A scientist casually pressing two fingers onto the anthropogenic pan of a laboratory balance, lifting natural variability into the air.

Science Blog · Methods

Method bias in climate records

The same ice, trees, flasks, and satellites can support different public stories. The difference is usually how the data were handled: how a stand-in is turned into temperature, which years are averaged away, what is pasted onto the end of a graph, and which energy term is treated as the cause. Most of that is bias in the method. One claim — the fossil-fuel “fingerprint” at −28‰ — is assembled after the measurement, not read from the flask.

A few terms

Proxy
A stand-in for temperature or CO₂ — ice, tree rings, leaf pores — not a thermometer.
Splice
Putting two different kinds of measurement on one graph, as when tree rings or ice are joined to weather-station temperatures.
Albedo
How much sunlight Earth reflects. Lower albedo means more heat absorbed.
Skin layer
The ocean’s top film. Infrared from the air stops here, in about ten micrometres. Sunlight heats much deeper water.
Keeling intercept
The isotopic tag of added CO₂, read from a mixing plot. Fossil fuel is claimed at about −28‰. The flasks sit near −13‰.

A published curve is often treated as a thermometer. It usually isn’t. An ice core is a local archive. The conversion from ice chemistry to temperature can be moved. A hockey-stick graph can flatten a medieval warm period and paste instruments over a volcanic cooling. Ice-core carbon isotopes are said to match flasks only after gravity, diffusion, and calibration corrections. Recent warming follows absorbed sunlight more closely than a leftover greenhouse term. The ocean stored about twenty times more heat leaving the ice age than it has in the industrial era. That medieval-to–Little Ice Age swing happened with almost no change in ice-core CO₂.

1. Ice cores are local, and the conversion is not unique

The Alley 2000 series is an ice core from one place in Greenland. It is a local archive, not a global thermometer.

The proxy is the oxygen-18 ratio in the ice (δ¹⁸O), converted to temperature with a slope. Young snow is not ice yet; that layer is called firn. Change the slope, the elevation correction, the site noise, or the 1855 firn cutoff, and the mid-Holocene warm peak — the Holocene Thermal Maximum, or HTM — can sit warmer than Summit today. Join the same ice to Arctic weather-station temperatures on one axis, and the story flips.

Summit Uncertainty lab: Alley 2000 proxy chart, uncertainty cards, and method-bias panel
Figure 1. Summit Uncertainty lab. Left: Alley 2000 GISP2 oxygen-18 anomalies versus a 1000–1850 baseline, with Arctic GISTEMP 64–90°N joined as a sharp black spike at right. Right: which way each method choice moves “HTM vs today.” Open Summit Uncertainty

With those published choices, the lab reports an adjusted Alley HTM of −28.70 °C at Summit. At the same site, on the same baseline, GISP2 ice for 2001–2010 is −29.90 °C. The mid-Holocene is then +1.20 °C warmer than that local mean. The number often used as “now” is GISTEMP 64–90°N for 2015–24: +3.38 °C, on a different baseline, in a different place.

Cards comparing adjusted HTM, Summit today at the same site, and Arctic GISTEMP now
Figure 2. Comparison cards. Ice HTM −28.70 °C; Summit 2001–2010 at the same site −29.90 °C; “misleading now” +3.38 °C from Arctic GISTEMP, not Summit. Method bias can hide a warmer Holocene at Summit, or invent a spike the borehole never measured. Open Summit Uncertainty
GISTEMP 64–90°N measures a different place. Using it as “now” against GISP2 “then” can hide a Holocene that was warmer at Summit, or invent an unprecedented spike the borehole never measured. Method bias can move the ice the other way.

δ¹⁸O is not a pure thermometer. Nearby Greenland cores still agree only about r ≈ 0.4. Moisture source, transport, season, elevation, drift, firn diffusion, and vapor exchange all move the isotope. The conversion slope was allowed to wander by about a factor of two.

