Where is everybody? · Working papers

Would a past presence on Earth have left a trace?

Revised after a second, separate analysis run for this project tried to break it. Neither analysis is an outside expert.

Would we know? Detectability of a past visit or industrial episode in Earth's rock record

Revised after review. Code: code/run_all.py regenerates every number and figure below.

Summary. Earth's rock record is close to silent on brief or local past presences and only weakly informative about a planet-wide industrial one. That qualitative result survived a hostile review; several first-pass numbers did not. The one quantity measured directly is how much ancient land surface has been closely inspected: a 100 km2 by 20-kyr cell placed at random in 3-500 Ma land space-time contains a terrestrial fossil collection with probability 1.0e-6, and a 10,000 km2 cell with probability 1.0e-4 (the referee reproduced this to 2% from a fresh download). Turning that into "we would know" needs unmeasured factors. With them, an installation occupied for 10 kyr and buried in deep time is known today with probability about 2.5e-7 (1 km2), 2.5e-5 (100 km2) and 2.3e-3 (10,000 km2) for a random time in the last 500 Myr, and five times less over 2.4 Gyr. Each is uncertain by about a factor of 10 either way, and those ranges are widths of assumed priors, not confidence intervals. Installations of 100 km2 or less would be known essentially only if they date from the last 0.06-0.13 Myr; that surface-survival term is an assumption with no dataset behind it, and it alone produces the first-pass values of 1.2e-4 and 3.4e-4. A human-scale industrial episode would be known with probability about 0.1-0.2 (0.01-0.7) in the last 500 Myr. The 500 GtC of fossil carbon burnt so far would be flagged in under 1% of Cenozoic cases; half of pulses are flagged at 1,500-1,900 GtC; the PETM is the only Cenozoic excursion above 2,000 GtC equivalent. Main caveats: everything between the measured probe and P(known) is assumed, pre-Cenozoic carbon detection is assumed, and the plutonium bound is conditional on an uptake assumption that the modern ocean does not support.

Question

If a visiting installation, or a home-grown industrial episode, existed on Earth at a random time in the past, what is the probability that we would know about it today? The Fermi model needs this before "there is no trace of anyone on Earth" can count as evidence.

Data

Source Rows used Cuts
Macrostrat API v2 (Peters, Husson & Czaplewski 2018) North America 949 columns, 24,141 units (20,593 sedimentary); South America 58 columns; Caribbean 64; New Zealand 329; Africa 2; deep sea 132 sites, 7,124 units Projects 1, 7, 8, 5, 9, 4. Offshore-drilling (eODP) units not used: the API returned HTTP 500
Macrostrat global bedrock map, coarsest scale 4,000 random land points (fixed seed), 3,560 mapped Land mask: Natural Earth 1:110m
Paleobiology Database (PBDB) 278,411 unique fossil collections; 47,525 in 36 terrestrial environment classes Needs coordinates and an age range
CENOGRID (Westerhold et al. 2020), PANGAEA 917660 23,939 benthic carbon-isotope values, 0-67.1 Ma 382 rows without a carbon-isotope value dropped
DM-SED v0.0.1 (Lai et al. 2025), Zenodo 14771859 63,627 marine-sediment geochemical samples, 5,766 sites Spacing statistics need 5 or more samples and a non-zero age span: 1,076 sites. 799 of 1,875 sites with 5+ samples carry one age and drop out

Macrostrat column coverage is 32.1 million km2, 22% of land area, 77% of it North America. DM-SED and CENOGRID are single compilations, not a census of what has been sampled.

Method

Preservation. From Macrostrat, per 1-Myr step from 0 to 3,500 Ma: the fraction of column area holding sedimentary rock of that age (marine and non-marine), hiatus durations, years per centimetre, and the slope of accumulation rate against time span (Sadler effect).

Examination. Each PBDB collection is one close inspection of a small patch of bedding of known place and age. An installation of area A occupied for a time tau counts as sampled if a terrestrial collection lies inside its footprint and the collection's age window overlaps the occupation. Collections exist only where sediment was deposited, survived and is exposed, so this one empirical number folds preservation, exposure and examination together.

Carbon. A pulse of M GtC of fossil carbon shifts the ocean's carbon-isotope ratio by -25 x M/(M + 40,000) per mil and recovers over about 100 kyr. Synthetic pulses are injected at random ages into CENOGRID and recovered with two independent detectors: a matched filter with a local baseline (4,000 injections) and a plain step statistic (mean of the 50 kyr after onset minus the 100 kyr before; 1,500 injections). A pulse is flagged when it is a 5-sigma outlier against local natural variability.

