The Phanerozoic Record of Global Sea-Level Change

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Science  25 Nov 2005:
Vol. 310, Issue 5752, pp. 1293-1298
DOI: 10.1126/science.1116412


We review Phanerozoic sea-level changes [543 million years ago (Ma) to the present] on various time scales and present a new sea-level record for the past 100 million years (My). Long-term sea level peaked at 100 ± 50 meters during the Cretaceous, implying that ocean-crust production rates were much lower than previously inferred. Sea level mirrors oxygen isotope variations, reflecting ice-volume change on the 104- to 106-year scale, but a link between oxygen isotope and sea level on the 107-year scale must be due to temperature changes that we attribute to tectonically controlled carbon dioxide variations. Sea-level change has influenced phytoplankton evolution, ocean chemistry, and the loci of carbonate, organic carbon, and siliciclastic sediment burial. Over the past 100 My, sea-level changes reflect global climate evolution from a time of ephemeral Antarctic ice sheets (100 to 33 Ma), through a time of large ice sheets primarily in Antarctica (33 to 2.5 Ma), to a world with large Antarctic and large, variable Northern Hemisphere ice sheets (2.5 Ma to the present).

Fluctuations in global sea level (eustasy) result from changes in the volume of water in the ocean or the volume of ocean basins (Fig. 1) (14). Water-volume changes are dominated by growth and decay of continental ice sheets, producing high-amplitude, rapid eustatic changes [up to 200 m and 20 m per thousand years (ky)]. Other processes that affect water volume occur at high rates (10 m/ky) and low amplitudes (∼5 to 10 m): desiccation and inundation of marginal seas, thermal expansion and contraction of seawater, and variations in groundwater and lake storage. Changes in ocean basin volume are dominated by slow variations in sea-floor spreading rates or ocean ridge lengths (100 to 300 m amplitude, rates of 10 m/My). Variations in sedimentation cause moderate amplitude (60 m), slow changes (10 m/My). Emplacement of oceanic plateaus produces moderately rapid rises (60 m/My) but slow falls due to thermal subsidence (10 m/My).

Fig. 1.

Timing and amplitudes of geologic mechanisms of eustatic change derived from (14). SF, sea floor; Cont, continental.

Eustatic variations can be estimated from satellite measurements, tide gauges, shoreline markers, reefs and atolls, oxygen isotopes (δ18O), and the flooding history of continental margins and cratons. Satellite measurements are limited to the past 10 years (5), whereas tide gauge records extend back only ∼150 years (3). The most recent pre-anthropogenic sea-level rise began at about 18 ka and can be measured by directly dating shoreline markers (fig. S1). Tropical reefs and atolls (fig. S2) provide the most reliable geological estimates by dating “fossil sunshine” (e.g., shallow-dwelling corals) and have provided a precise estimate for the last sea-level lowstand (120 ± 5 m below present at 18 ka) (fig. S2) (6, 7). However, most coral records are from regions with complicated uplift/subsidence histories, are difficult to recover and date (particularly beyond a few 100 ky), and have poorly preserved lowstand deposits.

The growth and decay of continental ice sheets causes eustatic changes that are indirectly recorded in the chemistry of foraminifera because ice has lower δ18O values than seawater (fig. S2) [e.g., (8, 9)]. Oxygen isotope values provide a proxy for glacioeustasy, but d18O-based reconstructions are subject to several uncertainties: (i) Calcite δ18O values also vary as a function of temperature. (ii) Surface-ocean δ18O values are influenced by local evaporation-precipitation effects on seawater. (iii) Postdepositional alteration (diagenesis) may overprint original δ18O values, limiting useful records to sediments younger than 100 My.

Continents have been flooded many times in the geologic past (Fig. 2). However, the flooding record is not a direct measure of eustatic change because variations in subsidence and sediment supply also influence shoreline location. Regional unconformities (surfaces of erosion and nondeposition) divide the stratigraphic record into sequences and provide a key to eustatic change. Unconformities result from sea-level fall or tectonic uplift (1012). Similar ages of sequence boundaries on different continents have been interpreted as indicating that the surfaces were caused by a global process, eustasy [e.g. (10, 11)]. The linkage with δ18O increases for the past 40 My (13) indicates that most sequence boundaries resulted from eustatic falls driven by the growth of continental ice sheets.

