2016
DOI: 10.1007/s00605-016-1001-2
|View full text |Cite
|
Sign up to set email alerts
|

Nodal intersections of random eigenfunctions against a segment on the 2-dimensional torus

Abstract: We consider random Gaussian eigenfunctions of the Laplacian on the standard torus, and investigate the number of nodal intersections against a line segment. The expected intersection number, against any smooth curve, is universally proportional to the length of the reference curve, times the wavenumber, independent of the geometry. We found an upper bound for the nodal intersections variance, depending on whether the slope of the straight line is rational or irrational. Our findings exhibit a close relation be… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1

Citation Types

0
18
0

Year Published

2017
2017
2023
2023

Publication Types

Select...
7

Relationship

3
4

Authors

Journals

citations
Cited by 16 publications
(18 citation statements)
references
References 12 publications
0
18
0
Order By: Relevance
“…[15,38] as m → ∞. Rudnick-Wigman [36] and subsequently Rossi-Wigman [34] and the author [31] investigated Z…”
Section: )mentioning
confidence: 99%
“…[15,38] as m → ∞. Rudnick-Wigman [36] and subsequently Rossi-Wigman [34] and the author [31] investigated Z…”
Section: )mentioning
confidence: 99%
“…Several recent papers investigate the nodal volume [37,24] and nodal intersections of arithmetic waves against a fixed curve [38,29,36,39,28].…”
Section: The Arithmetic Wavesmentioning
confidence: 99%
“…In particular, it is well‐known that isotropic random fields on the sphere can be decomposed by means of the spectral representation theorem into the sum of orthogonal components, each of them corresponding to a different multipole . The behavior of geometric functionals in the high‐frequency/high‐energy limit for these components has been studied by several authors in recent years, starting from Nazarov and Sodin (, ) for the number of connected components; Wigman () for the nodal length; and then including, among others, Marinucci and Rossi () and Marinucci and Wigman () for the excursion area; Marinucci and Wigman (), Marinucci and Wigman () and Rossi () for the defect; Cammarota and Marinucci () for the Euler‐Poincaré characteristic; Marinucci, Peccati, Rossi, and Wigman (), Marinucci, Rossi, and Wigman (), Rossi () and Wigman () for the distribution of the nodal length; Cammarota, Marinucci, and Wigman () for the critical values; and Cammarota and Wigman () for the total number of critical points (see also Dalmao, Nourdin, Peccati, and Rossi (), Krishnapur, Kurlberg, and Wigman (), Maffucci (), Peccati and Rossi (), Rossi and Wigman (), Rudnick and Wigman () for related works covering also the 2‐dimensional torus; Maffucci () for the 3‐dimensional torus; and Nourdin, Peccati, and Rossi () for planar random waves).…”
Section: Introductionmentioning
confidence: 99%