Synthesis. A 20,000-draw Monte Carlo combines the above. P(known) for an installation is the sum of a deep-time part (PBDB probe x E x recognition) and a surface part (remains still discoverable at today's land surface). Assumptions that are not data:

Assumption Range
E: all inspections that would report an artefact layer, per PBDB terrestrial collection 3-300, log-uniform
Probability an inspected artefact bed is recognised (also absorbs how densely artefacts fill the footprint and survive burial) 0.1-1
Time one inspected bed represents 3-100 kyr
Surface part: survival time 0.03-1 Myr; found if still there 0.1-0.7 (1 km2), 0.5-1 (100 km2), 0.8-1 (10,000 km2) no dataset
Carbon: pre-Cenozoic coverage (Mesozoic 0.14-0.8, Paleozoic 0.05-0.5, Precambrian 3e-4 to 1e-2) and noise 1-6 times the Paleocene level assumed
Carbon: a catalogued event is attributed to industry 0.003-0.3
Size of one independently preserved patch (100 km2); global-to-North-America scaling (8) drive the "preserved somewhere" model outputs only

Results

1. The deliverable. Medians with 5-95% ranges of the assumed priors.

Scenario (random time in window) Deep-time part, 500 Myr Surface part, 500 Myr (assumed) Combined, 500 Myr Combined, 2.4 Gyr
1 km2, 10 kyr 2.5e-7 (2e-8 to 3.4e-6) 1.2e-4 1.2e-4 (2e-5 to 8e-4) 2.6e-5
100 km2, 10 kyr 2.5e-5 (1.9e-6 to 3.3e-4) 2.5e-4 3.4e-4 (7e-5 to 1.4e-3) 7.1e-5
10,000 km2, 10 kyr 2.3e-3 (1.8e-4 to 3.1e-2) 3.1e-4 2.9e-3 (4.4e-4 to 3.1e-2) 6.1e-4
Human-scale built footprint, 1e6 km2 dispersed, 300 yr 0.09 (0.008 to 0.46) 3e-4 0.09-0.21 by variant (0.008 to 0.72) 0.02-0.045 (0.002 to 0.15)
Fossil-carbon pulse 5,000 GtC: catalogued as a singular event 0.13 measured + 0.16 assumed (0.07 to 0.31) 0.29 (0.20 to 0.44) 0.061 (0.042 to 0.094)
Same pulse recognised as industrial (assumed attribution) 0.009 (0.001 to 0.07) 0.002
Fossil-carbon pulse 500 GtC: catalogued 0.002 0.0005
244Pu fallout at 10% or more of weapons tests (conditional) 0.015, at most 0.05 0.003, at most 0.010

The surface part is equivalent to certain knowledge of the last 0.06 Myr (1 km2), 0.13 Myr (100 km2) and 0.15 Myr (10,000 km2), with ranges of 0.01 to 0.75 Myr. Conditional on the event lying within the last 1 Myr, P(known) is 0.06, 0.13 and 0.15. The deep-time parts over 2.4 Gyr are 5.3e-8, 5.1e-6 and 4.9e-4. At the extreme corner of the priors (E x recognition = 300, 100-kyr beds) the 500-Myr deep-time values reach only 2e-5, 2e-3 and 0.17. The 500 GtC row is almost entirely the assumption that ice cores register any pulse in the last 0.8 Myr.

2. What survives, and how finely it records time.

0-66 Ma 66-252 Ma 252-539 Ma older, to 2,400 Ma
North American area holding sediment of that age 0.17 0.18 0.20 0.037
Non-marine sediment only 0.095 0.050 0.010 0.007
Unit duration, time-weighted median / plain median (Myr) 8 / 1.5 16 / 4.6 13 / 2.9 79 / 23
Years per cm, time-weighted / plain median 270 / 170 560 / 340 600 / 370 900 / 340
Terrestrial fossil collections per Myr (PBDB) 291 92 15 2 in total

A typical North American column holds sediment for 18% of the last 500 Myr (16-84% of columns: 4.6-39%) and 5% of the last 2.4 Gyr, with 4,120 Phanerozoic gaps of median 12 Myr. Deep-sea sediment represents 900-3,300 years per centimetre (time-weighted; 470-1,500 plain). A 300-year episode is a centimetre or less.

3. Installations by age (10,000 km2, 10 kyr, central assumptions).

3-66 Ma 66-252 Ma 252-539 Ma 539-2,400 Ma
Terrestrial collections worldwide overlapping its time window (measured) 5.9 1.8 0.31 3e-4
P(a collection lies inside it): PBDB probe (measured) 3.5e-4 1.2e-4 2.0e-5 2e-8
P(known today) 8e-3 2.6e-3 4.6e-4 4e-7
P(some part preserved anywhere): model output 0.25 0.12 0.03 0.008

For 100 km2 the first three rows are 100 times lower. The last row depends on an assumed patch size and a Sadler extrapolation over three to five decades; across reasonable choices it spans 0.015-1.0 (3-66 Ma) and 0.002-0.71 (Paleozoic). It does not enter P(known). A 1-Myr occupation of 10,000 km2 raises the 500-Myr value to 0.037 (0.004-0.30).

