The Other Side

Physics expects quantum mechanics and gravity to meet at the Planck scale, 10⁻³⁵ m and 10¹⁹ GeV. In the substrate they meet at every seam, and the real curtain is the 97 μm lattice cell, a few meV, below the energy of visible light.

The familiar picture of everything, redrawn from inside the substrate. Plot every object, as Lineweaver & Patel do ([R269]), in the universe by mass and size and they all fall inside one triangle. On the left is the quantum edge: nothing can be smaller than its own wave, \lambda = \hbar/mc. On the right is the horizon edge: nothing can be denser than its own horizon, r = 2GM/c^2. Across the top is the radius of the visible universe. In the standard picture the two edges meet at the Planck point, 10^{-35} m and 22\;\mug, where quantum mechanics and general relativity are expected to collide in an unknown foam. The substrate reads both edges as one counter-rotating seam. Near resonance it pushes back hard (\alpha_{mf}=0.30, giving \hbar), and between cells it is a near-perfect mirror that leaks only \mathcal F\approx3\times10^{-62} (giving G). The real corner is the lattice cell, 97\;\mum, which cuts the triangle at almost exactly half height. On the quantum edge it sits at dc1, the vacuum’s own 2 meV quantum, whose Compton wavelength is the cell. On the horizon edge it sits at the smallest black hole, about a Moon’s mass. Above the cut is the drape: smooth flow, light at c, and the geometry of general relativity. Below it is the weave, where particles are stitches held by topology. Quantum rules still hold there, but there is no geometry to curve. Below the cut the horizon edge becomes a phantom, and the Planck point is that same cell folded together with gravity’s leak, \ell_\text{Pl}=\xi\sqrt{\mathcal F}. The search for new physics has pushed down the quantum edge toward ever higher energy. The real corner lies the other way, 150 times below the energy of visible light.

The Curtain Everyone Describes

Physics has two great theories, and each works superbly in its own territory. Quantum mechanics governs the very small: atoms, light, the particles in an accelerator. General relativity governs the very heavy: falling apples, orbiting planets, black holes, the expansion of the universe. Each has passed every test it has been given, yet they describe the world in incompatible languages. Quantum mechanics says everything is lumpy and uncertain, and general relativity says space and time form a smooth, exactly determined geometry.

For almost everything, the conflict never comes up. Atoms are too light for their gravity to matter, and planets are too big for their quantum jitter to matter. To force the two theories into the same room you need something both very small and very heavy, and the standard way to find out where that happens is to combine the constants of nature that each theory carries: Planck’s constant \hbar for quantum mechanics, Newton’s G for gravity, and the speed of light c for both. There is exactly one way to make a length, a mass and an energy from these three:

Planck unit Formula Value For scale
Length \ell_\text{Pl} = \sqrt{\hbar G/c^3} 1.6\times10^{-35} m a proton is 10^{20} times larger
Time t_\text{Pl} = \ell_\text{Pl}/c 5.4\times10^{-44} s
Mass M_\text{Pl} = \sqrt{\hbar c/G} 22\;\mug a grain of fine sand
Energy E_\text{Pl} = M_\text{Pl}c^2 1.2\times10^{19} GeV =2\times10^9 J the fuel in a car’s tank, in one particle

The usual story of why this is a curtain runs like a thought experiment with a microscope. To see something small you need a probe with a short wavelength, and a short wavelength costs energy. To resolve 10^{-35} m you would need to pack a Planck energy into a region that size, and general relativity says that much energy in that little space makes a black hole whose horizon is as big as the thing you were trying to see. The microscope swallows its own image. Below the Planck length, the story goes, space and time themselves stop being well defined, and something unknown takes over, which Wheeler called quantum foam.

The curtain is also hopelessly out of reach. The Large Hadron Collider collides protons at 13.6 TeV, about 10^{15} times short of the Planck energy, and the most energetic cosmic ray ever recorded falls short by a factor of about 4\times10^7. Nobody expects to see behind it directly.

This chapter asks what the curtain looks like from inside the substrate. The answer has three parts. The Planck scale is not where the substrate’s grain is; the substrate does have a grain, but it is enormous by comparison and sits at low energy, not high; and the reason the two theories refuse to merge is that they are two faces of one boundary, not two descriptions of the same tiny region.