Fig. 2.

Comparison of Phanerozoic backstripped eustatic estimates of this study, Watts (14), Sahagian (35), Kominz (29), Levy (30), and Bond (18); EPR records of Vail (10) and Haq (11, 16); continental flooding records of Sloss (15) and Ronov (17) plotted versus area, and Bond (18), Harrison (19), and Sahagian (4) plotted versus sea level; and evolutionary records compiled by Katz (52).

Although unconformities potentially provide the timing of eustatic lowstands, extracting global sea-level history from the stratigraphic record requires a quantitative method that distinguishes the contributions of eustasy, subsidence, and sediment accumulation. Backstripping is an inverse technique that can be used to quantitatively extract sea-level change amplitudes from the stratigraphic record. It accounts for the effects of sediment compaction, loading (the response of crust to overlying sediment mass), and water-depth variations on basin subsidence (14). Tectonic subsidence at a passive margin is modeled with thermal decay curves and removed to obtain a quantified eustatic estimate in the absence of local tectonic complexities.

We review the record of and uncertainties in eustatic changes over the past 543 My on three time scales: (i) a long-term trend (107 to 108 years) that has been attributed largely to variations in sea-floor spreading; (ii) the 106-year scale that is among the most prominent features of the stratigraphic record; and (iii) the 104- to 105-year scale that is dominated by changes in ice volume and controlled by astronomical variations in insolation. We present a new eustatic record for the past 100 My, with implications for causal mechanisms for both 107- and 106-year changes.

Long-Term Flooding of Continents

Sloss (15) recognized that North America experienced five major Phanerozoic floodings (Fig. 2) and attributed these changes to subsidence and uplift of the craton. Vail and colleagues at Exxon Production Research Company (EPR) recognized similar 107- to 108-year scale “supersequences” that they attributed to global sea-level changes (10, 11, 16). Others have reconstructed continental flooding history on the 107- to 108-year scale (4, 1719) (Fig. 2) and inferred eustatic changes from commonalities among continents.

High Late Cretaceous sea level has been attributed to high ocean-crust production rates that resulted in more buoyant ridges displacing seawater onto low-lying parts of continents (“tectonoeustasy”) (20). This concept has been extended to the Paleozoic through Early Mesozoic by assuming that 107- to 108-year scale continental flooding was caused by high sea-floor spreading rates, even though direct evidence for sea-floor spreading rates is absent owing to subduction.

Our sea-level record for the past 100 My has much lower amplitudes on the 107- to 108-year scale than previously inferred (Figs. 2 and 3 and fig. S3), with implications for sea-level change from 543 to 100 Ma. Our 100 to 7 Ma record (Fig. 2) is based on backstripping stratigraphic data from five New Jersey coastal plain coreholes (21, 22). Similar estimates obtained for each site suggest that we successfully accounted for the effects of thermal subsidence, sediment loading, compaction, and water-depth variations. Our long-term trend indicates that sea level was 50 to 70 m above present in the Late Cretaceous (∼80 Ma), rose to 70 to 100 m from 60 to 50 Ma, and fell by ∼70 to 100 m since 50 Ma (23). This contrasts with previously reported Late Cretaceous sea-level peaks of about 250 to 320 m based on sea-floor spreading reconstructions (2), although it is within error estimates of 45 to 365 m (best estimate 230 m) (24). It is lower than global continental flooding estimates [150 m (19), 80 to 200 m (18)].

Fig. 3.

