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Brunhes–Matuyama reversal

The Brunhes–Matuyama reversal, also referred to as the Matuyama–Brunhes reversal, is the most recent full geomagnetic polarity reversal in Earth's history, occurring approximately 774,000 years ago when the planet's magnetic field shifted from reversed polarity (the Matuyama reversed chron) to the current normal polarity (the Brunhes normal chron).^[1] This event marks a critical transition in the geomagnetic timescale, recorded globally in paleomagnetic archives such as marine sediments and volcanic rocks.^[2]^[3] Evidence for the reversal was first identified in 1906 by French geophysicist Bernard Brunhes, who detected reverse magnetization in basaltic lavas and underlying sediments from the Pontfarreyn region in Cantal, France, during his tenure as director of the Puy de Dôme Observatory.^[4] This discovery was later corroborated and expanded in 1929 by Japanese geologist Motonori Matuyama, who analyzed the magnetization of Quaternary volcanic rocks across Japan and identified a systematic pattern of reversed polarity in older formations, establishing the existence of multiple geomagnetic reversals.^[4] The reversal itself is named in honor of these pioneers, with the Brunhes chron encompassing the present normal polarity epoch and the preceding Matuyama chron characterized by reversed polarity.^[4] Paleomagnetic records indicate that the reversal was not instantaneous but unfolded over an extended period of geomagnetic instability spanning roughly 800,000 to 770,000 years ago, with the primary polarity switch dated to about 774,000 years ago.^[5]^[1] The process featured a gradual decay of the axial dipole field, dropping to critically low intensities of around 5 ZAm² or less, interspersed with transitional states dominated by non-axial dipole components and the emergence of high-latitude reverse flux patches at the core-mantle boundary.^[5]^[2] Detailed sequences from sites like the Chiba composite section in central Japan reveal four phases: initial weakening around 800–785 ka, partial recovery to reversed polarity, further instability with millennial-scale fluctuations from 783–763 ka, and final stabilization to normal polarity around 770 ka.^[3] As the best-documented reversal due to its recency and abundance of high-resolution records, the Brunhes–Matuyama event provides essential insights into the dynamics of Earth's geodynamo, including the mechanisms driving field weakening and recovery.^[2] It also holds stratigraphic importance as the defining marker for the base of the Chibanian stage (Middle Pleistocene) in the International Chronostratigraphic Chart, with the Global Boundary Stratotype Section and Point (GSSP) established at 1.1 ± 0.3 meters above the Byk-E tephra in Japan's Boso Peninsula.^[3] Studies of this reversal continue to inform models of potential future geomagnetic excursions and their implications for planetary habitability.^[5]

Background on Geomagnetic Reversals

Definition and Basic Mechanism

A geomagnetic reversal refers to a change in the dominant polarity of Earth's magnetic field, where the magnetic north pole and magnetic south pole effectively interchange positions. In normal polarity, the north-seeking pole of a compass aligns toward the geographic North Pole, corresponding to the current configuration, while in reversed polarity, the north-seeking pole points toward the geographic South Pole. These reversals are recorded in rocks and sediments that preserve the direction of the ancient field at the time of their formation.^[6] The underlying mechanism driving geomagnetic reversals is the geodynamo process in Earth's outer core, where convective flows of molten iron and nickel generate electric currents that sustain the planet's magnetic field. This self-sustaining dynamo arises from the motion of the electrically conductive fluid, influenced by heat from the inner core, Earth's rotation, and compositional differences, leading to a predominantly dipolar field under stable conditions. However, instabilities in these flows—potentially triggered by fluctuations in heat flux at the core-mantle boundary—can disrupt the dipole dominance, causing the field to weaken and the polarity to flip over time.^[7] Over geological timescales, geomagnetic reversals occur irregularly, with an average interval of approximately 200,000 to 250,000 years based on records from the past 10 million years, though intervals can vary widely from as short as 10,000 years to over 50 million years. These events form the basis of the geomagnetic polarity timescale, a global standard for correlating rock layers and dating geological events. During transitional periods, the magnetic field intensity often drops significantly, sometimes to 10% of its normal strength, and the virtual geomagnetic poles—calculated positions assuming a dipole field—wander erratically across the globe rather than following a simple path.^[8]^[6]^[9]

