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A Flow Tangent to the Ricci Flow via Heat Kernels and Mass Transport

Functional Analysis · Submitted 29 Aug 2012

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim We present a new relation between the short time behavior of the heat flow, the geometry of optimal transport and the Ricci flow.

how it is stated · asserted 1.00 read the record →

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arXiv ID1208.5815 (version 1)
Pith IDQCYI43MQ, Pith's permanent record of this paper and its review
CitationCarlo Mantegazza, Nicola Gigli. "A Flow Tangent to the Ricci Flow via Heat Kernels and Mass Transport." arXiv:1208.5815 (2012). https://pith.science/paper/QCYI43MQ
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 2,265 input tokens, $0.0001 reported.

What the abstract itself states, as probabilities: claims first 0.07 · states limitation 0.08 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.06 · compares with prior results 0.09 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

We present a new relation between the short time behavior of the heat flow, the geometry of optimal transport and the Ricci flow. We also show how this relation can be used to define an evolution of metrics on non-smooth metric measure spaces with Ricci curvature bounded from below.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We present a new relation between the short time behavior of the heat flow, the geometry of optimal transport and the Ricci flow. contribution 0.96 0.91 0.61 asserted 1.00
s1 We also show how this relation can be used to define an evolution of metrics on non-smooth metric measure spaces with Ricci curvature bounded from below. contribution 0.90 0.94 0.29 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 0.87 · evidence from proof or derivation 1.00.

What was examined, and what was not

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

We present a new relation between the short time behavior of the heat flow, the geometry of optimal transport and the Ricci flow. We also show how this relation can be used to define an evolution of metrics on non-smooth metric measure spaces with Ricci curvature bounded from below.

Human review
How the literature uses it

2 arXiv papers cite this in 23 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 15 sentences without a confident label

Builds on it 1 paper
  • Let us observe that from ([ref]) it easily follows that ([ref]) can be rewritten as [equation] or equivalently as [equation] Also note that by differentiating both members of ([ref]) with respect to $t$ we to get, for any $t>0$, (cf. [ref] Prop. 4.1 for a similar computation for the standard heat kernel), [equation] Since $∇^(z) ∂∂tp^(ω) _t(y , z)= ∇^(z) △_ω^(y) p^(ω) _t(y , z)$, and the weighted laplacian $△_ω^(y)$ acts with respect to the variable point $y$, we can write, after an obvious rearrangement of terms, [equation] By inserting the defining pde ([ref]) in $△_ω^(y) [U_⊥(z)· ∇^(z)p^(ω) _t(y , z) ]$, we eventually get [equation] where we dropped the superscript $(y)$ since the operators $∇$, $div_ω$, and $△_ω$ all act with respect to $y$.

    The Wasserstein geometry of non-linear sigma models and the Hamilton-Perelman Ricci flow · Heat kernel induced Ricci flow · 0.99

Uses its method or tool 1 paper
  • Writing, as usual, $ψ_(t):=ψ_(t, c_λ, c'_λ)$ for ease of notation we have, by an obvious transposition of the argument provided in [ref] , Prop. 3.7, [equation] where, in the last line, we exploited the pde ([ref]) defining the potential $ψ_(t, c_λ, c'_λ)$ corresponding to the tangent vector $c'_λ$.

    The Wasserstein geometry of non-linear sigma models and the Hamilton-Perelman Ricci flow · The induced G-M metric rescaling $(M,g)↦(M, g_t^(ω))$ · 0.86

What it cites · 5 sentences without a confident label

Cites as support 2 papers
  • Indeed, a lower Ricci curvature bound seems necessary due to the fact that the heat flow is well defined and nicely behaves in relation with the $W_2$–geometry only in presence of the $CD(K,∞)$ condition (see [ref] ).

    Calculus and heat flow in metric measure spaces and applications to spaces with Ricci bounds from below · The Construction in a Non–Smooth Setting · 0.99

  • This choice rules rules out Finsler–type geometries and ensures, on one hand, the existence of a heat kernel, on the other hand, the $W_2$–contraction along two heat flows (in [ref] Sturm and Ohta proved that on a normed space $(^d,·,ℒ^d)$ the heat flow never contracts the $W_2$–distance unless the norm comes from a scalar product, therefore, due to the spirit of the discussion here, it is natural to avoid considering this sort of spaces).

    Non-contraction of heat flow on Minkowski spaces · Introduction · 0.97

Cites as background 1 paper

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