Global sea level (light blue) for the interval 7 to 100 Ma derived by backstripping data (21). Global sea level (purple) for the interval 0 to 7 Ma derived from δ18O, shown in detail on Fig. 4. Shown for comparison is a benthic foraminiferal δ18O synthesis from 0 to 100 Ma (red), with the scale on the bottom axis in ‰ [reported to Cibicidoides values (0.64‰ lower than equilibrium)]. The portion of the δ18O curve from 0 to 65 Ma is derived using data from Miller (44) and fig. S1 recalibrated to the time scale of (71). The δ18O curve from 65 to 100 Ma is based on the data compiled by Miller (36) calibrated to the time scale of (72). Data from 7 to 100 Ma were interpolated to a constant 0.1-My interval and smoothed with a 21-point Gaussian convolution filter using Igor Pro. Pink box at ∼11 Ma is sea-level estimate derived from the Marion Plateau (51). Heavy black line is the long-term fit to our backstripped curve (23). Light green boxes indicate times of spreading rate increases on various ocean ridges (57). Dark green box indicates the opening of the Norwegian-Greenland Sea and concomitant extrusion of the Brito-Arctic basalts.

Our results are similar to backstripped estimates from the Scotian and New Jersey continental shelves (14), although the Late Cretaceous peak is lower (50 to 70 m versus ∼110 m) (fig. S3). One-dimensional (1D) backstripping may underestimate the Late Cretaceous peak because coastal plain subsidence results from a thermoflexural effect (14), and thermal subsidence curves may slightly overestimate the tectonic portion of subsidence of the older section. Considering backstripping and continental flooding estimates (18, 19) and errors in our paleowater depth estimates (eustatic error of ±10 to 35 m), we conclude that sea level in the Late Cretaceous was 100 ± 50 m higher than it is today.

Using new sea-floor age data, Rowley (25) suggested that there have been no changes in sea-floor spreading rates over the past 180 My. Our record implies a modest decrease in the rate of ocean-crust production because the long-term eustatic fall of 70 to 100 m since the early Eocene (Fig. 3) cannot be totally ascribed to permanent growth of ice sheets (26).

Our observation that long-term eustatic changes were appreciably smaller than previously thought has implications for geochemical models [e.g., (27)] that have used sea-level records to scale ocean production rates. Estimates derived from backstripping from the past 170 My (Fig. 2) show much lower long-term amplitudes than those published by EPR. Back-stripped sea-level records from the Cambrian-Devonian of the western United States show ∼200-m amplitudes on the 107-year scale (2830) (Fig. 2), although a Cambrian-Ordovician backstripped data set from the Appalachians shows a lower (∼70 m) amplitude (Fig. 2) (28). The sea-level rise in the Cambrian is attributed to the generation of new ocean ridges with the breakup of Pannotia (29), but the amplitude of this rise is still uncertain. Although the jury is still out on the amplitudes of Paleozoic sea level on the 107-year scale, our work suggests that the EPR records cannot be used to scale past spreading rates.

Sea-level changes on very long time scales (250 My) are related to the assembly and breakup of supercontinents. Formation of the supercontinents Pannotia (late Proterozoic to Early Cambrian) and Pangea (Permian to early Triassic) was associated with low levels of continental flooding (Fig. 2). This may be attributed to (i) a eustatic effect due to thickening of continents during orogeny resulting in increased oceanic area (2) and/or (ii) higher elevations that result when trapped heat builds up below the supercontinents (31).

Million-Year Scale Changes

In 1977, EPR surprised academic and industrial colleagues with the publication of a Phanerozoic eustatic record that showed more than 50 falls, some as large as 400 m (10). In 1987, the EPR group published a series of papers, including a synthesis in Science (11) that reported more than 100 sea-level falls during the past 250 My, with a maximum fall of 160 m. The EPR studies came under intense scrutiny because of the novel suggestions that (i) sequence boundaries are time-important features that could be recognized on seismic profiles and (ii) seismic profiles could be used to determine the history of sea level. The EPR curves have been strongly criticized for their methodology (12, 32), with critics suggesting that coastal onlap curves presented cannot be translated into a eustatic estimate.