Two Curtains, Not One

The substrate is a superfluid, and every fluid has a scale below which it stops being a smooth continuum and shows its parts. For water it is the size of a molecule. For the substrate it is the lattice cell, \xi\approx97\;\mum (Lattice Cell Size), about the width of a human hair. Above that size the medium flows smoothly, its sound mode travels at exactly c in every direction, and its flow defines the geometry that general relativity describes (Emergent Speed of Light). Below it, the fluid description ends and you see the weave of the medium: individual cells, each breathing against a counter-rotating partner (The Lattice Breathes in Pairs).

That makes the cell the substrate’s own Planck scale, the place where its emergent spacetime dissolves into microstructure. The idea is not exotic. Volovik worked out the analogous “Planck length” for the phonons of superfluid helium, and it came out at the spacing between helium atoms ([R156]): in a real laboratory fluid, the scale where sound-wave “spacetime” breaks down is simply the size of the fluid’s parts, and nobody would find it by combining constants from the phonon theory alone.

So there are two candidate curtains, and they are in very different places:

The Planck curtain The substrate’s curtain
Length 1.6\times10^{-35} m 97\;\mum, a hair’s width
Energy 1.2\times10^{19} GeV m_1c^2\approx2 meV; light’s floor 13 meV
Frequency \sim10^{43} Hz 3 THz, the far infrared
Relative to us 10^{15} beyond the largest accelerator 150 times below the energy of visible light
Where it comes from combining \hbar, G, c measured: dark-matter density, Weinberg angle, solar wind
What is behind it unknown (“foam”) the weave: paired, breathing cells

The same two curtains on a single ruler, sizes above and probe energies below:

The two are separated by a single number, and that number is the subject of the next section.

The Planck Length, Taken Apart

The gravity chapter writes Newton’s constant in the substrate’s own units. The substrate’s quantum has mass m_1, and if those quanta pulled on each other at full strength, gravity’s constant would be \hbar c/m_1^2. Real gravity is weaker than that by a pure number \mathcal F:

G = \frac{\hbar c}{m_1^2}\,\mathcal F, \qquad \mathcal F \approx 2.8\times10^{-62}.

\mathcal F measures how rarely the substrate leaks through its own boundaries. The counter-rotating layers between cells are nearly perfect mirrors, and about one breath of the cell in 2\times10^{30} lets a quantum through (f_\text{cross}\approx4.4\times10^{-31} per tick; \mathcal F is its square divided by a packing factor of about seven). Gravity is weak because the substrate is clean.

Now put that G into the Planck formulas. Every Planck quantity splits into a substrate quantity times a power of gravity’s weakness:

\boxed{\;\ell_\text{Pl} = \xi\,\sqrt{\mathcal F}, \qquad M_\text{Pl} = \frac{m_1}{\sqrt{\mathcal F}}, \qquad \frac{\xi}{\ell_\text{Pl}} = \frac{M_\text{Pl}}{m_1} = \frac{1}{\sqrt{\mathcal F}} \approx 6\times10^{30}\;}

The Planck length is the lattice cell multiplied by the square root of gravity’s leak fraction. It is not a smaller grain lying underneath the cell. It is what you get when a large, real length is folded together with a very small, real probability, and the result is reported as if it were a length on its own.

Physics has never been able to unfold the two, because it has measured G but not the cell. G arrives as one number with the size and the leak already multiplied together, and the only length you can build from it, \hbar and c is the folded one. The substrate supplies the missing measurement, \xi from the dark-matter density and the electroweak sector (Bridge Equation), and the fold comes apart.

A picture: the draft under the door. Imagine measuring the cold air leaking into a room through a closed door and, not knowing about the door, assuming it came through an open hole in the wall. You would compute the size of the hole that lets that much air through, and you would get something tiny. The hole would be real arithmetic and an imaginary object. The Planck area works the same way. Take one face of a substrate cell, \xi^2\approx9\times10^{-9} m², and ask how big an open hole would pass gravity’s whole leak:

\mathcal F\,\xi^2 = 2.6\times10^{-70}\ \text{m}^2 = \ell_\text{Pl}^2 .

One Planck area is the “equivalent pinhole” in each cell face. It is the right number for that job, and it is why the Planck area appears where gravity counts things (the black-hole entropy is one quarter per Planck area of horizon), but it is not a place you could go and look at. Shrinking a microscope toward 10^{-35} m to find it is like searching the wall for the hole when the air is coming under the door.

