Subsidence and tectonic controls on glacially influenced continental margins: examples from the Gulf of Alaska and the western Scotian Shelf and Slope

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    Quaternary International ] (]]]]) ]]]]]]

    Subsidence and tectonic controls on glacially influenced continental

    margins: examples from the Gulf of Alaska and the western Scotian

    Shelf and slope

    Michael R. Gipp*

    Department of Earth Sciences, University of Toronto, Scarborough Campus, Scarborough, Ont., Canada, M1C 1A4

    Abstract

    The glacial record on continental shelves and slopes at mid- to high latitudes is dominated by marine strata, but little is knownregarding the large-scale architecture of such deposits. Models showing the gross architecture and facies successions of Late

    Cenozoic deposits in the Gulf of Alaska and on the western portion of the Nova Scotian Shelf and Slope of southeastern Canada

    have been developed to guide the interpretation of ancient glacially influenced marine sequences and to illustrate the influences of

    their tectonic setting.

    The processes of deposition (including ice rafting, suspension rain-out, debris flows, and turbidity currents) are the same on both

    the Gulf of Alaska and the Scotian Shelf and Slope, yet the large-scale depositional architecture of glacially influenced marine

    deposits on both margins differs because sediment preservation is strongly influenced by the impact of tectonics on relative sea-level

    changes. Eustatic sea level was lower during major glaciations, enabling ice sheets to advance across the Scotian Shelf, whereas rapid

    ongoing subsidence in the forearc basin of the Gulf of Alaska restricted glacial advances to shallow, nearshore areas until the forearc

    basin filled with sediments to create a broad shelf. Both shelf and slope deposits are preserved in the Gulf of Alaska, which has

    developed by both progradation and aggradation, whereas slope deposits are selectively preserved on the Nova Scotia continental

    margin, which has developed by propagation.

    r 2002 Published by Elsevier Science Ltd.

    1. Introduction

    Glacigenic sediments in the rock record consist

    predominantly of glacially influenced marine deposits,

    which have been deposited numerous time in Earths

    history (Eyles, 1993). Typical deposits consists of poorly

    sorted diamictites, debris flows, and turbidites (Powell

    and Molnia, 1989). The relative importance of different

    mechanisms of deposition and the resulting facies

    successions are controlled in a complex fashion bytectonic setting, sea-level fluctuations, and climate

    change (Boulton, 1990). Attempts to model these

    deposits have drawn on extensive geophysical and

    geological databases (e.g., Gipp, 1994a; ten Brink et al.,

    1995; Steckler et al., 1999), yet they remain poorly

    understood in terms of their large-scale architecture and

    regional facies distributions. Recent controversy over

    the Snowball Earth hypothesis (Hoffman et al., 1998;

    Kennedy et al., 2001) has greatly increased the need to

    fully understand the marine record of glaciation.

    This paper contributes to the discussion by presenting

    models of glacially influenced continental margin devel-

    opment in two distinct tectonic settingsthe tectoni-

    cally passive southeastern continental margin of Canada

    (Scotian Shelf and Slope) and the tectonically active

    Gulf of Alaska. The model of the Scotian Shelf and

    Slope is constructed from offshore seismic profilescombined with core data and a large pre-existing

    database. The model of the Gulf of Alaska is

    constructed from extensive seismic-scale outcrop.

    Representative facies successions together with large-

    scale architecture are used to infer the influence of

    tectonic setting on subsidence rate and hence margin

    development.

    On the continental margin of Atlantic Canada,

    decades of hydrocarbon exploration, in conjunction

    with the Geological Survey of Canada, have resulted in

    a database of thousands of kilometres of seismic data,

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    3B2v7:51cGML4:3:1

    JQI : 779Prod:Type:com

    pp:1225col:fig::NIL

    ED:h:rameshPAGN: n:s: SCAN: radhika

    *Current address: Marine Mining Corp., 5829 Fieldon RD,

    Mississauga, Ont., Canada, L5M 5K3. Tel.: +1-905-821-9468; fax:

    +1-416-421-0949.

    E-mail address: [email protected] (M.R. Gipp).

    1040-6182/02/$ - see front matter r 2002 Published by Elsevier Science Ltd.

    PII: S 1 0 4 0 - 6 1 8 2 ( 0 2 ) 0 0 1 0 9 - X

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    thousands of square kilometres of sidescan sonar

    coverage and digital multibeam bathymetric data, and

    many boreholes and cores. In the Gulf of Alaska, a long

    and complete record of Cenozoic climatic deterioration,

    glacially influenced marine deposition, and active

    tectonism is exposed in outcrops of the 5 km thick

    Miocene-to-Recent Yakataga Formation, which can becorrelated with offshore boreholes and seismic reflection

    data (Eyles et al., 1991). Both of these margins have

    been characterized by warm-based ice with similar

    discharge rates during the Pleistocene (Gustavson and

    Boothroyd, 1987). The recent (o150 ka) glacial history

    of both margins is characterized by advances of

    grounded ice across a broad shelf (Eyles, 1988; Piper

    et al., 1990b).

    2. Nova Scotian Shelf and Slope

    The Nova Scotian Shelf and Slope (Fig. 1) is a passive

    margin formed by the opening of the North Atlantic

    Ocean. Seafloor spreading along the margin has

    occurred since the Jurassic, and it has been passive,

    but subsiding, since the late Mesozoic (Welsink et al.,1989). On the basis of its current physiography, it can be

    divided into an eastern and a western portion.

    The western portion is characterized by a broad (100

    200 km) shelf with small (o5000 km2) banks and is

    among the smoothest continental slopes in the North

    Atlantic (Swift, 1985). The slope varies from a gradient

    of about 1:7 in waters shallower than 500 m but the

    slope in deeper waters is about 1:40. The eastern portion

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    111Fig. 1. Scotian Shelf and Slope, on the southeastern margin of Canada, and location of study area. Seismic profiles in Figs. 46 are marked by

    dashed lines, cores are marked by circles. Line drawings of sections on upper slope modified from Piper (2001). Canyons seaward of Banquereau and

    Sable Island Bank are named. After Atlantic Geoscience Centre (1991) and Gipp (1996). Depths in metres; ebEmerald Basin.

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    is characterized by a very broad (>200 km) shelf with

    large (B10000km2) banks and a relatively steeper slope

    (1:61:30), which is dissected by large submarine canyon

    systems.

    Fluvial systems incised channels on the Scotian Shelf,

    and provided sediments to the continental slope

    throughout the Tertiary, particularly during times oflowered sea level, until the first glacial influences in the

    Pleistocene (Piper et al., 1990b). Tertiary fluvial

    channels have been overdeepened by Pleistocene glacia-

    tion, and glacial sediments have draped inner shelf

    bedrock highs, and partially filled deeper mid-shelf

    troughs (King and Fader, 1986). The outer Scotian Shelf

    was a major depocentre for glacially influenced marine

    sediments during the Late Wisconsinan, and sediments

    of this age unconformably overlie gently dipping

    Tertiary strata (Boyd et al., 1988).

    The first major (shelf-crossing) glaciation to affect the

    Scotian Slope occurred in the middle Pleistocene

    (Mosher et al., 1989), probably during isotopic stage

    12 (Piper et al., 1994), which appears to have been the

    most severe glaciation on the Scotian margin. Conse-

    quently, Pleistocene sediments on the Scotian Slope and

    Rise are limited in thickness, reaching a maximum of

    about 1 km (Swift, 1987).

    On the western Scotian Slope, rapid deposition of

    fine-grained glacial debris has lead to wide spread small-

    scale slope failure, transporting material to the rise in

    the form of distal turbidites and debris flows (Swift,

    1985). Debris flow deposits on the rise appear to

    correspond to major glacial cycles, with deposits

    correlated back to isotopic stage 16 (Berry and Piper,1993). Layers of red-brown mud provide direct evidence

    of turbidity currents from the Gulf of St. Lawrence at

    the end of isotopic stage 12 (Piper et al., 1994).