Drilling on the New Jersey margin has provided new insights into the amplitudes of and mechanisms for 106-year scale sea-level changes. Fourteen Late Cretaceous sequences and 33 Paleocene-Miocene sequences were identified in New Jersey coastal plain coreholes (13, 33) and dated by integrating biostratigraphy, Sr-isotopic stratigraphy, and magnetostratigraphy to produce a chronology with age resolution of better than ±0.5 My for the Cenozoic (13) and ±1.0 My for the Late Cretaceous (33). Onshore New Jersey sequence boundaries correlate with sequence boundaries in the Bahamas, northwest Europe, the U.S. Gulf Coast, Russia, offshore New Jersey, and those of EPR, which suggests that they are global and formed in response to eustatic falls (13, 33). Thus, drilling has validated the number and timing, although not the amplitude, of many of the EPR sea-level events for the past 100 My (13, 33). Oligocene-Miocene sequence boundaries can be firmly linked with global d18O increases, demonstrating a causal relation between sea level and ice volume (13, 33), as expected for the Icehouse world of the past 33 My.

Backstripping of the New Jersey records provides eustatic estimates from ∼100 to 7 Ma (Fig. 3). Paleocene-Eocene and Miocene estimates are derived from 1D backstripped records from five sites and Late Cretaceous sequences from two sites (34). Several Upper Cretaceous onshore sections capture full amplitudes of change; however, many Cretaceous and most Cenozoic onshore sections do not record sea-level lowstands. Eustatic estimates for the latest Eocene to earliest Miocene are derived from 2D backstripping (22) that addressed this problem.

Our backstripped eustatic estimate (table S1) shows that global sea level changed by 20 to 80 m during the Late Cretaceous to Miocene (this study) and the Middle Jurassic to Late Cretaceous (35). Our comparison shows that the amplitudes of the EPR sea-level curve, including the most recent update (16), are at least 2.5 times too high (Fig. 2 and fig. S3).

Eustatic changes with amplitudes of 10s of meters in less than 1 My pose an enigma for a supposedly ice-free Green-house world, because ice-volume changes are the only known means of producing such large and rapid changes. Our record (Fig. 3) quantifies high amplitudes and rates of eustatic change (>25 m in < 1 My) in the Late Cretaceous to Eocene Greenhouse world. Based on the sea-level history, we have proposed that ice sheets existed for geologically short intervals (i.e., lasting ∼100 ky) in the previously assumed ice-free Late Cretaceous-Eocene Greenhouse world (36). This view can be reconciled with previous assumptions of an ice-free world. Sea-level changes on the 106-year scale were typically ∼15 to 30 m in the Late Cretaceous-Eocene (∼100 to 33.8 Ma), suggesting growth and decay of small- to medium-sized (10 to 15 × 106 km3) ephemeral Antarctic ice sheets (36). These ice sheets did not reach the Antarctic coast; as a result, coastal Antarctica and deep-water source regions were warm even though there were major changes in sea level as the result of glaciation (36). These ice sheets existed only during “cold snaps,” leaving Antarctica ice-free during much of the Greenhouse Late Cretaceous to Eocene (36).

Sea-level changes on the 106-year scale occurred throughout the Phanerozoic. Studies from the Russian platform and Siberia provide backstripped records of 106-year sea-level changes that are remarkably similar to New Jersey in the interval of overlap and extend to the Middle Jurassic (∼170 Ma) (35). The stratigraphic record before 170 Ma is replete in 106-year sea-level changes (16, 37). However, it is unclear whether these variations represent global changes in sea level. Eustatic estimates have been extracted from backstripping of Paleozoic strata (28, 29) (Fig. 2), although differences in the Appalachian versus the western U.S. Cambrian-Ordovician sea-level amplitude estimates are large, and thus the eustatic imprint is ambiguous.

Eustatic changes on the 104- to 106-year scales were controlled primarily by variations in ice volume during the past 100 My and may be expected to be modulated by both short-period [19/23 (precession), 41 (tilt), and ∼100 ky (precession)] and long-period [1.2 (tilt) and 2.4 My (precession)] astronomical variations (38). Spectral analysis of our sea-level records shows that variations occur with an as-yet-unexplained, persistent 3-My beat and a second primary period varying from 6 to 10 My (fig. S4). Amplitudes in the ∼3-My bandwith are ∼10 m from 60 to 20 Ma, with lower amplitude from 90 to 60 Ma.