A borehole is a temperature profile down the ice, not a year-by-year record. Heat spreading through the ice blurs swings that lasted only a few decades. Those short swings are gone from the borehole even if they were real at the surface. The published Alley series stops in the 1850s because snow is not ice yet. Dating of layers is the strong part. Temperature is the weak part: ±1.4 K on gas-isotope inversions, versus about 0.05–0.1 K on instruments.

Six reasons the overlay is not a comparison, including oxygen-18 drivers
Figure 3. “Six reasons the overlay is not a comparison,” including the list of drivers that keep oxygen-18 from being read as temperature. Open Summit Uncertainty

2. The hockey stick flattens a volcanic century

Mann, Bradley and Hughes (1998/99) drew a flat thousand years with a sharp twentieth-century upturn. The nickname is a hockey stick: a long handle, then a blade. The Hockey Stick Lab rebuilds that shape from the published tree-ring network, then shows the same century with volcanic sulfate and a single overweighted site in view.

McIntyre and McKitrick (2005) showed the blade is what you get when one strip-bark bristlecone site — Sheep Mountain, ITRDB CA534 — is weighted over 390 times the rest of the network. Fifteen bristlecone and foxtail sites accounted for 93% of the first principal component, the statistical extract that dominates the reconstruction. Many of those trees are strip-bark. Graybill and Idso (1993) already argued their twentieth-century surge is CO₂ fertilization, not temperature.

Hockey Stick Lab: Northern Hemisphere reconstruction with volcanic eruption markers and 1910–1938, 1940–1970, 1976–2026 trend cards
Figure 4. Hockey Stick Lab. Hard stick from 2% Sheep Mountain weight. 1910–1938 already climbing at +1.98 °C/century; 1940–1970 trough −0.72 °C/century on a volcanic albedo dip (Bezymianny, Agung, Taal, Awu, Fernandina, Fuego); 1976–2026 blade +2.95 °C/century. Without volcanic dimming the century is one moderate climb, not a pause plus a blade. Open the Hockey Stick Lab

Sulfur dioxide from those eruptions becomes sulfate in the stratosphere. The droplets scatter incoming sunlight — higher albedo, cooler surface. Mount Agung (Bali, 1963) is the documented drop through 1964–66. Together they dent a rise that had already started in the 1910s, long before industrial CO₂ could explain it.

The stick hides that by flattening the earlier centuries — the handle — and joining weather stations on at the recovery. Tree-ring series are standardized growth indexes: ring width, not thermometers. HadCRUT5 is a mercury-and-satellite temperature field. Plotting them on one axis joins two different kinds of measurement.

MBH98 also never published that each North American tree-ring series was centered on the 1902–1980 mean, not the full record, before those principal components were taken. Short-centering throws any series that rises in the thermometer era far below zero in earlier centuries. The statistics then hunt those series. That is how a Medieval Warm Period and a Little Ice Age disappear into a handle.

Hockey Stick Lab apples-and-oranges panel: tree-ring growth indexes versus HadCRUT5 thermometer
Figure 5. “Apples and oranges.” Each tree card is independently scaled — a tall swing is that site’s own variance, not degrees Celsius. HadCRUT5 Northern Hemisphere is actual instrumental temperature, 1850–2025. The overlay desk rebases both to 1981–2010 so the shapes can sit on one axis; the units still are not the same quantity. Open the Hockey Stick Lab

3. Emails that treated the Medieval Warm Period as a problem

The method choices above are in the papers. The Climategate correspondence, which Kenneth Richard (@Kenneth72712993) has posted at length, shows something further: a decision to stop plotting tree rings where they diverge from weather stations, and a worry that a visible Medieval Warm Period would undercut the claim that recent warmth is unprecedented.

