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	<title>Famous Experiments - Revision history</title>
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		<title>JonoThora: Psionics expansion (01a + 01b): content authored / LaTeX-restored per local submodule; lint-clean.</title>
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		<updated>2026-05-11T20:48:35Z</updated>

		<summary type="html">&lt;p&gt;Psionics expansion (01a + 01b): content authored / LaTeX-restored per local submodule; lint-clean.&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;= Famous Experiments =&lt;br /&gt;
&lt;br /&gt;
{{Audience_Sidebar&lt;br /&gt;
| difficulty   = Beginner&lt;br /&gt;
| reading_time = 12 minutes&lt;br /&gt;
| prerequisites = High-school science vocabulary. Familiarity with the word &amp;quot;statistical significance&amp;quot; helps but isn&amp;#039;t required.&lt;br /&gt;
| if_too_basic_see = [[Anomalous_Cognition]]&lt;br /&gt;
| if_you_want_the_math_see = [[PEAR_Program]]; [[Ganzfeld_Procedure]]&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
The credibility of any psionic framework rests on data, not on philosophy. This page summarises five experiments — chosen for breadth, methodological care, and historical importance — that the curious public most often asks about.&lt;br /&gt;
&lt;br /&gt;
For each: &amp;#039;&amp;#039;&amp;#039;what was done&amp;#039;&amp;#039;&amp;#039;, &amp;#039;&amp;#039;&amp;#039;what was found&amp;#039;&amp;#039;&amp;#039;, &amp;#039;&amp;#039;&amp;#039;replication status&amp;#039;&amp;#039;&amp;#039;, and &amp;#039;&amp;#039;&amp;#039;what it does and does not prove&amp;#039;&amp;#039;&amp;#039;.&lt;br /&gt;
&lt;br /&gt;
== 1. The Ganzfeld experiments (1974–present) ==&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was done.&amp;#039;&amp;#039;&amp;#039; A &amp;quot;sender&amp;quot; looks at a randomly selected image for 30 minutes. A &amp;quot;receiver&amp;quot; is in a different soundproofed room with halved ping-pong balls over their eyes (the &amp;#039;&amp;#039;ganzfeld&amp;#039;&amp;#039;, or &amp;quot;whole field&amp;quot; — a uniform sensory environment) and white noise in headphones. The receiver describes any mental imagery that arises. After the session, the receiver is shown four candidate images (one true target + three decoys) and ranks them.&lt;br /&gt;
&lt;br /&gt;
By chance, the receiver picks the true target 25 % of the time. Above-chance picking would be evidence for information transfer.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was found.&amp;#039;&amp;#039;&amp;#039; Meta-analysis of decades of ganzfeld trials (Bem &amp;amp; Honorton 1994 &amp;#039;&amp;#039;Psychological Bulletin&amp;#039;&amp;#039;; Storm, Tressoldi, Di Risio 2010 &amp;#039;&amp;#039;Psychological Bulletin&amp;#039;&amp;#039;) gives a hit rate around 32 % — about 7 percentage points above chance. Across hundreds of trials this is statistically extraordinary (effect size ≈ 0.13; combined p far below 10&amp;lt;sup&amp;gt;−10&amp;lt;/sup&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Replication status.&amp;#039;&amp;#039;&amp;#039; &amp;#039;&amp;#039;&amp;#039;Replicated&amp;#039;&amp;#039;&amp;#039; across multiple independent labs. The methodological critiques (Hyman) have been largely addressed by autoganzfeld protocols (Honorton). Effect size is small but durable.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it proves.&amp;#039;&amp;#039;&amp;#039; That the human pair-receiver hit-rate exceeds chance, robustly, under controlled conditions. The mechanism is not specified by the experiment.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it does not prove.&amp;#039;&amp;#039;&amp;#039; That the mechanism is ψ-mediated. The data are consistent with (a) ψ-mediated information transfer, (b) some subtle methodological artefact still unidentified, or (c) an unknown sensory channel. The probabilistic case for ψ is strong; the proof is not closed.&lt;br /&gt;
&lt;br /&gt;
See [[Ganzfeld_Procedure]] for full methodological detail.&lt;br /&gt;
&lt;br /&gt;