The existence of continental ice sheets in the Greenhouse world is a controversial interpretation, but the study of ice-volume history has progressively tracked ice sheets back through the Cenozoic (36). After extensive debate, a consensus has developed that ice volume increased markedly in the earliest Oligocene (8, 9). We suggest that, at that time, the Antarctic ice sheet began to be a forcing agent of, and not just a response to, ocean circulation (36). The Antarctic continent (including west Antarctica) (39) was entirely covered by ice, and sea level was lower by ∼55 m (22). As a result, latitudinal thermal gradients (40) and deep-water circulation rates increased [with pulses of Southern Component and Northern Component Water (41)]. Diatoms diversified rapidly in response to increased surface-water circulation and nutrient availability (Fig. 2), resulting in increased export production and a positive feedback on CO2 drawdown and cooling.

The earliest Oligocene event represented a major change in climate state from a Greenhouse world with cold snaps to the Icehouse world that continues today. Sea-level changes from the Oligocene to the early Pliocene (∼33.8 to 2.5 Ma) were ∼30 to 60 m (Figs. 3 and 4), with growth and decay of a large (up to present volumes of 25 × 106 km3) ice sheet mostly in Antarctica. A middle Miocene δ18O increase is associated with deep-water cooling and two ice-growth events that resulted in the permanent development of the East Antarctic ice sheet (40). Northern hemisphere ice sheets (NHIS) have existed since at least the middle Miocene (41), but large NHIS with sea-level changes of 60 to 120 m only began during the late Pliocene to Holocene (∼2.5 to 0 Ma) (Fig. 4).

Fig. 4.

Oxygen isotopic-based sea-level estimate for the past 9 My. Isotopic values are reported to equilibrium, with coretop and last glacial maximum values indicated with arrows and thin vertical green lines. Thin black line is raw data plotted versus the δ18O scale (bottom). The purple line is the sea-level estimate (top scale), which is derived by correcting the δ18O data by 0.5‰ due to a ∼2°C cooling between 3.3 and 2.5 Ma (red line), scaling by δ18O to sea level using a calibration of 0.1‰/10 m, and scaling the result by 0.8 (45).

Milankovitch Scale Changes

The growth and decay of NHIS (the late Pliocene-Holocene “ice ages”) and attendant sea-level changes were paced by 104- to 105-year scale Milankovitch changes. The δ18O record shows a dominant 100 ky (eccentricity) beat over the past 800 ky, with secondary 19/23 (precession) and 41-ky (tilt) periods (42). Before ∼800 ky, the tilt cycle dominated δ18O (43) and sea-level records. Although strong precessional and eccentricity beats occur in the carbon system, the tilt cycle has dominated d18O and ice-volume records for much of the past 33.8 My (9). Growth and decay of small- to medium-sized ice sheets in the Late Cretaceous-Eocene on the Milankovitch scale probably lie near or below the detection limit of δ18O records [∼0.1 per mil (‰) = 10-m eustatic change].

Continental margins record 104- to 105-year scale sea-level changes only in very high sedimentation rate settings. Foraminiferal δ18O records reflect ice volume in addition to temperature changes and potentially provide a proxy for sea-level changes on the 104- to 105-year scale. The δ18O record provides continuity and excellent age control, although assumptions about thermal history must be made to use it as a sea-level proxy. In addition, diagenesis complicates planktonic foraminiferal d18O records, although benthic foraminifera generally show little evidence for diagenesis at burial depths less than 400 to 500 m (44).

We derive sea-level estimates from 9 to 0 Ma using benthic foraminiferal δ18O records because the New Jersey record is incomplete from 7 to 0 Ma (table S1). We scaled the benthic foraminiferal δ18O record (45) to sea level by making minimum assumptions about ocean thermal history (Fig. 4). The resultant sea-level curve (Fig. 4) aligns remarkably well with the backstripped record from 9 to 7 Ma (Fig. 3).

