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Anàlisi temps-freqüència de l’estat de polarització del senyal magnetotel·lúric

Polarisation analysis of the magnetotelluric signal in the time-frequency domain

Magdalena Escalas Oliver

Aquesta tesi doctoral està subjecta a la llicència Reconeixement- NoComercial – SenseObraDerivada 3.0. Espanya de Creative Commons.

Esta tesis doctoral está sujeta a la licencia Reconocimiento - NoComercial – SinObraDerivada 3.0. España de Creative Commons.

This doctoral thesis is licensed under the Creative Commons Attribution-NonCommercial- NoDerivs 3.0. Spain License.

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Conclusions i perspectives de futur

Conclusions

En aquesta tesi s’ha analitzat l’estat de polarització del senyal MT en el domini (t-f). S’ha creat una nova eina que permet calcular els atributs de polarització dels camps E i B a partir de la TW de les sèries temporals MT, i s’ha aplicat a la detecció i caracterització de fonts de soroll cultural i senyals geomagnètics polaritzats. D’aquesta manera l’objectiu principal de la tesi i els objectius concrets plantejats inicialment han estat completament assolits.

A cada capítol d’aquesta memòria s’han exposat detalladament les conclusions dels resultats obtinguts, a continuació s’analitzen de manera més general.

La contribució metodològica de la tesi ha estat el disseny d’un mètode que proporciona els atributs de polarització del senyal MT en el domini (t-f). Aquests són l’el·lipticitat, l’angle de polarització i el desfasament entre els components ortogonals de cada un dels camps, així com la diferència d’el·lipticitat entre ambdós camps i la desviació de l’angle que formen entre ells respecte a l’ortogonalitat. La base teòrica del mètode és la proposada per Diallo et al.

(2006) per a l’anàlisi de senyals sísmics. S’hi han fet nombroses modificacions, tant respecte al càlcul de la TW com al dels atributs. La modificació més rellevant és la que fa referència a la regió significativa del domini (t-f) on es calculen els atributs. S’ha dissenyat un nou procediment per obtenir-la, basat en el càlcul de la TWI, per a la qual també s’ha proposat una expressió empírica. Finalment s’ha dissenyat una estratègia de filtratge del senyal segons el valor dels seus atributs de polarització en el domini (t-f) tenint en compte la regió significativa i el càlcul de la TWI.

El mètode dissenyat s’ha implementat en el codi MTWAVELETS, en llenguatge Matlab.

Mitjaçant l’anàlisi de nombrosos senyals sintètics s’ha comprovat el seu correcte funcionament.

Per aplicar el nou mètode a l’anàlisi de senyals MT reals, en primer lloc s’ha dissenyat i dut a terme l’experiment “Hontomín-font” a Hontomín (Espanya). Ha consistit en la

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contaminació de sèries temporals MT amb el senyal generat per dos dipols elèctrics horitzontals alimentats per una font de corrent. L’anàlisi de les dades experimentals amb el codi MTWAVELETS ha permès diferenciar el senyal MT del senyal artificial generat amb la font, a partir de l’anàlisi del seu estat de polarització en el domini (t-f). En general el senyal MT no té un estat de polarització determinat, en canvi el senyal artificial es pot caracteritzar pels seus atributs de polarització. La realització de l’experiment i l’anàlisi de les dades obtingudes han resultat ser molt satisfactoris ja que han posat de manifest la utilitat del mètode desenvolupat en aqueta tesi per detectar una font de soroll EM.

S’ha modelitzat l’experiment amb el codi DIPOLE1D (Key, 2009), per conèixer el comportament teòric de l’amplitud dels camps E i B i els seus atributs de polarització en funció del medi, la freqüència i la posició respecte la font. D’aquesta manera s’han pogut interpretar els resultats de l’experiment obtinguts amb el codi MTWAVELETS. La modelització s’ha dut a terme considerant medis homogenis i el medi estratificat 1D- Hontomín (Ogaya et al., 2013). La comparació dels resultats experimentals i els modelitzats ha permès identificar el tipus de font utilitzada i la seva posició relativa respecte els punts de mesura. D’altra banda, ha posat de manifest la presència d’inhomogeneïtats en el medi, fet que era d’esperar tenint en compte el model 3D d’Hontomín (Ogaya et al., 2014).

El mètode desenvolupat s’ha aplicat també a l’anàlisi de senyals MT contaminats per fonts de soroll cultural. A diferència de les respostes MT, l’anàlisi de l’energia i els atributs de polarització en el domini (t-f) sí ha permès identificar en cada cas la font de soroll i la seva posició relativa. Així s’ha caracteritzat el senyal creat per línies elèctriques, la circulació de trens per vies fèrries electrificades amb CC, aerogeneradors i entorns industrials, a partir de dades mesurades a Hontomín i a Lamezia Terme (Itàlia). Gràcies a aquest estudi es coneix el patró que creen aquestes fonts de soroll, i per tant es podran identificar fàcilment en futures anàlisis de sèries MT contaminades. A més, la identificació concreta dels intervals de temps i les freqüències afectades pel soroll és molt útil de cara a filtrar el senyal MT en el domini (t-f) i seleccionar només els segments de major qualitat per obtenir les respostes MT.

Així mateix, amb el codi MTWAVELETS s’han detectat i caracteritzat senyals geomagnètics que presenten un estat de polarització determinat. Per una banda, l’anàlisi de les sèries temporals mesurades a Tramutola (Itàlia) ha permès identificar nombrosos esdeveniments com a pulsacions Pc3, i suggerir aquests senyals com una de les causes de les variacions de les respostes MT detectades en aquest site per Romano et al. (2014). Per l’altra banda, s’han detectat les SR a partir de les sèries temporals mesurades a Huidobro (Espanya), i s’ha caracteritzat el comportament de la seva energia i els seus atributs de polarització en el domini (t-f).

Els resultats obtinguts en aquesta tesi suposen una important contribució, ja que el mètode desenvolupat i la seva implementació en el codi MTWAVELETS permeten analitzar el senyal MT des d’una nova perspectiva. La seva aplicació per detectar fonts de soroll i senyals geomagnètics polaritzats ha mostrat el potencial de la metodologia desenvolupada.

En concret, pel que respecta al soroll cultural el mètode proposat suposa una nova eina per detectar-lo a partir de les sèries temporals MT, així com per determinar la posició relativa de

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189 la seva font respecte el punt de mesura. Actualment, gràcies al desenvolupament de codis d’inversió 3D, en els estudis MT es mesuren dades en un gran nombre de sites. El més habitual és intentar minimitzar el soroll cultural que les pot afectar en l’etapa de processat per obtenir les respostes MT, i en pocs casos s’analitzen prèviament i amb detall les sèries temporals mesurades (Chave i Jones, 2012). Per aquest motiu, la nova eina desenvolupada es considera útil per a detectar soroll cultural a partir de les sèries temporals, prèviament a realitzar el seu processat. D’aquesta manera, durant una campanya d’adquisició de dades MT ja es poden identificar les fonts culturals que les afecten, i si és possible modificar la posició dels sites. Una altra possibilitat que ofereix el mètode és poder seleccionar, en funció del temps i la freqüència, els segments més idonis (menys afectats pel soroll) per a realitzar-ne el seu processat.

Pel que fa als senyals geomagnètics analitzats, tant les pulsacions Pc3 com les SR se solen analitzar habitualment a partir dels registres del camp B en observatoris geomagnètics.

L’anàlisi de les sèries temporals MT en el domini (t-f) ha posat de manifest que tant el camp B com el camp E proporcionen informació útil sobre aquests senyals. Tenint en compte que tant l’energia com l’estat de polarització d’aquests senyals en el domini (t-f) són característics de cada un d’ells, el nou mètode proposat és molt útil per detectar-los i analitzar la seva evolució en el temps i la freqüència. L’estudi tant de les pulsacions Pc3 com de les SR té nombroses aplicacions, com per exemple determinar l’estat de la magnetosfera i la ionosfera.

El fet d’analitzar aquests senyals a partir de sèries temporals MT en comptes de fer-ho a partir del camp B mesurat en un observatori geomagnètic implica que també es pot conèixer la resposta geoelèctrica del medi on es detecten. És un aspecte a tenir en compte si es comparen en registres mesurats en localitzacions diferents. Pel que fa a les pulsacions Pc3, detectar la seva presència és especialment convenient en l’aplicació del mètode MT ja que s’ha mostrat com les respostes MT es poden veure modificades per aquests senyals. Caldrà determinar en cada cas fins a quin punt les variacions de les respostes són acceptables.

