4
TRAVELLING WAVES IN THE OCCURRENCEOF EARTHQUAKEIN TAIWAN Fu-Tai Wang*, Jenny Chih-Yu Lee**, Shun-Hsyung Chang**, Jhih-Jhen Chen*, Chiu-Hung Su*, Chen-Chain Hwu* and Haw-Jyi Lin* *Department of Electrical Engineering, Hwa Hsia Institute of Technology 111 Gong Jhuan Rd., 23568 Chung Ho, Taipei, Taiwan, Republic of China phone: + (886) 2-8941-5137 ext 25, fax: + (886) 2-8941-5161, email: [email protected] web: www.hwh.edu.tw **Department of Microelectronic Engineering, National Kaohsiung Marine University 142 Haichuan Rd., 81143 Nantzu, Kaohsiung, Taiwan, Republic of China ABSTRACT Predictions based on the past history of seismicity can be useful for reducing the earthquake loss. It can help people to prepare for shorter term forecasting. There is not a simple matter to predict the spatial-temporal pattern of earthquake over time and geography because of the presence of nonsta- tionarity and nonlinearity in fault movement data. An un- derstanding of the spatial-temporal pattern of past seismic events would aid the preparedness to moderate earthquake damage. In this paper, a method of empirical mode decom- position (EMD) to show a spatial-temporal travelling wave in the past history of seismicity is proposed. 1. INTRODUCTION For earthquake forecast, one has to specify three ele- ments,that is where, when and how large the earthquake mag- nitude scales will be. With regard to “when”, it customarily groups prediction techniques into three categories, namely the long-term (decades), medium (few years), and short-time intervals (less than one year) before a seismic event [1]. For- mer two classes of predictions are based on seismicity and the past history of fault movement. Short term prediction technique tends to measure earth properties that change be- fore fracture. These wide variety of precursor include seis- mological, geochemical, electromagnetic, hydrological and biological phenomena. A dilatancy model seems to give rea- sons for some of the observed precursor. The volume of mi- crofractures increase in the rocks as crustal stresses evolve [1, 2, 3, 4]. From the plot of precursor time against to the Richter magnitude “M” [5] of the main shock associated with those precursor, the precursor time “T” in days can be de- scribed by log 10 T=0.60M-1.01. Animals forecast earthquakes ranging from about one minute up to three months. It seems that small animals, rats, squirrels, moles are associated with precursor times from several hours up to 100 days, and have a mode at several days. Medium-sized animals, dogs, cats, monkeys exhibit the ability to sense something from a few days down to a minute. Pigs, cows, deer have a strong mode at a few hours. These numbers have some bias involved for reasons of hu- man reporting unreliability [1]. These seismic anomalous animal behaviors (SAABs) prior to an earthquake are often observed [6]. The author of [6] proposes that ionization in the lower atmosphere is responsible and akin to the piezo- electric effect that involves a pressure-induced charging of a crystal surface [1]. A model for the appearance of electric charges in order to illustrate seismoatmospheric phenomena is proposed. Based on this model, electric field effects that might elicit SAAB-like behaviors are demonstrated [4, 7, 8]. Seismological and geological field data help to under- stand the associated creation and development of a fault zone and determine the seismic fracture energy during an earthquake [5, 9]. Seismic forecasting involves probabil- ity and current behavior of secsmicity. An understanding of the spatial-temporal pattern of past seismic events would aid the preparedness to moderate earthquake damage. Due to the presence of nonstationarity and nonlinearity in fault movement data it is difficult to predict the spatial-temporal pattern of earthquake over time and geography. Empirical mode decomposition (EMD) is a new method pioneered by Huang et al. for non-linear and non-stationary signal anal- ysis [10]. Another available analysis for processing nonsta- tionary signals is the wavelet method [11]. Unlike wavelet analysis, EMD uses an adaptive basis derived from data set to decompose the variance of that set into a finite number of intrinsic mode function (IMFs) [10]. Some of its appli- cations have been made in signal detection underwater and some have also been made to the analysis of epidemiological data [12, 13, 14]. In this paper, a method of empirical mode decomposition (EMD) to show a spatial-temporal travelling wave in the past history of seismicity is proposed. 2. EMPIRICAL MODE DECOMPOSITION In most of the input data X (t ), more than one oscillatory mode is involved, and X (t ) are not IMFs. The process to re- duce the data into IMF components is designated as the em- pirical mode decomposition (EMD) of the HHT [10]. This EMD is illustrated in Fig. 1. All the local minima are linked by a cubic spline as the lower envelope. For the local max- ima, the upper envelope is produced. m 1 is denoted as the mean of these two envelopes. Two purposes of the sifting process are: (1) to eliminate riding waves; and (2) to make the wave-profiles more symmetrical [10]. As shown in Fig. 1, the wave h 1 is still asymmetric and it needs to be treated as the data and then take the the sifting process until h 1k is IMF. This IMF h 1k is then designated as the first IMF component of the data. The stopping criteria are provided in [15], [16]. The shortest period content of the data should be contained in c 1 . Separating c 1 from the rest of the data, we have the residue r 1 . By repeating the sifting process on r 1 and all the following r j s, the EMD of the HHT get X (t )= n i=1 c i + r n . (1) ©2007 EURASIP 1926 15th European Signal Processing Conference (EUSIPCO 2007), Poznan, Poland, September 3-7, 2007, copyright by EURASIP

