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Table 2 Summary of the waveform inversion results

From: Waveform inversion of the ultra-long-period seismic event associated with ground tilt motion during an eruption of Mount Kusatsu–Shirane, Japan, on January 23, 2018

Candidate

(x, y, z)

[m]

(θ, φ)

[°]

E

Nmax

[1015 N m]

ΔV

[105 m3]

L

[m]

W

[m]

Δd

[m]

Δt

[s]

(a)

(− 2200, 600, 1000)

(15, 35)

0.419

18.58

28.81

2311

1618

0.770

5.7

(b)

(200, − 2600, 600)

(20, 60)

0.437

4.55

7.06

1446

1012

0.482

8.9

(c)

(600, − 3400, − 200)

(30, 85)

0.439

1.61

2.50

1023

716

0.341

9.7

(d)

(− 600, − 200, 1400)

(90, 90)

0.263

2.18

3.38

1131

792

0.377

8.4

(e)

(200, − 1400, 1000)

(25, 90)

0.259

6.73

10.44

1648

1153

0.549

11.2

(f)

(1000, − 3400, − 200)

(25, 95)

0.251

1.86

2.88

1073

751

0.358

12.2

(g)

(− 1000, − 600, 1000)

(90, 95)

0.486

2.44

3.79

1175

823

0.392

11.2

(h)

(− 1400, 1400, 1000)

(15, 0)

0.484

18.87

29.26

2323

1626

0.774

10.0

(i)

(− 1000, 200, 1800)

(15, 55)

0.395

18.10

28.07

2291

1604

0.764

14.6

(j)

(200, − 600, 1800)

(25, 45)

0.387

17.01

26.39

2245

1571

0.748

13.1

(k)

(− 1000, − 3000, − 1000)

(65, 65)

0.394

1.56

2.41

1011

708

0.337

15.3

  1. Here, (x, y, z) indicates the source location; (θ, φ) indicates the crack orientation; E indicates the residual value; Nmax indicates the maximum moment amplitude of the source time function; ΔV indicates the volume change; L, W, Δd indicate the length, width, and aperture change of the crack; and Δt indicates the time difference between the start of the eruption and the maximum amplitude of the source time function