Actualment s’aplica molt sovint el mètode MT pel monitoratge de reservoris, per exemple en l’emmagatzematge de CO2, i el seguiment de fenòmens naturals com el vulcanisme. Per aquest motiu és molt important discriminar si les variacions observades en les respostes MT són degudes a canvis en el subsòl o bé son causades per la inestabilitat de les fonts del senyal MT. L’aplicació del mètode proposat en aquesta tesi pot ajudar a diferenciar aquestes situacions.

Perspectives de futur

En un futur seria convenient dur a terme les següents ampliacions del mètode desenvolupat per l’anàlisi del senyal MT en el domini (t-f) i el codi MTWAVELETS en què s’ha implementat:

• Analitzar l’efecte d’utilitzar noves wavelets mare en la TW. És ben conegut que la wavelet de Morlet és idònia per a l’anàlisi del senyal MT, però per a l’anàlisi del soroll cultural seria interessant investigar l’efecte que causa l’ús de wavelets mare diferents.

Podrien proporcionar una major resolució segons el tipus de soroll.

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• Detectar automàticament regions del domini (t-f) amb un estat de polarització determinat, per identificar de manera automàtica en una sèrie temporal MT la possible presència de soroll cultural o senyals geomagnètics polaritzats.

• En el cas del soroll cultural, un cop determinada la regió (t-f) afectada, filtrar-la per obtenir un senyal MT lliure de soroll, i en conseqüència, millorar la qualitat de les respostes MT

• Analitzar estadísticament els resultats obtinguts amb el codi MTWAVELETS en l’anàlisi de diversos segments d’una sèrie temporal de llarga durada, per poder extreure conclusions de l’estudi de sèries temporals MT en experiments de monitoratge.

Respecte els conjunts de dades analitzats, els dos següents ofereixen diverses possibilitats per ampliar-ne el seu estudi:

• Lamezia Terme, en l’anàlisi del soroll cultural creat per una via fèrria electrificada amb CC: ja que es disposa de dades mesurades a diferents sites al llarg d’un perfil que uneix els sites S4 i N6, amb freqüències de mostreig = 6.25 i

= 500 , es proposa dur a terme l’anàlisi complet de totes aquestes dades per conèixer el comportament de l’energia i els atributs de polarització dels camps en el domini (t-f) en funció de la posició dels sites respecte de les vies fèrries. D’aquesta manera es podria analitzar com la variació dels atributs al llarg d’un perfil pot proporcionar informació sobre la font de soroll. En concret, permetria determinar el patró que causa la circulació de trens per una via fèrria electrificada a diferents distàncies d’aquesta.

• Tramutola, en l’estudi de les pulsacions geomagnètiques Pc3: a partir dels registres complets del monitoratge de què es disposa, es podria identificar automàticament la presència de les pulsacions Pc3 amb dues finalitats:

analitzar amb detall l’efecte de les pulsacions Pc3 sobre les respostes MT per determinar fins a quin punt, en cada cas particular, aquests senyals constitueixen una font útil pel mètode MT o bé cal tractar-les com a soroll;

analitzar l’energia i els atributs de polarització dels seus camps E i B en el domini (t-f) segons l’hora del dia i l’estació de l’any, per conèixer millor les propietats de les regions de la magnetosfera on es generen aquestes pulsacions i per les quals es propaguen.

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Conclusions

In this thesis, the polarisation state of the magnetotelluric (MT) signal is analysed in the time- frequency (t-f) domain. A new tool has been developed to compute the polarisation attributes of the electric (E) and magnetic (B) fields from the wavelet transform (WT) of the MT time-series. It has been applied to the detection and characterisation of cultural noise sources and geomagnetic polarised signals. In this way, both the aim of this thesis and its specific objectives were achieved.

The specific conclusions inferred from the results obtained are presented in each chapter of this dissertation. Below, they are analysed in more general terms.

The methodological contribution of this thesis is the design of a method to obtain the polarisation attributes of the MT signal in the (t-f) domain. These attributes are the ellipticity, the polarisation angle, the phase difference between the orthogonal components of each field, the ellipticity difference between both fields and the deviation of the angle between them from the orthogonality. The theoretical background of the method is the same as the one proposed by Diallo et al. (2006) for the analysis of seismic signals. It has been modified in numerous aspects with regard to the calculation of the WT and the attributes. The most relevant modification concerns the significant region of the (t-f) domain where the attributes are computed. A procedure has been designed to obtain that region, based on the calculation of the inverse wavelet transform (IWT). In addition, an empirical expression has been proposed for the IWT. Finally, a filtering strategy is proposed according to the values of the polarisation attributes in the (t-f) domain, taking into account the significant region and the computation of the IWT.

The resulting method has been implemented in a Matlab code named MTWAVELETS. It has been successfully tested through the analysis of many synthetic signals.

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In order to apply the new method to the analysis of real MT signals, an experiment named

“Hontomín-font” has been designed and performed in Hontomín (Spain). It involved contamination of MT time-series with the signal transmitted from two horizontal electric dipoles powered by a current source. The analysis of the experimental data with the MTWAVELETS code has allowed differentiation of the artificial signal from the natural MT signal through the analysis of their polarisation state in the (t-f) domain. The MT signal does not generally have a specific polarisation state. In contrast, the artificial signal can be characterised in terms of its polarisation attributes. The performance of the experiment and the analysis of the experimental data have proven the utility of this new method in detecting sources of electromagnetic noise.

In addition, the experiment has been modeled with the DIPOLE1D code (Key, 2009). The results show the theoretical response of the amplitude and polarisation attributes of the E and B field as a function of the earth model, the frequency and the location with respect to the source. In this way, the experimental results obtained with the MTWAVELETS code are interpreted. The modeling was done using homogenous earth models and the stratified model 1D-Hontomín (Ogaya et al., 2013). The comparison of the experimental and modeled results allowed identifying the source used in the experiment and its location with respect to the sites. Furthermore, it suggests the presence of inhomogeneities in the earth models, which were already expected taking into account the 3D model of Hontomín (Ogaya et al., 2014).

The method developed was applied to the analysis of MT signals contaminated by sources of cultural noise. In contrast to the MT responses, the analysis of the energy and polarisation attributes in the (t-f) domain allowed identifying, in each case, the noise source and its location relative to the source. In this way, the signal created by power lines, electric railways with direct current (DC), wind turbines and industrial areas was characterised in data acquired at Hontomín and Lamezia Terme (Italy). This study has provided the pattern of these noise sources. Thus, in the future they will be identified more easily from the analysis of MT contaminated time-series. Furthermore, the accurate identification of time intervals and frequencies affected by noise is helpful to filter the MT signal in the (t-f) domain and select the highest quality segments to obtain the highest quality MT responses.

Moreover, geomagnetic signals with a particular polarisation state were detected and characterised with the MTWAVELETS code. On the one hand, the analysis of time-series acquired at Tramutola (Italy) has helped to identify numerous events as Pc3 pulsations. It has also suggested that these signals are one of the causes of the oscillation of the MT responses detected at this site by Romano et al. (2014). On the other hand, the Schumann resonances were detected in time-series acquired at Huidobro (Spain). The behavior of its energy and its polarisation attributes have been characterised in the (t-f) domain.

This thesis is an important contribution to the current knowledge in electromagnetic geophysical techniques since the method developed and the MTWAVELETS code are an innovative tool to analyse the MT signal. Its application to the detection of cultural noise sources and geomagnetic signals demonstrates the viability of the method.

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193 In particular, the proposed method has proven to be a new tool to detect cultural noise from MT time-series, and to identify its source and location. At present, in MT studies data are commonly acquired at a huge number of sites due to the development of 3D inversion codes. Cultural noise tends to be usually minimized during the processing stage to obtain the MT responses, and only in a small number of cases the MT time-series are analysed previously in detail (Chave and Jones, 2012). For that reason, the new method will help to identify sources of cultural noise from the time-series before the processing stage. In this way, the noise sources can be identified during a field campaign, and if it is possible, the location of the sites can be modified. Another advantage of the proposed method is that it allows doing the (t-f) selection of the best (less affected by noise) segments to process.