== 2. The PEAR program (1979–2007) ==&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was done.&amp;#039;&amp;#039;&amp;#039; At Princeton, the Engineering Anomalies Research lab ran 2.5 million human-machine interaction trials. Subjects sat in front of a random event generator (REG) — a quantum-noise-based binary random source — and tried to &amp;#039;&amp;#039;influence&amp;#039;&amp;#039; the long-run distribution of 0s and 1s by intention alone.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was found.&amp;#039;&amp;#039;&amp;#039; Across the full dataset, REG outputs deviated from chance in the intended direction by approximately 1 hit in 10,000 trials. Tiny per-trial effect; combined statistical significance ~ 7 sigma (p &amp;lt; 10&amp;lt;sup&amp;gt;−12&amp;lt;/sup&amp;gt;).&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Replication status.&amp;#039;&amp;#039;&amp;#039; &amp;#039;&amp;#039;&amp;#039;Partial.&amp;#039;&amp;#039;&amp;#039; The PEAR effect has been replicated by several independent groups (Mind-Matter Interaction Consortium, 2000) and also failed to replicate in others. The overall picture: the effect appears in some configurations and not in others; the meta-analysis is positive but the heterogeneity is high.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it proves.&amp;#039;&amp;#039;&amp;#039; That under specific (PEAR-replicating) conditions, intentional cognitive engagement with an REG produces measurable deviations from random behaviour.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it does not prove.&amp;#039;&amp;#039;&amp;#039; The exact mechanism. PEAR&amp;#039;s own [[Robert_G_Jahn|Jahn]] and [[Brenda_J_Dunne|Dunne]] favoured a consciousness-field interpretation; sceptics propose statistical artefacts, optional-stopping, or experimenter effects.&lt;br /&gt;
&lt;br /&gt;
See [[PEAR_Program]].&lt;br /&gt;
&lt;br /&gt;
== 3. Targ-Puthoff remote viewing (1974) ==&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was done.&amp;#039;&amp;#039;&amp;#039; At Stanford Research Institute (SRI), Targ and Puthoff worked with several subjects (most famously Pat Price and Ingo Swann) to test &amp;quot;remote viewing&amp;quot; — described as gathering information about a distant location using only mental focus.&lt;br /&gt;
&lt;br /&gt;
Targets were randomly selected from a sealed list. Subject described and sketched the target. Independent judges rated the match between description and target. Statistical analysis: did real-target matches outscore decoys?&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was found.&amp;#039;&amp;#039;&amp;#039; Published in &amp;#039;&amp;#039;Nature&amp;#039;&amp;#039; (Targ &amp;amp; Puthoff, 1974). Subjects&amp;#039; descriptions matched intended targets at rates far above chance. Combined p-values were astronomical for individual high-performing subjects.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Replication status.&amp;#039;&amp;#039;&amp;#039; &amp;#039;&amp;#039;&amp;#039;Partial.&amp;#039;&amp;#039;&amp;#039; The SRI / SAIC program (which became Star Gate) ran for 23 years and consumed about $20 million of US government funding ([[Star_Gate_Program]]). The 1995 AIR (American Institutes for Research) review found a statistically significant effect (&amp;quot;the laboratory studies provide evidence of a statistically significant effect that warrants further investigation&amp;quot;) but concluded the operational utility was unclear. Replication outside the US programme has been mixed.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it proves.&amp;#039;&amp;#039;&amp;#039; That under SRI / Star Gate conditions, a small number of operationally-screened individuals produced descriptions of remote targets that matched non-randomly at high statistical significance.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it does not prove.&amp;#039;&amp;#039;&amp;#039; Whether the effect scales to general populations, whether it can be made operationally reliable, and what the underlying mechanism is.&lt;br /&gt;
&lt;br /&gt;
See [[Remote_Viewing]] and [[Star_Gate_Program]].&lt;br /&gt;
&lt;br /&gt;