4. Global carbon episode (0-66 Ma, share of injected pulses flagged).

Pulse Recorded peak 5 sigma, matched filter / step 3 sigma, matched filter Natural excursions at least as large
500 GtC (fossil carbon emitted to date) -0.25 per mil 0.4% / 0.7% 7% 85
2,000 GtC -0.97 per mil 57% / 87% 95% 1
3,000 GtC -1.4 per mil 93% / 98% 99% 1
5,000 GtC (all conventional fossil fuel) -2.3 per mil 99% / 98% 99% 1

Half of pulses are flagged at 1,890 GtC (matched filter) or 1,480 GtC (step statistic), and 90% at 2,890 or 2,160 GtC. By epoch, a 3,000 GtC pulse is flagged 84% of the time in the Eocene and 96-100% elsewhere. The PETM (55.9 Ma) is equivalent to 8,300-9,800 GtC. The next largest excursions, at 10.8 Ma and 62.1 Ma, are equivalent to 1,400-1,700 GtC; they stay below 5 sigma with the matched filter and exceed it with the step statistic. So "the only 5-sigma event" depends on the detector; "the only event above 2,000 GtC equivalent" does not. Detectability depends on total carbon, not duration: releases over 300 and 10,000 years differ by under 5%, and 5,000 GtC spread over 1 Myr is flagged under 2% of the time. Before 66 Ma no injection test was run; the probabilities used (0.31 Mesozoic, 0.04 Paleozoic, 1e-4 Precambrian for 5,000 GtC) are assumed.

5. Fast markers. Share of 2.58-500 Ma time with at least one section sampled at a given spacing, as lower bounds:

Spacing DM-SED only CENOGRID only Combined floor
1 kyr or finer 0.021% 0.36% 0.38%
10 kyr or finer 1.0% 11% 12%
50 kyr or finer 17% 13% 28%

Within 2.58-66 Ma, CENOGRID alone covers 2.8% of time at 1-kyr spacing and 88% at 10 kyr. A random 300-year window holds an expected 0.1 existing samples in DM-SED and 0.5 in CENOGRID. A model extrapolation puts a 300-year marine layer in roughly 2 to 20 column-sized regions worldwide at any Phanerozoic date (P of surviving somewhere 0.8-1). So a 300-year layer probably survives somewhere, is rarely sampled at the needed resolution before the Quaternary, and would be smeared over about 7 kyr by sediment mixing even where sampling is dense.

6. Nuclear fingerprints. By decay alone, a 20th-century-scale inventory stays measurable for about 0.1 Myr (240Pu), 0.4 Myr (239Pu), 140 Myr (129I), 180 Myr (236U) and 620 Myr (244Pu). The archive is the real limit. Published crust counts (141 and 6.3 atoms of 244Pu in the 1.34-4.57 and 4.57-9 Myr layers) allow a past fallout pulse of at most about 10% of the weapons-test total, if a pulse enters the crust with the uptake of 0.17 adopted for interstellar dust. That condition fails where it can be tested: the same arithmetic predicts 2,200-12,000 bomb-derived counts in the top layer, while the published residual of 34 ± 17 leaves room for at most about 255. If a past pulse were taken up no better, the limit would be 0.9-5 times the weapons-test fallout, which excludes nothing.

7. What is excluded.

8. The Moon (preservation only). Features 10 m across are erased in 1-16 Myr, 30 m in 11-140 Myr, 100 m in 0.13-1.6 Gyr, and 300 m or more persist 1.1 to over 3.5 Gyr. On Earth the modelled chance that some part of a 10,000 km2 site is preserved is 0.008-0.25, so like-for-like preservation is roughly 4-120 times better on the Moon, with the terrestrial term itself poorly constrained. The larger difference is examination: lunar features sit at a surface that orbital imagery covers, while terrestrial remains are buried and almost entirely uninspected.

Robustness checks

Limitations

Closest prior work and what is new

Schmidt & Frank (2018) pose the question and conclude qualitatively that direct evidence older than about 4 Ma is unlikely. Wright (2018), Haqq-Misra & Kopparapu (2012), Davies (2012) and Haqq-Misra et al. (2022) are also qualitative. Peters & Heim (2010) already combined Macrostrat with PBDB to measure how much of the North American rock record has been sampled palaeontologically; Zalasiewicz (2008) and Zalasiewicz et al. (2014) treat the preservation of urban strata; Kemp et al. (2015) show how the record under-resolves rates. I found no work that assigns probabilities. New here: the PBDB probe expressed per installation footprint and duration; injection-recovery of industrial carbon pulses against a real record with two detectors; the split of P(known) into measured and assumed parts with marginalised exclusion counts; the conditional 244Pu bound with its modern-layer test. Confidence that this is new: medium.