Regarding the analysed geomagnetic signals, Pc3 pulsations and Schumann resonances are usually analysed from the B field recordings at geomagnetic observatories. The analysis of MT time-series in the (t-f) domain has shown that both fields, E and B, provide useful information of these signals. Since the energy and the polarisation state characterise these signals in the (t-f) domain, the proposed method is useful to detect them and analyse their evolution in time and frequency. The examination of Pc3 pulsations and Schumann resonances has many applications, as they reflect the ionosphere and magnetosphere state.

Contrary to the analysis of these signals from the B field recorded at geomagnetic observatories, their analysis from MT time-series also provides the geoelectric response of the earth where they are detected. This is an important aspect to consider in the comparison of data from different locations. With regard to Pc3 pulsations, their detection is particularly convenient for the MT method since it has been demonstrated that MT responses can be affected by these signals. The oscillation of MT responses must be evaluated in each case to determine its acceptability. At present, the MT method is applied to reservoir monitoring, for example in CO2 storage, and to the monitoring of natural phenomena, such as volcanism.

For this reason it is very important to determine if the oscillations of the MT responses are due to soil variations or due to the instability of MT sources. The method proposed in this thesis can help to differentiate between both situations.

Future work

Finally, some perspectives of future work are presented. Regarding the method developed for the analysis of the MT signal in the (t-f) domain and the MTWAVELETS code, the following tasks are proposed:

• Check the effect of using different mother wavelets for the WT. It is well known that the Morlet wavelet is appropriate for the analysis of the MT signal. However, it would be interesting to study up to what extent the use of a different mother wavelet modifies the results. It could provide a better resolution depending on the characteristics of the noisy signal.

• Automatically detect (t-f) regions with a fixed polarisation state. It would help to automatically identify the presence of cultural noise or geomagnetic polarised signals from MT time-series.

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• Regarding cultural noise, once the (t-f) affected region is detected, its filtering would be fundamental to obtain MT signals free of noise, and thus, improve the quality of the MT responses.

• Statistically analyse the results obtained with the MTWAVELETS code when it is applied to the analysis of several segments of long-term time-series. It would be useful in order to analyse MT time-series from monitoring experiments.

Regarding the analysed data sets, the two following sets offer several possibilities to continue their study:

• Lamezia terme, for the analysis of cultural noise created by DC electric railways: MT data acquired along a profile connecting sites S4 and N6 are available, with sampling frequencies = 6.25 and = 500 . A complete analysis of these data is proposed, in order to know the energy and polarisation attributes of the fields in the (t-f) domain, as a function of the location of the sites with respect to the railways. It would show how the polarisation attributes can provide information about the noise source when they are analysed from a profile. In particular, it would provide the pattern created by DC electric railways at different distances.

• Tramutola, for the study of geomagnetic Pc3 pulsations: the presence of Pc3 pulsations could be automatically detected from the complete monitored data set, with two purposes:

carefully analyse the effect of Pc3 pulsations on MT responses to determine, in each case, up to what extent they constitute a useful source for the MT method, or if they should be treated as noise.

analyse the energy and polarisation attributes of their E and B fields in the (t- f) domain as a function of daily and seasonal variations, to improve the knowledge of the state of the magnetosphere regions where these pulsations are generated and propagated.

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Addison, P.S., 2002. The Illustrated Wavelet Transform Handbook: Introductory Theory and Applications in Science, Engineering, Medicine and Finance. Institute of Physics Publishing Ltd, Bristol.

Ansari, I.A., Fraser, B.J., 1986. A multistation study of low latitude Pc3 geomagnetic pulsations. Planet. Space Sci. 34, 519–536. doi:10.1016/0032-0633(86)90090-5

Ansari, I.A., 2006. Solar wind velocity and its control on low latitude Pc3 geomagnetic pulsations, in: ILWS Workshop, GOA.

Ansari, I.A., 2007. Relation between low latitude Pc3 magnetic micropulsations and solar wind. Bull. Astr. Soc.

India 35, 523–531.

Arango, C., 2005. Estudio magnetotelúrico de la zona de Llucmajor (Mallorca): avances en el proceso de datos y modelo 3D. Universitat de Barcelona.

Arango, C., Marcuello, A., Ledo, J., Queralt, P., 2009. 3D magnetotelluric characterization of the geothermal anomaly in the Llucmajor aquifer system (Majorca, Spain). J. Appl. Geophys. 68, 479–488.

doi:10.1016/j.jappgeo.2008.05.006

Avdeev, D.B., 2005. Three-dimensional electromagnetic modelling and inversion from theory to application.

Surv. Geophys. 26, 767–799.

Balasco, M., Lapenna, V., Romano, G., Siniscalchi, A., Telesca, L., 2008. A new magnetotelluric monitoring network operating in Agri Valley (Southern Italy): Study of stability of apparent resistivity estimates. Ann.

Geophys. 51, 265–273.

Ballatore, P., 2002. Effects of fast and slow solar wind on the correlations between interplanetary medium and geomagnetic activity. J. Geophys. Res. 107, 1227. doi:10.1029/2003JA009840

Banks, R.J., 1998. The effects of non-stationary noise on electromagnetic response estimates. Geophys. J. Int.

135, 553–563. doi:10.1046/j.1365-246X.1998.00661.x

Barros, J., De Apraiz, M., Diego, R.I., 2007. Measurement of subharmonics in power voltages. 2007 IEEE Lausanne POWERTECH, Proc. 9, 1736–1740. doi:10.1109/PCT.2007.4538578

(12)

196

Becken, M., Burkhardt, H., 2004. An ellipticity criterion in magnetotelluric tensor analysis. Geophys. J. Int. 159, 69–82. doi:10.1111/j.1365-246X.2004.02376.x

Becken, M., Ritter, O., Burkhardt, H., 2008. Mode separation of magnetotelluric responses in three-dimensional environments. Geophys. J. Int. 172, 67–86. doi:10.1111/j.1365-246X.2007.03612.x

Berdichevsky, M.N., Dmitriev, I. V, 2008. Models and methods of magnetotellurics. Springer, Berlin.

Bering, E.A., Benbrook, J.R., Engebretson, M.J., Arnoldy, R.L., 1998. Simultaneous electric and magnetic field observations of Pc1–2, and Pc3 pulsations. J. Geophys. Res. 103, 6741–6761. doi:10.1029/97JA03327 Bier, E.A., Owusu, N., Engebretson, M.J., Posch, J.L., Lessard, M.R., Pilipenko, V. a., 2014. Investigating the

IMF cone angle control of Pc3-4 pulsations observed on the ground. J. Geophys. Res. Sp. Phys. 119, 1797–1813. doi:10.1002/2013JA019637

Boerner, D.E., 1993a. Tensor CSAMT studies at the Buchans Mine in central Newfoundland. Geophysics 58, 12–19. doi:10.1190/1.1443342

Boerner,D.E.,1993b. Orthogonality in CSAMT and MT measurements. Geophysics 58, 924–934.

doi:10.1190/1.1443483

Born, M., Wolf, E., 1999. Principles of Optics: Electromagnetic Theory of Propagation, Interference and Diffraction of Light. Cambridge University Press, Cambridge.

Bourgeois, B., Girard, J.F., 2010. First modelling results of the EM response of a CO2 storage in the Paris basin. Oil Gas Sci. Technol. Rev. IFP 65, 597–614.

Brändlein, D., Lühr, H., Ritter, O., 2012. Direct penetration of the interplanetary electric field to low geomagnetic latitudes and its effect on magnetotelluric sounding. J. Geophys. Res. Sp. Phys. 117, 1–13.

doi:10.1029/2012JA018008

Brigham, E.O., 1974. The Fast Fourier Transform. Prentice-Hall, Inc., New Jersey.

Cagniard, L., 1953. Basic theory of the magnetotelluric method of geophysical prospecting. Geophysics 18, 605–635. doi:10.1190/1.1437915

Campbell, W.H., 2003. Introduction to Geomagnetic Fields. Cambridge University Press, Cambridge.

Chaize, L., Lavergne, M., 1970. Signal et bruit en magnétotellurique. Geophys Prosp 18, 64–87.

Chand, R., Israil, M., Rai, J., 2009. Schumann resonance frequency variations observed in magnetotelluric data recorded from Garhwal Himalayan region India. Ann. Geophys. 27, 3497–3507. doi:10.5194/angeo-27- 3497-2009

Chant, I.J., Hastie, L.M., 1992. Time-frequency analysis of magnetotelluric data. Geophys. J. Int. 111, 399–413.