Role in the Geomagnetic Polarity Timescale

The Geomagnetic Polarity Timescale (GPTS) is a chronological framework that records the history of Earth's magnetic field polarity changes as a sequence of alternating normal and reversed polarity intervals known as chrons and subchrons.^[10] These polarity zones provide a global standard for dating and correlating geological records, particularly in the Cenozoic era.^[11] For instance, the Matuyama reversed chron spans from 2.58 Ma to 0.78 Ma, while the overlying Brunhes normal chron extends from 0.78 Ma to the present.^[11] Geomagnetic reversals serve as isochrons—synchronous global events that enable precise stratigraphic correlation across diverse rock records, such as marine sediments and continental volcanics, independent of biostratigraphic markers like fossil assemblages.^[12] This utility arises because the reversal process occurs rapidly on geological timescales, typically within thousands of years, allowing paleomagnetists to match polarity patterns worldwide without relying on regional faunal or floral changes.^[13] The Brunhes–Matuyama reversal, as the most recent full polarity transition, demarcates the boundary between the Matuyama and Brunhes chrons, anchoring this portion of the GPTS.^[11] The GPTS is constructed by integrating paleomagnetic data from oceanic magnetic anomalies, which reflect seafloor spreading rates and polarity intervals, with absolute age controls.^[10] Radiometric dating, primarily using ⁴⁰Ar/³⁹Ar methods on volcanic rocks that capture reversal boundaries, provides key calibration points for chron ages.^[10] Additionally, orbital tuning of deep-sea sediment cores aligns polarity zones with Milankovitch cycles in oxygen isotope records, refining the timescale's resolution, especially for the Quaternary period.^[10]

Historical Discovery and Dating

Early Observations

The initial recognition of geomagnetic field reversals began with the pioneering work of Bernard Brunhes in 1906, who discovered reversed remanent magnetization in Miocene-age volcanic rocks from the Massif Central in France. Specifically, Brunhes measured antiparallel inclinations (ranging from -69° to -78°) in a basaltic lava flow and underlying baked clays at Pont Farein near Saint-Flour, which contrasted sharply with the expected normal polarity aligned to the present-day field.^[14] This finding puzzled contemporaries, as it implied that the magnetic north pole had once been near the geographic south pole during the rocks' formation, challenging prevailing assumptions about the stability of Earth's magnetic field.^[15] Building on this, Motonori Matuyama provided systematic evidence in the late 1920s through paleomagnetic measurements of Quaternary basalts across Japan, South Korea, and northeast China. Analyzing 139 samples from 36 localities, Matuyama identified two distinct magnetization groups: one normal (aligned with the current field) in younger Pleistocene lavas and one reversed (antipodal) in older, pre-Pleistocene volcanics, suggesting a reversed geomagnetic epoch predating the present normal interval.^[14] His observations, published in 1929, marked the first comprehensive demonstration of a temporal sequence in polarity changes, though the full implications remained debated until later decades.^[16] Post-World War II advancements revitalized interest in these anomalies, culminating in the Vine-Matthews-Morley hypothesis of 1963, which linked symmetric magnetic stripe patterns on the ocean floor to episodic field reversals recorded during seafloor spreading at mid-ocean ridges. This model explained the global nature of reversals by proposing that newly formed oceanic crust acquires thermoremanent magnetization in the direction of the prevailing field, creating alternating normal and reversed bands as the crust spreads.^[17] Concurrently, in the 1960s and 1970s, N.D. Opdyke and collaborators extended these insights to marine sediments, identifying the Brunhes-Matuyama boundary in deep-sea cores from the Antarctic and Pacific Oceans through detailed inclination and intensity measurements, thereby correlating continental volcanic records with oceanic ones and affirming the reversal's worldwide synchroneity.^[18] Early paleomagnetic studies provided an initial age estimate of approximately 700,000 years for the Brunhes–Matuyama reversal, which built upon the foundational observations by Brunhes and Matuyama in the early 20th century.^[19] This was refined through 40Ar/39Ar radiometric dating of volcanic lavas that straddle the reversal, yielding an age of 780,000 ± 5,000 years.^[20] These incremental heating analyses on samples from Maui, Hawaii, offered a more precise chronological anchor by directly dating the igneous rocks recording the polarity transition.^[20] Subsequent refinements employed astronomically tuned cyclostratigraphy from marine sediments to enhance accuracy. Shackleton et al. (1990) established an age of 780 ka by correlating oxygen isotope records from Ocean Drilling Program Site 677 with orbital cycles of insolation. Hilgen (1991) confirmed an age of approximately 780 ka through calibration of sapropel layers in Mediterranean sediments against Milankovitch forcing, highlighting discrepancies with earlier radiometric dates and emphasizing the role of delayed remanence acquisition in sediments. More recent studies, incorporating data from Integrated Ocean Drilling Program/International Ocean Discovery Program cores, have pinpointed the reversal at 781 ± 3 ka using combined astrochronological and paleomagnetic records.^[2] Complementary techniques include U-series disequilibrium dating of corals and speleothems, which extend reliable chronologies to beyond 1 Ma and constrain the reversal's timing through associated paleomagnetic signals in these archives.^[21] The Brunhes–Matuyama reversal serves as the Global Boundary Stratotype Section and Point (GSSP) for the base of the Chibanian Stage and Middle Pleistocene Subseries, ratified by the International Commission on Stratigraphy in 2020 at the Chiba section in Japan.^[1] This designation leverages the reversal's global synchroneity, with the boundary marker placed 1.1 m below the directional midpoint of the paleomagnetic transition, tied to an astronomical age of 774.1 ± 5.0 ka.^[1]