Implications for the Fermi paradox

Largest number of past episodes compatible with no known trace (95%), with the uncertainty in P marginalised:

Scenario Last 500 Myr Last 2.4 Gyr P(no trace) if one per stellar passage (21,000 in 2.33 Gyr)
1 km2, 10 kyr 61,000 290,000 0.52
100 km2, 10 kyr 18,000 87,000 0.28
10,000 km2, 10 kyr 2,700 13,000 0.021
Human-scale industrial episode 60-130 290-600

One installation of 100 km2 or less per stellar passage is compatible with what we know, and the residual constraint (0.3-0.5) comes from the assumed surface term: with a visit every 110 kyr the latest would be recent. On buried strata alone the limits are 2.7 million (100 km2) and 28,000 (10,000 km2). One 10,000 km2, 10-kyr installation per passage is disfavoured at about 98% under the stated assumptions (94-99.8% across the fly-by study's 11,000-59,000 range); the 95% limit is about 60% of passages. The Fermi model should give the terrestrial null result a likelihood ratio near 1 for brief presences of 100 km2 or less at any plausible E, weak weight for 10,000 km2 installations, and an assumption-dependent 0.01-0.7 per event for planet-wide industrial episodes. The Moon's surface is the more informative archive if it has been adequately searched.

Figures

Figure 1. Top: the fraction of a continent that still holds sedimentary rock of a given age, which falls from about half for the last million years to a few per cent beyond 500 million years. Bottom: how many years one centimetre of the surviving rock represents. A typical centimetre spans several hundred years, so an episode of 300 years would be about a centimetre thick.
Figure 1. Top: the fraction of a continent that still holds sedimentary rock of a given age, which falls from about half for the last million years to a few per cent beyond 500 million years. Bottom: how many years one centimetre of the surviving rock represents. A typical centimetre spans several hundred years, so an episode of 300 years would be about a centimetre thick. Open at full size.
Figure 2. Top: how many fossil collections and geochemical samples exist for each million years of the Earth’s history. Bottom: the chance that a fossil collection from land falls inside the area and time of an installation occupied for ten thousand years, for three sizes of installation. Even for one of 10,000 square kilometres the chance is below one in a thousand.
Figure 2. Top: how many fossil collections and geochemical samples exist for each million years of the Earth’s history. Bottom: the chance that a fossil collection from land falls inside the area and time of an installation occupied for ten thousand years, for three sizes of installation. Even for one of 10,000 square kilometres the chance is below one in a thousand. Open at full size.
Figure 3. A test on the best record of the last 66 million years, the deep-sea carbon-isotope record. Top: the record. Middle: a scan for the mark an industrial release of carbon would leave, a sudden drop with a slow recovery; only the known natural warming event of 56 million years ago stands out. Bottom: the fraction of artificial pulses added to the record that the scan finds. A pulse the size of all fossil carbon burnt so far is found less than 1 time in 100 at the strict threshold and 7 to 16 times in 100 at the loose one.
Figure 3. A test on the best record of the last 66 million years, the deep-sea carbon-isotope record. Top: the record. Middle: a scan for the mark an industrial release of carbon would leave, a sudden drop with a slow recovery; only the known natural warming event of 56 million years ago stands out. Bottom: the fraction of artificial pulses added to the record that the scan finds. A pulse the size of all fossil carbon burnt so far is found less than 1 time in 100 at the strict threshold and 7 to 16 times in 100 at the loose one. Open at full size.
Figure 4. (a) The probability that an installation would be known today, split into remains still at the surface (assumed) and remains buried in rock (data and assumptions). (b) The same probability by when the installation existed. (c) The probability that a release of fossil carbon would be in today’s catalogue of events, by size and age. (d) The largest number of past episodes consistent with nothing having been found, beside the number of star systems that have passed close to the Sun.
Figure 4. (a) The probability that an installation would be known today, split into remains still at the surface (assumed) and remains buried in rock (data and assumptions). (b) The same probability by when the installation existed. (c) The probability that a release of fossil carbon would be in today’s catalogue of events, by size and age. (d) The largest number of past episodes consistent with nothing having been found, beside the number of star systems that have passed close to the Sun. Open at full size.
Figure 5. Left: how long the radioactive traces of a nuclear age on the scale of the twentieth century would stay measurable, from about 100,000 years for plutonium-240 to about 600 million years for plutonium-244. Right: for an installation of 10,000 square kilometres, the successive losses: the fraction of its rock layers that survive, the fraction now exposed at the surface, and the chance that a fossil collection samples it.
Figure 5. Left: how long the radioactive traces of a nuclear age on the scale of the twentieth century would stay measurable, from about 100,000 years for plutonium-240 to about 600 million years for plutonium-244. Right: for an installation of 10,000 square kilometres, the successive losses: the fraction of its rock layers that survive, the fraction now exposed at the surface, and the chance that a fossil collection samples it. Open at full size.