Chave, A.D., Jones, A.G., 2012. The magnetotelluric method: Theory and practice. Cambridge University Press, Cambridge.

Chave, A.D., Thomson, D.J., 2004. Bounded influence magnetotelluric response function estimation. Geophys J Int 157, 988–1006.

Chave, A.D., Thomson, D.J., Ander, M.E., 1987. On the robust estimation of power spectra, coherences, and transfer functions. J. Geophys. Res. 92, 633–648. doi:10.1029/JB092iB01p00633

Chen, J., Heincke, B., Jegen, M., Moorkamp, M., 2012. Using empirical mode decomposition to process marine magnetotelluric data. Geophys. J. Int. 190, 293–309. doi:10.1111/j.1365-246X.2012.05470.x

(13)

197

Colombo, D., Keho, T., Janoubi, E., Soyer, W., 2011. Sub-basalt imaging with broadband magnetotellurics in NW Saudi Arabia. SEG Tech. Prog. Exp. Abstr. 30, 619–623.

Constable, S., 2010. Ten years of marine CSEM for hydrocarbon exploration. Geophysics 75, 75A67–75A81.

doi:10.1190/1.3483451

Constable, S., Cox, C.S., 1996. Marine controlled-source electromagnetic sounding: 2. The PEGASUS experiment. J. Geophys. Res. 101, 5519–5530. doi:10.1029/95JB03738

Constable, S.C., Parker, R.L., Constable, C.G., 1987. Occam’s inversion: A practical algorithm for generating smooth models from electomagnetic sounding data. Geophysics 52, 289–300.

Cruz, P.L., 2000. Análisis, cálculo y técnicas de mitigación de campos magnéticos creados por líneas eléctricas de alta tensión. Universidad de Sevilla.

Daubechies, I., 1990. The wavelet transform, time-frequency localization and signal analysis. IEEE Trans. Inf.

Theory 36, 961–1005. doi:10.1109/18.57199

de Groot-Hedlin, C.D., Constable, S.C., 1990. Occam’s inversion to generate smooth, two-dimensional models from magnetotelluric data. Geophysics 55, 1613–1624.

De Lauretis, M., Francia, P., Regi, M., Villante, U., Piancatelli, a., 2010. Pc3 pulsations in the polar cap and at low latitude. J. Geophys. Res. Sp. Phys. 115, 1–10. doi:10.1029/2010JA015967

Diallo, M.S., Kulesh, M., Holschneider, M., Scherbaum, F., Adler, F., 2006. Characterization of polarization attributes of seismic waves using continuous wavelet transforms. Geophysics 71, V67–V77.

doi:10.1190/1.2194511

Egbert, G., Booker, J., 1986. Robust estimation of geomagnetic transfer functions. Geophys J R Astr Soc 87, 173–194. doi:10.1111/j.1365-246X.1986.tb04552.x

Egbert, G., Kelbert, A., 2012. Computational recipes for electromagnetic inverse problems. Geophys. J. Int.

189, 251–267.

Egbert, G.D., 1997. Robust multiple-station magnetotelluric data processing. Geophys. J. Int. 130, 475–496.

doi:10.1111/j.1365-246X.1997.tb05663.x

Egbert, G.D., Eisel, M., Boyd, O.S., Morrison, H.F., 2000. DC trains and Pc3s: Source effects in mid-latitude geomagnetic transfer functions. Geophys. Res. Lett. 27, 25–28.

Eisel, M., Egbert, G.D., 2001. On the stability of magnetotelluric transfer function estimates and the reliability of their variances. Geophys. J. Int. 144, 65–82. doi:10.1046/j.1365-246X.2001.00292.x

Escalas, M., Queralt, P., Ledo, J., Marcuello, A., 2013. Polarisation analysis of magnetotelluric time series using a wavelet-based scheme: A method for detection and characterisation of cultural noise sources. Phys.

Earth Planet. Inter. 218, 31–50. doi:10.1016/j.pepi.2013.02.006

Farge, M., 1992. Wavelet transforms and their applications to turbulence. Annu. Rev. Fluid Mech. 24, 395–457.

Ferguson, I.J., 2012. Instrumentation and field procedures, in: Chave, A.D., Jones, A.G. (Eds.), The Magnetotelluric Method: Theory and Practice. Cambridge University Press, Cambridge, pp. 421–479.

Fontes, S.L., Harinarayana, T., Dawes, G.J.K., Hutton, V.R.S., 1988. Processing of noisy magnetotelluric data using digital filters and additional selection criteria. Phys. Earth Planet. Inter. 52, 30–40.

(14)

198

Fornieles-Callejón, J., Salinas, A., Toledo-Redondo, S., Portí, J., Méndez, A., Navarro, E. A., Morente-Molinera, J. A., Soto-Aranaz, C., Ortega-Cayuela, J.S., 2015. Extremely low frequency band station for natural electromagnetic noise measurement. Radio Sci. 50, 191–201. doi:10.1002/2014RS005567

Foufoula-Georgiou, E., Kumar, P., 1994. Wavelets in Geophysics. Academic Press, San Diego.

Fukunishi, H., Lanzerotti, L.J., 1974. ULF Pulsation Evidence of the Plasmapause. 2. Polarization Studies of Pc3 and Pc4 Pulsations Near L=4 and at a Latitude Network in the Conjugate Region. J. Geophys. Res.

79, 4632–4647.

Gabàs, A., Macau, A., Benjumea, B., Bellmunt, F., Figueras, S., Vilà, M., 2014. Combination of Geophysical Methods to Support Urban Geological Mapping. Surv. Geophys. 35, 983–1002. doi:10.1007/s10712-013- 9248-9

Gamble, T.D., 1979. Magnetotellurics with a remote magnetic reference. Geophysics 44, 53-68.

doi:10.1190/1.1440923

Garcia, X., Jones, A.G., 2008. Robust processing of magnetotelluric data in the AMT dead band using the continuous wavelet transform. Geophysics 73, 223–234.

Goldak, D., Goldak, M.S., 2001. Transient magnetotellurics with adaptive polarization stacking, in: Technical Program Expanded Abstracts, Vol 20. SEG Annual Meeting, pp. 1509–1512.

Goldstein, M.A., Strangway, D.W., 1975. Audiofrequency magnetotellurics with a grounded electric dipole source. Geophysics 40, 669–683.

Goupillaud, P., Grossmann, A., Morlet, J., 1984. Cycle-ocatve and related transforms in seismic signal analysis.

Geoexploration 23, 85–102.

Grayver, A. V., Streich, R., Ritter, O., 2014. 3D inversion and resolution analysis of land-based CSEM data from the Ketzin storage formation. Geophysics 79, E101–E114. doi:10.1190/geo2013-0184.1

Greenberg, E., Price, C., 2004. A global ligthning location algorithm based on the electromagnetic signature in the Schumann resonance band. J. Geophys. Res. D Atmos. 109, 1–8. doi:10.1029/2004JD004845 Grossmann, A., Morlet, J., 1984. Decomposition of Hardy Functions into Square Integrable Wavelets of

Constant Shape. SIAM J. Math. Anal. 15, 723–736. doi:10.1137/0515056

Hatakeyama, H., Hirayama, M., 1934. On the phase difference between the pulsation of terrestrial magnetism and of earth current. J. Meteorol. Soc. Japan 12, 449–459.

Hayakawa, M., Nickolaenko, A.P., Sekiguchi, M., Yamashita, K., Ida, Y., Yano, M., 2008. Anomalous ELF phenomena in the Schumann resonance band as observed at Moshiri (Japan) in possible association with an earthquake in Taiwan. Nat. Hazards Earth Syst. Sci. 8, 1309–1316. doi:10.5194/nhess-8-1309-2008 Hayakawa, M., Ohta, K., Nickolaenko, A.P., Ando, Y., 2005. Anomalous effect in Schumann resonance

phenomena observed in Japan, possibly associated with the Chi-chi earthquake in Taiwan. Ann. Geophys.

