roadband and narrowband variability in abyssal hill bathymetry - - PowerPoint PPT Presentation

roadband and narrowband variability in abyssal hill
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roadband and narrowband variability in abyssal hill bathymetry - - PowerPoint PPT Presentation

roadband and narrowband variability in abyssal hill bathymetry Cristian Proistosescu (University of Washington, Harvard University) May 17, 2017 VOICE meeting LDEO, Columbia University Pleistocene sea level variability characterized by


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Βroadband and narrowband variability in abyssal hill bathymetry

Cristian Proistosescu (University of Washington, Harvard University) May 17, 2017 VOICE meeting LDEO, Columbia University

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1/41 kyr-1 1/23 kyr-1 1/100 kyr-1

Pleistocene sea level variability characterized by Milankovitch frequencies

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(Crowley et al., 2015,Science)

Australian-Antarctic ridge

Milankovitch frequency variability identified in abyssal hill bathymetry

model bathymetry

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Milankovitch frequency variability identified in abyssal hill bathymetry

(Huybers et al., 2015,Science)

Chilean Rise

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Stay tuned: Comprehensive Survey

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(Olive et al., 2015,Science)

  • Filtering by width of emplacement
  • Filtering by flexural compensation
  • Intermittent Magma Supply

Tectonic processes imply a decrease in abyssal hill wavelength with increasing spreading rate

(Goff et al., 2015,Science)

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Wavelength defined as covariance length scale

(Goff 1998)

Kν : modified Bessel function C(r) = σ2 · [(r/λ)ν · Kν(r/λ)/Kν(0)] Commonly referred to as Matérn process λ

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200 400 600 800 1000

bath [normalized]

  • 5

5 20 40 60 80 100 120

freq

10-3 10-2 10-1

PSD [m2/cycle]

100 102 10-2 10-1 100

lag

  • 100
  • 50

50 100

acf

0.5 1-15

  • 10
  • 5

5 10 15

Matérn process is a broadband process yielding a spectral continuum

kyr km kyr km 1/kyr 1/km

S=6.6 cm/yr

ν λ 2πλ

Three parameters

  • variance
  • smoothness
  • characteristic scale

σ2, ν, λ

σ2

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200 400 600 800 1000

bath [normalized]

  • 5

5 20 40 60 80 100 120

freq

10-3 10-2 10-1

PSD [m2/cycle]

100 10-2 10-1 100

lag

  • 100
  • 50

50 100

acf

0.5 1-15

  • 10
  • 5

5 10 15

Influence of characteristic length scale

kyr km kyr km 1/kyr 1/km

S=6.6 cm/yr

λ 2πλ

  • characteristic scale

ν, λ 2πλ

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200 400 600 800 1000

bath [normalized]

  • 5

5 20 40 60 80 100 120

freq

10-3 10-2 10-1

PSD [m2/cycle]

100 10-2 10-1 100

lag

  • 100
  • 50

50 100

acf

0.5 1-15

  • 10
  • 5

5 10 15

Influence of smoothness

kyr km kyr km 1/kyr 1/km

S=6.6 cm/yr

λ

  • smoothness parameter

2, ν,

ν = 2 ν = 0

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Broadband variability can arise from filtering of anomalies

freq

10-3 10-2 10-1

PSD [m2/cycle]

10-1 100 101 102 10-2 10-1 100

⇥ r2 + λ−2⇤(ν+1)/2 | {z } b(r) = εσ2(r) F−1 b(f) = F(f) · ε(f)

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(Olive et al., 2015,Science)

Melt flux Crustal thickness Filter

∆h(τ) = Fw(τ) · φ(τ) ∆h

Filtering by width of emplacement

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(adapted from Olive et al., 2015,Science)

Filtering by flexural compensation

λ[km] Fc[%] b(λ) = Fc(λ) · ∆h(λ) λ = τ · S

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(adapted from Olive et al., 2015,Science)

Continuum variability: Summary

  • Characteristic length scale (λ), is a decorrelation

length scale/ frequency:

✦ Excursions above/below mean bathymetry last, on

average, λ.

  • Record looks peaked, but it has no true periodicity.
  • Arises naturally in geophysical processes as a

consequence of integrating perturbations

  • Implications for detecting orbital peaks
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Characteristic length scale

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Fit to bathymetry transects

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Matérn fit

ν = 0.25 2π · λ/S = 95 ± 45[kyr]

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Null Hypothesis for a single transect

db/dt b

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Null hypothesis distribution for 16 transects

Each Monte Carlo draw: average over 16 Matern process realizations, each with λ set to λ of profile

db/dt b

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Work in progress

…provided one has access to a reasonable amount of time

  • n a reasonably powerful computer, an exact test of

significance is something one never need be without. G.A. Bamard. 1963

  • Caveats:
  • Improve fitting algorithm
  • Generate processes with non-integer ν
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Glacial Cycles: Ice Sheet Dynamics filters Insolation forcing

V (f) = F(f) · I(f)

(Huybers & Tziperman 2008)

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Glacial Cycles

1/41 kyr-1 1/23 kyr-1 1/100 kyr-1

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Pre-whitening highlights higher frequency

1/41 kyr-1 1/23 kyr-1 1/100 kyr-1

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100kyr cycle contains most of the variance

5% 18% 45%

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Narrowband variability

  • 100kyr Glacial Cycle is not a direct orbital response. One

likely mechanism is pacing by Obliquity and Precision of thresholding processes in Ice-Sheets (Calving?) or Carbon Cycle.

  • More general: Non-linear phase locking (Tziperman et al

2006).

  • Obliquity and Precession can be identified despite increased

additional variance at lower frequencies

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Last thoughts: Thresholding process faulting

  • 100kyr Glacial Cycle is not a direct orbital response. One

likely mechanism is pacing by Obliquity and Precision of thresholding processes in Ice-Sheets (Calving?) or Carbon Cycle.

  • More general: Non-linear phase locking (Tziperman et al

2006). Can lead to quasi-periodic features:

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Τhanks!

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Abyssal hill bathymetry

(Science News, 2015)