“I’ve just completed Mike’s Nature trick of adding in the real temps to each series for the last 20 years (ie from 1981 onwards) and from 1961 for Keith’s to hide the decline.”Phil Jones, 16 November 1999, to Mann, Bradley and Hughes

A later processing note is sharper. Maximum latewood density (MXD) is a tree-ring density series used as a temperature proxy. The note says “we have applied a completely artificial adjustment to the data after 1960,” and “we set all post-1960 values to missing in the MXD data set (due to decline), and the method will infill these, estimating them from the real temperatures — another way of ‘correcting’ for the decline, though may be not defensible.”

Kenneth Richard post quoting Climategate emails on hide the decline and setting post-1960 values to missing
Figure 6. Kenneth Richard posting the Jones “hide the decline” line next to the note that post-1960 tree-ring density values were set to missing and filled in from the instrumental temperatures, “though may be not defensible.” The decline being hidden is the tree-ring series after about 1960, covered with thermometers so the blade continues. Open the post

Richard’s follow-up is the bristlecone point the lab makes quantitative. Rocky Mountain strip-bark series produced hockey sticks. Trees that were not bristlecone showed cooling after the 1950s, after a rise from the 1900s to the 1940s. That is why the post-1960 values had to be replaced. The World Meteorological Organization diagram Jones was finishing did not disclose the splice.

Hide the decline graphic: proxy reconstructions versus the same series with instrumental splice after 1960
Figure 7. Graphic Richard has used at NoTricksZone: reconstructions with the proxy decline visible (left) versus the same story after Mike’s Nature trick replaces the post-1960 tree rings with the instrumental blade (right). Xing et al. 2016, D’Arrigo 2006, Schneider 2015, Wilson 2016, Christiansen & Ljungqvist 2012. Open the NoTricksZone article

The Medieval Warm Period was the other obstacle. Jonathan Overpeck, writing as an IPCC coordinating lead author in January 2005, told Keith Briffa and Tim Osborn he wanted to “deal a mortal blow to the misuse of supposed warm period terms and myths in the literature.” Briffa wrote back that some of Peck’s messages could be read as trying to “nail” the Medieval Warm Period — “trying to say there was no such thing.” David Deming later testified that a correspondent he believed to be Overpeck had told him, years earlier, “we have to get rid of the Medieval Warm Period.” Overpeck denied the wording. The 2005 email is not in dispute.

Richard’s most widely shared posts are reconstructions that keep the Medieval Warm Period and the Little Ice Age in the picture. Poland’s early-medieval July about 2.5–3 °C warmer than now. China about 2.8 °C warmer in the Roman and Medieval intervals than 1970–2000. Southern Hemisphere proxies from South America, Antarctica, Australia/New Zealand and the sub-Antarctic as warm or warmer than modern times. Those papers are why a flat handle was so useful.

Reconstruction showing Poland July temperatures around 20.6°C in medieval times versus 17.4°C today
Figure 8. From Richard: Poland’s July temperatures about 20.6 °C in medieval times versus 17.4 °C recently. Little Ice Age Julys sit not far from the modern mean. North American and European mean annual temperatures near the low end of the last 4,500 years in that compilation. Open the post
China reconstruction: Roman and Medieval Warm Periods about 2.8°C warmer than 1970–2000
Figure 9. Richard posting a China reconstruction: Roman Warm Period about 2.89 °C and Medieval Warm Period about 2.81 °C above the 1970–2000 mean. A handle that has already erased those peaks does not need a volcanic 1940–70 dip to look unprecedented. The millennial context is gone before the blade is drawn. Open the post

This does not require a conspiracy. It requires reading the methods next to the mail. Jones’s “trick” and the “not defensible” fill-in are presentation choices. Overpeck’s “mortal blow” is a framing choice for an IPCC box. Together they help explain how a local, volcanic, conversion-dependent century could be sold as a unique blade.