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Page 1: Travelling Waves in the Occurrence of Earthquake in Taiwan€¦ · toprepareforshorterterm forecasting. Thereis nota simple matter to predict the spatial-temporal pattern of earthquake

TRAVELLING WAVES IN THE OCCURRENCE OF EARTHQUAKE IN TAIWAN

Fu-Tai Wang*, Jenny Chih-Yu Lee**, Shun-Hsyung Chang**,Jhih-Jhen Chen*, Chiu-Hung Su*, Chen-Chain Hwu* and Haw-Jyi Lin*

*Department of Electrical Engineering, Hwa Hsia Institute of Technology111 Gong Jhuan Rd., 23568 Chung Ho, Taipei, Taiwan, Republic of China

phone: + (886) 2-8941-5137 ext 25, fax: + (886) 2-8941-5161, email: [email protected]: www.hwh.edu.tw

**Department of Microelectronic Engineering, National Kaohsiung Marine University142 Haichuan Rd., 81143 Nantzu, Kaohsiung, Taiwan, Republic of China

ABSTRACTPredictions based on the past history of seismicity can be

useful for reducing the earthquake loss. It can help peopleto prepare for shorter term forecasting. There is not a simplematter to predict the spatial-temporal pattern of earthquakeover time and geography because of the presence of nonsta-tionarity and nonlinearity in fault movement data. An un-derstanding of the spatial-temporal pattern of past seismicevents would aid the preparedness to moderate earthquakedamage. In this paper, a method of empirical mode decom-position (EMD) to show a spatial-temporal travelling wavein the past history of seismicity is proposed.

1. INTRODUCTION

For earthquake forecast, one has to specify three ele-ments,that is where, when and how large the earthquake mag-nitude scales will be. With regard to “when”, it customarilygroups prediction techniques into three categories, namelythe long-term (decades), medium (few years), and short-timeintervals (less than one year) before a seismic event [1]. For-mer two classes of predictions are based on seismicity andthe past history of fault movement. Short term predictiontechnique tends to measure earth properties that change be-fore fracture. These wide variety of precursor include seis-mological, geochemical, electromagnetic, hydrological andbiological phenomena. A dilatancy model seems to give rea-sons for some of the observed precursor. The volume of mi-crofractures increase in the rocks as crustal stresses evolve[1, 2, 3, 4]. From the plot of precursor time against to theRichter magnitude “M” [5] of the main shock associated withthose precursor, the precursor time “T” in days can be de-scribed by log10T=0.60M-1.01.