    On the eastern Scotian Slope, hemipelagic sedimenta-

    tion occurred at a lower rate and was less prone to

    failure (Swift, 1985), and much sediment bypassed the

    shelf entirely through submarine canyons, located

    seaward of outer shelf banks (Fig. 1), leading to

    widespread deposition of turbidites and contourites on

    the eastern portion of the rise. Intercanyon areas of the

    Scotian Slope are characterized on sidescan sonar

    records and digital multibeam bathymetry by recent

    activity and slope failure (Piper et al., 1999b; Baltzer

    et al., 1994).

    3. Gulf of Alaska

    The southern continental margin of Alaska (Fig. 2) is

    an active, collisional setting, characterized by several

    allochthonous terranes that were assembled in their

    present-day positions during the Mesozoic and Cen-

    ozoic by the northward motion of the Pacific Plate

    against the North American Plate (Plafker et al., 1994).

    The Yakutat terrane is currently colliding with accreting

    onto the North American Plate in the Gulf of Alaska

    area, undergoing oblique subduction along the Fair-

    weatherQueen Charlotte transform fault (Plafker et al.,

    1994). Rotation of the Pacific Plate since 6 Ma has

    resulted in the rapid uplift of the FairweatherSt. Elias

    orogen, which as the greatest coastal relief on Earth, andis experiencing extremely rapid erosion (Meigs and

    Sauber, 2000). This orogen is responsible for the

    initiation of Late Cenozoic glaciation and the deposition

    of the 5 km thick Late Miocene-to-Recent Yakataga

    Formation (Armentrout, 1983; Lagoe et al., 1993).

    The Yakataga Formation is deposited within a

    forearc basin that has subsided throughout the Tertiary,

    with the rate of subsidence increasing since the latest

    Miocene. Using an assumed function for porosity of the

    Yakataga Formation, Gipp (1996) demonstrated that

    this subsidence can be explained by compaction and

    isostatic loading in response to rapid deposition of

    Yakataga Formation sediments, and may be partially

    accommodated by movement along the Dangerous

    River Zone. The great thickness of the Yakataga

    Formation is attributed to a combination of the

    glaciation and rapid uplift (Armentrout, 1983; Eyles

    et al., 1991), which has resulted in the greatest sediment

    yields in the world (Hallet et al., 1996). The Yakataga

    Formation is exposed in coastal mountains because the

    central portion of the Yakutat Block is currently

    undergoing uplift, which is accommodated along the

    Dangerous River Zone (Fig. 2).

    The strata of Yakataga Formation provide a detailed

    geological and paleontological record of Late Cenozoicclimate change (e.g., Eyles et al., 1992; Lagoe et al.,

    1993, 1994; Zellers, 1994). Paleomagnetic, biostrati-

    graphic, and K/Ar dating of glauconites from the

    lowermost Yakataga Formation established that glacia-

    tion in the Gulf of Alaska was initiated between 6.5 and

    5 M a (Lagoe et al., 1993) in agreement with sites

    elsewhere in the northern hemisphere (e.g., Jansen and

    Sjoholm, 1991; Geirsdottir and Eiriksson, 1994). The

    latest Miocene glaciation was followed by a warm

    interval that lasted through the mid-Pliocene, and by a

    major expansion of regional ice cover from 2.52 Ma

    (Eyles et al., 1991; Lagoe et al., 1993). The thickness of

    the Yakataga Formation can thus be related both to the

    longer time of deposition relative to the timing of

    Pleistocene glaciation in eastern Canada, and to high

    precipitation and rapid (10 m/ky) uplift of coastal

    mountains (Meigs and Sauber, 2000).

    The Yakataga Formation, which outcrops between

    Cape Yakataga and Icy Bay, has undergone about 25%

    crustal shortening (Plafker et al., 1994). Exposures on

    Middleton Island are virtually undeformed, although

    extensive exposures were elevated above sea level by the

    1964 Alaska earthquake (Plafker, 1965).

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    4. Physiographic characteristics and deposits

    Over 200 linekm of airgun and high-resolution

    seismic data were collected on the Scotian Slope,

    including alongslope and downslope lines. Nineteen

    cores were studied in order to characterize facies in shelf

    basins, and on the upper, middle, and lower slope

    (Fig. 1).

    Aerial photographs covering approximately 25 km2 of

    outcrops of the Yakataga Formation have been taken in

    the Robinson Mountains. Sections representative of

    outer shelf/upper slope, middle slope, and lower slope

    facies have been studied at Middleton Island, Icy Bay,

    and Cape Yakataga, respectively (Fig. 2).

    4.1. Scotian Shelf

    Cores and high-resolution seismic data collected on

    the Scotian Shelf (Fig. 1) can be integrated with previous

    work (e.g., King and Fader, 1986; Amos and Knoll,

    1987; Piper et al., 1990b; Gipp, 1994b; King, 1996; Stea

    et al., 1998) to produce a comprehensive catalogue of

    sedimentary facies and structural features. The Scotian

    Shelf has been divided into three physiographic zones

    the inner shelf, the middle shelf basins, and the outer

    shelf banks (King and MacLean, 1976).

    The inner shelf slopes gently seawards, but is highly

    irregular locally, with its topography controlled by

    bedrock. Overdeepended basins and valleys are filled by

    acoustically stratified sediments. Five physiographic

    zones have been defined, characterized by terminal

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    Fig. 2. Summary of tectonics of the Gulf of Alaska, showing the docking of the Yakutat terrane against the Chugach and Prince William terranes by

    the motion of the Pacific Plate. Locations of photographs in Figs. 710, including Middleton Island, are marked by circles. Interpreted cross-section

    of Yakutat Block modified from Ehm (1983). Location of modern submarine canyons in the northern Gulf of Alaska from Carlson et al. (1990) and

    Dobson et al. (1998). Zones of failed sediment on the modern shelf from Schwab and Lee (1992). Location of the shelf break is approximately

    denoted by the 200 m contour. Abbreviations as follows: YBYakutat Bay; CYCape Yakataga. Simplified from Plafker et al. (1994).

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    moraines, small basins, bedrock outcrop, smaller

    moraines, and modern erosion (Stea et al., 1998).

    The middle shelf basins are filled with Late Wisconsi-

    nan sediments, which unconformably overlie seaward-

    dipping Tertiary strata (King and Fader, 1986; Gipp

    and Piper, 1989; Piper et al., 1990a, b; Gipp, 1994b).

    Core lithofacies (Fig. 3) have been described followingthe scheme of Eyles et al. (1983). Sediments in shelf

    basins consist of a sequence of brown and olive-grey

    massive (occasionally weakly stratified) muds (Fm or

    Fl), which are frequently heavily bioturbated and

    contain abundant ice-rafted debris (- -d). Occasional

    sandy or silty interbeds are noted. Muds in the lower

    sections of the cores also contain abundant rolled

    sediment clasts (- -r). Cores from Emerald and LaHave

    Basins contain abundant shell material, and dates

    obtained have constrained the recovered sediments to

    the Late Wisconsinan and Holocene epochs (Gipp and

    Piper, 1989; Piper et al., 1990a; Piper and Fehr, 1991).

    On the basis of seismic profiles, Gipp (1994b)

    identified four acoustic facies in Late Wisconsinan

    sediments in Emerald Basin, which were attributed to

    the Scotian Shelf Drift, Emerald Silt, and LaHave Clay

    facies of King and Fader (1986), and to diffused gas insediment (Fig. 4). Seismic profiles show a basal acous-

    tically incoherent layer of uniform thickness (King and

    Fader, 1986). The basal layer is overlain by a draped

    acoustically stratified layer and topped by a ponded

    acoustically transparent layer (Emerald Silt and LaHave

    Clay ofKing and Fader, 1986). Other features identified

    on seismic profiles are: (1) buried subparallel ridges on

    the top of the basal layer (lift-off moraines of King and

    Fader, 1986), and interpreted as forming in transverse

    basal crevasses (Gipp, 2000); (2) tongue- and lens-

    shaped acoustically incoherent units interpreted vary-

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    111Fig. 3. Lithological description of cores from the Scotian Shelf and Slope. Lithofacies descriptions follow those of Eyles et al. (1983). Cores are

    depicted in order of increasing water depth. Vertical scale in metres. Note compressed vertical scale for cores 87-02 and 87-06. Dates from Gipp and

    Piper (1989), Piper and Fehr (1990) and Piper and Skene (1998).

