General conjecture for the stationary behavior of multi-floor TASEP

Consider a finite multi-floor TASEP with c1c\ge 1 floors and attempted particle arrival and departure rates α>0\alpha>0 and β>0\beta>0. Let

ζ(α,β,c)=max1cmin{ϕ(α,c+1),ϕ(β,)},\zeta(\alpha,\beta,c)=\max_{1\le \ell\le c}\min\{\phi(\alpha,c-\ell+1),\phi(\beta,\ell)\},

and let

L=argmax1cmin{ϕ(α,c+1),ϕ(β,)}.L^*=\operatorname*{\arg\,\max}_{1\le \ell\le c}\min\{\phi(\alpha,c-\ell+1),\phi(\beta,\ell)\}.

Assume condition (a): LL^* consists of a single element \ell^* and ϕ(α,c+1)ϕ(β,)\phi(\alpha,c-\ell^*+1)\ne\phi(\beta,\ell^*); or condition (b): ζ(α,β,c)=1/4\zeta(\alpha,\beta,c)=1/4. General multi-floor TASEP conjecture. As NN\to\infty, the limiting flux is ζ(α,β,c)\zeta(\alpha,\beta,c). Under condition (a), assume without loss of generality that ϕ(α,c+1)<ϕ(β,)\phi(\alpha,c-\ell^*+1)<\phi(\beta,\ell^*). There is one large stable zone on floor \ell^*, within which the stationary distribution converges to Ψ1νγ\Psi_{\ell^*-1}\nu_\gamma, where γ<1/2\gamma<1/2 satisfies

γ(1γ)=ϕ(α,c+1)=ζ(α,β,c).\gamma(1-\gamma)=\phi(\alpha,c-\ell^*+1)=\zeta(\alpha,\beta,c).

The left-side limit is Hl=Ψ1L(α,c+1){\cal H}_l=\Psi_{\ell^*-1}{\cal L}(\alpha,c-\ell^*+1) and behaves like Ψ1νγ\Psi_{\ell^*-1}\nu_\gamma at infinity. The right-side limit Hr{\cal H}_r has effective floor c+1c-\ell^*+1, behaves like [Ψcν1γ][\Psi_{c-\ell^*}\nu_{1-\gamma}]^{\updownarrow} at infinity, and equals the limit for the one-sided system with \ell^* floors, attempted hole arrival rate β\beta, and attempted hole departure rate γ\gamma, lifted by cc-\ell^* floors. Under condition (b), there are exactly L=c+2cαcβ|L^*|=c+2-c_\alpha-c_\beta large stable zones, of asymptotically equal size, on floors =cβ,,ccα+1\ell=c_\beta,\ldots,c-c_\alpha+1, and within them the stationary distribution converges to Ψ1ν1/2\Psi_{\ell-1}\nu_{1/2}. The left-side asymptotic limit is Hl=ΨccαL(α,cα){\cal H}_l=\Psi_{c-c_\alpha}{\cal L}(\alpha,c_\alpha), and the right-side asymptotic limit, viewed from the perspective of holes, is

Hr=[ΨccβL(β,cβ)].{\cal H}_r=[\Psi_{c-c_\beta}{\cal L}(\beta,c_\beta)]^{\updownarrow}.

This conjecture predicts the limiting flux and the macroscopic stable-zone structure of the multi-floor TASEP, extending the corresponding one-sided behavior to finite systems; the parser supplies no evidence that it has been proved or disproved.

Sources & referencesView supporting material

Primary source

Yuliy Baryshnikov and Alexander Stolyar, “Multi-floor generalization of TASEP”, arXiv:2603.13610 (2026).

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