Animals forecast earthquakes ranging from about oneminute up to three months. It seems that small animals, rats,squirrels, moles are associated with precursor times fromseveral hours up to 100 days, and have a mode at severaldays. Medium-sized animals, dogs, cats, monkeys exhibitthe ability to sense something from a few days down to aminute. Pigs, cows, deer have a strong mode at a few hours.These numbers have some bias involved for reasons of hu-man reporting unreliability [1]. These seismic anomalousanimal behaviors (SAABs) prior to an earthquake are oftenobserved [6]. The author of [6] proposes that ionization inthe lower atmosphere is responsible and akin to the piezo-electric effect that involves a pressure-induced charging of acrystal surface [1]. A model for the appearance of electriccharges in order to illustrate seismoatmospheric phenomena

is proposed. Based on this model, electric field effects thatmight elicit SAAB-like behaviors are demonstrated [4, 7, 8].

Seismological and geological field data help to under-stand the associated creation and development of a faultzone and determine the seismic fracture energy during anearthquake [5, 9]. Seismic forecasting involves probabil-ity and current behavior of secsmicity. An understandingof the spatial-temporal pattern of past seismic events wouldaid the preparedness to moderate earthquake damage. Dueto the presence of nonstationarity and nonlinearity in faultmovement data it is difficult to predict the spatial-temporalpattern of earthquake over time and geography. Empiricalmode decomposition (EMD) is a new method pioneered byHuang et al. for non-linear and non-stationary signal anal-ysis [10]. Another available analysis for processing nonsta-tionary signals is the wavelet method [11]. Unlike waveletanalysis, EMD uses an adaptive basis derived from data setto decompose the variance of that set into a finite numberof intrinsic mode function (IMFs) [10]. Some of its appli-cations have been made in signal detection underwater andsome have also been made to the analysis of epidemiologicaldata [12, 13, 14]. In this paper, a method of empirical modedecomposition (EMD) to show a spatial-temporal travellingwave in the past history of seismicity is proposed.

2. EMPIRICAL MODE DECOMPOSITION

In most of the input data X(t), more than one oscillatorymode is involved, and X(t) are not IMFs. The process to re-duce the data into IMF components is designated as the em-pirical mode decomposition (EMD) of the HHT [10]. ThisEMD is illustrated in Fig. 1. All the local minima are linkedby a cubic spline as the lower envelope. For the local max-ima, the upper envelope is produced. m1 is denoted as themean of these two envelopes. Two purposes of the siftingprocess are: (1) to eliminate riding waves; and (2) to makethe wave-profiles more symmetrical [10].

As shown in Fig. 1, the wave h1 is still asymmetric andit needs to be treated as the data and then take the the siftingprocess until h1k is IMF. This IMF h1k is then designated asthe first IMF component of the data. The stopping criteriaare provided in [15], [16]. The shortest period content of thedata should be contained in c1. Separating c1 from the restof the data, we have the residue r1. By repeating the siftingprocess on r1 and all the following r js, the EMD of the HHTget

X(t) =n

∑i=1

ci + rn. (1)

©2007 EURASIP 1926

15th European Signal Processing Conference (EUSIPCO 2007), Poznan, Poland, September 3-7, 2007, copyright by EURASIP

Page 2: Travelling Waves in the Occurrence of Earthquake in Taiwan€¦ · toprepareforshorterterm forecasting. Thereis nota simple matter to predict the spatial-temporal pattern of earthquake

1500 2000 2500 3000 3500

−2

0

2

4 Solid line : The data X(t).

Illustration of the sifting processes.

Am

plitu

de

1500 2000 2500 3000 3500

−2

0

2

4 Dash line : The upper and lower envelops.

Thick solid line : The mean m1

Am

plitu

de

1500 2000 2500 3000 3500

−2

0

2

4Solid line : The first component h

1.

