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Uhlmann Phase as a Topological Measure for One-Dimensional Fermion Systems
Quantum Physics · Submitted 4 Sep 2013
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We illustrate these ideas with some paradigmatic models and find that there exists a critical temperature $T_c$ at which the Uhlmann phase goes discontinuously and abruptly to zero.
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The abstract, sentence by sentence
We introduce the Uhlmann geometric phase as a tool to characterize symmetry-protected topological phases in 1D fermion systems, such as topological insulators and superconductors. Since this phase is formulated for general mixed quantum states, it provides a way to extend topological properties to finite temperature situations. We illustrate these ideas with some paradigmatic models and find that there exists a critical temperature $T_c$ at which the Uhlmann phase goes discontinuously and abruptly to zero. This stands as a borderline between two different topological phases as a function of the temperature. Furthermore, at small temperatures we recover the usual notion of topological phase in fermion systems.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We introduce the Uhlmann geometric phase as a tool to characterize symmetry-protected topological phases in 1D fermion systems, such as topological insulators and superconductors. | contribution 1.00 | 0.89 | 0.14 | asserted 1.00 |
| s1 | Since this phase is formulated for general mixed quantum states, it provides a way to extend topological properties to finite temperature situations. | contribution 0.36 | 0.13 | 0.06 | asserted 0.92 |
| s2 | We illustrate these ideas with some paradigmatic models and find that there exists a critical temperature $T_c$ at which the Uhlmann phase goes discontinuously and abruptly to zero. | result 1.00 | 0.96 | 0.56 | asserted 1.00 |
| s3 | This stands as a borderline between two different topological phases as a function of the temperature. | interpretation 0.97 | 0.70 | 0.20 | asserted 1.00 |
| s4 | Furthermore, at small temperatures we recover the usual notion of topological phase in fermion systems. | result 0.74 | 0.82 | 0.09 | asserted 1.00 |
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The paper
Original abstract
We introduce the Uhlmann geometric phase as a tool to characterize symmetry-protected topological phases in 1D fermion systems, such as topological insulators and superconductors. Since this phase is formulated for general mixed quantum states, it provides a way to extend topological properties to finite temperature situations. We illustrate these ideas with some paradigmatic models and find that there exists a critical temperature $T_c$ at which the Uhlmann phase goes discontinuously and abruptly to zero. This stands as a borderline between two different topological phases as a function of the temperature. Furthermore, at small temperatures we recover the usual notion of topological phase in fermion systems.
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References
How later papers used it
61 later papers cite it
1 later paper by other authors is listed below: 1 compared its own results with it.
Compares with it 1 of 7 papers with this label
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Showed in its figure that in the limit g→0 its temperature gap of the Uhlmann phase tends to the known result for spin-1/2 fermions in crystal momentum k-space given by this paper.
Thermal Uhlmann phase in a locally driven two-spin system (2023) · 0.96 · paraphrased: the licence does not allow quoting
How the literature uses it
3 arXiv papers cite this in 5 sentences
Papers whose main result relates to this one's
States a conflicting result 1 paper
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In contrast to a previous finding that topological properties may not survive above a certain critical temperature, we find that topological properties of open systems, in the sense of the measure suggested here, can persist at any finite temperature and disappear only in the mathematical limit of infinite temperature.
Topological characterization of one-dimensional open fermionic systems · 0.89
Papers citing it · 3 sentences without a confident label
Builds on it 1 paper
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The idea of the topological order is extended to finite temperature in terms of the Uhlmann phase [ref] .
Quark number holonomy and confinement-deconfinement transition · Introduction · 0.87
Compares with it 1 paper
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The quark number holonomy seems to be a similar quantity with the Uhlmann phase [ref] .
Quark number holonomy and confinement-deconfinement transition · Introduction · 0.95
What it cites
Cites as background 1 paper
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In addition, the role played by external dissipative effects and thermal baths in topological insulators and superconductors has attracted much interest both in quantum simulations with different platforms and in condensed matter [ref] .
Topology by dissipation · Introduction · 0.88
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