Key Characteristics of the Reversal

Duration and Transitional Field Behavior

The Brunhes–Matuyama reversal, marking the transition from the reversed polarity of the Matuyama chron to the normal polarity of the Brunhes chron, spanned approximately 20,000 to 30,000 years based on high-resolution paleomagnetic records.^[3]^[22]^[23] The onset of instability for this event is dated to around 795–800 ka, with the main polarity switch at ~778 ka.^[21]^[24] Within this period, the most rapid directional changes occurred in less than 5,000 years, with some analyses indicating the core polarity switch completed in as little as 1.1 ± 0.4 kyr.^[3] During the transitional phase, the geomagnetic field exhibited pronounced instability, with intensity dropping to 5–10% (~2–5 μT) of its normal value, reflecting a significant weakening of the dipole component.^[25]^[26] Virtual geomagnetic poles (VGPs) migrated along preferred longitudinal bands, clustering over the Americas (American path) and Asia-Australia, indicative of nondipolar field dominance during the low-intensity interval.^[27]^[22] This behavior included multiple oscillations, with VGPs fluctuating between low latitudes and specific hemispheric preferences before stabilizing. An immediate precursor event around 795 ka involved initial field decay and directional anomalies, preceding the main transition.^[2] The reversal was preceded by several aborted reversals or geomagnetic excursions, such as the Kamikatsura event at approximately 886 ka and the Santa Rosa event at 922 ka, which acted as precursors within the late Matuyama chron.^[28] These short-lived polarity instabilities, lasting on millennial scales, involved brief shifts toward normal polarity that failed to persist.^[28] Models of geomagnetic behavior differentiate such excursions as incomplete reversal attempts, where the field intensity recovers without a full flip, in contrast to the Brunhes–Matuyama event, which featured a transient normal excursion phase amid ongoing instability before achieving stable normal polarity.^[29]^[2] Cryptochrons like Kamikatsura and Santa Rosa represent these precursor intervals, embedded within the broader transitional dynamics ~1 Ma ago.^[28]