23, 1335–1346. doi:10.5194/angeo-23-1335-2005

Heilig, B., Lotz, S., Vero, J., Sutcliffe, P., Reda, J., Pajunpää, K., Raita, T., 2010. Empirically modelled Pc3 activity based on solar wind parameters. Ann. Geophys. 28, 1703–1722. doi:10.5194/angeo-28-1703-2010 Hermance, J.F., 1973. Processing of magnetotelluric data. Phys. Earth Planet. Inter. 7, 349–364.

doi:10.1016/0031-9201(73)90060-5

Hirayama, M., 1934. On the relations between the variations of earth potential gradient and terrestrial magnetism. J. Meteorol. Soc. Japan 12, 16–22.

(15)

199

Huang, N.E., Shen, Z., Long, S.R., Wu, M.C., Shih, H.H., Zheng, Q., Yen, N.-C., Tung, C.C., Liu, H.H., 1998.

The empirical mode decomposition and the Hilbert spectrum for nonlinear and non-stationary time series analysis. Proc. R. Soc. A Math. Phys. Eng. Sci. 454, 903–995. doi:10.1098/rspa.1998.0193

Iliceto, V., Santarato, G., 1999. On the interference of man-made EM fields in the magnetotelluric “dead band.” Geophys. Prospect. 47, 707–719. doi:10.1046/j.1365-2478.1999.00153.x

Institut Català d’Energia, 2003. Linies elèctriques aèries i subterrànies a Catalunya, in: Estudis Monogràfics, 13.

Direcció General d’Energia i Mines i Institut Català d'Energia. Generalitat de Catalunya.

IPCC, 2005. Intergovernamental Panel on Climate Change. Special Report on Carbon Dioxide Capture and Storage. Cambridge University Press, Cambridge.

Itonaga, M., Yumoto, K., 1998. ULF waves and the ground magnetic field. J. Geophys. Res. 103, 9285–9291.

Jacobs, J.A., Kato, Y., Matushita, S., Troitskaya, V.A., 1964. Classification of geomagnetic micropulsations. J.

Geophys. Res. 69, 180–181.

Jones, A.G., 1983. The problem of current channelling: A critical review. Geophys. Surv. 6, 79–122.

Jones, A.G., 2006. Electromagnetic interrogation of the anisotropic Earth: Looking into the Earth with polarized spectacles. Phys. Earth Planet. Inter. 158, 281–291. doi:10.1016/j.pepi.2006.03.026

Jones, A.G., 2012. Distortion of magnetotelluric data: its identification and removal, in: Chave, A.D., Jones, A.G. (Eds.), The Magnetotelluric Method: Theory and Practice. Cambridge University Press, Cambridge, pp. 219–302.

Jones, A.G., Chave, A.D., Egbert, G.D., Auld, D., Bahr, K., 1989. A Comparison of Techniques for Magnetotelluric Response Function Estimation. J. Geophys. Res. 94, 14201–14213.

doi:10.1029/JB094iB10p14201

Junge, A., 1996. Characterization of and correction for cultural noise. Surv. Geophys. 17, 361–391.

doi:10.1007/BF01901639

Kaiser, G., 2002. A Friendly Guide to Wavelets. Birkhaüser, Boston.

Kappler, K.N., Morrison, H.F., Egbert, G.D., 2010. Long-term monitoring of ULF electromagnetic fields at Parkfield, California. J. Geophys. Res. 115, 1–27. doi:10.1029/2009JB006421

Kato, Y., Kikuchi, T., 1950a. On the phase difference of earth current induced by the changes of the earth’s magnetic field, part 1. Sci. Rep. Tohoku Univ. 5th Ser., 2, 139–141.

Kato, Y., Kikuchi, T., 1950b. On the phase difference of earth current induced by the changes of the earth’s magnetic field, part 2. Sci. Rep. Tohoku Univ. 5th Ser., 2, 142–145.

Kaufmann, A.A., Keller, G. V, 1981. The Magnetotelluric Sounding Method, Methods in Geochemistry and Geophysics, 15. Elsevier, Amsterdam-Oxford-New York. doi:10.1029/EO063i029p00578-06

Kellett, R., Bishops, J., Reed, E. Van, 1993. The effects of source polarization in CSAMT data over two massive sulfide deposits in Australia. Geophysics 59, 1764–1772.

Key, K., 2009. 1D inversion of multicomponent, multifrequency marine CSEM data: Methodology and synthetic studies for resolving thin resistive layers. Geophysics 74, F9–F20. doi:10.1190/1.3058434 Key, K., Lockwood, A., 2010. Determining the orientation of marine CSEM receivers using orthogonal

Procrustes rotation analysis. Geophysics 75, F63–F70. doi:10.1190/1.3378765

(16)

200

Kleimenova, N.G., Francia, P., Villante, U., Kozyreva, O. V, Bitterly, J., Schott, J.J., 1999. The temporal and spatial variatons of low frequency geomagnetic pulsations at polar cusp and cap latitudes. Ann. di Geofis.

42, 675–682.

Kleimenova, N.G., Zelinskii, N.R., Kozyreva, O. V., Malysheva, L.M., Solov’ev, A. A., Bogoutdinov, S.R., 2013.

Pc3 geomagnetic pulsations at near-equatorial latitudes at the initial phase of the magnetic storm of April 5, 2010. Geomagn. Aeron. 53, 313–320. doi:10.1134/S0016793213030092

Kronland-Martinet, R., Morlet, J., Grossmann, A., 1987. Analysis of sound patterns through wavelet transforms. Int. J. Pattern Recognit. Artif. Intell. 01, 273–302. doi:10.1142/S0218001487000205

Kulesh, M., Holschneider, M., Diallo, M.S., 2008. Geophysical wavelet library: Applications of the continuous wavelet transform to the polarization and dispersion analysis of signals. Comput. Geosci. 34, 1732–1752.

doi:10.1016/j.cageo.2008.03.004

Kulesh, M., Nosé, M., Holschneider, M., Yumoto, K., 2007. Polarization analysis of a Pi2 pulsation using continuous wavelet transform. Earth Planets Sp. 59, 961–970.

Kumar, M., Singh, B., 2014. An attempt to correlate first mode Schumann resonance intensity with ground surface temperature at low latitudes. J. Atmos. Electr. 34, 69–77.

Labendz, D., 1998. Investigation of Schumann resonance polarization parameters. J. Atmos. Solar-Terrestrial Phys. 60, 1779–1789.

Lanzerotti, L.J., Medford, L. V, Maclennan, C.G., Hasegawa, T., Acuna, M.H., Dolce, S.R., 1981. Polarization characteristics of hydromagnetic waves at low geomagnetic latitudes. J. Geophys. Res. 86, 5500–5506.

Larsen, J.C., Mackie, R., Fiordelisi, A., Manzella, A., Rieven, S., 1996. Robust smooth magnetotelluric transfer functions. Geophys. J. Int. 124, 801–819. doi:10.1111/j.1365-246X.1996.tb05639.x

Latorraca, G.A., Madden, T.R., Korringa, J., 1986. An analysis of the magnetotelluric impedance for three- dimensional conductivity structures. Geophysics 51, 1819–1829.

Ledo, J., 2006. 2-D versus 3-D magnetotelluric data interpretation. Surv. Geophys. 27, 511–543.

Ledo, J., Queralt, P., Martí, A., Jones, A.G., 2002. Two-dimensional interpretation of three-dimensional magnetotelluric data: an example of limitations and resolution. Geophys. J. Int. 150, 127–139.

Lezaeta, P., Chave, A., Jones, A.G., Evans, R., 2007. Source field effects in the auroral zone: Evidence from the Slave craton (NW Canada). Phys. Earth Planet. Inter. 164, 21–35. doi:10.1016/j.pepi.2007.05.002

Lilley, F.E.M., Bennett, D.J., 1972. Array Experiment With Magnetic Variometers Near Coasts of Southeast Australia. Geophys. J. R. Astron. Soc. 29, 49–64.

Lin, J., Qu, L., 2000. Feature Extraction Based on Morlet Wavelet and Its Application for Mechanical Fault Diagnosis. J. Sound Vib. 234, 135–148. doi:10.1006/jsvi.2000.2864

Lomb, N.R., 1976. Least -squares frequency analysis of unequally spaced data. Astrophys. Sp. Sci 39, 447–462.

Lorrain, P., Corson, D.R., 1986. Campos y ondas electromagnéticos. Selecciones Científicas, Madrid.

Loseth, L.O., 2007. Modelling of Controlled Source Electromagnetic Data. Norwegian University of Science and Technology.

