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Arithmetic Anyons: The Bounded-Occupation Family, Gentile Statistics, and the Roots of Unity That Carry Braid Phases
In the paper's words
Three spatial dimensions admit exactly two exchange statistics for identical particles, and a recent record reads the two occupation distributions as maximum-entropy occupations of one integer lattice under two multiplicity rules, closing with an open correspondence: the bounded-occupation family interpolates between the fermionic and bosonic cases and is proposed as the arithmetic object that intermediate (anyonic) statistics must contact. This paper settles the correspondence computationally. The family is the partition function of Gentile intermediate statistics - an occupation cap per mode - and it carries no exchange phase for any cap: permuting occupation labels yields only the signs +1 and -1, every observable is invariant under any inserted phase, and the canonical symmetric reading assigns the phase +1 for every cap, including the cap that reproduces Fermi counting, where fermions carry -1.
The abstract, verbatim, and its opening sentence is the claim. Every line below is quoted from the text.
Numbers it reports
Table 3 reports it. $\beta$ $\Delta C_V$ bosonic relative $\Delta C_V$ fermionic relative 1.1 $-1.386$ 2.9 % $-1.629$ 3.6 % 1.25 $-0.874$ 4.1 % $-1.221$ 6.4 % 1.5 $-0.358$ 4.2 % $-0.786$ 11.2 % 2.0 $+0.139$ 3.9 % $-0.289$ 10.9 % 3.0 $+0.429$ 27.6 % $+0.173$ 14.4 % 4.0 $+0.428$ 47.7 % $+0.312$ 40.8 % 6.0 $+0.255$ 73.7 % $+0.238$ 72.5 % Table 3: Specific-heat deviation of the primon gas from the smooth staircase, $P = 10^6$ (78,498 modes), both statistics.
from 6. A distinguishing observable: the prime-gap specific heatThe two standard Fibonacci braid eigenvalues are $q^4 = e^{4\pi i/5}$ and $-q^2 = -e^{2\pi i/5}$, of orders $5$ and $10$; the Temperley-Lieb loop parameter at the same point is $|q + q^{-1}| = 2\cos(\pi/5) = \varphi$, the golden ratio.
from 5. The phase carriers: characters at roots of unity
How it is done
The bosonic sum diverges as $\beta \to 1^+$: the partial sums $\sum_{p \le x} 1/p$ track Mertens' law $\ln \ln x + B$ and grow without bound, so the Hagedorn-type point of the model sits at $\beta = 1$, in the neighborhood of the Bost-Connes phase-transition point.
from 6. A distinguishing observable: the prime-gap specific heatConstraining the occupation bound of a register — a cap $m$ per mode — changes the accessible counting statistics (Fermi-like, intermediate, Bose-like) and nothing about exchange phases.
from 8. What a practitioner can do
What would falsify it
Whether any intermediate $m$ reproduces any known anyonic observable is left unproven there.
from 1. IntroductionThird, the prime-gap structure of the integer lattice supplies a computable thermodynamic observable — a specific-heat deviation from the smooth-density-of-states ideal gas — that separates the arithmetic construction from the standard derivation and is quantified at every sampled temperature.
from 1. IntroductionPhase insertion leaves every observable fixed.
from 3. The family carries no exchange phase
Where the claim stops
The stronger statement is that the cap does not determine any phase.
from 3. The family carries no exchange phaseThe phase is a free datum the cap does not fix.
from 3. The family carries no exchange phaseThis is the structural reason, and the computation confirms it rather than assuming it.
from 3. The family carries no exchange phase
Where to read
- 1. Introduction409 words · 2 min
- 2. The bounded-occupation family371 words · 2 min
- 3. The family carries no exchange phase399 words · 2 min
- 4. Gentile statistics is not Haldane exclusion statistics274 words · 1 min
- 5. The phase carriers: characters at roots of unity354 words · 2 min
- 6. A distinguishing observable: the prime-gap specific heat433 words · 2 min
- 7. Crosswalk of terminology179 words · 1 min
- 8. What a practitioner can do267 words · 1 min
- 9. Premise depth and boundaries182 words · 1 min
- 10. Verification and reproducibility193 words · 1 min
Read from the paper itself: 10 sections, 3,061 words. Nothing on this page is written by a model; a line that is not a sentence of the paper is not shown. Have a specific question? Ask this paper.