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    ingly as till tongues (King et al., 1991) or debris flows

    (Gipp, 1994b; Stravers and Powell, 1997); 30 buried

    iceberg scours (Gipp, 1993); and (4) surficial or buried

    gas-escape features, or pockmarks (Hovland and

    Judd, 1988; Fader, 1991).

    The outer shelf banks are broad, flat mesas, which cut

    across seaward-dipping strata of Tertiary to Quaternary

    age (Boyd et al., 1988), and are covered by thick sands

    and gravels, which are reworked by shelf currents

    (Amos and Knoll, 1987). Few cores have been recovered

    from the outer shelf and uppermost slope, because the

    piston corer cannot penetrate sands and gravels, and the

    core catcher is not strong enough to support sediment

    that does not adhere to the liner. Sidescan sonar reveals

    the presence of abundant bioherms, predominantly

    composed of scallops (Fader, 1991). Seismic profiles

    rarely show anything below a highly reflective seafloor,

    because there is little penetration by acoustic energy,

    and the water is so shallow that multiples are closely

    spaced and of greater amplitude than reflections from

    depth.

    Relict tunnel valleys of Late Wisconsinan age occur at

    the surface on the Scotian Shelf between Sable Island

    and Cape Breton (Loncarevic et al., 1992) and are

    interpreted to have been formed by basal ice melting or

    catastrophic release of meltwaters. Similar anastomos-

    ing and overdeepened valleys, cut to depths >550 m

    below present-day sea level mapped on Sable Island

    Bank (Boyd et al., 1988) and on Banquereau (Amos and

    Knoll, 1987), are inferred to be older examples of such

    features. Boyd et al. (1988) demonstrated that the

    volume of meltwaters stored subglacially on the Scotian

    Shelf in unnamed basins landward of Banquereau, and

    in Brandal, Emerald, and LaHave Basins (Fig. 1) may

    have been as large as 490 km3, sufficient to have

    maintained a flow of 1 m/s through the largest tunnel

    valley for 9 days. Rising sea level, possibly due to local

    isostatic downwarping, may have acted as a trigger for

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    Fig. 3 (continued).

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    the release of these meltwaters by decoupling the ice

    sheet from its bed (e.g., Hughes, 1987). Catastrophic

    discharge of meltwaters was probably associated with

    large discharges of icebergs into the North Atlantic

    (Heinrich events, e.g., Heinrich, 1988), recording the

    collapse of the ice sheet margin, and acting as a major

    influence on submarine canyon development.

    4.2. Western Scotian Slope

    Sediments on the Scotian Slope typically consist of

    greyish brown to reddish brown bioturbated muds,

    usually massive, but occasionally laminated (Fm, Fl).

    The laminations are frequently deformed. The upper few

    metres are of Holocene age (Piper and Skene, 1998), and

    are usually free of dropstones, but both dropstones (- -d)

    and rolled sediment clasts (- -r) are common in the lower

    (Late Wisconsinan) portions of the cores. Chaotic

    deposits (C) are noted in some cores (Fig. 3), and are

    recognized by large numbers of rolled and distorted

    sediment clasts of varying overconsolidation, layered

    sediment clasts with widely varying shapes, and blocks

    of slightly deformed sediments, with recognizable

    internal structures that have been slightly deformed by

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    seafloor

    debris flow

    debris flow 160

    180

    140 m

    160 m

    180

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    200

    seafloor

    lift-off moraines

    0 1000 2000 3000 m

    seafloorpockmark

    hydrocarbon gas

    LaHave Clay

    0 1000 2000 m

    0 1000 2000 3000 m

    220 m

    240

    260

    Emerald Silt

    Emerald Silt

    Scotian Shelf Drift

    Emerald Silt

    (a)

    (b)

    (c)

    Fig. 4. Seismic profiles from basins on the Scotian Shelf, showing acoustic facies and typical features of proglacial marine sediments in shelf basins,

    including (a) Emerald Silt, Scotian Shelf Drift and debris flows; (b) lift-off moraines (Gipp, 2000); and (c) LeHave Clay, disseminated hydrocarbon

    gas and surficial pockmarks, or gas-escape structures (Hovland and Judd, 1988). Note vertical exaggeration.

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    folding and/or faulting. The chaotic deposits are all

    matrix-supported (Cm).

    On the basis of single channel airgun acoustic profiles,

    four acoustic facies can be defined. Facies S1 is

    acoustically stratified, characterized by continuous

    coherent internal reflections, which are approximately

    equal in both spacing and apparent reflectance. Theinternal reflections are continuous over a few to tens of

    kilometres. This facies is predominantly observed near

    the surface on the upper part of the slope, to depths of

    about 1000 m.

    Facies S2 is acoustically stratified, but characterized

    by discontinuous internal reflections. The reflections are

    coherent, but not continuous, and frequently show

    opposing dips at low angles.

    Facies S3 is an acoustically incoherent facies, devoid

    of internal reflections and often displaying a ponded,

    depression-filling geometry and an uneven upper sur-

    face, frequently with hyperbolic diffractions. It may

    form continuous (although uneven) units or discontin-

    uous lenses and wedges. Returns from underlying facies

    are strong, suggesting that very little energy is absorbed

    by this facies. Facies S2 has been interpreted as

    including debris flows, debris avalanches, and rotational

    slumps (Piper, 2001). This facies is also observed with a

    mounded appearance, particularly on slopes and fre-

    quently exhibits diapiric geometry (Fig. 5).

    Facies S4 is observed on the outer shelf and upper

    slope, and consists of a hard surficial reflection with no

    clearly identifiable continuous internal reflections. The

    apparent internal reflections are either discontinuous

    and high in amplitude, or, more likely, are the result ofscattering at the surface. This facies is only observed on

    the upper slope and outer shelf, and represents till or

    sands and gravels, and passes downslope into facies S

    (Fig. 5).

    On the basis of physiographic features interpreted

    from seismic profiles, Piper and Sparkes (1987) divided

    the Scotian Slope into an upper, middle, and lower

    slope. The upper slope, from the shelf break to about the

    500 m isobath, is characterized by a steep slope (51), and

    a highly reflective seafloor (Fig. 5), which allows little

    penetration of seismic energy (facies S4).

    Submarine canyons, 24 km wide and up to 500 m

    deep, are observed on the upper slope (Fig. 6), seaward

    of the outer shelf banks (Fig. 1). As in the shelf basins

    and banks, iceberg scouring appears to have been a very

    important reworking process (Pickrill et al., 2001).

    Pockmarks are not observed, probably because the

    sediments are too coarse to entrap gas.

    The middle slope, to about 1000 m water depth,

    consists of acoustically stratified sediments (facies S1

    and S2) dissected by canyons, with a wide range of sizes

    (5002000 m wide and 150350 m deep) (Fig. 6). These

    canyons are not observed in water depths greater than

    1300 m; whereas the canyons on the eastern Scotian

    Slope extend to the continental rise (Pickrill et al., 2001).

    Canyon geometry compares favourably with modern

    submarine canyons investigated by sidescan sonograms

    and seismic profiles (e.g., Hugh Clarke et al., 1990;

    Pratson et al., 1994). Buried canyons are also observed,

    and are o1 km wide and 200 m deep, making them

    much smaller than the active canyons (Fig. 6). Theactive canyons commonly show evidence of repeated

    incision after partial infill. Canyon C in Fig. 6, for

    instance, shows at least two incision events which

    happened after the initial canyon-cutting event. Sub-

    sequent incisions are probably related to repeated

    discharge of sediment-laden meltwater during times of

    glacial retreat and repeated sediment failure. The larger

    slope canyons on the eastern slope may be incised (and

    reincised) by the meltwater discharges from subglacial

    tunnel valleys.

    Canyon cutting began at about the beginning of the

    Pleistocene, likely due to lowered sea levels (Piper et al.,

    1999a). Subsequent deposition infilled the canyons on

    the western part of the slope, whereas those on the

    eastern slope were maintained by erosion (Swift, 1987).

