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Asymptotics for Erdos-Solovej zero modes in strong fields

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Asymptotics for Erdos-Solovej zero modes in strong fields. / Elton, Daniel Mark.
In: Annales Henri Poincaré, Vol. 17, No. 10, 10.2016, p. 2951-2973.

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Elton DM. Asymptotics for Erdos-Solovej zero modes in strong fields. Annales Henri Poincaré. 2016 Oct;17(10):2951-2973. Epub 2016 Apr 9. doi: 10.1007/s00023-016-0478-5

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Elton, Daniel Mark. / Asymptotics for Erdos-Solovej zero modes in strong fields. In: Annales Henri Poincaré. 2016 ; Vol. 17, No. 10. pp. 2951-2973.

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@article{c398544ed6ea48888d383e3bd1f96f02,
title = "Asymptotics for Erdos-Solovej zero modes in strong fields",
abstract = "We consider the strong field asymptotics for the occurrence of zero modes of certain Weyl-Dirac operators on $\R^3$. In particular we are interested in those operators $\Dirac{B}$ for which the associated magnetic field $B$ is given by pulling back a $2$-form $\beta$ from the sphere $\sphere$ to $\R^3$ using a combination of the Hopf fibration and inverse stereographic projection. If $\int_{\sphere}\beta\neq0$ we show that\[\sum_{0\le t\le T}\dim\Ker\Dirac{tB}=\frac{T^2}{8\pi^2}\,\biggl\lvert\int_{\sphere}\beta\biggr\rvert\,\int_{\sphere}\abs{\beta}+o(T^2)\]as $T\to+\infty$. The result relies on Erd\H{o}s and Solovej's characterisation of the spectrum of $\Dirac{tB}$ in terms of a family of Dirac operators on $\sphere$, together with information about the strong field localisation of the Aharonov-Casher zero modes of the latter. ",
keywords = "Weyl-Dirac operator, zero modes",
author = "Elton, {Daniel Mark}",
note = "The final publication is available at Springer via http://dx.doi.org/10.1007/s00023-016-0478-5",
year = "2016",
month = oct,
doi = "10.1007/s00023-016-0478-5",
language = "English",
volume = "17",
pages = "2951--2973",
journal = "Annales Henri Poincar{\'e}",
issn = "1424-0637",
publisher = "Birkhauser Verlag Basel",
number = "10",

}

RIS

TY - JOUR

T1 - Asymptotics for Erdos-Solovej zero modes in strong fields

AU - Elton, Daniel Mark

N1 - The final publication is available at Springer via http://dx.doi.org/10.1007/s00023-016-0478-5

PY - 2016/10

Y1 - 2016/10

N2 - We consider the strong field asymptotics for the occurrence of zero modes of certain Weyl-Dirac operators on $\R^3$. In particular we are interested in those operators $\Dirac{B}$ for which the associated magnetic field $B$ is given by pulling back a $2$-form $\beta$ from the sphere $\sphere$ to $\R^3$ using a combination of the Hopf fibration and inverse stereographic projection. If $\int_{\sphere}\beta\neq0$ we show that\[\sum_{0\le t\le T}\dim\Ker\Dirac{tB}=\frac{T^2}{8\pi^2}\,\biggl\lvert\int_{\sphere}\beta\biggr\rvert\,\int_{\sphere}\abs{\beta}+o(T^2)\]as $T\to+\infty$. The result relies on Erd\H{o}s and Solovej's characterisation of the spectrum of $\Dirac{tB}$ in terms of a family of Dirac operators on $\sphere$, together with information about the strong field localisation of the Aharonov-Casher zero modes of the latter.

AB - We consider the strong field asymptotics for the occurrence of zero modes of certain Weyl-Dirac operators on $\R^3$. In particular we are interested in those operators $\Dirac{B}$ for which the associated magnetic field $B$ is given by pulling back a $2$-form $\beta$ from the sphere $\sphere$ to $\R^3$ using a combination of the Hopf fibration and inverse stereographic projection. If $\int_{\sphere}\beta\neq0$ we show that\[\sum_{0\le t\le T}\dim\Ker\Dirac{tB}=\frac{T^2}{8\pi^2}\,\biggl\lvert\int_{\sphere}\beta\biggr\rvert\,\int_{\sphere}\abs{\beta}+o(T^2)\]as $T\to+\infty$. The result relies on Erd\H{o}s and Solovej's characterisation of the spectrum of $\Dirac{tB}$ in terms of a family of Dirac operators on $\sphere$, together with information about the strong field localisation of the Aharonov-Casher zero modes of the latter.

KW - Weyl-Dirac operator

KW - zero modes

U2 - 10.1007/s00023-016-0478-5

DO - 10.1007/s00023-016-0478-5

M3 - Journal article

VL - 17

SP - 2951

EP - 2973

JO - Annales Henri Poincaré

JF - Annales Henri Poincaré

SN - 1424-0637

IS - 10

ER -