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Record W4392428531 · doi:10.1073/pnas.2320384121

Dichotomous dynamics of magnetic monopole fluids

2024· preprint· en· W4392428531 on OpenAlexaff
Chun-Chih Hsu, Hiroto Takahashi, Fabian Jerzembeck, Jahnatta Dasini, Chaia Carroll, Ritika Dusad, Jonathan Ward, S. Sharma, G. M. Luke, Stephen J. Blundell, Claudio Castelnovo, Jonathan N. Hallén, Roderich Moessner, J. C. Davis

Bibliographic record

VenueProceedings of the National Academy of Sciences · 2024
Typepreprint
Languageen
FieldPhysics and Astronomy
TopicTheoretical and Computational Physics
Canadian institutionsMcMaster University
FundersHORIZON EUROPE European Research CouncilEngineering and Physical Sciences Research CouncilIrish Research CouncilScience Foundation IrelandRoyal SocietyDeutsche ForschungsgemeinschaftUK Research and InnovationHORIZON EUROPE Framework ProgrammeGovernment of the United KingdomGordon and Betty Moore Foundation
KeywordsMagnetic monopolePhysicsMagnetic fieldDissipative systemMagnetic fluxCondensed matter physicsQuantum mechanics

Abstract

fetched live from OpenAlex

A recent advance in the study of emergent magnetic monopoles was the discovery that monopole motion is restricted to dynamical fractal trajectories [J. N. Hallén et al. , Science 378 , 1218 (2022)], thus explaining the characteristics of magnetic monopole noise spectra [R. Dusad et al., Nature 571 , 234 (2019); A. M. Samarakoon et al. , Proc. Natl. Acad. Sci. U.S.A. 119 , e2117453119 (2022)]. Here, we apply this novel theory to explore the dynamics of field-driven monopole currents, finding them composed of two quite distinct transport processes: initially swift fractal rearrangements of local monopole configurations followed by conventional monopole diffusion. This theory also predicts a characteristic frequency dependence of the dissipative loss angle for AC field–driven currents. To explore these novel perspectives on monopole transport, we introduce simultaneous monopole current control and measurement techniques using SQUID-based monopole current sensors. For the canonical material Dy 2 Ti 2 O 7 , we measure <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi mathvariant="normal">Φ</mml:mi> <mml:mo stretchy="false">(</mml:mo> <mml:mi>t</mml:mi> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> </mml:math> , the time dependence of magnetic flux threading the sample when a net monopole current <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi>J</mml:mi> <mml:mfenced close=")" open="("> <mml:mi>t</mml:mi> </mml:mfenced> <mml:mo>=</mml:mo> <mml:mover accent="true"> <mml:mi mathvariant="normal">Φ</mml:mi> <mml:mo>˙</mml:mo> </mml:mover> <mml:mrow> <mml:mo stretchy="false">(</mml:mo> <mml:mi>t</mml:mi> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> <mml:mo stretchy="false">/</mml:mo> <mml:msub> <mml:mi>μ</mml:mi> <mml:mn>0</mml:mn> </mml:msub> </mml:mrow> </mml:math> is generated by applying an external magnetic field <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mi>B</mml:mi> <mml:mn>0</mml:mn> </mml:msub> <mml:mfenced close=")" open="("> <mml:mi>t</mml:mi> </mml:mfenced> <mml:mo>.</mml:mo> </mml:mrow> </mml:math> These experiments find a sharp dichotomy of monopole currents, separated by their distinct relaxation time constants before and after t ~ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mn>600</mml:mn> <mml:mo> </mml:mo> <mml:mi mathvariant="normal">μ</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> </mml:math> from monopole current initiation. Application of sinusoidal magnetic fields <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:msub> <mml:mi>B</mml:mi> <mml:mn>0</mml:mn> </mml:msub> <mml:mfenced close=")" open="("> <mml:mi>t</mml:mi> </mml:mfenced> <mml:mo>=</mml:mo> <mml:mi>B</mml:mi> <mml:mi mathvariant="normal">c</mml:mi> <mml:mi mathvariant="normal">o</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> <mml:mfenced close=")" open="(" separators=""> <mml:mi>ω</mml:mi> <mml:mi>t</mml:mi> </mml:mfenced> </mml:mrow> </mml:math> generates oscillating monopole currents whose loss angle <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mrow> <mml:mi>θ</mml:mi> <mml:mfenced close=")" open="("> <mml:mi>f</mml:mi> </mml:mfenced> </mml:mrow> </mml:math> exhibits a characteristic transition at frequency <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mi>f</mml:mi> <mml:mo>≈</mml:mo> <mml:mn>1.8</mml:mn> <mml:mo> </mml:mo> <mml:mi mathvariant="normal">kHz</mml:mi> </mml:math> over the same temperature range. Finally, the magnetic noise power is also dichotomic, diminishing sharply after t ~ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline" overflow="scroll"> <mml:mn>600</mml:mn> <mml:mo> </mml:mo> <mml:mi mathvariant="normal">μ</mml:mi> <mml:mi mathvariant="normal">s</mml:mi> </mml:math> . This complex phenomenology represents an unprecedented form of dynamical heterogeneity generated by the interplay of fractionalization and local spin configurational symmetry.

Fetched live from OpenAlex and de-inverted. Abstracts are not stored in this database: the inverted indexes are 8.6 GB of the frame’s 9.3 GB of text, and the host has 13 GB free.

How this classification was reachedexpand

Full frame distilled prediction

Teacher imitation

Not calibrated prevalence, not ground truth. Human validation pending. Learned from the 10,348 direct Codex labels and 10,348 direct Gemma labels. Candidate is the union of thresholded teacher heads; consensus is their intersection. These outputs are machine_predicted_unvalidated and are not human labels or direct frontier model labels.

metaresearch head score (Codex)0.000
metaresearch head score (Gemma)0.000
Version: codex-gemma-dda1882f352aValidation status: machine_predicted_unvalidated
Candidate categoriesnone
Consensus categoriesnone
DomainCandidate signal: none · Consensus signal: none
Study designCandidate signal: Theoretical or conceptual · Consensus signal: Theoretical or conceptual
GenreCandidate signal: Empirical · Consensus signal: Empirical
Teacher disagreement score0.064
Threshold uncertainty score0.417

Codex and Gemma teacher scores by category

CategoryCodexGemma
Metaresearch0.0000.000
Meta-epidemiology (narrow)0.0000.000
Meta-epidemiology (broad)0.0000.000
Bibliometrics0.0000.000
Science and technology studies0.0000.001
Scholarly communication0.0000.000
Open science0.0010.001
Research integrity0.0000.000
Insufficient payload (model declined to judge)0.0000.000

Machine scores (provisional)

The two teacher heads of the student model, read on this work. A score orders the frame for review; it never asserts a category, and the validation status ships verbatim with every row.

Baseline scores from an immature model (maturity gate not passed, 7 training rounds). Scores rank; they never assert a category.

Opus teacher head0.015
GPT teacher head0.278
Teacher spread0.263 · how far apart the two teachers sit on this one work
Validation statusscore_only:v0-immature-baseline · verbatim from the scoring run: score_only means the number may rank works, and no category label ships from it

Classification

machine, unvalidated

Machine predicted; a candidate call from one teacher head, not a consensus.

The models applied no category: nothing in the taxonomy fit this work.
Study designTheoretical or conceptual
Domainnot available
GenreEmpirical

How this classification was reached, model by model and score by score, is at the end of the page under "How this classification was reached".

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Citations7
Published2024
Admission routes1
Has abstractyes

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