Axion string source modeling

In this paper, we investigate the effect of the string radius of curvature <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:msub><a:mrow><a:mi>R</a:mi></a:mrow><a:mrow><a:mtext>Gaussian</a:mtext></a:mrow></a:msub></a:mrow></a:math> on the massive and massless scalar radiation emitted from collisions of traveling waves propagating along an axion (global cosmic) string. We construct initial conditions for two colliding Gaussians and perform parameter scans over their amplitude <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mi>A</c:mi></c:math> and standard deviation <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msub><e:mi>σ</e:mi><e:mi mathvariant="normal">d</e:mi></e:msub></e:math>. We show that these collisions emit isotropic bursts of massless radiation and that the energy emitted via this channel obeys a power law <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"><h:mrow><h:mrow><h:mover><h:mrow><h:mo stretchy="false">∼</h:mo></h:mrow><h:mrow><h:mo>∝</h:mo></h:mrow></h:mover></h:mrow><h:msup><h:mrow><h:mi>A</h:mi></h:mrow><h:mrow><h:mi>γ</h:mi></h:mrow></h:msup></h:mrow></h:math>, where the coefficient <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:mi>γ</k:mi></k:math> depends on the regime of <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:mi>A</m:mi><m:mo>/</m:mo><m:mi>δ</m:mi></m:math> and <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>δ</o:mi></o:math> is the string width. Massive radiation is exponentially suppressed <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"><q:mrow><q:mover><q:mrow><q:mo stretchy="false">∼</q:mo></q:mrow><q:mrow><q:mo>∝</q:mo></q:mrow></q:mover><q:msup><q:mrow><q:mi>e</q:mi></q:mrow><q:mrow><q:mo>−</q:mo><q:mi>ζ</q:mi><q:msub><q:mrow><q:mi>R</q:mi></q:mrow><q:mrow><q:mtext>Gaussian</q:mtext></q:mrow></q:msub></q:mrow></q:msup></q:mrow></q:math> in the quasilinear regime <t:math xmlns:t="http://www.w3.org/1998/Math/MathML" display="inline"><t:msub><t:mi>σ</t:mi><t:mi mathvariant="normal">d</t:mi></t:msub><t:mo>≫</t:mo><t:mi>δ</t:mi></t:math> and exhibits power-law decay <w:math xmlns:w="http://www.w3.org/1998/Math/MathML" display="inline"><w:mrow><w:mover><w:mrow><w:mo stretchy="false">∼</w:mo></w:mrow><w:mrow><w:mo>∝</w:mo></w:mrow></w:mover><w:msubsup><w:mrow><w:mi>R</w:mi></w:mrow><w:mrow><w:mtext>Gaussian</w:mtext></w:mrow><w:mrow><w:mo>−</w:mo><w:msup><w:mrow><w:mi>γ</w:mi></w:mrow><w:mrow><w:mo>′</w:mo></w:mrow></w:msup></w:mrow></w:msubsup></w:mrow></w:math> in the nonlinear regime <z:math xmlns:z="http://www.w3.org/1998/Math/MathML" display="inline"><z:mrow><z:msub><z:mrow><z:mi>σ</z:mi></z:mrow><z:mrow><z:mi mathvariant="normal">d</z:mi></z:mrow></z:msub><z:mo>≲</z:mo><z:mn>2</z:mn><z:mi>δ</z:mi></z:mrow></z:math>, with different <cb:math xmlns:cb="http://www.w3.org/1998/Math/MathML" display="inline"><cb:mi>ζ</cb:mi></cb:math> and <eb:math xmlns:eb="http://www.w3.org/1998/Math/MathML" display="inline"><eb:msup><eb:mi>γ</eb:mi><eb:mo>′</eb:mo></eb:msup></eb:math> in different regimes of <gb:math xmlns:gb="http://www.w3.org/1998/Math/MathML" display="inline"><gb:msub><gb:mi>R</gb:mi><gb:mtext>Gaussian</gb:mtext></gb:msub></gb:math>. In this nonlinear regime, massive particle radiation can comprise up to 50% of the total energy emitted. Drawing on a known parallel between axion radiation from global strings and gravitational radiation from Abelian-Higgs strings, this suggests that massive particle radiation may become significant with respect to the massless (gravitational) channel for such nonlinear burst signals. For all configurations studied, we obtain a spectral index <ib:math xmlns:ib="http://www.w3.org/1998/Math/MathML" display="inline"><ib:mi>q</ib:mi><ib:mo>≳</ib:mo><ib:mn>1</ib:mn></ib:math> for the axion radiation, where <kb:math xmlns:kb="http://www.w3.org/1998/Math/MathML" display="inline"><kb:mi>q</kb:mi><kb:mo stretchy="false">→</kb:mo><kb:mn>1</kb:mn></kb:math> as <nb:math xmlns:nb="http://www.w3.org/1998/Math/MathML" display="inline"><nb:mi>A</nb:mi></nb:math> increases; i.e., a higher proportion of radiation is emitted in high-frequency modes. Published by the American Physical Society 2024