Intensity and Directional Variations

During the Brunhes–Matuyama reversal, the geomagnetic field intensity underwent a significant decline, dropping from typical normal values of approximately 50 μT to less than 10 μT (or ~2–5 μT at nadir) at the transition's nadir, as evidenced by paleointensity measurements from volcanic sequences.^[26] This low-intensity phase reflects a collapse of the dipole component, with virtual dipole moments (VDMs) falling to around 1 × 10²² Am² or lower, compared to ~5–8 × 10²² Am² in the pre- and post-reversal stable periods.^[26]^[23] Recovery following the transition was asymmetric, with the field rebuilding more gradually in the early Brunhes normal phase, reaching stable intensities of 14–21 μT only after an extended stabilization period.^[26] The reversal exhibited pronounced asymmetry in its transitional dynamics, with the decay phase from reversed to transitional polarity lasting approximately 19–20 kyr, significantly longer than the subsequent growth phase to full normal polarity, which spanned about 6–10 kyr.^[24] This temporal imbalance, documented in global paleomagnetic reconstructions, underscores a prolonged weakening of the dipole prior to the polarity flip, followed by a more rapid re-establishment of the normal field orientation.^[24] Directional variations during the transition were equally dramatic, with inclination shifting from approximately -60° (reversed polarity) to +60° (normal polarity) at mid-latitudes, indicating a full geomagnetic flip over the event's duration.^[30] Declination exhibited swings of up to 180°, reflecting multipolar field configurations and rapid pole migrations, while virtual geomagnetic poles (VGPs) preferentially clustered along two longitudinal bands, one in the Americas-Africa sector and another in the Asia-Pacific region, as compiled from multiple sedimentary and volcanic records.^[31] These paths suggest longitudinal asymmetries in non-dipole field dominance during the reversal.^[31] Paleointensity proxies, particularly relative paleointensity (RPI) records from marine sediments, reveal oscillations during the transition, with intensity fluctuating amid the overall decline, often normalized using anhysteretic remanent magnetization (ARM) or low-field susceptibility. Absolute estimates from the Thellier-Coe method on volcanic samples confirm these patterns, yielding values as low as 4.7–5 μT during directional instability, with RPI showing precursor dips and post-transitional rebounds.^[26]

Paleomagnetic Records

Evidence from Sedimentary Cores

Sedimentary cores provide continuous records of the Brunhes–Matuyama reversal through the acquisition of detrital remanent magnetization (DRM), where magnetic minerals in clays align with the ambient geomagnetic field during deposition, resulting in relatively smoothed paleomagnetic signals due to typical sedimentation rates of 1–10 cm/kyr in marine and lacustrine environments.^[32]^[33] High-resolution paleomagnetic data from Ocean Drilling Program (ODP) Site 983 in the North Atlantic capture the reversal sequence over an approximately 20 kyr interval, with mean sedimentation rates around 12 cm/kyr enabling detailed tracking of directional changes during the transition.^[32] Similarly, cores from Lake Biwa in Japan, featuring annual varves in overlying sections, resolve sub-kiloyear-scale variations in the reversal record through high accumulation rates that preserve fine-scale field fluctuations.^[34] These records document a gradual shift in magnetic inclination over 4–6 kyr, reflecting the transitional geomagnetic field behavior, alongside intensity minima indicated by low normalized remanence values during the polarity switch.^[35] A comprehensive study of the full Matuyama-Brunhes sequence in the Chiba composite section, Central Japan, published in 2020, further illustrates these patterns in a marine sedimentary archive with centennial-scale resolution, highlighting consistent directional and intensity variations across the reversal.^[3] Virtual geomagnetic pole (VGP) paths in these sedimentary records often cluster along longitudinal bands, providing insights into the transitional field's spatial complexity.^[32] However, post-depositional remanent magnetization (PDRM) processes can smooth the recorded transitions by locking in the signal over a depth interval of several centimeters below the sediment-water interface, potentially delaying or broadening the apparent duration of the reversal in these archives.^[33]