4. Smoothing can make the present look unique

Ice-core CO₂ and temperature are heavily smoothed. Smoothing averages neighboring years so short swings disappear and the line looks cleaner. Plant stomata — the pores on leaves, counted as a growing-season CO₂ proxy — still show century-scale swings. Those swings only meet the ice where the instrumental record is joined on. Presenting the smoothed ice as “the” CO₂ history, then calling the industrial tick unique, is a resolution choice, not a new measurement.

Stomata versus ice-core CO2 during the industrial rise
Figure 10. Stomata vs Ice lab. Ice (points) climbs from about 286 to 370 ppm by the late 1990s and onward with Mauna Loa. Dashed stomatal means keep extra century-scale structure; Beck 2007 (dotted) spikes near 1940. Open Stomata vs Ice

On glacial timescales, the nested paleoclimate desk shows eight Antarctic cycles keeping CO₂ between about 170 and 300 ppm, with the industrial rise as a vertical tick at the right edge. Raw data versus a 5,000-year or 200-year smooth changes how large those earlier swings look next to that tick. The official geologic clock makes the same point: everything measured by satellite sits in the top pixel of Earth history. That is context, not a claim that recent warming is unreal. It is a warning against treating a spliced, smoothed proxy as a single thermometer.

International Chronostratigraphic Chart on the paleoclimate desk
Figure 11. Instrument Record paleoclimate desk: the official geologic chart used as the clock before the ice. The Holocene is the sliver labelled modern time — 11,700 years. Open paleoclimate desk

5. Recent warming tracks absorbed sunlight, not a CO₂ leftover

The Nikolov & Zeller atlas does not claim Earth has not warmed. It claims the usual ledger — greenhouse forcing, a leftover energy imbalance at the top of the atmosphere, and stored heat — is the wrong way to count. Surface temperature tracks absorbed sunlight: the solar energy Earth keeps after clouds, ice, and the rest reflect some of it away. For 2000–2026 the lab reports:

Nikolov and Zeller atlas showing ASR vs GSAT R2 0.84 versus EEI R2 0.45
Figure 12. Nikolov & Zeller atlas. Same months, same global surface temperature. Absorbed sunlight explains 84% of the variance; the energy-imbalance leftover explains 45%. Open the albedo atlas

That solar-plus-albedo reconstruction follows the GISTEMP–NOAA average through July 2026. The 2023 spike sits on a record-low planetary albedo, driven mainly by reduced low cloud over oceans — not by a jump in solar output, and not mostly by polar ice. Polar ice is only a small share of the absorbed-sunlight change.

Modeled versus observed global surface temperature using only albedo and solar output
Figure 13. Atlas time series: black curve is albedo plus solar output only — no CO₂ forcing term, no optical depth, no energy-imbalance leftover. If a greenhouse term were required, the solar-only model would miss the trend. It does not. Open the albedo atlas

Whether the cloud decline itself is from human activity, natural, or mixed is a separate question. Once absorbed sunlight is counted, this window does not need a large leftover CO₂ term. That is method bias in what gets counted: forcing and a leftover imbalance as the ledger, versus absorbed sunlight as the ledger.

6. Ocean heat is sunlight. Greenhouse “forcing” is a lid we have not isolated.

A zettajoule (ZJ) is 10²¹ joules — a huge pile of energy. The Zettajoule atlas puts the industrial ocean-heat pile next to the last deglaciation: the roughly 10,000-year exit from the ice age. Gebbie’s review of noble-gas estimates of mean ocean temperature puts that uptake at 12,000–20,000 ZJ, with a best estimate of about 14,000 ZJ, against roughly 500 ZJ for the industrial ocean through about 2017. That is at least a factor of twenty.

Kenneth Richard (@Kenneth72712993) has posted the same inventory from the literature: deglaciation 20–30 times today’s stored heat; the Medieval Climate Anomaly (the medieval warm interval) about 1,500 ZJ; modern about 500 ZJ— only a third of the way back to the ocean of a thousand years ago. Melting about 130 m of sea-level-equivalent ice took another 15,800 ZJ of latent heat. Public charts that start in 1955 hide the rest of the inventory.