    A second episode re-excavated canyons in the latest

    Pleistocene (Figs. 5 and 6). On the basis of their

    morphology, canyon excavations are thought to have

    been caused by turbidites, either related to a lowered sea

    level, to the formation of tunnel valleys on the shelf

    banks, or to proximal ice margins. The relative lack of

    canyons on the western slope has been interpreted to

    suggest a more distal ice margin (Swift, 1987), but

    according to Grant (1989), major ice streams are likely

    to have flowed through Emerald and LaHave Basinsthrough to the Scotian Gulfconsequently, the western

    Scotian Slope to Browns Bank Would be expected to

    have a proximal ice margin.

    The intercanyon seafloor is characterized by numer-

    ous features suggestive of slope failure (Piper et al.,

    1999b), including large-scale rotational failures which

    pass into eroded seabed (Baltzer et al., 1994). The base

    of the erosion is commonly planar, corresponding to

    particular bedding planes, and therefore represents

    block failure (Piper, 2000). Pockmarks are commonly

    observed on sidescan sonar profiles on the eastern slope,

    particularly between 500 and 900 m depth (Baltzer et al.,

    1994), and the presence of free gas within sediments

    likely adds to sediment instability (Piper et al., 1999a).

    Actual failure may be attributed to fluid overpressures

    associated with iceberg loading (Mulder and Moran,

    1995), earthquakes (Mosher et al., 1994), or sublimation

    of gas hydrates (Piper et al., 1999a).

    Sediment cores from the middle slope usually include

    a thin (o1 m) surficial layer of sandy silt, which is

    commonly bioturbated, and which likely represents a lag

    deposit (Piper, 2001). These silts overlie massive to

    laminated bioturbated muds and silts (Fig. 3). Drop-

    stones and overconsolidated clay rafts are present in

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    sediments (o5 m deep), but appear to be absent in the

    uppermost (postglacial) sediments.

    The lower slope, down to the continental rise

    (B2000 m) is characterized by a slope ofB21, and by

    the appearance of seismic facies S3, showing lenticular,

    ponded, or diapiric geometries (Figs. 5 and 6). Sedi-

    ments of facies S3 are interbedded with facies S1.

    Further downslope, in water depths >2000 m, there is a

    decrease in slope due to the ponding of thicker debris

    flows on the continental rise (Fig. 5). Turbidite se-

    quences are inferred on the Scotian rise (Berry and

    Piper, 1993). Pockmarks are observed on the lower

    slope, down to water depths of 2200 m (Piper, 2001),

    although they are not as common as they are on the

    middle slope.

    Cores from the lower slope show a variety of muds,

    including sediment rafts and disseminated gravel and

    dropstones, but also include chaotic deposits which

    incorporate folded and faulted blocks of laminated

    muds and concentrically banded clay rafts. Unlike the

    muds with sediment rafts, the chaotic facies are

    dominated by deformed resedimented material (Fig. 4).

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    Fig. 5. Downslope seismic profiles. (a) The change in acoustic character from upper slope sediments characterized by poor penetration to middle

    slope sediments with clear stratification and the development of structures, such as gullying is likely due to the downslope thinning of sand sheets that

    have been swept off the outer shelf banks, and the predominance of finer grained sediments. (b) Acoustically stratified lower slope sediments show a

    variety of deformation structures, including diapirs and slope failures.

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    Fig. 6. Seismic profiles from the Scotian Slope, showing submarine canyons and their associated downslope facies. (a) On the upper slope, large

    canyons are incised into poorly stratified (presumably sandy) sediments. Feeder channels are not apparent. Channel C may have undergone more

    than one episode of canyon cutting. (b) On the middle slope, canyons of all sizes are noted, and buried canyons are apparent. Canyons AC can be

    correlated from the upper slope to the middle slope. Note that these canyons have all been incised to different depths. (c) On the lower slope, canyons

    are not apparent, but the stratified sediments consists largely of thin, lenticular deposits of variable extent, interpreted as debris flows (Gipp, 1996).

    (d) Sediments on the continental rise consists of much thicker (>100 m) debris flows. The seafloor is very uneven, probably due to sediment failure

    and diapirism.

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    The uppermost (Holocene) sediments of these cores are

    commonly bioturbated, and contain no dropstones.

    On the western slope, there is a noted downslope

    facies change from stratified muds with abundant

    sediment clasts, to slump deposits and debris flow.

    Debris flows are noted to have started being deposited

    dating from the pliocene (Piper et al., 1999a), suggestingthat glaciation is not the only cause of sediment failure.

    4.3. Gulf of Alaska

    4.3.1. Outer shelf

    Outcrops of Yakataga Formation sediments on

    Middleton Island form a succession about 1.25 km thick

    which is characterized by thick sandy to silty matrix-

    supported diamictites, interbedded with graded and

    ungraded sands and gravels, and minor laminated and

    massive muds (Miller, 1953; Plafker and Addicott, 1976;

    Eyles, 1987, 1988; Eyles and Lagoe, 1990).

    The diamictites are poorly sorted sandy muds with

    abundant dispersed gravels. The gravels range in size

    from granules to boulders, and include striated and

    faceted clasts. Diamicts may be massive or stratified, but

    stratification, where present, is generally weak (Eyles

    and Lagoe, 1990). Deformation features are common

    and include rafts of muds emplaced within the

    diamicities (Fig. 7a) and injection structures (Eyles and

    Lagoe, 1990). Other structures noted within the

    diamictite include coquinas (Fig. 7b), boulder pave-

    ments (Fig. 7c), and deformed laminated sands and silts

    (Fig. 7d). Massive diamicts are thought to represent

    deposition by a combination of suspension rain-out andice rafting (Miller, 1953), whereas the deformed

    diamictites represent remobilized sediment (Eyles and

    Lagoe, 1990). They are likely related to the sediment

    failure in response to storm-wave loading or tectonic

    shock. Similar failures are noted on the present-day Gulf

    of Alaska continental shelf (Fig. 2), especially seaward

    of major glacial outlets such as Icy Bay and Yakutat

    Bay (Schwab and Lee, 1992).

    Coquinas are composed of pecten shells on a gravelly

    substrate, are usually only a few centimetres thick, and

    extend over 100m (Eyles and Lagoe, 1989). Boulder

    pavements are lateral concentrations of striated

    boulders, which appear to have been loaded into a

    softer substrate, and planed off along the former

    bedding plane (Eyles, 1988). Laminated sands and silts

    include ice-rafted debris, and are frequently strongly

    sheared, Similar to proglacial sediments that have

    undergone subglacial deformation ( !O Cofaigh and

    Dowdeswell, 2001). On Middleton Island, the deforma-

    tion is highly localized and occurs near features

    suggestive of ploughing (Fig. 7e and f), and may be

    related to the impact of floating ice on the seafloor.

    Sediments at the base of the exposed section form a

    submarine channel system filled with a complex series of

    sandy and gravelly facies (Eyles, 1987). Small cut-and-

    fill channels, on the order of a few metres across and

    deep, are filled with a variety of normally graded,

    inversely graded, and ungraded sandstones, diamictites,

    and conglomerates (Fig. 8ad). They occasionally un-

    dercut their sidewalls (Fig. 8c) and incorporate large

    contorted sediment rafts in their fill (Fig. 8d). Largerchannels are also apparent (Fig. 8d), which are up to

    500 m across and 70 m deep (Eyles and Lagoe, 1990).

    Sediments exposed on Middleton Island glacially

    influences on the deposition of outer shelf and upper

    slope sediments. The dominant sediment types represent

    deposition by suspension rain-out and ice rafting, and

    show the influence of bottom traction currents, ice

    scour, and sediment failure due to tectonic shock or

    storm-wave loading. They have been interpreted to

    represent deposition on the outer margin of a glacially

    influenced continental shelf (Eyles et al., 1991). Given its

    present physiographic setting, it is likely that Middleton

    Island is an analogue for the banks on the outer part of

    the Scotian Shelf.

    4.3.2. Continental slope

    Yakataga Formation outcrops between Cape Yaka-

    taga and Icy Bay (Fig. 9) consist of massive and

    laminated sandstones, massive mudstones, and both

    massive and stratified diamictite facies. Sandstones and

    mudstones are interpreted as turbidites (Eyles et al.,

    1991). Massive diamictites consists of a sandy and silty

    matrix supporting scattered clasts and shells and may

    display tabular or lenticular geometry. Stratified dia-

    mictites are clast-rich and include sediment clastsconsisting of deformed sandstone. These olistoliths

    range in size from a few centimetres to some tens of

    metres in length.