Response to referee

Referee point Action
DM-SED used as a census; 0.08% a grid artefact Accepted. Exact interval union (0.021%); relabelled as lower bounds; CENOGRID floors added; "none at 100-yr spacing" and "has not been looked at" removed; mixing caveat added. My CENOGRID floor at 1 kyr is 0.36%, not 0.5%, because Quaternary samples lie outside the 2.58-500 Ma window
Exclusion counts ignore uncertainty in P; fly-by sentence false for 10,000 km2 Accepted. Marginalised limits replace 3/median (reproducing the referee's values); fly-by statement rewritten by footprint size
Headline for 100 km2 or less is an assumption Accepted. Surface and deep-time parts reported separately everywhere; deep-only values lead the summary
244Pu bound too strong and conditional Accepted. Bound is now about 10%, labelled conditional; modern-layer test added; crusts attributed correctly. I quote modern uptake as at most 2-12% of the model's assumption (from the published error bar), not "about 1%"
"Only 5-sigma event" depends on the statistic; Eocene weaker Accepted. Second detector added; claim restated as "only event above 2,000 GtC equivalent"; completeness by epoch; 50% mass 1,500-1,900 GtC
Weighted medians reported as plain Accepted. Both given
Moon comparison mixes preservation with P(known) Accepted. Restated as preservation plus surface visibility; the ratio is quoted as rough because the terrestrial term is uncertain
Human-scale number biased low Accepted. Per-inspection and lowland variants added; median 0.09-0.21, envelope 0.008-0.72 (a factor of 1.3-2.3 higher, not 2-3)
Missing assumptions; carbon mixes measured and assumed; 700 GtC includes land use Accepted. Patch size and scaling listed and tested; "preservation is not the bottleneck" withdrawn; 5,000 GtC given as 0.13 measured + 0.16 assumed; 500 GtC used for emissions to date; recorded peak -2.3 per mil
Prior work Added and verified by search: Peters & Heim 2010, Zalasiewicz 2008, Zalasiewicz et al. 2014, Davies 2012, Kemp et al. 2015, Haqq-Misra et al. 2022
Ranges are prior widths Accepted and stated throughout

No point was rejected outright.

References

Davies 2012, Acta Astronaut. 73, 250. Fassett & Thomson 2014, JGR Planets 119, 2255. Friedlingstein et al. 2025, Earth Syst. Sci. Data 17, 965. Haqq-Misra & Kopparapu 2012, Acta Astronaut. 72, 15. Haqq-Misra et al. 2022, arXiv:2209.11685. Kemp, Eichenseer & Kiessling 2015, Nat. Commun. 6, 8890. Kirtland Turner et al. 2017, Nat. Commun. 8, 353. Lai et al. 2025, DM-SED, Zenodo 10.5281/zenodo.14771859. Peters & Heim 2010, Paleobiology 36, 61. Peters, Husson & Czaplewski 2018, Geochem. Geophys. Geosyst. 19, 1393. Schmidt & Frank 2018, Int. J. Astrobiol. 18, 142. Steier et al. 2013, Nucl. Instrum. Methods B 294, 160. Wallner et al. 2015, Nat. Commun. 6, 5956; 2021, Science 372, 742 (counts as tabulated by Wang et al. 2021, arXiv:2105.05178). Westerhold et al. 2020, Science 369, 1383. Wright 2018, Int. J. Astrobiol. 17, 96. Zalasiewicz 2008, The Earth After Us, Oxford University Press. Zalasiewicz et al. 2014, Anthropocene Review 1, 34. Zeebe et al. 2016, Nat. Geosci. 9, 325.