== 4. The Tate Cooper-pair mass anomaly (1989) ==&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was done.&amp;#039;&amp;#039;&amp;#039; James Tate, Blas Cabrera, Susan Felch, and James Anderson at Stanford precisely measured the effective mass of a Cooper pair in a rotating superconducting ring. The result — a fundamental quantum property — should match the prediction from condensed-matter physics ([[BCS_Theory|BCS]] times some small corrections) to high precision.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was found.&amp;#039;&amp;#039;&amp;#039; Published in &amp;#039;&amp;#039;Physical Review Letters&amp;#039;&amp;#039; (Tate et al. 1989). The measured Cooper-pair mass was &amp;#039;&amp;#039;heavier&amp;#039;&amp;#039; than the BCS prediction by 84 parts per million — far outside the experimental uncertainty.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Replication status.&amp;#039;&amp;#039;&amp;#039; &amp;#039;&amp;#039;&amp;#039;Unreplicated to date&amp;#039;&amp;#039;&amp;#039;; no group has redone the experiment with comparable precision. The result has stood unchallenged but also unconfirmed for nearly four decades.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it proves.&amp;#039;&amp;#039;&amp;#039; That as of 1989 the most careful measurement of a Cooper-pair mass disagreed with the standard theoretical prediction by a statistically significant amount.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it does not prove.&amp;#039;&amp;#039;&amp;#039; Why. Several explanations have been proposed: hidden systematic error, missing electromagnetic correction, [[Modified_Einstein_Equations_with_Psi|coupling to a scalar field]] (the present framework&amp;#039;s interpretation), or unknown condensed-matter effect. The framework specifically predicts ~10&amp;lt;sup&amp;gt;−4&amp;lt;/sup&amp;gt;–10&amp;lt;sup&amp;gt;−5&amp;lt;/sup&amp;gt;-level corrections of exactly this scale — fitting the data — but until the experiment is repeated, the case is not closed.&lt;br /&gt;
&lt;br /&gt;
See [[Cooper_Pair_Mass_Anomaly]] and [[Tate_Experiment]].&lt;br /&gt;
&lt;br /&gt;
== 5. The Tajmar gravitomagnetic London moment (2007) ==&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was done.&amp;#039;&amp;#039;&amp;#039; Martin Tajmar&amp;#039;s group (originally at Austrian Research Centers, later TU Dresden) measured the gravitomagnetic field around a rotating ring of niobium superconductor at cryogenic temperatures. Standard GR predicts a &amp;quot;gravitomagnetic London moment&amp;quot; — a tiny gravitational analogue of the magnetic London moment — but the GR prediction is far below any existing detector.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What was found.&amp;#039;&amp;#039;&amp;#039; Published in arXiv (Tajmar et al. 2007 and subsequent papers). The measured signal was 28 orders of magnitude larger than the GR prediction — extraordinary if real.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Replication status.&amp;#039;&amp;#039;&amp;#039; &amp;#039;&amp;#039;&amp;#039;Mixed.&amp;#039;&amp;#039;&amp;#039; Some follow-up groups (Tajmar&amp;#039;s own; Graham et al.) confirmed the basic effect; others (Lipa et al.) found null results. The disagreement appears to depend on temperature, geometry, and shielding details. As of 2024 the picture is unsettled.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it proves.&amp;#039;&amp;#039;&amp;#039; That under some conditions, rotating superconductors emit (or appear to emit) much stronger gravitomagnetic-like signals than mainstream GR allows.&lt;br /&gt;
&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;What it does not prove.&amp;#039;&amp;#039;&amp;#039; Whether the signal is gravitomagnetic, electromagnetic-contamination-of-the-detector, or a different anomaly. The framework&amp;#039;s interpretation: ψ-field-mediated amplification (the e&amp;lt;sup&amp;gt;kψ&amp;lt;/sup&amp;gt; F&amp;lt;sub&amp;gt;μν&amp;lt;/sub&amp;gt;F&amp;lt;sup&amp;gt;μν&amp;lt;/sup&amp;gt; coupling) in a high-coherence Cooper-pair condensate. Not the only explanation, but a clean one.&lt;br /&gt;
&lt;br /&gt;
See [[Gravitomagnetic_London_Moment]] and [[Tajmar_Experiments]].&lt;br /&gt;
&lt;br /&gt;
== Honourable mentions ==&lt;br /&gt;
&lt;br /&gt;