Our δ18O-derived sea-level estimate for the past 9 My (Fig. 4) shows that the record is dominated by the response to the 41-ky period tilt forcing, which increases in amplitude toward the present, and a low-amplitude ∼21-ky precession response. The major 100-ky events of the past 900 ky stand out in the sea-level record (Fig. 4). There are prominent 106-year scale sea-level falls (the 2.5, 3.3, 4.0, 4.9, 5.7, and 8.2 Ma events) (Fig. 4), but these are not obviously paced by amplitude modulations of either precession or tilt (fig. S4).

Suborbital Scale

Very large (>100 m) sea-level rises are associated with glacial terminations of the past 800 ky (fig. S1) (6).Themostrecentrisethatfollowed the last glacial maximum at 18 ka occurred as two major steps associated with meltwater pulses (MWP) 1a (13.8 ka) and 1b (11.3 ka), punctuated by a slowing at ∼12 ka (6). Sea-level rise slowed at about 7 to 6 ka (fig. S1). Some regions experienced a mid-Holocene sea-level high at 5 ka, but we show that global sea level has risen at ∼1 mm/year over the past 5 to 6 ky. We present new core data from New Jersey covering the past 6 ky that show a rise of 2 mm/year over the past 5 ky (fig. S1). This New Jersey curve is remarkably similar to sea-level records from Delaware (46) and southern New England (47), with a eustatic rise of 1 mm/year over the past 5 ky once corrected for subsidence effects (48), virtually identical to that obtained from Caribbean reef localities (49) (fig. S1) accounting for subsidence.

Error Estimates

Long-term sea-level estimates show considerable differences, with a large range of Late Cretaceous sea-level estimates: ∼110 m (14), 150 m (19), 250 m (4), and 80 to 200 m (18), and our best estimate of 100 ± 50 m. We conclude that sea-level amplitudes on this scale were substantially lower than generally believed (100 versus 250 m) over the past 170 My, with uncertain amplitude before this (Fig. 2).

Sea-level estimates on the 106-year scale have an uncertainty, typically, of at best ±10 to ±50 m. The two main sources of errors in backstripping relate to hiatuses (time gaps) and paleowater depth estimates. New Jersey coastal plain sequences represent primarily inner-shelf to middle-shelf environments, with eustatic errors from paleowater depth estimates of ±10 to 20 m (50). Hiatuses in our record potentially explain why amplitudes of change might not be fully recorded, and the effect of hiatuses can be evaluated only by comparing our record with other regions. Drilling on the Marion Plateau (offshore northeast Australia) targeted an ∼11 Ma eustatic lowering (51); backstripping yields a sea-level estimate of 56.5 ± 11.5 m for this event (pink bar on Fig. 3). Our estimate for this event is ∼40 ± 15 m (Fig. 1); these estimates are consistent, within error, but suggest that we may underestimate sea-level falls by 5 to 30 m.

The record of the past 130 ky illustrates the errors in converting a δ18O record into a sea-level proxy (fig. S1). Benthic foraminiferal d18O records can be scaled to a faithful proxy for glacial to cool interglacials [Marine Isotope Chron (MIC) 2d to 5d] (fig. S2), with sea level and δ18O in phase and lagging insolation. However, large deviations of the δ18O-based sea-level curve occur during peak warm intervals (Holocene and MIC 5e) (Fig. 2), with a hint that deep-sea temperature change leads sea level. We have attempted to correct for this temperature effect by scaling to the Barbados sea-level record (6). However, this results in underestimating amplitudes of glacials and overestimating amplitudes of interglacials, with a resultant 20% uncertainty.

Relation of Sea Level to Evolution and Climate Changes

Episodes of supercontinent rifting and sea-level rise on the 107- to 108-year scale played a role in phytoplankton evolution since the Proterozoic by flooding continental shelves and low-lying inland areas and increasing the total length of coastline. The resulting increases in habitat heterogeneity, ecospace, and nutrient availability favored plankton that lived along continental margins. Accordingly, diversity increases in phytoplankton (Fig. 2) appear to correlate with continental rifting of Pannotia (Early Paleozoic) and Pangea (Jurassic) (Fig. 2), ultimately resulting in the three groups of eukaryotic phytoplankton (coccolithophores, diatoms, and dinoflagellates) that dominate the modern ocean (52).