The Planck mass is not small. Read the same way, M_\text{Pl} is the mass at which a single object’s gravity would be as strong as its quantum circulation, about 6\times10^{30} substrate quanta packed together. That is 22 micrograms, a grain of sand about a quarter of a millimetre across. (That such a grain happens to be roughly one cell wide is a coincidence of how dense rock is, not physics. It is still a useful picture: the “Planck scale” of mass is something you could hold on a fingertip.)

Where the cell sits. One more way to place the numbers. On a logarithmic ruler running from the Planck length to the radius of the observable universe, c/H_0\approx1.4\times10^{26} m, the cell sits almost exactly halfway: \xi^2\approx4\,\ell_\text{Pl}\,c/H_0 (Gravity § One number, three hats). It is the smallest scale that matters to gravity’s geometry and the largest scale that matters to the substrate’s quanta, and it lands in the middle of the ruler. The framework inherits this long-noticed coincidence rather than explaining it; deriving \mathcal F would explain it.

Why the Two Theories Will Not Merge

The usual program for “quantum gravity” takes general relativity’s geometry and tries to make it quantum, the way electromagnetism was made quantum. Gravity resists. Its strength grows with energy, as (E/E_\text{Pl})^2, and every attempt to compute quantum corrections produces infinities that cannot be absorbed. In the language of the field, general relativity is “non-renormalizable.” Most physicists now read that as a sign that it is an effective theory, a large-scale description of something whose parts it does not know about, much as the equations of fluid flow describe water without mentioning molecules.

The substrate says what the parts are, and it says why quantizing the geometry is the wrong direction.

In the substrate, quantum mechanics and gravity are two coefficients of one physical process: what happens when flow meets a counter-rotating boundary (HVBK Mutual Friction § Gravity — the reactive twin).

  • The quantum face. At the inner scale, where particles live, the boundary sits near resonance and its friction is large, \alpha_{mf}=0.30. That friction is what makes a particle’s boundary layer push back on the flow, and the push-back is the quantum potential, the source of wave behaviour and of \hbar itself (Two Fluids → Quantum Potential).
  • The gravity face. At the outer scale, between cells, the same boundary is deep in its clean limit, nearly a perfect mirror. What trickles through is the slow, one-way leak the framework calls the ebb, and summed over many cells that leak is gravity (Gravity as Boundary-Layer Ebbing).

So the two theories are not two descriptions of the same small region that must be reconciled at the smallest scale. They are the same boundary read at opposite ends of its response curve. On the triangle at the top of this chapter, these are its two edges. Quantum mechanics is the strong, reactive end. Gravity is the weak, leaking end, averaged over enough cells that the leak looks like a smooth geometry.

That changes what “quantizing gravity” would mean. Gravity’s geometry is already made of quantum parts: the cells, the quanta that cross them, and the circulation that comes in units of \hbar. Making the geometry quantum on top of that is like quantizing the flow of a river in order to discover water molecules. You would get sound waves in the river (gravity has those too, the gravitational waves riding the lattice’s collective mode), but not the molecules, because the molecules were never inside the flow equations to begin with. The infinities of quantum gravity are what you get when you push a flow law far below the size of the things that flow. In the substrate, that size is 97\;\mum, which is thirty-one orders of magnitude before the arithmetic reaches the Planck length.

The Microscope That Cannot Swallow Itself

Go back to the thought experiment that put the curtain at the Planck length: concentrate enough energy to probe 10^{-35} m, and you make a black hole that hides it.

In the substrate, a black hole’s horizon is a place where the inflowing ebb outruns the speed of light, the medium’s own sound speed. Both of those are flow speeds, and a flow speed only means something averaged over many cells. A “horizon” smaller than one cell has no inside for the flow to be fast in. The black-holes chapter turns that into a floor: a horizon needs a trapped region at least one cell across, r_s\ge\xi, so

M_\text{min} = \frac{\xi c^2}{2G}\approx6.5\times10^{22}\ \text{kg},

about nine-tenths of the mass of the Moon. Below a lunar mass, the substrate has no black holes at all.

Compare that with the Planck mass, which is the mass whose horizon would be a Planck length across. The ratio between the smallest black hole the substrate allows and the Planck-scale black hole the thought experiment needs is

\frac{M_\text{min}}{M_\text{Pl}} = \frac{\xi}{2\,\ell_\text{Pl}} = \frac{1}{2\sqrt{\mathcal F}} \approx 3\times10^{30},

the same number again. The microscope argument assumed that general relativity’s horizon formula holds at every size. In the substrate it holds only down to the cell, and a Planck-energy collision, two billion joules in one particle, would not make a black hole. It would make what every collision makes: shed light, freed pairs, and showers of particles, the energy spreading out through the medium rather than closing a horizon around itself.