Am

plitu

de

Time (sec)

Figure 1: Illustration of the sifting process.

0 1000 2000 3000 4000 5000 6000

−2

0

2

4

x

The EMD result showing three IMFs and a residue for analytical signal x.

0 1000 2000 3000 4000 5000 6000

−1

0

1

c1

0 1000 2000 3000 4000 5000 6000

−1

0

1

c2

0 1000 2000 3000 4000 5000 6000−2

0

2

c3

0 1000 2000 3000 4000 5000 6000

−2

0

2

r3

Time (sec)

Figure 2: The EMD result showing three IMFs and a residuefor analytical signal x.

Then a decomposition of the input data into n IMFs and oneresidue is achieved. The detail of the decomposition processis presented in [10]. Let us examine the linear sum of threecosine waves

x(t) = cos2

10πt + cos

220

πt + cos2

200πt. (2)

The EMD of HHT has to be used for the asymmetric waveform. The three IMF components after applying the EMDare shown in Fig. 2.

3. TRAVELLING WAVES

Empirical mode decomposition (EMD) is a new method fornon-linear and non-stationary signal analysis [10]. An ap-plications have been made to the analysis of epidemiologicaldata [14]. The spatial-temporal dynamics of dengue haem-orrhagic fever (DHF) incidence are examined in a data set

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 20030

2

4

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−2

0

2

4

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−5

0

5

10

NO

. of

eart

hqua

kes

that

the

Ric

hter

sca

le >

3.

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−10

−5

0

5

Weeks

Figure 3: Example of the EMD sifting process. a. Timeseries of the weekly occurrence of Earthquake in Pingtung,Taiwan, 1998-2003. b. Time series of the highest frequencyIMF. c. The second IMF component obtained by the EMD.d. The third IMF component.

describing 850,000 infections occurring in 72 provinces ofThailand during the period 1983 to 1997.

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 20030

20

40

60

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−50

0

50

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−50

0

50

NO

. of

eart

hqua

kes

that

the

Ric

hter

sca

le >

3.

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−20

−10

0

10

Weeks

Figure 4: Example of occurrence of Earthquake in Taitung,Taiwan, 1998-2003.

EMD isolates a 3-yr periodic mode of variance which isthought to reflect hostpathogen population dynamics. Thenonparametric covariance function is used to characterizethe spatial synchrony of incidence fluctuations. Spatial syn-chrony reflects both the amplitude and relative timing of in-cidence across provinces. Time series decomposition revealsa phenomenon that is not apparent in the raw incidence dataand can aid the formation of hypotheses [14]. Motivated bythis application, a method of EMD to show a spatial-temporaltravelling wave in the past history of seismicity is proposed.Data of occurrence of Earthquakes in Taiwan are available onthe Central Weather Bureau for Earthquakes Report website

http://www.cwb.gov.tw/V5e/index.htm

©2007 EURASIP 1927

15th European Signal Processing Conference (EUSIPCO 2007), Poznan, Poland, September 3-7, 2007, copyright by EURASIP

Page 3: Travelling Waves in the Occurrence of Earthquake in Taiwan€¦ · toprepareforshorterterm forecasting. Thereis nota simple matter to predict the spatial-temporal pattern of earthquake

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 20030

5

10

15

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−20

−10

0

10

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−20

0

20

NO

. of

eart

hqua

kes

that

the

Ric

hter

sca

le >

3.

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−5

0

5

10

Weeks

Figure 5: Example of occurrence of Earthquake in Kaohsi-ung, Taiwan, 1998-2003.

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 20030

10

20

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−10

0

10

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−20

0

20

NO

. of

eart

hqua

kes

that

the

Ric

hter

sca

le >

3.

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−20

0

20

Weeks

Figure 6: Example of occurrence of Earthquake in Chyayi,Taiwan, 1998-2003.