Evidence from Volcanic Sequences

Volcanic sequences provide discrete paleomagnetic records of the Brunhes–Matuyama reversal through thermal remanent magnetization (TRM), which is acquired as lava flows cool below the Curie temperature of magnetic minerals, locking in the ambient geomagnetic field direction and intensity at the time of eruption.^[2] This process yields high-fidelity snapshots of the field, typically spaced 1–10 kyr apart depending on eruption frequency, offering less smoothing compared to continuous sedimentary deposition but with potential gaps from irregular volcanic activity.^[36] Prominent sites include lava flows in the Hawaiian Islands, such as those on Maui and O'ahu, where stacked basaltic sequences capture polarity transitions with detailed virtual geomagnetic pole (VGP) paths. For instance, on Maui, 24 flows record the reversal with VGPs migrating from reverse to normal polarity along the Americas, followed by an oscillation in the Pacific, spanning the transition dated to approximately 776 ka.^[37] Similarly, sequences on O'ahu reveal large inclination variations and non-dipole field influences during transitional phases, highlighting recurring patterns in field behavior.^[38] In the Canary Islands, lava flows from La Palma preserve multiple records of the reversal, with intermediate VGPs showing no strong clustering and a notable rebound excursion linked to low field intensities dropping to one-tenth of modern values.^[39] Studies from the 1990s on these flows demonstrated discrete polarity flips and transitional directions over roughly 5 kyr, supported by paleointensity estimates from the modified Thellier method.^[39] Japanese volcanic sections, including tephra layers from the Older Ontake volcano, contribute to reversal records in central Japan, such as the Chiba composite section on the Boso Peninsula, where the Byk-E tephra (sourced from Ontake) serves as a stratigraphic marker just below the boundary.^[3] This aids in correlating the full reversal sequence, with the polarity switch occurring over about 1.1 kyr at 773 ka.^[3] Recent global modeling incorporating volcanic data from these and other sites confirms the robustness of reversal characteristics, including a sawtooth-like dipole moment decay and recovery over 21–32 kyr, with consistent transitional behaviors despite sparse southern hemisphere coverage.^[5] These records align well with sedimentary cores, providing global confirmation of the event's timing and field dynamics.^[5]

Geological and Biological Significance

Use as a Stratigraphic Boundary

The Brunhes–Matuyama reversal serves as the primary stratigraphic marker for the base of the Chibanian Stage and Middle Pleistocene Subseries, designated as the Global Stratotype Section and Point (GSSP) by the International Commission on Stratigraphy in January 2020. Located at the Chiba composite section along the Yoro River gorge in the Boso Peninsula, Japan, the GSSP is fixed at the Ontake-Byakubi-E (Byk-E) tephra bed, which immediately underlies the onset of the reversal at an astronomical age of 774.1 ± 5.0 ka. This precise definition leverages the reversal's global detectability in paleomagnetic records, providing a robust isochronous boundary for Quaternary chronostratigraphy.^[1] The reversal facilitates worldwide correlation of Quaternary sedimentary sequences, enabling alignment of continental, marine, and cryospheric archives. In Chinese loess-paleosol sequences on the Loess Plateau, it demarcates a transitional zone between paleosol S8 and loess L8, anchoring magnetostratigraphic frameworks to orbital cycles and aiding reconstruction of East Asian monsoon variability. Similarly, in Antarctic ice cores like EPICA Dome C, elevated cosmogenic ^{10}Be concentrations signal the reversal's field intensity low, synchronizing glacial-interglacial records with geomagnetic events. The boundary coincides with the upper part of Marine Isotope Stage 19, linking paleomagnetic data to oxygen isotope stratigraphy for enhanced temporal resolution in global climate proxies.^[40]^[41] Integration of the reversal with complementary dating methods strengthens stratigraphic correlations, particularly in regions with sparse radiometric data. Tephrochronology, exemplified by the Byk-E tephra's U-Pb age of 772.7 ± 7.2 ka, provides direct ties to volcanic ash layers for inter-site matching.^[42] Amino acid racemization in fossil mollusks calibrates relative ages against the reversal, as seen in Mediterranean coastal deposits where epimerization ratios align pre- and post-boundary units. Biostratigraphic markers, such as the transition across mammalian biozones (e.g., from the Emilian to Ionian large mammal ages in Europe), co-occur with the reversal, supporting faunal turnover correlations in continental sequences.^[43] Refinements in 2023, based on global paleomagnetic models synthesizing hemispheric records, confirm the reversal's synchroneity within ±2 kyr, resolving prior discrepancies in onset timing between Northern and Southern Hemisphere sites and solidifying its utility as a uniform stratigraphic horizon.^[23]