Sea-level changes are expected with beats of 19/23, 41, and 100 ky, but similar changes on the 106-year scale (Fig. 3) have puzzled geologists. Sea-level cyclicity on the 106-year scale can be explained by a modulation of the shorter term Milankovitch-scale sea-level events (fig. S5). For example, a prominent seismic disconformity spanning the Oligocene/Miocene boundary (∼23.8 Ma) on the New Jersey slope (13) can be correlated to a detailed δ18O record at deep-sea Site 929 (53), showing that the 106-year scale sea-level fall at the Oligocene/Miocene boundary occurred as a series of 41-ky δ18O increases and sea-level changes. The 41-ky sea-level falls are reflected in core photographs by a series of dark-light changes (fig. S5), resulting from variations in glauconite transported downslope during lowstands. The seismic reflection is a concatenation of these beds and the ice-volume events that caused them.

The high sea levels of the Late Cretaceous and early Eocene are associated with peak benthic foraminiferal δ18O values (Fig. 3) (table S1), and it has long been suggested that sea level covaries with δ18O on the 107-year scale [e.g., (54)]. On the 105- to 106-year scales, such covariance can be explained by ice-volume changes in concert with temperature changes (8, 13). However, this cannot be true on the 107- to 108-year scale because most of the d18O signal must be attributed to temperature changes. For example, 3.6‰ of the 4.4‰ increase from 50 to 0 Ma (Fig. 3) must be attributed to deep-water cooling (15°C overall) rather than to ice storage (55). The link between sea level and temperature on the 107- to 108-year scale cannot be due to cooling alone, because this would explain only ∼15 m of eustatic fall since 50 Ma. The link between d18O and sea-level variations on the 107- to 108-year scale can be explained by CO2 variations controlled by tectonics (changes in ocean-crust production and mountain uplift).

High ocean-crust production rates have long been linked to high sea level, high CO2, and warm global temperatures [e.g., (54)]. Warm Late Cretaceous climates and elevated sea level may be attributable to moderately higher sea-floor production rates, although our results require that crustal production rates were lower than previously thought. However, the intensity of spreading ridge hydrothermal activity (a major source of CO2 outgassing) appears also to correlate with times of major tectonic reorganizations (56). We propose that the early Eocene peak in global warmth and sea level (Fig. 3) was due not only to slightly higher ocean-crust production but also to a late Paleocene-early Eocene tectonic reorganization. The largest change in ridge length of the past 100 My occurred ∼60 to 50 Ma (57), associated with the opening of the Norwegian-Greenland Sea, a significant global reorganization of spreading ridges, and extrusion of 1 to 2 × 106 km3 of basalts of the Brito-Arctic province (58). A late Paleocene to early Eocene sea-level rise coincides with this ridge-length increase, suggesting a causal relation. We suggest that this reorganization also increased CO2 outgassing and caused global warming to an early Eocene maximum. Subsequent reduced spreading rates and hydrothermal activity resulted in lower long-term sea level, reduced CO2 outgassing, and a cooling of deep-water by ∼8°C (44). CO2 may have been further lowered by an increase in continental weathering rates during the remainder of the Cenozoic (59), explaining an additional deep-water cooling of 7°C to 9°C (44).

Our studies of the past 100 My provide clues to the tempo of climate and ice-volume changes for other Icehouse and Green-house worlds of the Phanerozoic (Fig. 2). Icehouse worlds of the past 33 My, the Pennsylvanian to Early Permian, Late Devonian, and Late Ordovician (60), can be characterized by ice-volume changes that caused sea-level variations up to 200 m. Greenhouse worlds characterize much of the Phanerozoic, but we note that small (10 to 15 × 106 km3), ephemeral ice sheets occurred in the Greenhouse of the Late Cretaceous to Eocene. This raises the question as to whether any portion of the Phanerozoic was ice-free. The Triassic and Cambrian pose two of the best candidates for an ice-free world (60), yet Haq (11, 16) noted numerous 106-year scale sea-level variations at these times (Fig. 2). If corroborated, these changes suggest the presence of ephemeral ice sheets even in the warmest of the Greenhouse periods.

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