Example of the EMD sifting process of the weekly oc-currence of Earthquake in Pingtung, Taiwan 1998-2003, isshown in Fig. 3. Fig. 4 shows the IMF components ob-tained by the EMD for raw data of occurrence of Earthquakein Taitung, Taiwan 1998-2003. And Fig. 5 indicates timeseries of the weekly occurrence of Earthquake in Kaohsiung,Taiwan, 1998-2003 and the highest frequency IMF, the sec-ond IMF component, and the third IMF component obtainedby the EMD. Examples of the EMD sifting process of oc-currence of Earthquake in two middle provinces, Chyayi andNantou, are shown in Fig. 6 and Fig. 7, respectively . Fig.8 shows the weekly epicenter of earthquake for each Taiwanprovince. Data are presented for provinces from the mostsoutherly to the most northerly from top to bottom. Fig. 9shows the IMFs of the first periodic mode for these provincesof Taiwan. The IMFs of the second periodic mode for theseprovinces is illustrated in Fig. 10. The IMFs of the thirdperiodic mode is shown in Fig. 11.

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 20030

20

40

60

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−20

0

20

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−10

0

10

NO

. of

eart

hqua

kes

that

the

Ric

hter

sca

le >

3.

1998 1998.5 1999 1999.5 2000 2000.5 2001 2001.5 2002 2002.5 2003−10

0

10

Weeks

Figure 7: Example of occurrence of Earthquake in Nantou,Taiwan, 1998-2003.

19981999

20002001

20022003

2

4

6

8

10

12−1

−0.5

0

0.5

1

WeeksRank of province

NO

. of e

pice

nter

s in

eac

h of

the

12 p

rovi

nces

of T

aiw

an th

at th

e M

L >

3

Figure 8: Weekly epicenter in each of the 12 provinces ofTaiwan. Data are presented for provinces from the mostsoutherly to the most northerly from top to bottom. Thereare 3756 individual data points.

4. CONCLUSION

Empirical mode decomposition (EMD) is a method pio-neered by Huang et al. for non-linear and non-stationarysignal analysis. In this paper, the EMD to show a spatial-temporal travelling wave in the past history of seismicity isproposed. In the seismological sense, analysis of frequency,magnitude and location of past seismic events can help peo-ple to prepare for shorter term forecasting. An understandingof the spatial-temporal pattern of past seismic events wouldaid the preparedness to moderate earthquake damage.

REFERENCES

[1] H. T. Ore, “Seismic forecasting,” IEEE Potentials, vol.9, pp. 19–22, April 1990.

[2] D. A. Lockner and M. J. S. Johnston, and J. D. Byerlee,“A Mechanism to explain the generation of earthquakelights,” Nature, vol. 302, pp. 28–33, March 1983.

©2007 EURASIP 1928

15th European Signal Processing Conference (EUSIPCO 2007), Poznan, Poland, September 3-7, 2007, copyright by EURASIP

Page 4: Travelling Waves in the Occurrence of Earthquake in Taiwan€¦ · toprepareforshorterterm forecasting. Thereis nota simple matter to predict the spatial-temporal pattern of earthquake

19981999

20002001

20022003

2

4

6

8

10

12−1

−0.5

0

0.5

1

WeeksRank of province

NO

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pice

nter

s in

eac

h of

the

12 p

rovi

nces

of T

aiw

an th

at th

e M

L >

3

Figure 9: The first periodic mode for each of the 12 provincesof Taiwan. Data are presented for provinces from the mostsoutherly to the most northerly from top to bottom.

19981999

20002001

20022003

2

4

6

8

10

12−1

−0.5

0

0.5

1

WeeksRank of province

NO

. of e

pice

nter

s in

eac

h of

the

12 p

rovi

nces

of T

aiw

an th

at th

e M

L >

3

Figure 10: The second periodic mode for each of the 12provinces of Taiwan. Data are presented for provinces fromthe most southerly to the most northerly from top to bottom.