Lowes, F.J., 2009. DC railways and the magnetic fields they produce-the geomagnetic context. Earth, Planets Sp. 61, 1–15.

(17)

201

Mallat, S., 1998. A Wavelet Tour of Signal Processing. Academic Press, San Diego.

MacGregor, L.M., Constable, S., Sinha, M.C., 1998. The RAMESSES experiment-III. Controlled-source electromagnetic sounding of the Reykjanes Ridge at 57°45’N. Geophys. J. Int. 135, 773–789.

doi:10.1046/j.1365-246X.1998.00705.x

Madden, T., Thompson, W., 1965. Low-frequency electromagnetic oscillations of the Earth-ionosphere cavity.

Rev. Geophys. 3, 211. doi:10.1029/RG003i002p00211

Martí, A., Queralt, P., Ledo, J., 2009. WALDIM: A code for the dimensionality analysis of magnetotelluric data using rotational invariants of the magnetotelluric tensor. Comput. Geosci. 35, 2295–2303.

McNeice, G., Jones, A.G., 2001. Multisite, multifrequency tensor decomposition of magnetotelluric data.

Geophysics 66, 158–173.

McPherron, R.L., 2005. Magnetic pulsations: Their sources and relation to solar wind and geomagnetic activity.

Surv. Geophys. 26, 545–592. doi:10.1007/s10712-005-1758-7

McPherron, R.L., Russell, C.T., Coleman, P.J., 1972. Fluctuating magnetic fields in the magnetosphere. Space Sci. Rev. 13, 411–454.

Meyers, S.D., Kelly, B.G., O’Brien, J.J., 1993. An Introduction to Wavelet Analysis in Oceanography and Meteorology: With Application to the Dispersion of Yanai Waves. Mon. Weather Rev. 121, 2858–2866.

Morlet, J., Arens, G., Fourfgeau, E., Giard, D., 1982a. Wave propagation and sampling theory-Part I: Complex signal and scattering in multilayered media. Geophysics 47, 203–221.

Morlet, J., Arens, G., Fourgeau, E., Giard, D., 1982b. Wave propagation and sampling theory-Part II: Sampling theory and complex waves. Geophysics 41, 222–236.

Morris, R.J., Cole, K.D., 1987. Pc3 magnetic pulsations at Davis, Antarctica. Planet. Space Sci. 35, 1437–1447.

Morrison, K., 1991. On the nature of Pc3 pulsations at L = 4 and their solar wind dependence. Planet. Space Sci. 39, 1017–1023. doi:10.1016/0032-0633(91)90107-L

Nakatsuka, Y., Xue, Z., Garcia, H., Matsuoka, T., 2010. Experimental study on CO2 monitoring and quantification of stored CO2 in saline formations using resistivity measurements. Int. J. Greenh. Gas Control 4, 209–216.

Neska, A., Reda, J., Neska, M., Sumaruk, Y., 2013. On the influence of DC railway noise on variation data from Belsk and Lviv geomagnetic observatories. Acta Geophys. 61, 385–403. doi:10.2478/s11600-012-0058-0 Neukirch, M., 2014. Non stationary magnetotelluric data processing. Universitat de Barcelona.

Nickolaenko, A.P., Hayakawa, M., Hobara, Y., 1999. Long-term periodical variations in global lightning activity deduced from the Schumann resonance monitoring. J. Geophys. Res. 104, 27585.

doi:10.1029/1999JD900791

Nickolaenko, A.P., Rabinovich, L.M., Shvets, A. V, Shchekotov, A.Y., 2004. Polarization Characteristics of Low-Frequency Resonances in the Earth – Ionosphere Cavity. Radiophys. Quantum Electron. 47, 238–

259.

Nickolaenko, A.P., Sentman, D.D., 2007. Line splitting in the Schumann resonance oscillations. Radio Sci. 42, 1–12. doi:10.1029/2006RS003473

Odera, T.J., 1986. Solar wind controlled pulsations: A review. Rev. Geophys. 24, 55–74.

(18)

202

Oettinger, G., Haak, V., Larsen, J.C., 2001. Noise reduction in magnetotelluric time-series with a new signal – noise separation method and its application to a field experiment in the Saxonian Granulite Massif.

Geophys. J. Int. 146, 659–669.

Ogaya, X., Ledo, J., Queralt, P., Marcuello, Á., Quintà, A., 2013. First geoelectrical image of the subsurface of the Hontomín site (Spain) for CO2 geological storage: A magnetotelluric 2D characterization. Int. J.

Greenh. Gas Control 13, 168–179. doi:10.1016/j.ijggc.2012.12.023

Ogaya, X., Queralt, P., Ledo, J., Marcuello, Á., Jones, A.G., 2014. Geoelectrical baseline model of the subsurface of the Hontomín site (Spain) for CO2 geological storage in a deep saline aquifer: A 3D magnetotelluric characterisation. Int. J. Greenh. Gas Control 27, 120–138.

doi:10.1016/j.ijggc.2014.04.030

Ondrášková, A., Ševčík, S., Kostecký, P., 2011. Decrease of Schumann resonance frequencies and changes in the effective lightning areas toward the solar cycle minimum of 2008-2009. J. Atmos. Solar-Terrestrial Phys. 73, 534–543. doi:10.1016/j.jastp.2010.11.013

Pádua, M.B., Padilha, A.L., Vitorello, I., 2002. Disturbances on magnetotelluric data due to DC electrified railway: A case study from southeastern Brazil. Earth Planets Sp. 54, 591–596.

Palacky, G.J., 1987. Resistivity Characteristics of Geologic Targets, in: Nabighian, M. (Ed.), Electromagnetic Methods in Applied Geophyiscs-Vol 1. Soc. Expl. Geophys, Tulsa.

Papoulis, A., 1962. The Fourier integral and its applications. Mc-Graw Hill Book Company, Inc., New Yok.

Pellerin, L., Alumbaugh, D., Cuevas, N., 2003. Characterization of cultural noise in the AMT band, in: ASEG 16th Geophysics Conference and Exhibition, Extended Abstracts. Brisbane, Australia.

Pellerin, L., Alumbaugh, D.L., Reinemann, D.J., Thompson, P.D., 2004. Power line induced current in the Earth determined by magnetotelluric techniques. Appl. Eng. Agric. - Am. Soc. Agric. Eng. 20, 703–706.

Pilipenko, V.A., Chugunova, O.M., Engebretson, M.J., 2008. Pc3-4 ULF waves at polar latitudes. J. Atmos.

Solar-Terrestrial Phys. 70, 2262–2274. doi:10.1016/j.jastp.2008.09.006

Ponomarenko, P. V., Fraser, B.J., Menk, F.W., Ables, S.T., Morris, R.J., 2002. Cusp-latitude Pc3 spectra: band- limited and power-law components. Ann. Geophys. 20, 1539–1551. doi:10.5194/angeo-20-1539-2002 Piña-Varas, P., Ledo, J., Queralt, P., Marcuello, a., Bellmunt, F., Hidalgo, R., Messeiller, M., 2014. 3-D

Magnetotelluric Exploration of Tenerife Geothermal System (Canary Islands, Spain). Surv. Geophys. 35, 1045–1064. doi:10.1007/s10712-014-9280-4

Pirjola, R., 2011. Modelling the magnetic field caused by a dc-electrified railway with linearly changing leakage currents. Earth, Planets Sp. 63, 991–998. doi:10.5047/eps.2011.06.032

Price, C., Melnikov, A., 2004. Diurnal, seasonal and inter-annual variations in the Schumann resonance parameters. J. Atmos. Solar-Terrestrial Phys. 66, 1179–1185. doi:10.1016/j.jastp.2004.05.004

Qian, W., Pedersen, L.B., 1991. Industrial interference magnetotellurics: An example from the Tangshan area, China. Geophysics 56, 265–273. doi:10.1190/1.1443039

Queralt, P., Jones, A.G., Ledo, J., 2007. Electromagnetic imaging of a complex ore layer: 3D forward modelling, sensitivity tests, and down-mine measurements. Geophysics 72, F85–F95.

Rankin, D., Reddy, I.K., 1970. Polarization of the Magneto-Telluric Fields over an Anisotropic Earth. Pure Appl. Geophys. 78, 58–65.

Rikitake, T., 1948. Notes on the Electromagnetic Induction within the Earth. Bull. Earthq. Res. Inst.