    Features observed in Icy Bay outcrops include

    olistoliths loaded onto muds (Fig. 9a); large submarine

    canyons, up to 4 km wide and 750 m deep, previously

    identified as megachannels (Armentrout, 1983), only

    identifiable because of the extent and quality of the

    outcrop (Fig. 9a); large (up to 20 m) sediment loads and

    diapirism at the tops and bases of muddy units ( Fig. 9b);

    and lenticular debris flows interbedded with stratified

    sands and silts over a range of scales (Fig. 9c and d).

    Many of the features exposed in the Yakataga Forma-

    tion near Icy Bay resemble features interpreted from

    seismic records on the middle Scotian Slope.

    Submarine canyons are filled with basal conglomer-

    ates, which fine upwards into turbiditic sandstones and

    heavily bioturbated mudstones (Eyles et al., 1992). They

    are comparable to submarine canyons described in other

    outcropping marine sediments (e.g., Morris and Busby-

    Spera, 1988). Microfauna in the canyon-fill sediments

    suggest that they formed in outer neritic to upper

    bathyal water depths, but debris flows in these canyons

    contain displaced shallow-water foraminifera (Lagoe

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    et al., 1994). Active submarine canyons in the northern

    Gulf of Alaska show a dendritic pattern, which has been

    modified in places by compressive ridges around which

    some of the canyons meander (Fig. 2). Modern canyons

    are commonly 5 km wide and may be greater than 1 km

    deep, with individual canyons as much as 12 km wide

    (Carlson et al., 1990; Dobson et al., 1998).

    Lenticular and tongue-shaped deposits of massive

    sands and diamictites (Fig. 9c and d) are exposed near

    Icy Bay. Topologically, these appear similar to debris

    flows observed in seismic profiles on the Scotian Shelf

    and upper slope. In detail, these can be seen to have a

    depression-filling geometry, and demonstrate little basal

    scour, and are commonly interbedded with turbidites.

    The oldest sediments of the Yakataga Formation are

    exposed at Yakataga Reef, across a wave-cut platform

    raised above sea level by the 1964 Alaska earthquake

    (Fig. 10a). The first appearance of dropstones marks the

    onset of tidewater glaciation during the latest Miocene

    (Lagoe et al., 1993). The strata at Yakataga Reef are

    dominated by fine-grained graded sandstones and

    mudstones, interpreted as turbidites, with a single

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    Fig. 7. Facies and features exposed on Middleton Island. (a) Detail of coquina, which is composed of pectin shells and abundant gravel, and can be

    traced laterally over hundreds of metres (Eyles and Lagoe, 1989). (b) Outcrop of boulder pavement exposed on Middleton Island. Note that the

    planation of the boulders, which is also striated, dips towards the right at an angle of about 25 1. (c) Finely laminated sands and silts, including

    dispersed clasts and sandy and gravelly sediment clasts, representing ice-rafted debris. (d) Mud rafts incorporated into sandy sediments. (e) Possible

    ice scour, showing erosive centre and berm. (f) Detail of scour deformation, showing normal faulting of underlying sediments.

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    stratified diamictite unit approximately 20 m thick

    (Fig. 10d). Individual thin debris flows can be identified

    amongst the turbidites as ungraded sands with clay rafts

    (Fig. 10b). The turbidites exhibit extensive bioturbation

    and carry abundant shells and their imprints.

    The diamictite exhibits complex stratification and

    numerous rock and sediment clasts and abundant soft-

    sediment deformation structures. It exhibits a broadly

    channelized geometry, and its basal contact is sharp and

    slightly scoured, penetrating into the underlying turbi-

    dites (Eyles et al., 1991).

    Depositional depths estimated from foraminiferal

    assemblages suggest that the sediments have been

    deposited glacially derived outer shelf and upper slope

    sediments and remobilized downslope, presumably as a

    result of seismic shock (Eyles et al., 1991). Such an

    interpretation is supported by calculations showing that

    several kilometres of sediment could be accommodated

    in a shallow forearc basin B500 m deep, assuming

    normal compaction and isostatic adjustment in response

    to the weight of the sediments (Gipp, 1996).

    4.4. Features common to the Scotian margin and in the

    Gulf of Alaska

    Many glacial marine sedimentary processes are

    expected to be common to both study areas, although

    their recognition is often difficult because of the

    different databases available in the two study areas.

    These similarities allow sediment facies types and

    structures to be compared, which is a useful exercise

    as the types of information revealed in outcrop is

    different in scale than that inferred from seismic profiles.

    4.4.1. Submarine canyons

    Submarine canyons are recognized on both margins,

    where they typically have gullied walls and numerous

    minor tributary canyons, which feed sediments from the

    continental shelf and upper slope to the lower slope and

    continental rise (e.g., Dobson et al., 1998; Weaver et al.,

    2000).

    Submarine canyons on the eastern margins of North

    and south America appear to be restricted to areas of

    high Neogene sedimentation (Emery and Uchupi, 1984),

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    (b)

    (c)

    (a)

    Fig. 8. Details of gravelly cut-and-fill channels on Middleton Island. (a) Detail of side wall of a cut-and-fill channel shows undercutting of incised

    diamictite, suggesting erosion by sediment-charged waters under high hydrostatic pressure. Arrow shows bedding plane of incised diamictite. Note

    hammer for scale, left of centre. Stratigraphic top to top of photograph. (b) Two cut-and-fill channels, one infilled with normally graded fine

    conglomerate and sandstone (black arrows), the other steeply incised into the first. Stratigraphic top to right. (c) Reworked sediments raft

    incorporated in channel-fill conglomerate. The deformation of the diamictite suggests that channels have been cut into unlithified sediment.

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    including the glaciated margin of North America andthe mouths of large river systems. Similar spatial

    distribution has been noted on the eastern Atlantic

    margin, with canyons noted on the glacially influenced

    portion of the margin (Weaver et al., 2000). Sediment

    supply, therefore, plays an important role in their

    formation.

    Tectonic setting also plays an important role in

    governing the formation of submarine canyon systems.

    The low tectonic gradient and the presence of a board

    continental shelf inland of the Scotian Slope permitted

    the storage of large volumes of meltwaters which, when

    suddenly released, carved deep canyons across the Sable

    Island Bank to the top of the slope (Boyd et al., 1988;

    Loncarevic et al., 1992). Such discharges must have

    played a key role in the development of the large

    submarine canyons on the eastern part of the Scotian

    Slope, where broad banks on the outer shelf acted as

    grounding points for an ice sheet that could dam up

    these waters. In the Gulf of Alaska, by contrast, rapid

    subsidence created a steep regional slope and the lack (at

    least initially) of a broad shelf meant that there was little

    storage space for subglacial meltwaters. Discharges of

    meltwater were thus small and of less importance in the

    development of submarine canyon systems. Submarine

    canyons in the Gulf of Alaska must have formed by thesteady erosion of numerous turbidity currents rather

    than a few large discharges, and are thus similar in

    origin to the submarine canyons on the western Scotian

    Slope. The canyons on the western Scotian Slope are

    most deeply incised on the upper slope, and become less

    prominent downslope, until they are not visible on the

    lower slope (Fig. 6), suggestion that the Icy Bay section

    represents the upper to middle slope. The geometry and

    dimensions of the Icy Bay canyons are very similar to

    those of the Scotian Slope (Pickrill et al., 2001).

    Tectonic setting may also influence the orientation of

    canyon systems, especially the variability in flow

    directions through time. Submarine canyons on the

    Aleutian arc are deflected away from regional slope and

    into forearc basins by compressive ridges (Dobson et al.,

    1991). Present-day upper slope canyon systems in the

    Gulf of Alaska are similarly influenced by compressive

    ridges (Carlson et al., 1990), which are caused by folding

    and thrusting associated with crustal foreshortening

    observed on the Yakutat Block (Plafker et al., 1994).