[3] B. T. Brady and G. A. Rowell, “Laboratory investiga-tion of the electrodynamics of rock fracture,” Nature,vol. 321, pp. 488–492, May 1986.

[4] M. Ikeya and S. Takaki, “Electromagnetic fault for earth-quake lightning,” Jpn. J. Appl. Phys., vol. 35, pp. 355–357, March 1996.

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[6] H. Tributsch, “Do aerosol anomalies precede earth-quakes,” Nature, vol. 276, pp. 606–608, Dec. 1978.

[7] M. Ikeya, Y. Kinoshita, and H. Matsumoto, “A model ex-periment of electromagnetic wave propagation over longdistances using waveguide terminology,” Jpn. J. Appl.Phys., vol. 36, pp. 1558–1561, Nov. 1997.

[8] M. Ikeya and S. Takaki, and D. Takashimizu, “Electricshocks resulting in seismic animal anomalous behav-iors,” J. Phys. Soc. Japan, vol. 65, pp. 710–712, March1996.

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0

0.5

1

WeeksRank of province

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pice

nter

s in

eac

h of

the

12 p

rovi

nces

of T

aiw

an th

at th

e M

L >

3

Figure 11: The third periodic mode for each of the 12provinces of Taiwan. Data are presented for provinces fromthe most southerly to the most northerly from top to bottom.

[9] K. F. Ma, H. Tanaka, S. R. Song, C. Y. Wang, J. H.Hung, Y. B. Tsai, J. Mori, Y. F. Song, E. C. Yeh, W.Soh, L. W. Kuo, and H. Y. Wu, “Slip zone and energeticsof a large earthquake from the Taiwan Chelungpu-faultDrilling Project,” Nature, vol. 444, pp. 473–476, Nov.2006.

[10] N. E. Huang, Z. Shen, S. R. Long, M. C. Wu, H. H.Shih, Q. Zheng, N. C. Yen, C. C. Tung and H. H. Liu,“The empirical decomposition and the Hilbert spectrumfor nonlinear and non-stationary time series analysis,”Proc. R. Soc. Lond. A., No. 454, pp. 903–995, 1998.

[11] S. H. Chang and F. T. Wang, “The application of therobust discrete wavelet transform to underwater sound,” in Proc. EUSIPCO 2000, Tampere, Finland, Sept. 4-8.2000, pp. 1097–1100.

[12] F. T. Wang, S. H. Chang, and J. C. Y. Lee, “Signal De-tection in Underwater Sound using the Empirical ModeDecomposition,” IEICE Trans. on Fundamentals, vol.E89-A, No. 9, pp. 2415–2421, Sept. 2006.

[13] F. T. Wang, S. H. Chang, and J. C. Y. Lee, “Hybridwavelet- Hilbert-Huang spectrum analysis, ” in proc.IEEE OCEANS 2005 Europe, Brest, France, June 4-8.2005, pp. 902–905.

[14] D. A. T. Cummings, R. A. Irizarry, N. E. Huang, T.P. Endy, A. Nisalak, K. Ungchusak, and D. S. Burke,“Travelling waves in the occurrence of dengue haemor-rhagic fever in Thailand,” Nature, vol. 427, pp. 344–347,Jan. 2004.

[15] N. E. Huang, M. L. Wu, S. R. Long, S. P. Shen, W. Q.Per, P. Gloersen, K. L. Fan, “A confidence limit for theempirical mode decomposition and the Hilbert spectralanalysis,” Proc. R. Soc. Lond., no. 459, pp. 2317–2345,2003.

[16] A. D. Veltcheva, C. G. Soares, “Identification of thecomponents of wave spectra by the Hilbert Huang trans-form method,” Applied Ocean Research, no. 26, pp. 1–12, 2004.

©2007 EURASIP 1929

15th European Signal Processing Conference (EUSIPCO 2007), Poznan, Poland, September 3-7, 2007, copyright by EURASIP