(19)

203

Rikitake, T., 1951. Changes in earth current and their relation to the electrical state of the earth’s crust. Bull.

Earthq. Res. Inst. 29, 271–276.

Risk, G.F., Caldwell, T.G., Bibby, H.M., 1999. Use of magnetotelluric signals from 50 Hz power lines for resistivity mapping of geothermal fields in New Zealand. Geophys. Prospect. 1091–1104.

doi:10.1046/j.1365-2478.1999.00167.x

Ritter, O., Junge, A., Dawes, G., 1998. New equipment and processing for magnetotelluric remote reference observations. Geophys. J. Int. 132, 535–548. doi:10.1046/j.1365-246X.1998.00440.x

Rizzo, E., Iovine, G., Muto, F., Pizzino, L., Caputi, A., Romano, G., Balasco, M., Votta, M., Terranova, O., Greco, R., Iaquinta, P., Soleri, S., Quattrocchi, F., Caielli, G., Aldighieri, B., Franco, R. De, Manzella, A., 2013. Terme Caronte geothermal area (Lamezia Terme-Calabria , Italy ): preliminary results, in: European Geothermal Congress 2013. Pisa, Italy, pp. 1–5.

Rodi, W., Mackie, R.L., 2001. Nonlinear conjugate gradients algorithm for 2-D magnetotelluric inversion.

Geophysics 66, 174–187.

Roldugin, V.C., Vasiljev, A.N., Ostapenko, A.A., 2006. Comparison of the Schumann resonance parameters in horizontal magnetic and electric fields according to observations on the Kola Peninsula. Radio Sci. 41, 1–

12. doi:10.1029/2006RS003475

Roldugin, V.K., Vasil’ev, A.N., 2012. Variations in the schumann resonance polarization ellipse in the horizontal and vertical planes according to observations at the Barentsburg and Lovozero observatories.

Geomagn. Aeron. 52, 68–76. doi:10.1134/S0016793211060144

Romano, G., Balasco, M., Lapenna, V., Siniscalchi, A., Telesca, L., Tripaldi, S., 2014. On the sensitivity of long- term magnetotelluric monitoring in Southern Italy and source-dependent robust single station transfer function variability. Geophys. J. Int. 197, 1425–1441. doi:10.1093/gji/ggu083

Saito, T., 1969. Geomagnetic Pulsations. Space Sci. Rev. 10, 319–412.

Saka, O., Itonaga, M., Kitamura, T., 1982. Ionospheric control of polarization of low-latitude geomagnetic micropulsations at sunrise. J. Atmos. Terr. Phys. 44, 703–712. doi:10.1016/0021-9169(82)90132-5 Santarato, G., Spagnolini, U., 1995. Cancelling directional EM noise in magnetotellurics. Geophys. Prospect. 43,

605–621.

Sentman, D.D., 1987. Magnetic elliptical polarization of Schumann resonances. Radio Sci. 22, 595–606.

Sentman, D.D., 1989. Detection of elliptical polarization and mode splitting in discrete Schumann resonance excitations. J. Atmos. Terr. Phys. 51, 507–519. doi:10.1016/0021-9169(89)90090-1

Shaofeng, Y., Yonghua, L., 1999. Polarization characteristics of Pc3 pulsations at Zhongshan Station of Antarctica. Chinese J. Polar Sci. 10, 155–162.

Shyu, H.C., Sun, Y.S., 2002. Construction of a Morlet Wavelet Power Spectrum 1. Multidimens. Syst. Signal Process. 13, 101–111.

Simões, F., Pfaff, R., Hamelin, M., Klenzing, J., Freudenreich, H., Béghin, C., Berthelier, J.-J., Bromund, K., Grard, R., Lebreton, J.-P., Martin, S., Rowland, D., Sentman, D., Takahashi, Y., Yair, Y., 2012. Using Schumann Resonance Measurements for Constraining the Water Abundance on the Giant Planets—

Implications for the Solar System’S Formation. Astrophys. J. 750, 85. doi:10.1088/0004-637X/750/1/85 Simpson, F., Bahr, K., 2005. Practical Magnetotellurics. Cambridge University Press, Cambridge.

(20)

204

Sinitsin, V.G., Yampolski, Y.M., Zalizovski, A. V., Groves, K.M., Moldwin, M.B., 2003. Spatial field structure and polarization of geomagnetic pulsations in conjugate areas. J. Atmos. Solar-Terrestrial Phys. 65, 1161–

1167. doi:10.1016/j.jastp.2003.08.001

Siripurnvaraporn, W., Egbert, G., 2000. An efficient data-subspace inversion method for 2-D magnetotelluric data. Geophysics 65, 791–803.

Siripurnvaraporn, W., Egbert, G., Lenbury, Y., Uyeshima, M., 2005. Three-dimensional magnetotelluric inversion: Data-space method. Phys. Earth Planet. Inter. 150, 3–14.

Streich, R., Becken, M., Matzander, U., Ritter, O., 2011. Strategies for land-based controlled-source electromagnetic surveying in high-noise regions. Lead. Edge 30, 1174–1181. doi:10.1190/1.3657078 Sutcliffe, P.R., Heilig, B., Lotz, S., 2013. Spectral structure of Pc3-4 pulsations: Possible signatures of cavity

modes. Ann. Geophys. 31, 725–743. doi:10.5194/angeo-31-725-2013

Szarka, L., 1988. Geophysical aspects of man-made electromagnetic noise in the earth-A review. Surv. Geophys.

9, 287–318. doi:10.1007/BF01901627

Testa, A., Langella, R., 2005. Power system subharmonics. IEEE Power Eng. Soc. Gen. Meet. 2005.

doi:10.1109/PES.2005.1489461

Tikhonov, A.N., 1950. On determining electrical characteristics of the deep layers of the Earth’s crust. Dokl.

Acad. Nauk SSSR 73, 295–297.

Toledo-Redondo, S., Salinas, A., Portí, J., Morente, J.A., Fornieles, J., Méndez, A., Galindo-Zaldívar, J., Pedrera, A., Ruiz-Constán, A., Anahnah, F., 2010. Study of schumann resonances based on magnetotelluric records from the western Mediterranean and Antarctica. J. Geophys. Res. 115, 1–11.

doi:10.1029/2010JD014316

Torrence, C., Compo, G.P., 1998. A Practical Guide to Wavelet Analysis. Bull. Am. Meteorol. Soc. 79, 61–78.

Torta, J.M., Marsal, S., Quintana, M., 2014. Assessing the hazard from geomagnetically induced currents to the Spanish entire high-voltage power network in Spain. Earth Planets Sp. 66:87, 1–17.

Trad, D.O., Travassos, J.M., 2000. Wavelet filtering of magnetotelluric data. Geophysics 65, 482-491.

doi:10.1190/1.1444742

Tran, A., Polk, C., 1979a. Schumann resonances and electrical conductivity of the atmosphere and lower ionosphere-I. Effects of conductivity at various altitudes on resonance frequencies and attenuation. J.

Atmos. Terr. Phys. 41, 1241–1248.

Tran, A., Polk, C., 1979b. Schumann resonances an electrical conductivity of the atmosphere and lower ionosphere-II. Evaluation of the conductivity profiles from experimental Schumann resonance data. J.

Atmos. Terr. Phys. 41, 1249–1261.

Troitskaya, V.A., Plyasova, T.A., Gul’elmi, A. V, 1971. Relationship between Pc2-4 pulsations and the interplanetary field. Dokl. Acad. Nauk SSSR 197, 1312.

Tzanis, A., Beamish, D., 1987. Audiomagnetotelluric sounding using the Schumann resonances. J Geophys 61, 97–109.

Uyeshima, M., Kanda, W., Nagao, T., Kono, Y., 1998. Directional properties of VAN’s SES and ULF MT signals at Ioannina, Greece. Phys. Earth Planet. Inter. 105, 153–166. doi:10.1016/S0031-9201(97)00088-5

(21)

205

Vellante, M., De Lauretis, M., Förster, M., Lepidi, S., Zieger, B., Villante, U., Pilipenko, V. a., Zolesi, B., 2002.

Geomagnetic field line resonances at low latitudes: Pulsation event study of 16 August 1993. J. Geophys.