    The deep-water fans associated with modern canyons in

    the Gulf of Alaska are gradually translated away from

    sedimentary point sources by the motion of the Pacific

    Plate (Dobson et al., 1998). By contrast, submarine

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    Fig. 9. Outcrops and features exposed in the Robinson Mountains near Icy Bay. (a) Large section showing olistoliths (or boundinage?) due to

    downslope failure, submarine canyon (at right) and progressive tilting of block due to deformation in the Pamplona Zone. All sediments were

    originally horizontal. (b) Large (>30 m) sediment loads observed at two distinct horizons. (c) Lenticular debris flow (maximum thickness about

    30 m) and small channels (arrows denote erosive base of channels). (d) Interbedded debris flow and turbidites in Yakataga Formation sediments in

    Icy Bay. Section is 2 m thick.

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    canyons on the Scotian Slope appear to trend directly

    downslope. Little meandering is noted for canyons on

    the Atlantic margin of the North America (Emery and

    Uchupi, 1984), although it should be noted that a

    branching dendritic pattern of tributary channels may

    lead to local variations in channel orientation exceeding

    901.

    4.4.2. Sediment failure

    Evidence for diapirism and sediment loading is

    present in both study areas, indicating that rapid

    downslope sediment reworking is common to both

    margins (Figs. 5, 9 and 10). Olistoliths are common in

    middle and upper slope outcrops of the Yakataga

    Formation (Fig. 9), but there is only circumstantial

    evidence for them on the Scotian Slope. Apparent

    bedding plane failures in canyons (especially in canyon

    A in Fig. 6) may be expected to have produced large

    blocks of sediment that have been incorporated into

    debris flows, or remain as olistoliths.

    Block failures may be inferred on the lower Scotian

    Slope (Piper, 2001), and sidescan sonograms and digital

    multibeam bathymetry imagery both show relatively

    recent large-scale bedding-plane failures on the middle

    slope (Baltzer et al., 1994; Piper et al., 1999b). Such

    events in older sediments may have resulted in

    olistoliths, but features of the scale observed in outcrop

    are too small to be resolved in seismic profiles and too

    large to be clearly identified in boreholes or piston cores.

    Rolled sediment clasts record episodes of sediment

    failure and are observed in most piston cores on the

    western Scotian Slope. Geotechnical measurements of

    the sediment blocks observed within chaotic facies of

    piston cores show that many of them are extremely

    overconsolidated, suggesting that the depth of burial of

    the original sediment (and consequently the failure

    depth) frequently exceeded 50 m (Mulder et al., 1997).

    Wedge-shaped acoustically transparent bodies on the

    Nova Scotia continental margin are lenticular in cross-

    section, and have been interpreted as debris flows based

    on detailed seismic stratigraphic and geometric work

    (Gipp, 1994b) Similar debris flows have been described

    from seismic records on the Norwegian Shelf (King

    et al., 1991), the Baffin Island Shelf (Stravers and

    Powell, 1997), the Newfoundland Slope (Aksu and

    Hiscott, 1992), the Hebrides Slope (Baltzer et al., 1998),

    and many are recognized on the Scotian Slope (Fig. 6).

    Unfortunately, cored intervals through these features

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    Fig. 10. (a) Aerial view of Cape Yakataga shows interbedded turbidites and thick diamictite bed. Stratigraphic top is towards the bottom of

    photograph. (b) Massive sandstone and muddy sediment rafts in Cape Yakataga turbidites. Arrowed raft is 5 cm in diameter. (c) Muddy facies with

    scallop valve impression in Cape Yakataga turbidites. (d) Chaotically stratified diamictite, representing a slump deposit or debris flow. Boulders at

    centre is 50 cm in length.

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    are very rare, and their sedimentology remains unclear.

    One cored debris flow has been described as a chaotic

    deposit of overconsolidated sediment clasts in a poorly

    consolidated muddy matrix (Piper, 2001).

    Debris flows are also present in slope facies within the

    Yakataga Formation, particularly near Icy Bay (Fig. 9),

    and at Cape Yakataga (Fig. 10). These appear as verythin, apparently tabular beds containing rip-up clasts, as

    chaotically bedded diamictites (Fig. 10b), with channe-

    lized or wedge-shaped geometries.

    Sediment instability on the upper Scotian Slope is

    related to the high sensitivity of undisturbed sediments,

    meaning that their undrained shear strength is much

    greater than their remoulded strength. Failure may be

    triggered by cyclical wave loading during storms,

    possibly amplified by simultaneous iceberg-seabed im-

    pacts (Bolen, 1987), or ice loading (Mulder and Moran,

    1995), neither of which is likely to be of significance in

    water depths greater than 500 m. Sediment instability on

    the middle and lower slope has a number of possible

    triggers, including tectonic shock (Mosher et al., 1994),

    the migration of hydrocarbon gas (Piper et al., 1999a),

    and the inability of pressurized fluids to escape through

    a cap of relatively impermeable sediment (Piper, 2001).

    The Brand Banks 1929 earthquake resulted in massive

    turbidity currents, moving 175 m3 of sediment down-

    slope (Piper et al., 1988). Seismic activity has been a

    major factor in the Gulf of Alaska (Hampton et al.,

    1987), although other possible mechanisms such as gas

    seeps and dewatering cannot be ruled out.

    4.4.3. CoquinasCoquinas have been noted on Middleton Island

    (Fig. 7a), and are composed primarily of pectinids

    (Eyles and Lagoe, 1989). The presence of broken valves

    and shell debris suggests that local sediment starvation,

    wave reworking and scouring of the substrate are a

    factor in their formation.

    Similarly, scallop beds are commonly detected atop

    banks on the outer Scotian Shelf at present, where they

    are recognized on sidescan sonograms as small zones of

    enhanced seafloor reflectivity and are often less than

    2500m2, although larger ones are possible (Fader,

    1991). They tend to be very closely spaced, and may

    be related to areas of gas venting (Levy and Lee, 1988).

    Given the physiographic similarities between Middleton

    Island and the banks of the outer Scotian Shelf, scallop

    beds and coquinas are probably analogous. Their

    abundance on the outer Scotian Shelf also suggests that

    they would probably be very common in outer shelf

    sediments where these are preserved, and that no great

    climatic significance needs to be attributed to them.

    4.4.4. Boulder pavements

    Planar concentrations of striated boulders are ob-

    served in diamictite facies on Middleton Island (Fig. 7b).

    On the basis of the parallel striations on all of the

    boulder, and their loading into underlying sediments,

    these boulder pavements were interpreted to have

    formed when boulder and cobble lag horizons were

    overridden and striated by a buoyant ice shelf (Eyles,

    1988). Lag boulder horizons in the glacial marine setting

    may be formed by: (1) wave and current winnowing; (2)iceberg scouring, particularly during storms; or (3)

    loading of clasts into fine material by floating ice on a

    very shallow or emergent platform.

    There is no direct evidence for boulder pavements on

    the outer Scotian Shelf; however, the author has

    encountered a boulder pavement during a geotechnical

    drilling program at the current site of the Hibernia

    platform, on the Grand Banks of Newfoundland. This

    buried boulder horizon likely resulted from iceberg

    impacts on a locally sediment-starved and winnowed

    area. As these are conditions we would expect to have

    existed on the Scotian Shelf, there may be boulder

    pavements in the sediments of the outer banks.

    4.4.5. Ice scour

    Recognition of ice scour in sediments is a difficult

    problem, and few field observations are documented in

    the literature (Eden and Eyles, 2001). Possible scour

    features are observed on Middleton Island in conjunc-

    tion with highly localized distortion, including the

    downward piercement of sedimentary horizons and

    stretched and faulted sediments below the scours

    (Fig. 7). Observations resemble the not only ice scours,

    but deformed sediment suggestive of the ice keel

    turbates exposed in Pleistocene sediments in theScarborough Bluffs in Toronto, Canada (Eden and

    Eyles, 2001). Scouring by floating ice was probably an

    important process in the Gulf of Alaska, but due to the

    uncertainty of the water depth, it is unclear if this

    scouring would be caused by icebergs or by pans of sea

    ice.

    Ice scour has been an important process on the shelf

    and upper slope of the Scotian margin (King and Fader,

    1986; Gipp, 1994b; Pickrill et al., 2001). Due to the

    extreme depths (often >200 m), the scours are almost

    certainly the result of icebergs. Iceberg scour directions

    have been used to infer dominant current or wind

    directions (Gipp, 1993).