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Journal
Physical review. D/Physical review. D.
Published
2024-08-12
DOI
https://doi.org/10.1103/physrevd.110.043513
Citations
10
Primary Topic
Dark Matter and Cosmic Phenomena
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article
Field-Weighted Citation Impact
6.60

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article

Axion string source modeling

E. P. S. Shellard, Amelia Drew, Tomasz Kinowski
10 citations
Physical review. D/Physical review. D.
Dark Matter and Cosmic Phenomena
6.60
article

Axion string source modeling

E. P. S. Shellard, Amelia Drew, Tomasz Kinowski
article en
10 citations

Abstract

In this paper, we investigate the effect of the string radius of curvature <a:math xmlns:a="http://www.w3.org/1998/Math/MathML" display="inline"><a:mrow><a:msub><a:mrow><a:mi>R</a:mi></a:mrow><a:mrow><a:mtext>Gaussian</a:mtext></a:mrow></a:msub></a:mrow></a:math> on the massive and massless scalar radiation emitted from collisions of traveling waves propagating along an axion (global cosmic) string. We construct initial conditions for two colliding Gaussians and perform parameter scans over their amplitude <c:math xmlns:c="http://www.w3.org/1998/Math/MathML" display="inline"><c:mi>A</c:mi></c:math> and standard deviation <e:math xmlns:e="http://www.w3.org/1998/Math/MathML" display="inline"><e:msub><e:mi>σ</e:mi><e:mi mathvariant="normal">d</e:mi></e:msub></e:math>. We show that these collisions emit isotropic bursts of massless radiation and that the energy emitted via this channel obeys a power law <h:math xmlns:h="http://www.w3.org/1998/Math/MathML" display="inline"><h:mrow><h:mrow><h:mover><h:mrow><h:mo stretchy="false">∼</h:mo></h:mrow><h:mrow><h:mo>∝</h:mo></h:mrow></h:mover></h:mrow><h:msup><h:mrow><h:mi>A</h:mi></h:mrow><h:mrow><h:mi>γ</h:mi></h:mrow></h:msup></h:mrow></h:math>, where the coefficient <k:math xmlns:k="http://www.w3.org/1998/Math/MathML" display="inline"><k:mi>γ</k:mi></k:math> depends on the regime of <m:math xmlns:m="http://www.w3.org/1998/Math/MathML" display="inline"><m:mi>A</m:mi><m:mo>/</m:mo><m:mi>δ</m:mi></m:math> and <o:math xmlns:o="http://www.w3.org/1998/Math/MathML" display="inline"><o:mi>δ</o:mi></o:math> is the string width. Massive radiation is exponentially suppressed <q:math xmlns:q="http://www.w3.org/1998/Math/MathML" display="inline"><q:mrow><q:mover><q:mrow><q:mo stretchy="false">∼</q:mo></q:mrow><q:mrow><q:mo>∝</q:mo></q:mrow></q:mover><q:msup><q:mrow><q:mi>e</q:mi></q:mrow><q:mrow><q:mo>−</q:mo><q:mi>ζ</q:mi><q:msub><q:mrow><q:mi>R</q:mi></q:mrow><q:mrow><q:mtext>Gaussian</q:mtext></q:mrow></q:msub></q:mrow></q:msup></q:mrow></q:math> in the quasilinear regime <t:math xmlns:t="http://www.w3.org/1998/Math/MathML" display="inline"><t:msub><t:mi>σ</t:mi><t:mi