Key numbers

Quantity Value Uncertainty Note
PBDB space-time probe: P(a terrestrial fossil collection lies inside the footprint and a 20-kyr window), averaged over 3-500 Ma 1.05e-8 (1 km2), 1.05e-6 (100 km2), 1.0e-4 (10,000 km2) referee reproduced to 2% from a fresh download with a different method; 0.3-0.6 times these if same-formation collections count once The only directly measured quantity in the installation chain. 47,525 terrestrial of 278,411 collections.
P(known today), installation occupied 10 kyr, deep-time part (buried strata: PBDB probe x E x p_recognise), random time in last 500 Myr 2.5e-7 (1 km2); 2.5e-5 (100 km2); 2.3e-3 (10,000 km2) 5-95% of assumed priors: 2e-8 to 3.4e-6; 1.9e-6 to 3.3e-4; 1.8e-4 to 3.1e-2 Last 2.4 Gyr: 5.3e-8, 5.1e-6, 4.9e-4. Extreme corner of the priors (E x p_recognise = 300, 100-kyr beds): 2e-5, 2e-3, 0.17.
Surface part (assumed): remains still discoverable at or near today's land surface equivalent to certain knowledge of the last 0.06 Myr (1 km2), 0.13 Myr (100 km2), 0.15 Myr (10,000 km2) 5-95%: 0.01-0.38, 0.03-0.64, 0.03-0.75 Myr No dataset behind it. P(known | within the last 1 Myr) = 0.06, 0.13, 0.15. Contributes 1.2e-4, 2.5e-4, 3.1e-4 to the 500-Myr values.
P(known today), combined (surface + deep), installation 10 kyr, last 500 Myr 1.2e-4 (1 km2); 3.4e-4 (100 km2); 2.9e-3 (10,000 km2) 5-95%: 2e-5 to 8e-4; 7e-5 to 1.4e-3; 4.4e-4 to 3.1e-2 Unchanged from the first pass, but 99.8% (1 km2) and 91% (100 km2) of it is the assumed surface term. Last 2.4 Gyr: 2.6e-5, 7.1e-5, 6.1e-4.
P(known today), dispersed human-scale built footprint (1e6 km2, 300 yr), last 500 Myr 0.09 baseline; 0.12-0.21 in modelling variants envelope of 5-95% ranges: 0.008-0.72 Variants: recognition per inspection, lowland concentration x1-5, both. Last 2.4 Gyr: 0.019 baseline, up to 0.045; envelope 0.002-0.15. By era (baseline, central): 0.34 (3-66 Ma), 0.14 (Mesozoic), 0.03 (Paleozoic), 2.5e-5 (older).
95% upper limit on the number of past episodes given no known trace, uncertainty in P marginalised, last 2.4 Gyr 290,000 (1 km2); 87,000 (100 km2); 13,000 (10,000 km2); 600 (human-scale, 290-600 across variants) 3/P at the 95th to 5th percentile of P: 19,000-730,000; 11,000-200,000; 460-32,000; 31-1,800 Last 500 Myr: 61,000; 18,000; 2,700; 130. First-pass 3/median values were 2-4 times too strong. Using the deep-time part only: 2.6e8, 2.7e6, 28,000, 640.
P(no known trace | one 10-kyr installation per stellar passage within 1 pc; 21,000 passages in 2.33 Gyr) 0.52 (1 km2); 0.28 (100 km2); 0.021 (10,000 km2) for 11,000-59,000 passages: 0.67-0.29; 0.44-0.09; 0.06-0.002 The 1 and 100 km2 values come from the assumed surface term (a visit every 110 kyr leaves a recent one); with buried strata only they would be about 1. For 10,000 km2 the 95% limit is 60% of passages.
Carbon pulse flagged in CENOGRID at 5 sigma: mass for 50% / 90% detection 1,890 / 2,890 GtC (matched filter); 1,480 / 2,160 GtC (step statistic) matched-filter robustness range for the 50% mass: 1,490-2,780 GtC 3,000 GtC flagged 93% overall: 84% Eocene, 96-100% other epochs (98% with the step statistic).
Fraction of injected 500 GtC pulses (fossil carbon emitted to date) flagged in CENOGRID 0.4% (matched filter) to 0.7% (step) at 5 sigma; 7% to 16% at 3 sigma 85 natural excursions in 66 Myr are at least as large. Recorded peak after sediment mixing: -0.25 per mil. For 700 GtC (fossil + land use, an upper bound): 0.9-2.5% and 17-35%.
Largest natural Cenozoic carbon-isotope excursions, as equivalent fossil-carbon pulses PETM 8,300-9,800 GtC; next largest 1,400-1,700 GtC (10.8 Ma and 62.1 Ma) The PETM is the only event above 2,000 GtC equivalent under both detectors. Only the PETM reaches 5 sigma with the matched filter; three events do with the step statistic.
P(5,000 GtC fossil-carbon pulse is catalogued as a singular event), last 500 Myr 0.29 = 0.13 measured (Cenozoic injection test) + 0.16 assumed (pre-Cenozoic) assumed part 0.07-0.31; total 0.20-0.44 Last 2.4 Gyr: 0.061 = 0.027 measured + 0.034 (0.014-0.067) assumed. Recognised as industrial (assumed attribution 0.003-0.3): 0.009 (0.001-0.07) and 0.002.
Floor on the share of 2.58-500 Ma time with at least one geochemically sampled section at <=1 kyr / <=10 kyr / <=50 kyr spacing 0.38% / 12% / 28% (DM-SED and CENOGRID combined) DM-SED alone: 0.021% / 1.0% / 17% (exact interval union; the first-pass 0.08% was a grid artefact). CENOGRID alone: 0.36% / 11% / 13%. Lower bounds from two compilations, not a census.
Global 244Pu fallout pulse allowed by deep-sea crust counts, 1.34-9 Myr ago at most about 10% of 20th-century weapons-test fallout, conditional on crust uptake of 0.17 for a pulse 2.6% if the tabulated flux is read as a flux in space; 3-4% from the 4.57-9 Myr layer alone The same arithmetic predicts 2,200-12,000 bomb counts in the top layer, against at most about 255 compatible with the published 34 +- 17 residual. If a past pulse were taken up no better than that, the limit is 0.9-5 times the weapons-test fallout, which is no exclusion.
North American area still holding sedimentary rock of a given age 0.20 (mean, last 500 Myr); 0.037 (500-2400 Ma) Non-marine only: 0.095 (0-66 Ma), 0.050 (Mesozoic), 0.010 (Paleozoic), 0.007 (older). Macrostrat, 949 columns; referee reproduced.
Share of time represented by sediment in a typical North American column 18% of the last 500 Myr; 5% of the last 2.4 Gyr 16-84% of columns: 4.6-39% (500 Myr) 4,120 Phanerozoic hiatuses, median 12 Myr, on a 1-Myr grid.
Time resolution of surviving sediment (unit duration / thickness) time-weighted medians 250-1,000 yr/cm (continental), 900-3,300 (deep sea); plain medians of units 170-370 and 470-1,500 yr/cm Unit duration: time-weighted median 8-16 Myr by era, plain median 1.5-4.6 Myr (3.1 Myr over all 20,593 units).
Modelled P(some part of a 10,000 km2, 10-kyr site is preserved anywhere) 0.25 (3-66 Ma), 0.12 (Mesozoic), 0.03 (Paleozoic), 0.008 (539-2400 Ma) 0.015-1.0, 0.007-0.99, 0.002-0.71, 0.0004-0.32 across patch size 10-1,000 km2, Sadler exponent 0.38-0.6 and unit-duration convention Model output, not a measurement. Does not enter P(known), which uses the PBDB probe.
Lunar surface feature lifetime 10 m: 1-16 Myr; 30 m: 11-140 Myr; 100 m: 0.13-1.6 Gyr; 300 m and larger: 1.1 to over 3.5 Gyr Two scalings of Fassett & Thomson 2014. Like-for-like preservation is roughly 4-120 times better than the terrestrial baseline; the larger difference is that the lunar surface is visible from orbit.