Potential Impacts on Environment and Life

During the Brunhes–Matuyama reversal, the geomagnetic field weakened significantly, dropping to approximately 10–20% of its present intensity for several thousand years, which allowed a greater influx of galactic cosmic rays (GCRs) to penetrate Earth's atmosphere.^[44] This resulted in an estimated 1.9- to 2-fold increase in GCR flux at the surface, enhancing atmospheric ionization rates and potentially promoting the formation of low-level clouds through ion-induced nucleation processes.^[45] Such cloud increases could have raised planetary albedo, contributing to minor regional cooling effects, including midlatitude temperature drops of about 2–3°C during the transitional period around 783–778 ka.^[45]^[44] The weakened field also led to heightened radiation exposure on Earth's surface, with models indicating a roughly 2- to 3-fold increase in cosmic particle influx and potential ultraviolet (UV) radiation due to transient ozone perturbations.^[45] Atmospheric chemistry simulations suggest minimal global ozone depletion, with polar regions experiencing temporary losses of up to 30% in total ozone column (around 60–170 Dobson units regionally), but these effects were short-lived and did not persist beyond the reversal's duration.^[46] Despite this elevated radiation, paleontological records show no evidence of mass extinctions directly linked to the event, as statistical analyses of reversal timings and biodiversity patterns reveal no significant correlation with global faunal die-offs.^[47] Biological impacts appear subtle, with no abrupt extinction spikes but possible correlations to regional faunal turnovers around 780 ka, particularly in Africa and Europe, where shifts in mammalian assemblages coincided with the reversal.^[48] For instance, the period aligns temporally with a hominin population bottleneck (~930–813 ka) and migrations of Homo erectus out of Africa into Eurasia, potentially exacerbated by combined radiation stress and climatic pressures, though orbital forcing remains the dominant driver. Ongoing debates highlight the limited climatic forcing from the reversal, with recent studies emphasizing that any cooling or environmental shifts were overshadowed by Milankovitch orbital cycles and glacial-interglacial dynamics during Marine Isotope Stage 19.^[5] Models and proxy data from 2023–2024 underscore that geomagnetic effects on climate were regionally variable and secondary to insolation changes, with no strong evidence for widespread biosphere disruption beyond localized adaptations.^[23]

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[44]
An ice core perspective on the age of the Matuyama–Brunhes ...
Sep 30, 2008 · In fact, the highest point of the peak, indicating the reversal boundary, is dated at 766.4 ka based on the EDC3 age model used by Dreyfus et al ...
[45]
Amino acid geochronology applied to the correlation and dating of ...
The Brunhes-Matuyama boundary at ... Isoleucine epimerization in fossil mollusc shells applied to problems of Quaternary stratigraphy and climatic change.
[46]
An early Brunhes (<0.78 Ma) age for the Lower Paleolithic tool ...
Dec 15, 2017 · Large mammal biostratigraphy seems to indicate that Layers 11b to 13c should belong to Mammal ... Brunhes–Matuyama boundary (0.78 Ma). Encouraged ...
[47]
Geological support for the Umbrella Effect as a link between ... - Nature
Jan 16, 2017 · During geomagnetic polarity reversals, the geomagnetic field intensity drops to 10–20% of the present value, which increases the GCR by 90–70%.
[48]
Midlatitude cooling caused by geomagnetic field minimum during ...
Jan 7, 2013 · The CR–cloud connection suggests that variations in geomagnetic field intensity could change climate through modulation of CR flux.
[49]
Modeling impacts of geomagnetic field variations on middle ...
Jan 17, 2008 · The last full polarity reversal, the Matuyama/Brunhes transition, occurred about 780,000 years ago. It is clearly recorded in volcanic and ...
[50]
Geomagnetic, cosmogenic and climatic changes across the last ...
Ages of two polarity reversals, the Matuyama-Brunhes boundary and base Olduvai, are at odds with ages given in popular geomagnetic polarity timescales.Missing: synchroneity | Show results with:synchroneity
[51]
Human Evolution at the Matuyama-Brunhes Boundary | Request PDF
Aug 9, 2025 · This discontinuity is related to a major step in human evolution: the transition from Homo ergaster/erectus to Homo heidelbergensis. View.
[52]
Global Geomagnetic Field Evolution From 900 to 700 ka Including ...
May 27, 2023 · This study examines the Matuyama-Brunhes (MB) reversal using a new reconstruction of the global geomagnetic field based on paleomagnetic data.