Res. Sp. Phys. 107. doi:10.1029/2001JA900123

Vellante, M., Lühr, H., Zhang, T.L., Wesztergom, V., Villante, U., De Lauretis, M., Piancatelli, a., Rother, M., Schwingenschuh, K., Koren, W., Magnes, W., 2004. Ground/satellite signatures of field line resonance: A test of theoretical predictions. J. Geophys. Res. Sp. Phys. 109, 1–13. doi:10.1029/2004JA010392

Vellante, M., Villante, U., Core, R., Best, A., Lenners, D., Pilipenko, V.A., 1993. Simultaneous geomagnetic pulsation observations at two latitudes: resonant mode characteristics. Ann. Geophys. 11, 734.

Vellante, M., Villante, U., de Lauretis, M., Barchi, G., 1996. Solar cycle variation of the dominant frequencies of Pc3 geomagnetic pulsations at L=1.6. Geophys. Res. Lett. 23, 1505.

Vellante, M., Villante, U., de Lauretis, M., Cerulli-Irelli, P., 1989. An analysis of micropulsation events at a low- latitude station during 1985. Planet. Space Sci. 37, 767–773.

Vilamajó, E., 2011. CSEM terrestre: desenvolupament del mètode i estudi sobre la viabilitat de monitoratge d’un reservori. Universitat de Barcelona-Universitat Ramon Llull.

Vilamajó, E., Rondeleux, B., Queralt, P., Marcuello, A., Ledo, J., 2015. A land controlled-source electromagnetics experiment using a deep vertical electric dipole. Geophys. Prospect. (En revisió).

Vilamajó, E., Queralt, P., Ledo, J., Marcuello, A., 2013. Feasibility of Monitoring the Hontomín (Burgos, Spain) CO2 Storage Site Using a Deep EM Source. Surv. Geophys. 34, 441–461. doi:10.1007/s10712-013-9238-y Villante, U., 2011. Ultra low frequency waves in the magnetosphere, in: Kamide, Y., Chian, A. (Eds.),

Handbook of the Solar-Terrestrial Environment. Springer, Berlin, pp. 397–422.

Villante, U., de Lauretis, M., Francia, P., Lepidi, S., Cafarella, L., Meloni, A., Lazarus, A.J., Lepping, R.P., Mariani, F., 1998. Low frequency geomagnetic field variations at low and high latitude during the January 10-11, 1997 magnetic cloud. Geophys. Res. Lett. 25, 2593.

Villante, U., de Paulis, C., Francia, P., 2011. The transmission of upstream waves to the magnetosphere: An analysis at widely separated ground stations. J Geophys Res 116, A06219.

Villante, U., Lepidi, S., Francia, P., Vellante, M., Meloni, A., Lepping, R.P., Mariani, F., 1999. Pc3 pulsations during variable IMF conditions. Ann. Geophys. 17, 490. doi:10.1007/s005850050776

Villante, U., Lepidi, S., Vellante, M., Lazarus, A.J., Lepping, R.P., 1992. Pc3 activity at low geomagnetic latitudes: a comparison with solar wind observations. Planet. Space Sci. 40, 1399.

Villante, U., Tiberi, P., 2015. A comprehensive analysis of the occurrence and characteristics of midperiod ULF waves at low latitude. J. Geophys. Res. Sp. Phys. 120, 1784–1802. doi:10.1002/2014JA020558

Wang, B., Wang, Y., 1996. Temporal Structure of the Southern Oscillation as Revealed by Waveform and Wavelet Analysis. J. Clim. 9, 1586–1598. doi:10.1175/1520-0442(1996)009<1586:TSOTSO>2.0.CO;2 Wannamaker, P.E., 1984. Magnetotelluric responses of three-dimensional bodies in layered earths. Geophysics

49, 1517–1533. doi:10.1190/1.1441777

Wannamaker, P.E., 1997. Tensor CSAMT survey over the Sulphur Springs thermal area, Valles Caldera, New Mexico, United States of America, Part II: Implications for CSAMT methodology. Geophysics 62, 466–

476. doi:10.1190/1.1444157

Ward, S.H., Hohmann, G.W., 1988. Electromagnetic theory for geophysical applications, in: Nabighian, M.N.

(Ed.), Electromagnetic Methods - Theory and Practice, Vol 1. Soc. Expl. Geophys, Tulsa.

(22)

206

Weckmann, U., Magunia, A., Ritter, O., 2005. Effective noise separation for magnetotelluric single site data processing using a frequency domain selection scheme. Geophys. J. Int. 161, 635–652.

doi:10.1111/j.1365-246X.2005.02621.x

Williams, E.R., 1992. The Schumann resonance: A global tropical thermometer. Science 256, 1184–1187.

Williams, E.R., Mushtak, V.C., Nickolaenko, A.P., 2006. Distinguishing ionospheric models using Schumann resonance spectra. J. Geophys. Res. Atmos. 111, 1–10. doi:10.1029/2005JD006944

Yatsevich, E.I., Nickolaenko, a. P., Pechonaya, O.B., 2008. Diurnal and seasonal variations in the intensities and peak frequencies of the first three schumann-resonance modes. Radiophys. Quantum Electron. 51, 528–

538. doi:10.1007/s11141-008-9056-0

Yedidia, B.A., Vellante, M., Villante, U., Lazarus, A.J., 1991. A study of the relationship between micropulsations and solar wind properties. J. Geophys. Res. 96, 3465–3470.

Yumoto, K., 1986. Generation mechanism of Pc3 magnetic pulsations at very low latitudes. Planet. Space Sci.

34, 1329–1334. doi:10.1016/0032-0633(86)90069-3

Yumoto, K., Saito, T., Tanaka, Y., 1985. Low-latitude Pc 3 magnetic pulsations observed at conjugate stations (L ~1.5). J Geophys Res 90, 12201–12207.

Zanandrea, A., Da Costa, J.M., Dutra, S.L.G., Rosa, R.R., Saotome, O., 2004. Spectral and polarization analysis of geomagnetic pulsations data using a multitaper method. Comput. Geosci. 30, 797–808.

doi:10.1016/j.cageo.2004.03.016

Zelinskiy, N.R., Kleimenova, N.G., Kozyreva, O. V., Agayan, S.M., Bogoutdinov, S.R., Soloviev, A. A., 2014.

Algorithm for recognizing Pc3 geomagnetic pulsations in 1-s data from INTERMAGNET equatorial observatories. Izv. Phys. Solid Earth 50, 240–248. doi:10.1134/S106935131402013X

Zhang, Y., Paulson, K. V., 1997. Enhancement of Signal-to-noise Ratio in Natural-source Transient Magnetotelluric Data with Wavelet Transform. Pure Appl. Geophys. 149, 405–419.

doi:10.1007/s000240050033

Zhou, H., Yu, H., Cao, B., Qiao, X., 2013. Diurnal and seasonal variations in the Schumann resonance parameters observed at Chinese observatories. J. Atmos. Solar-Terrestrial Phys. 98, 86–96.

doi:10.1016/j.jastp.2013.03.021

Ziesolleck, C.W.S., Fraser, B.J., Menk, F.W., McNabb, P.W., 1993. Spatial characteristics of low-latitude Pc3–4 geomagnetic pulsations. J. Geophys. Res. 98, 197–207. doi:10.1029/92JA01433

Zonge, K.L., Hughes, L.J., 1991. Controlled source audio-frequency magnetotellurics, in: Nabighian, M.N.

(Ed.), Electromagnetic Methods in Applied Geophyiscs, 2B. Soc. Expl. Geophys, Tulsa.

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Annex

Annex A: Expressió per calcular la TW de manera computacional

A continuació s’indica com s’obté l’expressió (2.12) utilitzada en aquesta tesi per calcular de manera computacional la TW mitjançant algoritmes de TF. Més detalls sobre la TF es poden trobar a Brigham (1974) i Papoulis (1962), i sobre la TW a Addison (2002) i Kaiser (2002).

La TF del senyal es defineix de la següent manera:

i la TF inversa (TFI):

La TF en cas de translació és:

i en cas de canvi d’escala:

La Identitat de Parseval relaciona el producte intern de dues funcions en el domini temporal i en el domini de freqüències:

[ ] ≡ = +∞

−∞ , ( A.1. )

= = 12

+∞

−∞ . ( A.2. )

[ − ]= , ( A.3. )

[ ] = 1| | " # , $ % ≠ 0. ( A.4. )

+, · )

-, = 1

2 +, · ).

-, , ( A.5. )

Riferimenti

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