    5. Models of the development of the Scotian Shelf and

    Slope, and the Gulf of Alaska

    On the basis of single- and multichannel seismic data,

    piston cores, sidescan sonar and digital bathymetry

    images, and study of exposures of sediment along

    coastal mountains, generalized sedimentation models

    for glacially influenced continental margins have been

    developed for the Scotian margin and for the Gulf of

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    Alaska. These models are presented as a series of

    illustrations showing dominant depositional processes,

    tectonic activity, and resultant stratal geometry from a

    typical cycle or sequence of glacial cycles.

    5.1. The Nova Scotia continental margin

    5.1.1. Ice advance

    Ice advance (Fig. 11a) occurs during a fall in eustatic

    sea level. A thin sheet of glacial ice advances across the

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    Fig. 11. Model of Pleistocene development of the Nova Scotia continental margin representing (a) glacial advance, (b) glacial maximum, and (c) late

    glacial retreat. Numbers on the diagram label processes referred to in text according to the following: (1) proglacial muds, including sediment raining

    from suspension and ice-rafted debris; (2) massive lenticular debris flows at points of sediment instability on slopes; (3) subglacial meltwater stream

    outlet, releasing sediment-charged fresh water; (4) icebergs and ice-rafted debris; (5) small debris flows of uncertain geometry; (6) steep-sides incised

    channels, filled with gravels and sands; (7) large submarine canyons, which (8) progressively widen and shallow downslope; (9) sediment failure in

    intercanyon areas; (10) overdeepened shelf basins carved by subglacial meltwaters under high hydrostatic pressure; (11) subglacial tunnel valleys; (12)

    gas-escape structures (pockmarks); (13) bioherms and shell beds on the modern shelf banks; and (14) icebergs (from coastal glaciers) and currents

    winnow coarse gravels into lag boulder horizons. Modified after Gipp (1996).

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    shelf, crossing Cretaceous and Tertiary seaward-dipping

    beds. A thin layer of pre-existing proglacial sediments

    (1), deposited during a previous glacial retreat or ahead

    of the advancing ice, acts as a deforming bed to aid ice

    advance (Hart and Boulton, 1991). The advancing ice

    planes off the most recent sediments, locally eroding

    into bedrock, especially along pre-existing structuralweaknesses, which become overdeepened (e.g., Ehlers,

    1990). Although some of this sediment will remain on

    the shelf in the form of a basal or deformation till (King

    and Fader, 1986), most of it is removed. If the ice is

    sufficiently thick when it reaches the shelf edge, it may

    advance a short distance downslope, depositing till

    tongues (Mosher et al., 1989), debris flows (2) (Bonifay

    and Piper, 1988), or turbidity currents, which may be

    funnelled into submarine canyons and gullies (7) (e.g.,

    Piper et al., 1988). Other sediment is suspended in

    subglacial meltwaters (3) and dropped from icebergs (4)

    (Powell and Molnia, 1989).

    5.1.2. Glacial maxima

    During glacial maxima (Fig. 11b) lenticular bodies of

    till (King and Fader, 1986; Mosher et al., 1989) form

    along the glacier margin. These sediments may be

    reworked downslope into debris flows (5) and turbidites,

    draped by hemipelagic sediments. The upper slope

    deposits consist of debris flows (composed of eroded

    bedrock and reworked shelf sediments), proglacial

    sediments, and ice-rafted debris overlain by finer silts

    and muds (Eyles, 1993). On the uppermost slope,

    ephemeral channels as small as a few metres deep and

    10 m wide, are cut by turbidity currents (6) and filledwith sands and gravels.

    Intercanyon sediments on the upper and middle slope

    may be remobilized (9) by storms, tectonic activity

    (Hampton et al., 1987; Piper et al., 1988), gas hydrate

    phase changes (Locat, 2001), or by increased bearing

    stresses related to the weight of ice on the outer

    continental shelf (Mulder and Moran, 1995). The rapid

    deposition of sediments on the upper slope leads to

    sediment instability and likely slope failure. On the

    lower and middle slope, failure occurs because muddy

    proglacial sediments are relatively impermeable com-

    pared to the underlying sediments, causing sediment

    instability where the overburden is thinner. Fluid

    overpressures may be cause by migration of ground-

    waters down the pressure gradient (from thick over-

    burden to thinner overburden) (Dugan and Flemings,

    2000), migration of hydrocarbon gas resulting from the

    sublimation of gas hydrates (Piper et al., 1999a), or by

    dewatering of buried sediments.

    Overdeepened troughs form on the shelf at the

    boundary between crystalline and sedimentary bedrock

    by ice and subglacial meltwaters under high hydrostatic

    pressure (10) and act as storage areas and conduits for

    meltwaters, which can carve subglacial tunnel valleys

    (11) when they are released (Boyd et al., 1988;

    Loncarevic et al., 1992). Such sediment-charged melt-

    water outbursts are most likely to cascade downslope in

    the form of turbidity currents, deepening pre-existing

    submarine canyons or gullies (7), or eroding new ones.

    Submarine canyons may also form by the progressive

    gullying caused by repeated sediment failure. They maybe up to 500 m deep and 4 km wide, but become broader

    and shallower on the lower slope (8) for two reasons: (1)

    they are filled in by debris flows and turbidites, and (2)

    the erosive power of the flows decreases as they disperse

    downslope.

    The lower slope is characterized by thin lenticular

    debris flow deposits downslope of the canyons (2)

    (Fig. 6). On the rise, the debris flows are thicker and are

    Shingled (e.g., Aksu and Hiscott, 1992; Baltzer et al.,

    1998). As these sediments are unstable, subsequent

    sediment loading may lead to the development of mud

    diapers (Fig. 5).

    5.1.3. Ice retreat

    As the ice retreats (Fig. 11c), the sequence is

    blanketed by a seaward-thinning prism of proglacial

    muds (1). Shelf depressions, including overdeepened

    basins and tunnel valleys, are infilled by a sequence

    consisting of a thin basal till layer (likely deformation

    till) covered by heavily bioturbated muds with drop-

    stones and sediment rafts (1) (Gipp, 1994b; King, 1996).

    The Entire sequence may be over 100 m thick (King and

    Fader, 1986), yet despite this thickness, its preservation

    potential remains poor, as it is likely to be planed off by

    subsequent glacial advances.Where fine sediments are exposed the seafloor is

    marked by circular gas-escape structures up to 400 m

    wide and 20m deep (12), known as pockmarks

    (Hovland and Judd, 1988). The gas is supplied from

    older hydrocarbon-bearing strata, phase changes in gas

    hydrates, or from the decay of organic material within

    the most recent sediments. The eruptive nature of the

    gas release from the sediments may become a factor in

    sediments instability on the upper slope (Locat, 2001).

    Gas seeps in sandy outer shelf sediments do not form

    pockmarks, because the gas can seep out without being

    trapped by fine sediments, but may become sites for

    bioherm accumulation (13) (Levy and Lee, 1988).

    Subsequent glacial advances will destroy pockmarks

    on the shelf, but pockmarks on the slope may be

    preserved through burial.

    During interglacials, the sedimentation rate on the

    shelf and upper slope declines. Sedimentation within the

    shelf basins consists of remobilized inner shelf sediments

    reworked by rising sea levels and hemipelagic sediments.

    Pockmarks may become greatly enlarged during this

    time (Gipp, 1994b). Storm-wave activity reworks sands

    and gravels on the outer shelf, occasionally sweeping

    sands over the shelf break and down the slope, and also

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    rewards upper to middle slope muds, leaving a relatively

    coarse lag (Piper, 1991). Sands which are swept into

    slope canyons may ignite small turbidity currents,

    cutting networks of small channels into the canyon

    heads (Baltzer et al., 1994). Canyons which survive infill

    during deglaciation are probably enlarged by storm-

    driven downvalley surges (Shepard, 1979), headwarderosion (Farre et al., 1983), cold seeps of pressurized

    fluids on the lower slope (Dugan and Flemings, 2000),

    or lateral expulsion of hydrocarbon gas from sublimated

    gas hydrates. Interestingly, the presence of the canyon

    may add to the stability of nearby intercanyon

    sediments by allowing for pressurized fluids to escape

    laterally into the canyon (Piper et al., 1999a). Small

    tributary channel feeding submarine canyon systems are

    likely to be completely filled during this phase.