Zettajoule atlas: each square is 500 ZJ, deglaciation 28 squares, medieval 3, modern 1
Figure 14. Zettajoule atlas. Each square is 500 ZJ — the entire modern-era ocean-heat pile. Deglaciation about 14,000 ZJ (28 squares). Medieval Warm Period versus Little Ice Age 1,500 ZJ (3 squares). Modern era 1 square. This is a pile of joules, not a rate: deglaciation ran about 10,000 years at about 0.1 W/m². The industrial ocean is faster, and still a rounding error as a pile. Open the Zettajoule atlas

The medieval ocean held about 1,000 ZJ more than the year-2000 ocean. Preindustrial ice-core CO₂ sits at about 277–285 ppm across that whole medieval-to–Little Ice Age swing of about 1,500 ZJ. The deep ocean still carries Little Ice Age water. Whatever filled and drained those zettajoules, it was not a CO₂ control we can point to in the ice.

Common Era ocean heat: medieval ocean about 1000 ZJ above year 2000, ice-core CO2 nearly flat
Figure 15. Common Era inversion (Gebbie & Huybers): the medieval ocean stored about 1,000 ZJ more than year 2000; the 500 ZJ of modern uptake is one-third of the way back. Law Dome CO₂ is almost flat across the same centuries. Cycles are in the papers — glacial, millennial overturning, Holocene drift into the Little Ice Age. They are not a 500 ZJ alibi, and they are not a CO₂ story. Open the Zettajoule atlas

That inventory sits on a physics point the energy-budget language usually skips. Seawater is heated by shortwave sunlight — visible light — absorbed over metres in the mixed layer, the stirred upper ocean. Thermal infrared from the air, the downward beam in a greenhouse-forcing diagram, is absorbed in about ten micrometres of skin. It never reaches the volume that Argo floats and expendable probes call ocean heat content.

Greenhouse forcing and feedbacks are therefore not a heat engine for the ocean. In theory they only slow cooling at that skin: a thicker lid on the leak, so yesterday’s sunlight stays a little longer. That is a slower leak, not a new source. We have not isolated that lid in the numbers.

Ocean heat enters as shortwave sunlight, not as greenhouse forcingVisible sunlight is absorbed over metres in the mixed layer. Thermal infrared from the atmosphere is absorbed in a ten-micrometre skin and cannot heat the ocean volume. Forcing, if it does anything, can only slow cooling at that skin.SunShortwavevolume heatAtmosphere · H₂O, CO₂, cloudsLongwave IR (~10 μm) cannot enter the water columnSKIN ~10 μm — every downwelling IR photon stops hereMixed layer · metres to tens of metresThis is where sunlight becomes ocean heatThermocline / deep oceanNo sunlight left · infrared never arrived · heat only by mixing from aboveskin coolingForcing and feedbacks are not a heat source for seawaterIn theory a greenhouse lid slows skin cooling. That lid has not been isolated in the ocean-heat inventory.
Figure 16. All ocean heat that is actually in the water arrived as sunlight. Longwave from the air dies in the skin. Forcing, if it does anything, can only slow that skin’s cooling. We do not have a verified isolation of that lid in the deglacial 14,000 ZJ, the medieval 1,000 ZJ surplus, or the industrial 500 ZJ.

Richard has been citing that physics from the papers. Absorbed solar radiation, unlike CO₂, directly heats the ocean and is what tracks global heat content. CO₂ longwave can radiatively touch only the top 0.01 mm of a ~1 mm thermal skin — about 1% of the skin, none of the mixed layer, none of the deep Pacific with its centuries-long lag. A 4 W/m² forcing on that film is a calculated 0.008 K skin-temperature change. That is not a heat engine for the top 2,000 metres.

