slichter mode
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2021 ◽  
Author(s):  
Vadim Milyukov ◽  
Michail Vinogradov ◽  
Alexey Mironov ◽  
Andrey Myasnikov

<p>The Slichter mode (<sub>1</sub>S<sub>1</sub>) is the longest-period mode of the free oscillations of the Earth. The period of the Slichter mode directly depends on density jump between the outer liquid and the inner solid core which makes the detection of this oscillation very important for gaining a more detailed insight into the structure of the Earth’s interior. Reliable empirical data on the detection of Slichter mode are absent, which is associated with the rather low amplitude of this mode on the surface.</p><p>In this work, for the first time, an attempt is made to detect the Slichter mode using the strain data from the largest 2010 Chilean earthquake recorded by the Baksan laser interferometer–strainmeter (Sternberg Astronomical Institute of the Moscow State University (SAI MSU)) with a measuring arm length of 75 m in the Elbrus region, the Northern Caucasus.</p><p>A new asymptotically optimal algorithm for data analysis is developed. The algorithm uses the maximum likelihood method and takes into account the features of the detected signal and the properties of seismic noise. The algorithm is based on the fundamental principles of the theory of optimal signal reception against the background of non-Gaussian noise, which provides the most effective signal detection in accordance with the Neumann-Pearson optimality criterion. Simultaneously with the detection, the degenerate frequency of the mode and splitting parameter <em>b</em> are estimated. Applying the developed algorithm to the strain data of the Chilean earthquake yielded two sets of the most probable candidates for the Slichter mode parameters: <em>T<sub>1</sub></em> = 5.905 h at <em>b<sub>1</sub></em>= 0.1038 and <em>T<sub>2</sub></em> = 6.581 h at <em>b<sub>2</sub></em>= 0.1046. The obtained sets of the Slichter mode parameters have a false-alarm probability of 0.012 and 0.005, respectively.</p><p>The comparison of our results with the theoretical models and the previous results of experimental determinations of the period of the Slichter mode shows a close correspondence of the period <em>T<sub>1</sub></em> = 5.905 h to the period in the CORE11 model (Widmer et al., 1988); the difference is below 1.5%. In the case of the PREM models (Rosat et al., 2006), the obtained periods correspond to the density jumps between the inner and outer cores of <em>Δρ<sub>1</sub></em> = 0.456 g/cm<sup>3</sup> for <em>T<sub>1</sub></em>= 5.905 h and <em>Δρ<sub>2 </sub></em>= 0.360 g/cm<sup>3</sup> for <em>T<sub>2</sub></em> = 6.581 h.</p><p>This work is supported by the MSU Interdisciplinary Scientific and Educational School of Moscow University "Fundamental and Applied Space Research" and the Russian Foundation for Basic Research under Grant No Grant No 19-05-00341.</p>


2020 ◽  
Vol 56 (11) ◽  
pp. 1447-1455
Author(s):  
V. K. Milyukov ◽  
M. P. Vinogradov ◽  
A. P. Mironov ◽  
A. V. Myasnikov
Keyword(s):  

2020 ◽  
Author(s):  
Vadim Milyukov ◽  
Mikhail Vinogradov ◽  
Alexey Mironov ◽  
Andrey Myasnikov

<p>Traditionally, searching the Slichter mode (the longest-period mode of the Earth's free oscillations <sub>1</sub>S<sub>1</sub>) is based on the data of the superconducting gravimeters of the international GGP network. Currently this network is included in the International Geodynamics and Earth Tide Service (IGETS).</p><p>The sensitivity limit of the best superconducting gravimeters is about 1 nGal and not sufficient for direct observation of the Slichter mode even after the significant earthquakes. To reduce the detection threshold, the researchers used the “stacking” procedure — an joint data processing of the several instruments, but the different sensitivity level of the gravimeters prevents the achievement of maximum efficiency.</p><p>We have developed an asymptotically optimal algorithm based on the maximum likelihood method that takes into account the features of the Slichter mode and seismic noise. An important feature of the algorithm is its ability to evaluate the splitting parameter b which determines the distance between the side singlets of the triplet, simultaneously with the mode period T. The use of a non-linear inertial converter allows to take into account the non-Gaussian noise of real data. The use of the Neumann-Pearson criterion makes also possible to determine confidence level of detection: the false alarm probability and the correct detection probability, depending on the signal-to-noise ratio).</p><p>The algorithm was tested on synthetic data. A computer experiment has shown that the algorithm can detect the Slichter mode for a signal-to-noise ratio of 10<sup>-4</sup>. The algorithm was used to search the Slichter mode after the largest earthquakes based on the data of the IGETS network.</p><p>The results of the analysis are reported.</p><p>This work is supported by the Russian Foundation for Basic Research under Grant No Grant No 19-05-00341.</p>


2012 ◽  
Vol 543 ◽  
pp. A40 ◽  
Author(s):  
A. Coyette ◽  
T. Van Hoolst ◽  
V. Dehant
Keyword(s):  

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