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Force on a moving object in an ideal quantum gas

General Physics · Submitted 25 Jul 2023

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

The authors' main claim Quantum statistics causes a deviation from the $\sqrt{T}$-dependence and shows that the force scales with $T^2$ at low temperatures.

how it is stated · asserted 1.00 read the record →

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arXiv ID2307.13276 (version 1)
Pith ID2VLJBLJA, Pith's permanent record of this paper and its review
CitationPattarapon Tanalikhit, Wittaya Kanchanapusakit. "Force on a moving object in an ideal quantum gas." arXiv:2307.13276 (2023). https://pith.science/paper/2VLJBLJA
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The compiled record

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-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,186 input tokens.

What the abstract itself states, as probabilities: claims first 0.02 · states limitation 0.12 · human participants 0.01 · controlled comparison 0.20 · randomized assignment 0.01 · states quantitative result 0.55 · compares with prior results 0.80 · mentions code or data availability 0.02.

The abstract, sentence by sentence

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

We consider a heavy external object moving in an ideal gas of light particles. Collisions with the gas particles transfer momentum to the object, leading to a force that is proportional to the object's velocity but in the opposite direction. In an ideal classical gas at temperature $T$, the force acting on the object is proportional to $\sqrt{T}$. Quantum statistics causes a deviation from the $\sqrt{T}$-dependence and shows that the force scales with $T^2$ at low temperatures. At $T=0$, the force vanishes in a Bose gas but is finite in a Fermi gas.

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 consider a heavy external object moving in an ideal gas of light particles. background 0.51 0.37 0.03 asserted 0.73
s1 Collisions with the gas particles transfer momentum to the object, leading to a force that is proportional to the object's velocity but in the opposite direction. result 0.70 0.54 0.16 asserted 1.00
s2 In an ideal classical gas at temperature $T$, the force acting on the object is proportional to $\sqrt{T}$. background 0.81 0.34 0.08 asserted 1.00
s3 Quantum statistics causes a deviation from the $\sqrt{T}$-dependence and shows that the force scales with $T^2$ at low temperatures. result 1.00 0.77 0.54 asserted 1.00
s4 At $T=0$, the force vanishes in a Bose gas but is finite in a Fermi gas. result 1.00 0.76 0.25 asserted 1.00

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.98.

What was examined, and what was not

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  • arXiv listing abstract v1
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  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
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  • P abstract
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  • S sections
  • T body sentences
  • C citations
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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 consider a heavy external object moving in an ideal gas of light particles. Collisions with the gas particles transfer momentum to the object, leading to a force that is proportional to the object's velocity but in the opposite direction. In an ideal classical gas at temperature $T$, the force acting on the object is proportional to $\sqrt{T}$. Quantum statistics causes a deviation from the $\sqrt{T}$-dependence and shows that the force scales with $T^2$ at low temperatures. At $T=0$, the force vanishes in a Bose gas but is finite in a Fermi gas.

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