    Presently, on the Scotian Shelf, a thin (o100 m)

    veneer of Quaternary sediments rests unconformably on

    Tertiary and Cretaceous bedrock (King and Fader,

    1986). Glacial marine sediments which predate the last

    glacial cycle are rare (o1 km over 1000+line km

    surveyed), and only occur where bedrock highs offer

    some protection from glacial erosion.

    5.2. Gulf of Alaska

    In the Gulf of Alaska, rising mountain ranges

    intercepted moisture-laden air masses from the Pacific

    Oceanthe resulting orogenic precipitation initiated

    alpine glaciers, which supplied large volumes of

    sediment to the forearc basin (Hallet et al., 1996). The

    absence of a broad continental shelf prevents glacial icefrom advancing far offshore (Fig. 12a). Sediment

    accumulates in front of the glacier terminus, and is

    resedimented downslope in the form of debris flows (2)

    and turbidites. The initial depth of the forearc need not

    be significant, as subsidence caused by sediment

    compaction and isostatic loading allows it to accom-

    modate tremendous thicknesses of sediments (Gipp,

    1996).

    Submarine canyons (7) are incised on the upper slope

    by the entrainment of turbidites, and broaden down-

    slope. They do not necessarily follow regional slope, but

    will drain towards the centre of the forearc basin, the

    location of which will vary through time (Dobson et al.,

    1991).

    Ice rafting (4) supplies coarse material into the basin,

    as dropstones in otherwise fine-grained sediments.

    Debris flows and turbidity currents, caused by rapid

    deposition on the upper slope, combined with ice push,

    tectonic shock, and storm-wave loading, also move

    coarse sediments downslope (Hampton et al., 1987).

    The rapidly deposited sediments on the upper and

    middle slope are unstable and subject to remobilization

    by repeated tectonic shock, release of pressurized fluids,

    or sublimation of gas hydrates due to changing water

    temperatures (cf. Piper et al., 1999a). These sediments

    are remobilized downslope as slumps, debris flows,

    olistoliths, and turbidity currents (5), where they fill up

    the forearc basin, which is subsiding in response to

    tectonics and isostasy (Fig. 12b). The balance between

    continuing subsidence and sediment accumulation

    results in a basin filled with aggrading remobilizedsediments. On the upper slope, gravel- and sand-charged

    meltwaters carve small feeder channels (6), which supply

    submarine canyons (7) with sediment-laden water from

    beneath the glacier. Submarine canyons eventually cross

    the forearc basin and carry sediments towards the

    trench, and may change regional orientation at different

    stratigraphic intervals, in response to tectonic activity

    (e.g., Carlson et al., 1990; Dobson et al., 1991). During

    deglaciation and interglacial episodes, enough sediment

    is introduced to the basin from rising coastal mountain

    chains that the ephemeral feeder channels, gullies, and

    even the largest submarine canyons may be completely

    buried.

    As the forearc basin fills with sediment (Fig. 12c), a

    broad shelf may be built. The shelf differs in geometry

    from the broad shelf on the passive margin, as it is

    largely aggradational (Fig. 2). Muddy proglacial sedi-

    ments are deposited by suspension rain-out (1) (Eyles

    et al., 1991), but during the next glacial advance, the

    shelf will have subsided sufficiently to either prevent

    grounded ice from advancing across the shelf, or prevent

    it from eroding deeply into pre-existing sediments,

    allowing their preservation. On the outer shelf, currents

    and icebergs may form lag gravels (14), which may

    subsequently be overridden by grounded ice to formstriated boulder pavements.

    Only when a board shelf is developed is there storage

    space for significant volumes of subglacial meltwater to

    be stored, and thus for subglacial tunnel valleys (11) to

    form. For this reason, the present submarine canyons in

    the Gulf of Alaska may be related to catastrophic

    discharges of subglacial meltwaters, and in this way they

    may differ somewhat from the older canyons exposed in

    outcrop around Icy Bay.

    Large pockmarks are unlikely, despite the presence of

    hydrocarbon seepages from bedrock, because sedimen-

    tation rates remain high during interglacials, and pock-

    mark formation apparently occurs when sediment rates

    are low (Gipp, 1994b). Small unit pickmarks (Hov-

    land and Judd, 1988), which are too small to be

    observed on seismic profiles, may occur, and may be

    observable in outcrop. Seepages of gas may be an

    important factor in supporting colonies of macrofauna

    on the seafloor, which appear in outcop as coquinas

    (13).

    Thus, the earliest sediments in the sequence will be

    dominated by debris flows, but suspension rain-out

    sediments and ice-rafted debris increase in stratigraphic

    importance upsection. Debris flows and turbidites are

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    important before the forearc basin is completely filled.

    Once the shelf extends across the previous forearc basin,

    resedimentation becomes only of local importance. The

    new continental slope is seaward of the forearc basin

    and remobilized sediments drain directly into the trench.

    As long as the margin continues to subside, grounded

    ice sheets will not entirely remove pre-existing shelf

    deposits. Thus, the sequence is capped by a thick

    succession of shelf facies.

    5.3. Facies successions of glacially influence marine

    settings in contrasting tectonic settings

    The models described above can be used to construct

    facies successions for tectonically active and passive

    glacially influenced continental margins. A generalized

    facies model depicting the Pleistocene glaciation of the

    Scotian margin (Fig. 13) consists of an interbedded

    sequence of thick debris flows and turbidites, represent-

    ing deposition on the continental rise, grading upwards

    into turbidites and thin-bedded debris flows, with

    considerable slumped material, olistoliths, and loading

    structures, including diapirs, representing deposition on

    the lower slope (Figs. 3, 5 and 6). Turbidites become

    coarser upsection, and submarine canyons, character-

    istic of the middle slope, may be observed in middle

    slope strata. Canyons are filled by diamictites, olisto-

    liths, debris flows, and turbidites. Intercanyon facies

    include debris flows and reworked sediments, and are

    capped with dropstone-free sandy silts, representing

    winnowed interglacial sediments and sands swept over

    the shelf edge. These coarsen upsection where they are

    capped by sandstones and conglomerates with small cut-

    and-fill channels, near the shelf break (e.g., Fig. 7). Till

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    Fig. 12. Model depicting development of the Yakataga Formation in the Gulf of Alaska, representing (a) initial deposition into a relatively narrow,

    shallow forearc basin, which (b) subsides, and is infilled by progressively larger amounts of sediment, resulting in (c) a broad shelf, which may become

    entirely glaciated. Numbering scheme as in Fig. 9. Modified after Gipp (1996).

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    tongues occur on the upper slope when ice advances to

    the shelf edge. The sequence is capped locally by tabular

    sandstones with coquinas and boulder pavements,

    representing outer shelf deposition, or by bioturbated

    shelly mudstones with dropstones and clay rafts (Fig. 4),

    representing deposition within a basin on the shelf.

    The facies model for the Yakataga Formation

    (Fig. 13) consists of a basal sequence of turbidites with

    debris flows (Fig. 10) containing abundant sediments

    clasts, olistoliths and mud diapirs, representing deposi-

    tion on the lower slope. These deposits grade upwards

    into turbidites and debris flows cut by submarine

    canyons (Fig. 9). The orientation of submarine canyons

    may change dramatically upsection, due to change in the

    location of the forearc basin (Dobson et al., 1991) or the

    formation of compressive ridges on the slope (Carlson

    et al., 1990).

    Atop the middle slope facies are turbidites and sand

    sheets, representing upper slope facies, which are over-

    lain by a thick succession of grades and ungraded

    sandstones and conglomerates characterized by abun-

    dant cut-and-fill channels (Fig. 8). The Yakataga For-

    mation is capped by a thick shelf sequence (>1 km on

    Middleton Island) of diamictites and sandstones, with

    coquinas, striated boulder pavements, and other evi-

    dence of ice scour (Fig. 7). Successions of heavily

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    Fig. 13. Comparison of facies successions on the Scotian margin and Gulf of Alaska. Major changes may be noted in the variability of paleocurrent

    directions shown by the large submarine canyons, the geometry of debris flows, and the development of a thick sequence of shelf deposits in the Gulf

    of Alaska that is accommodated by rapid subsidence of the forearc basin. Modified from Gipp (1996).

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