Nothing reaches Bob faster than those bits. One entangled pair is used up per qubit moved, and the original is destroyed.

supports

Weak form

The state moves. 4 of 4 simulator predictions held.

undercuts

Strong form

Faster-than-light or matter transport: ruled out by the no-correction run.

A run on real quantum hardware is done and will be added to this page after review.

Infrastructure · WAVE2D

A check that can actually fail

The Foundry's old wave-scattering gate checked an S-matrix that the candidate supplied, so any unitary matrix passed. That gate could never fail on physics, and an audit said so. The replacement computes the S-matrix itself from a real geometry (a hard cylinder in a channel) and cross-examines it with a second, independent calculation.

One pre-registered gate missed: at the largest offset the dip had moved 0.03 away, because an offset cylinder is a different obstacle. The extrapolation that fixes it is labelled post hoc. The unitarity check caught a real phase bug in the first version, which is the best sign that it works.

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Designed, not yet built

Each has its predictions written before it exists.

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