Kenneth Richard post: CO2 can only radiatively affect the top 0.01 mm of the 1 mm thermal skin layer
Figure 17. Richard on the deep-Pacific lag: CO₂ longwave does not reach water that takes centuries to mix. It stops in the top 0.01 mm of the millimetre-scale skin. The volume Argo reports as ocean heat was never in that film. Open the post
“Longwave radiation penetrates less than a millimeter through water, thus its heating and cooling effects are restricted to the very surface of the ocean: the skin layer.”Wong and Minnett 2018, as posted by Richard — who adds that any thermal-skin longwave effect is dominated by cloud forcing, with CO₂’s longwave impact too small to detect. Open the post

The next step in the literature is the one the energy-budget diagrams skip: it is not possible for the extra energy in the thermal skin to be conducted into the bulk ocean beneath the viscous skin layer. That is the difference between a lid on cooling and a source of zettajoules. Nikolov and Zeller 2024, in a widely circulated post of Richard’s, put the observational counterpart: a global longwave radiative forcing of the sort the models attribute to rising CO₂ “does not exist in reality”. Absorbed solar, not the greenhouse leftover, accounts for the post-2000 trend.

Kenneth Richard quoting literature that extra thermal-skin energy cannot be conducted into the bulk ocean
Figure 18. Richard quoting the thermal-skin literature: CO₂’s radiative reach is the skin, and the extra energy there is not conducted into the ocean beneath the viscous layer. That is the published reason forcing is a lid, not a heat source — and why it has not been isolated as the cause of 12,000–20,000 ZJ of deglacial uptake. Open the post

The leftover we cannot close is large. Average deglacial uptake (about 99 mW/m²) is in the same neighborhood as geothermal heat through the seafloor. Modern imbalance estimates (0.5–0.7 W/m²) are faster, and still reconstructed from sparse floats, expendable probes, and inversions. “Every ZJ here comes from a model of a measurement,” as the atlas puts it. We do not yet have a closed, instrument-verified explanation of why the ocean held more heat a thousand years ago, at 280 ppm, than in 2000. Treating the industrial 500 ZJ as a greenhouse receipt is a choice of ledger, not a completed energy audit.

7. The isotopic “fingerprint” was assembled, not observed

This is the section that goes beyond ordinary calibration bias. Carbon-13 (δ¹³C) is a heavy isotope of carbon. Fossil coal, oil, and gas are depleted in it, so a fossil dump in the air should drag the air’s δ¹³C toward about −28‰. The isotopic lab’s headline is that the number actually read from the flasks is not that fingerprint.

Isotopic δ¹³C Lab: signature assembled not observed, intercept -13.3 versus fossil -28
Figure 19. Isotopic δ¹³C Lab. Observed Keeling intercept −13.3‰ at four stations versus the fossil-fuel claim −28‰. Industrial change in δ¹³C about 1.6‰; largest ice revision 0.2‰. Open the isotopic lab
Francey et al. (1999) and the CSIRO GASLAB flask programme are cited as the fossil-fuel fingerprint in air: falling δ¹³C. Rebuild their record, strip the documented corrections, and the mixing intercept stays near −13‰ — not the −28‰ of coal, oil and gas. The fossil number is a model term, not a measurement.

A Keeling plot graphs δ¹³C against 1/[CO₂]. The intercept of that line is the net isotopic signature of the carbon being added. Seasonally adjusted flasks at Utqiaġvik, La Jolla, Mauna Loa, and South Pole recover intercepts about −12.9 to −13.3‰, with R² near 0.99. If the rise were a fossil dump, that intercept would sit near −28‰, or drift toward it as the fuel mix changed. In the lab’s epoch table it does not:

Keeling plot with observed intercept near -13.4 per mil and fossil line at -28
Figure 20. Keeling geometry as used in the lab: observed mixing intercept near −13.4‰, fossil claim drawn at −28‰. The intercept does not migrate to the fossil line as emissions climb. Open the isotopic lab

Francey et al. (1999) themselves wrote that firn-air δ¹³C agrees with Cape Grim only after correction for gravitational separation, diffusion, and a latitudinal gradient, and that “complex calibration strategies are required.” Those are not hidden emails. They are the methods section. Later Rubino revisions moved a ~0.2‰ South Pole firn mismatch on paper, and applied sample selection plus a 50-year smooth. Cape Grim baseline hours reject a large fraction of flasks. Rejected air is systematically more depleted.