mathvariant="normal">d</t:mi></t:msub><t:mo>≫</t:mo><t:mi>δ</t:mi></t:math> and exhibits power-law decay <w:math xmlns:w="http://www.w3.org/1998/Math/MathML" display="inline"><w:mrow><w:mover><w:mrow><w:mo stretchy="false">∼</w:mo></w:mrow><w:mrow><w:mo>∝</w:mo></w:mrow></w:mover><w:msubsup><w:mrow><w:mi>R</w:mi></w:mrow><w:mrow><w:mtext>Gaussian</w:mtext></w:mrow><w:mrow><w:mo>−</w:mo><w:msup><w:mrow><w:mi>γ</w:mi></w:mrow><w:mrow><w:mo>′</w:mo></w:mrow></w:msup></w:mrow></w:msubsup></w:mrow></w:math> in the nonlinear regime <z:math xmlns:z="http://www.w3.org/1998/Math/MathML" display="inline"><z:mrow><z:msub><z:mrow><z:mi>σ</z:mi></z:mrow><z:mrow><z:mi mathvariant="normal">d</z:mi></z:mrow></z:msub><z:mo>≲</z:mo><z:mn>2</z:mn><z:mi>δ</z:mi></z:mrow></z:math>, with different <cb:math xmlns:cb="http://www.w3.org/1998/Math/MathML" display="inline"><cb:mi>ζ</cb:mi></cb:math> and <eb:math xmlns:eb="http://www.w3.org/1998/Math/MathML" display="inline"><eb:msup><eb:mi>γ</eb:mi><eb:mo>′</eb:mo></eb:msup></eb:math> in different regimes of <gb:math xmlns:gb="http://www.w3.org/1998/Math/MathML" display="inline"><gb:msub><gb:mi>R</gb:mi><gb:mtext>Gaussian</gb:mtext></gb:msub></gb:math>. In this nonlinear regime, massive particle radiation can comprise up to 50% of the total energy emitted. Drawing on a known parallel between axion radiation from global strings and gravitational radiation from Abelian-Higgs strings, this suggests that massive particle radiation may become significant with respect to the massless (gravitational) channel for such nonlinear burst signals. For all configurations studied, we obtain a spectral index <ib:math xmlns:ib="http://www.w3.org/1998/Math/MathML" display="inline"><ib:mi>q</ib:mi><ib:mo>≳</ib:mo><ib:mn>1</ib:mn></ib:math> for the axion radiation, where <kb:math xmlns:kb="http://www.w3.org/1998/Math/MathML" display="inline"><kb:mi>q</kb:mi><kb:mo stretchy="false">→</kb:mo><kb:mn>1</kb:mn></kb:math> as <nb:math xmlns:nb="http://www.w3.org/1998/Math/MathML" display="inline"><nb:mi>A</nb:mi></nb:math> increases; i.e., a higher proportion of radiation is emitted in high-frequency modes. Published by the American Physical Society 2024

Physical review. D/Physical review. D.Vol. 110(4)
University of Cambridge (GB), Homerton University Hospital (GB), Canisius College (US)
Intel Corporation, Department for Business, Energy and Industrial Strategy, UK Government, University of Cambridge, European Cooperation in Science and Technology, Engineering and Physical Sciences Research Council, Science and Technology Facilities Council, Fundação para a Ciência e a Tecnologia, Homerton College, University of Cambridge
Openalex Percentile: Top 3%
Dark Matter and Cosmic Phenomena
6.60
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