Four Failures, Four Floors

The Planck curtain is really a place where four different calculations break down at once. In each case the substrate stops the calculation at a floor of its own, long before it reaches the Planck scale.

The failure Standard symptom The substrate’s floor Where it bites
Vacuum energy summing zero-point energy to the Planck scale gives 10^{120} times too much energy is counted per cell, not per mode, and the paired part does not weigh (Quantum Foam § The 10^{120}) the cell, 2 meV
Singularities density without limit at the centre of a black hole the logarithmic equation of state has a densest possible state (Black Holes § No singularity) maximal packing
Gravity’s infinities quantum corrections to the geometry diverge the geometry is a flow law, valid only above the cell; below it are solitons, not more geometry the cell, 97\;\mum
The microscope a Planck-energy probe makes a Planck-size black hole a horizon needs at least one cell inside it a lunar mass

None of these floors was introduced to fix the problem it fixes. Each is a property the medium already has for other reasons: the cell sets the speed of light and the photon’s smallest packet, the logarithmic equation of state is what makes the speed of light the same at every density, and the horizon floor is just the statement that a fluid cannot flow inside a space smaller than its parts.

Where the Real Curtain Hangs

If the Planck curtain is a fold of arithmetic, the substrate’s curtain at the cell is the real one: the place where the smooth description ends and the weave begins. And it hangs in a direction most people would not think to look.

The search for new physics has mostly pushed up in energy, to ever larger accelerators, because the Planck curtain points that way. The substrate’s curtain points the other way. Its energy, 13 meV for the smallest packet of light, is about 150 times less than a photon of visible light and about half the thermal energy of everything at room temperature. Its frequency, 3 THz, is in the far infrared, the deep red tail of the glow your own body gives off. It is not beyond the reach of instruments. It is beneath the light we see by.

It has stayed hidden there for three reasons the paper develops elsewhere.

  1. It sits in the terahertz gap. Between about 0.1 and 10 THz, electronics runs out of speed and optics runs out of photon energy. That band was the last part of the spectrum to get good instruments, and they matured only in the last two decades (The Modon Floor § The Substrate Hides in the Terahertz Gap).
  2. The weave cancels itself. Every cell breathes against a partner in exact anti-phase, so on any scale larger than one cell the breathing sums to zero. The vacuum is not quiet because nothing is happening. It is quiet because what happens is perfectly balanced (Quantum Foam § Why you don’t see it; The Stealth Vacuum).
  3. The edge is transparent. Light passes through the cell scale without slowing or dimming. What changes is what carries it: a compact, countable soliton above 3 THz, a single winding spread over many cells below it. An instrument that measures only brightness walks straight across the edge and sees nothing (The Modon Floor § Why the Edge Is Transparent).

This is a big, fuzzy boundary, seen from both sides. It is big, a hair’s width rather than a hundred-billion-billionth of a proton. It is fuzzy because it is a crossover, not a wall: light changes its character there rather than stopping, and the onset of the weave is spread across the terahertz band rather than falling at one sharp line. And it is a boundary in the substrate’s literal sense, the counter-rotating seam between cells whose two faces give us quantum mechanics and gravity.

What Lies on the Other Side

Cross the substrate’s curtain going down in size, and what you find is not a froth of wormholes but the fabric of the medium: cells about 100\;\mum across, paired and breathing at 3\times10^{12} times a second, arranged so evenly that they scatter nothing (Quantum Foam § What It Changes). Smooth geometry, and with it general relativity’s description, belongs to the drape of that fabric over many cells. Inside one cell there is no drape, only weave.

This raises a fair question: if the fabric’s grain is 100\;\mum, how can an electron or a proton be so much smaller? The answer is that particles are not pieces of the fabric’s drape. They are stitches: knots of circulation in the condensate, held together by topology. The electron’s vortex core is about 150 fm across, a billion times smaller than the cell (Substrate Particles § The Three-Tier Hierarchy), and the proton’s junction is smaller still. The rules of quantum mechanics, which come from circulation arriving in whole units of \hbar, hold wherever there is condensate to circulate, so they hold perfectly well inside a cell. What does not exist inside a cell is a smooth geometry for gravity to curve.

