Dynamic fluctuations of current and mass in nonequilibrium mass transport processes

Abstract We study steady-state dynamic fluctuations of current and mass in several variants of random average processes on a ring of L sites. These processes violate detailed balance in the bulk and have nontrivial spatial structures: their steady states are not described by the Boltzmann–Gibbs distribution and can have nonzero spatial correlations. Using a microscopic approach, we exactly calculate the second cumulants, or the variance, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mi>T</mml:mi> <mml:mo stretchy="false">)</mml:mo> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> </mml:mrow> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mrow> <mml:mtext>sub</mml:mtext> </mml:mrow> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mi>l</mml:mi> <mml:mo>,</mml:mo> <mml:mi>T</mml:mi> <mml:mo stretchy="false">)</mml:mo> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> </mml:mrow> </mml:math> , of cumulative (time-integrated) currents up to time T across the i th bond and across a subsystem of size l (summed over bonds in the subsystem), respectively. We also calculate the (two-point) dynamic correlation function of the subsystem mass. In particular, we show that, for large <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>L</mml:mi> <mml:mo>≫</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:math> , the second cumulant <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mi>T</mml:mi> <mml:mo stretchy="false">)</mml:mo> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> </mml:mrow> </mml:math> of the cumulative current up to time T across the i th bond grows linearly as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> <mml:mo>∼</mml:mo> <mml:mi>T</mml:mi> </mml:mrow> </mml:math> for initial times <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>T</mml:mi> <mml:mo>∼</mml:mo> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">O</mml:mi> </mml:mrow> <mml:mo stretchy="false">(</mml:mo> <mml:mn>1</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> </mml:math> , subdiffusively as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mi>Q</mml:mi> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> <mml:mo>∼</mml:mo> <mml:msup> <mml:mi>T</mml:mi> <mml:mrow> <mml:mn>1</mml:mn> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> for intermediate times <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mn>1</mml:mn> <mml:mo>≪</mml:mo> <mml:mi>T</mml:mi> <mml:mo>≪</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:math> , and then again linearly as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> <mml:mo>∼</mml:mo> <mml:mi>T</mml:mi> </mml:mrow> </mml:math> for long times <jats:inlin

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Journal
Journal of Statistical Mechanics Theory and Experiment
Published
2024-08-12
DOI
https://doi.org/10.1088/1742-5468/ad5c56
Citations
3
Primary Topic
Advanced Thermodynamics and Statistical Mechanics
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article
Field-Weighted Citation Impact
0.84
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article

Dynamic fluctuations of current and mass in nonequilibrium mass transport processes

Anirban Mukherjee, Animesh Hazra, Punyabrata Pradhan
3 citations
Journal of Statistical Mechanics Theory and Experiment
Advanced Thermodynamics and Statistical Mechanics
0.84
article

Dynamic fluctuations of current and mass in nonequilibrium mass transport processes

Anirban Mukherjee, Animesh Hazra, Punyabrata Pradhan
article en
3 citations

Abstract

Abstract We study steady-state dynamic fluctuations of current and mass in several variants of random average processes on a ring of L sites. These processes violate detailed balance in the bulk and have nontrivial spatial structures: their steady states are not described by the Boltzmann–Gibbs distribution and can have nonzero spatial correlations. Using a microscopic approach, we exactly calculate the second cumulants, or the variance, <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mi>T</mml:mi> <mml:mo stretchy="false">)</mml:mo> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> </mml:mrow> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mrow> <mml:mtext>sub</mml:mtext> </mml:mrow> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mi>l</mml:mi> <mml:mo>,</mml:mo> <mml:mi>T</mml:mi> <mml:mo stretchy="false">)</mml:mo> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> </mml:mrow> </mml:math> , of cumulative (time-integrated) currents up to time T across the i th bond and across a subsystem of size l (summed over bonds in the subsystem), respectively. We also calculate the (two-point) dynamic correlation function of the subsystem mass. In particular, we show that, for large <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>L</mml:mi> <mml:mo>≫</mml:mo> <mml:mn>1</mml:mn> </mml:mrow> </mml:math> , the second cumulant <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo stretchy="false">(</mml:mo> <mml:mi>T</mml:mi> <mml:mo stretchy="false">)</mml:mo> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> </mml:mrow> </mml:math> of the cumulative current up to time T across the i th bond grows linearly as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> <mml:mo>∼</mml:mo> <mml:mi>T</mml:mi> </mml:mrow> </mml:math> for initial times <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mi>T</mml:mi> <mml:mo>∼</mml:mo> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">O</mml:mi> </mml:mrow> <mml:mo stretchy="false">(</mml:mo> <mml:mn>1</mml:mn> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> </mml:math> , subdiffusively as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mi>Q</mml:mi> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> <mml:mo>∼</mml:mo> <mml:msup> <mml:mi>T</mml:mi> <mml:mrow> <mml:mn>1</mml:mn> <mml:mrow> <mml:mo>/</mml:mo> </mml:mrow> <mml:mn>2</mml:mn> </mml:mrow> </mml:msup> </mml:mrow> </mml:math> for intermediate times <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mn>1</mml:mn> <mml:mo>≪</mml:mo> <mml:mi>T</mml:mi> <mml:mo>≪</mml:mo> <mml:msup> <mml:mi>L</mml:mi> <mml:mn>2</mml:mn> </mml:msup> </mml:mrow> </mml:math> , and then again linearly as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo fence="false" stretchy="false">⟨</mml:mo> <mml:msubsup> <mml:mrow> <mml:mi class="MJX-tex-calligraphic">Q</mml:mi> </mml:mrow> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> <mml:msub> <mml:mo fence="false" stretchy="false">⟩</mml:mo> <mml:mi>c</mml:mi> </mml:msub> <mml:mo>∼</mml:mo> <mml:mi>T</mml:mi> </mml:mrow> </mml:math> for long times <jats:inlin

Journal of Statistical Mechanics Theory and ExperimentVol. 2024(8)
S.N. Bose National Centre for Basic Sciences (IN)
Openalex Percentile: Top 29%
Advanced Thermodynamics and Statistical Mechanics
0.84
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