Changes made after the referee report

Referee points not accepted

Code

Every number above is produced by these scripts from public data. The data tables themselves are not hosted here; the scripts download them.

common.py run_all.py s00_fetch.py s01_macrostrat.py s02_mapsample.py s03_pbdb.py s04_cenogrid.py s05_dmsed.py s06_signals.py s07_synthesis.py s08_figures.py

Referee report

A second, separate analysis re-ran the code, recomputed the main numbers by its own route and tried to break the result. Like the first, it was run by Claude for this project; it is not an outside expert. In its report “the analyst” is the first analysis, which wrote the paper, and file names that are not linked on this page are its own working files. The paper above is the version revised in response.

Verdict: sound with fixes. Results reproduced: yes.

RERUN. I copied code/ to a separate working folder and ran run_all.py --no-fetch s01..s07 on the cached raw files (113 s). All 36 CSV/JSON outputs are byte-identical to the analyst's data/ directory. I did not repeat the cold download.

INDEPENDENT RECOMPUTES:

  1. PBDB probe (chk_pbdb.py). Fresh PBDB API download using PBDB's own envtype=terrestrial filter instead of the analyst's 36-class list, and a random-disc Monte Carlo on the sphere instead of a fixed grid. P(collection inside a 10,000 km2 footprint and 20-kyr window):
Period Referee Analyst
Paleogene 2.76e-4 2.75e-4
Cretaceous 1.82e-4 1.85e-4
Permian 5.90e-5 5.86e-5

The probe is in effect N_collections/Myr x (tau+h) x A/A_land; clustering changes it by about 10%.

  1. Macrostrat (chk_macro.py), my own parser and interval-union code:
Quantity Referee Analyst
North American sediment area fraction, 0-500 Ma 0.197 0.197
Non-marine fraction, 0-66 / 66-252 / 252-500 Ma 0.091 / 0.050 / 0.012 0.095 / 0.050 / 0.010
Per-column time with sediment, last 500 Myr (median; 16-84%) 18.0%; 4.5-38.6% 18.2%; 4.6-38.7%
500-2400 Ma area fraction 0.0367 0.0367
  1. CENOGRID (inj_ceno.py). A deliberately different detector: step statistic (mean of the 50 kyr after onset minus the 100 kyr before), no template fit, 1,500 injections.
Quantity Referee Analyst
50% detection mass at 5 sigma 1,470 GtC 1,890 GtC (own robustness range 1,490-2,780)
700 GtC flagged at 5 sigma 2.4% 0.85%
700 GtC flagged at 3 sigma 33% 17%
3,000 GtC or more flagged 98.5% 93-99%
PETM z = -20.9, raw benthic step about -3.0 per mil z = -14.7

The carbon thresholds are confirmed to about 25%. The PETM is by far the largest event in both.