That is the substrate’s answer to why quantum mechanics seems to work at every scale we can probe while gravity’s geometry has a breaking point: the stitches can be as small as their topology allows, but the drape has a minimum fold.

Cross the curtain going up in energy from there, toward the Planck scale, and nothing new appears. There is no second grain at 10^{-35} m waiting to be found. The Planck length was the cell all along, seen through a factor of 10^{-31}.

How to Look

Each piece of this picture has a place where it could be caught out.

  • Light at 3 THz. A laboratory terahertz measurement should find a sharp, transparent feature fixed at 3 THz, with an exponential rather than power-law change in how light propagates as the frequency approaches it (The Modon Floor § What the Measurement Should Show). A smooth, featureless terahertz band falsifies the curtain’s location.
  • Forces near 100\;\mum. The Casimir force between plates should bend away from its standard law as the gap approaches the cell (Casimir Effect), and sub-millimetre gravity is the gravitational companion. Torsion-balance experiments have tested Newton’s law down to about 50\;\mum without finding a departure, so whatever happens to gravity at the cell must be small; the framework has not yet calculated how small (see Honest Accounting).
  • No small black holes. No primordial black holes below about a lunar mass, and no Planck-mass remnants, ever (Black Holes § What this rules out). A confirmed asteroid-mass black hole would break the horizon floor.
  • No Planck-scale foam. Searches for foam at the Planck scale, through delayed gamma-ray photons, blurred images of distant quasars, and correlated jitter in interferometers, have all come back empty (Quantum Foam § What the Searches for Foam Have Found). The substrate expects them to keep coming back empty, because there is nothing at 10^{-35} m to find.

Honest Accounting

The fold is exact; the leak behind it is not yet derived. \ell_\text{Pl}=\xi\sqrt{\mathcal F} is an identity once G is written as (\hbar c/m_1^2)\mathcal F, and that form is the only one dimensional analysis allows. What the framework does not have is a derivation of \mathcal F itself. It is measured, through G, and read as a boundary leak; the gravity sector’s one owed number is exactly this one (Gravity; WIP-15). Until it is derived, “the Planck length is the cell seen through gravity’s weakness” is a re-reading of a measured number, not a prediction of it.

The pinhole is a picture, not a mechanism. The leak happens as a rare crossing per breath of the cell, f_\text{cross}\approx4.4\times10^{-31}, not through a literal hole. The equivalent-area reading is offered because it makes the size of the Planck area intuitive and links it to horizon entropy, and it should not be read further than that.

The horizon floor is soft by an order of magnitude or two. Whether a horizon needs one cell inside it or a few tens is not computed, so M_\text{min}\sim10^{23} kg is a scale, not a sharp line (Black Holes). The conclusion that the floor sits about 10^{30} above the Planck mass does not depend on the coefficient.

Gravity below the cell is unquantified. The framework says smooth geometry is a description valid above \xi, and it predicts that sub-millimetre gravity should show the cell. It has not produced the size and shape of that departure to set against the torsion-balance limits, and those limits already reach below 100\;\mum. This is an open item for the sub-millimetre prediction, and until it is closed the gravitational side of the curtain is a direction to look, not a number.

The cell’s place on the ruler is inherited. That \xi sits near the geometric mean of the Planck length and the Hubble radius is a known coincidence that the substrate shares with every dark-energy model at the meV scale. It becomes an explanation only when \mathcal F is derived.

Place in the Framework

The Boundary Energy section follows the substrate’s energy to the places where it can be read with nothing in between: the outer rim in the solar wind, the inner rim in runaway electrons, the modon floor in the terahertz gap. This chapter turns the same lens on the most famous boundary in physics and finds that it is two boundaries. The real one is the cell, at a hair’s width and a few meV, where the medium’s smooth drape gives way to its weave and where the modon floor and the Casimir bend are waiting to be read. The other, at the Planck length, is that same cell folded together with gravity’s leak, \ell_\text{Pl}=\xi\sqrt{\mathcal F}, and nothing physical sits there.

Seen this way, quantum mechanics and general relativity do not meet at some unreachable small scale. They meet at every counter-rotating boundary in the vacuum, as the strong and weak faces of one friction. Physics has been looking for the other side of the curtain at 10^{19} GeV, and the substrate puts it at 13 meV, in the far infrared, below the energy of visible light.