Table of documented isotopic processing corrections
Figure 21. Processing-chain magnitudes compiled from Francey 1999, Allison/GASLAB, and Rubino 2013/2019 as laid out in the lab. Yellow rows are the steps that most change the public fingerprint story. Gravity and diffusion sculpt tenths of a per mil. The leap from −13‰ to −28‰ is an isotopic-flux term in a model inversion, not a flask reading. Open the isotopic lab

The physical firn corrections are ordinary ice-core practice. The bias claim is narrower. The public talking point that “the isotopes prove fossil fuel” presents a hybrid reconstruction plus a model identity as if it were a raw flask intercept. The flask intercept is −13‰. The −28‰ number is assembled afterwards. That is why this article treats the isotopic signature as the case that crosses from method bias into fabrication of a fingerprint.

8. Alternative reconstructions meet dossiers, not just reviews

Scientists who keep these method choices visible report a second kind of bias: rejection by identity, and reputational packaging.

Judith Curry, former chair of Earth and Atmospheric Sciences at Georgia Tech and an AMS/AGU Fellow, has described a fortress mentality after she began emphasizing uncertainty and engaging outsider blogs. Search results filled with “climate denier” frames. She left her academic chair. DeSmog’s Climate Disinformation Database entry on her is the standard package: photograph, credentials, consulting clients, selected quotes, resignation framed as citing the “craziness” of climate science.

DeSmog Climate Disinformation Database profile page for Judith Curry
Figure 22. DeSmog database page for Judith Curry. Breadcrumb: Databases → Climate Disinformation Database → Judith Curry. The page leads with a portrait and then a compiled biography — a pre-built personal file that travels with the name. Open the DeSmog dossier

Ned Nikolov and Karl Zeller stated that manuscripts challenging the conventional greenhouse framing were rejected, sometimes without review, after editors Googled their names. They published under reversed-name pseudonyms (Den Volokin, Lark ReLlez) to get a content-first reading. One paper was later withdrawn over the names rather than the calculations. Their later invited Geomatics paper is the atlas shown above. DeSmog maintains a Karl Zeller page that leads with the pseudonym episode.

Willie Soon is the other recurring dossier: solar papers plus energy-related funding packaged as the story, with journal ethics reviews and congressional interest following the funding narrative more loudly than the energy-balance critiques.

DeSmog presents this as accountability journalism about fossil-fuel influence. The scientists above present it as a blacklist that makes dissenters unhirable and hands activists a ready-made personal file. Political organizations that publish such dossiers know they will be used for targeting. What is not in dispute is the mechanism: a searchable personal dossier attached to a methods disagreement.

Harassment of climate researchers runs in more than one direction. Mainstream scientists have also received abuse and threats. The point here is specific: when the reply to a slope slider, a Keeling intercept, or an albedo leftover is a compiled biography rather than a competing reconstruction, the bias has left the data.

What the figures carry

The labs are public. The underlying papers — Alley 2000, Mann et al. 1998/99, McIntyre & McKitrick 2005, Vinther 2009, Kobashi, Francey 1999, Allison/GASLAB, Rubino 2013/2019, CERES EBAF, Nikolov & Zeller 2024, Gebbie 2021, Gebbie & Huybers 2019 — are public. The Jones, Briffa/Osborn, and Overpeck correspondence is public. Readers can move the sliders and watch the headline move. That is ordinary scientific hygiene. Treating the sliders as heresy is the bias that does not show up in the data file.