  1. Monte Carlo (marg.py). I rebuilt the 20,000-draw synthesis from the same seed and reproduced all installation medians and ranges exactly. The same draws give the surface/deep split and the marginalised exclusion numbers used in the errors below.

  2. E factor, back-of-envelope. About 10^4 coal mines, each cutting roughly 0.5 Myr of terrestrial strata, give a probe of about 7e-4 for a 10,000 km2 site over 500 Myr. That is roughly 7 times the PBDB probe, consistent with the assumed E of order 10-30.

CITATIONS CHECKED. Wang et al. 2021 (arXiv:2105.05178) Table 2: Crust-3 layers 0-1.34 / 1.34-4.57 / 4.57-9.0 Myr, counts 34±17 / 141±19 / 6.3, fluxes 930 / 1990 / 270, uptake 0.17. All match the code. Zeebe et al. 2016 (at least 4,000 yr, under 1.1 PgC/yr) confirmed. Steier et al. 2013 ratio (5.7±1.0)e-5 confirmed, and the 7.94e-5 Baltic value exists. Kirtland Turner et al. 2017 is Nat. Commun. 8, 353; the '<5 kyr' wording could not be read from the truncated abstract (it matches my memory of the paper). Fassett & Thomson's 5.5 m2/Myr is supported by later Fassett abstracts. The CENOGRID file header confirms PANGAEA 917660 and Westerhold et al. 2020.

Strongest objection

A stratigrapher would say the study measures one thing well and then multiplies it by guesses. The measured quantity is the share of ancient land-surface space-time that sits inside a PBDB terrestrial fossil collection: about 1e-4 for a 10,000 km2 by 20-kyr cell averaged over 3-500 Ma. I reproduced that from a fresh download by a different method to within 2%. Everything between that number and 'P(known today)' is unmeasured: the ratio of all rock inspections to PBDB collections (E, 3-300), the chance an artefact bed is recognised (0.1-1), the time one bed represents (3-100 kyr), and, for sites of 100 km2 or less, an assumed Quaternary survival term that supplies 91-99.8% of the headline value. Treating a fossil collection as an inspection that would reveal an installation also assumes artefacts are dense across the whole footprint and survive burial alteration in recognisable form. The quoted 5-95% ranges are widths of assumed priors, not confidence intervals.

Does the conclusion survive? In its qualitative form, yes. Space-time coverage is 1.3e-6 x E for 100 km2 by 20-kyr cells, so no defensible E brings it near 1. Even at the extreme corner of the analyst's priors (E x p_recognise = 300, h = 100 kyr), the 500-Myr deep-time probability is at most about 2e-3 for 100 km2 and about 0.17 for 10,000 km2. An independent mining-based estimate puts E at order 10. 'Near-silent on brief, local presences' is therefore robust.

The specific central values do not survive as defensible numbers. The 1 km2 and 100 km2 values are restatements of the surface-survival assumption. The human-scale 0.09 could lie anywhere from about 0.01 to 0.5 and is probably biased low. The pre-Cenozoic carbon probabilities are assumed. They should go into the Fermi model as order-of-magnitude conditional estimates with the surface and deep-time parts separated, and the exclusion counts must be marginalised.

Errors found

Overclaims

Novelty check

Novel: partly. Three searches (two extended) found no published work that assigns probabilities to the Silurian question. Schmidt & Frank 2018 and later reviews (the 2022 decadal white paper arXiv:2209.11685, a recent technosignature review) stay qualitative and repeat the 'older than about 4 Ma, small chance' judgement. The PBDB space-time probe and the CENOGRID injection-recovery test appear to be new as applied to this question, and I reproduced both independently. The ingredients are standard, and the combined p(known) values are assumption-driven rather than measured. The analyst's 'medium' confidence is fair. Prior work that should be added: Peters & Heim 2010 (Paleobiology 36, 61), which already combines Macrostrat with PBDB to measure how much of the rock record palaeontologists have sampled; Zalasiewicz et al. 2014 ('The technofossil record of humans') and Zalasiewicz 2008 ('The Earth After Us') on the preservation potential of urban strata; Davies 2012 (Acta Astronautica 73, 250) on terrestrial traces of alien technology; Kemp et al. 2015 on resolving rates in the record. These four are cited from memory and were not re-verified by search today.

Required changes