A handful of additional results that didn&amp;#039;t make the top-five list but are widely cited:&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;The presentiment / pre-cognition studies&amp;#039;&amp;#039;&amp;#039; (Bem 2011 &amp;#039;&amp;#039;JPSP&amp;#039;&amp;#039;) — controversial, mixed replication.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Global Consciousness Project&amp;#039;&amp;#039;&amp;#039; (Nelson 1998–present) — REG anomalies correlated with global events.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Sheldrake &amp;quot;sense of being stared at&amp;quot;&amp;#039;&amp;#039;&amp;#039; meta-analysis — small positive effect.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Dotta-Persinger photon emission during cognition&amp;#039;&amp;#039;&amp;#039; (2012) — biophoton anomaly during focused thought.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Ning Li / Podkletnov gravity-shielding&amp;#039;&amp;#039;&amp;#039; — historically important but heavily contested.&lt;br /&gt;
&lt;br /&gt;
Each is treated in detail at its own page; see also [[Anomalous_Cognition]] and [[Replication_Crisis_in_Parapsychology]].&lt;br /&gt;
&lt;br /&gt;
== What a curious reader should take away ==&lt;br /&gt;
&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;The data is not &amp;quot;all noise&amp;quot;.&amp;#039;&amp;#039;&amp;#039; Multiple independent paradigms produce statistically significant effects. Sceptics dispute the interpretation, not the existence of the deviations.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;The effects are usually small.&amp;#039;&amp;#039;&amp;#039; Even the strongest paradigms produce effect sizes of a few percent over chance. This is the typical signature of a weak-coupling phenomenon, which is consistent with the framework&amp;#039;s prediction of a weakly-coupled ψ field.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;The mechanism is not yet proven.&amp;#039;&amp;#039;&amp;#039; &amp;quot;Something is happening&amp;quot; is well-established; &amp;quot;what is happening&amp;quot; remains the central open question — which the present framework attempts to answer.&lt;br /&gt;
* &amp;#039;&amp;#039;&amp;#039;Replication is improving.&amp;#039;&amp;#039;&amp;#039; Preregistration, autoganzfeld, modern statistics, and open data have all raised the standard of the recent literature.&lt;br /&gt;
&lt;br /&gt;
== Where to go next ==&lt;br /&gt;
&lt;br /&gt;
* For a structured falsification list: [[Falsification_Criteria_for_Psionics]].&lt;br /&gt;
* For the methodological context: [[Replication_Crisis_in_Parapsychology]].&lt;br /&gt;
* For the open questions the framework cannot yet answer: [[Open_Questions_in_Psionics]].&lt;br /&gt;
* For the history: [[History_of_Psionics_Research]].&lt;br /&gt;
&lt;br /&gt;
== See Also ==&lt;br /&gt;
&lt;br /&gt;
* [[Psionics_Primer]]&lt;br /&gt;
* [[Anomalous_Cognition]]&lt;br /&gt;
* [[Ganzfeld_Procedure]]&lt;br /&gt;
* [[PEAR_Program]]&lt;br /&gt;
* [[Remote_Viewing]]&lt;br /&gt;
* [[Star_Gate_Program]]&lt;br /&gt;
* [[Cooper_Pair_Mass_Anomaly]]&lt;br /&gt;
* [[Gravitomagnetic_London_Moment]]&lt;br /&gt;
&lt;br /&gt;
== References ==&lt;br /&gt;
&lt;br /&gt;
* Bem, D. J., Honorton, C. (1994). &amp;quot;Does psi exist? Replicable evidence for an anomalous process of information transfer.&amp;quot; &amp;#039;&amp;#039;Psychological Bulletin&amp;#039;&amp;#039; 115: 4–18.&lt;br /&gt;
* Storm, L., Tressoldi, P. E., Di Risio, L. (2010). &amp;quot;Meta-analysis of free-response studies, 1992–2008: Assessing the noise reduction model in parapsychology.&amp;quot; &amp;#039;&amp;#039;Psychological Bulletin&amp;#039;&amp;#039; 136: 471–485.&lt;br /&gt;
* Jahn, R. G., Dunne, B. J. (1987). &amp;#039;&amp;#039;Margins of Reality.&amp;#039;&amp;#039; Harcourt Brace Jovanovich.&lt;br /&gt;
* Targ, R., Puthoff, H. E. (1974). &amp;quot;Information transmission under conditions of sensory shielding.&amp;quot; &amp;#039;&amp;#039;Nature&amp;#039;&amp;#039; 251: 602–607.&lt;br /&gt;
* Mumford, M. D., Rose, A. M., Goslin, D. A. (1995). &amp;#039;&amp;#039;An Evaluation of Remote Viewing: Research and Applications.&amp;#039;&amp;#039; AIR.&lt;br /&gt;
* Tate, J., Cabrera, B., Felch, S. B., Anderson, J. T. (1989). &amp;quot;Precise determination of the Cooper-pair mass.&amp;quot; &amp;#039;&amp;#039;Physical Review Letters&amp;#039;&amp;#039; 62: 845–848.&lt;br /&gt;
* Tajmar, M., et al. (2007). &amp;quot;Experimental detection of the gravitomagnetic London moment.&amp;quot; arXiv:gr-qc/0603033.&lt;br /&gt;
&lt;br /&gt;
[[Category:Psionics]]&lt;br /&gt;
[[Category:Plain language]]&lt;br /&gt;
[[Category:Experiments]]&lt;/div&gt;</summary>
		<author><name>JonoThora</name></author>
	</entry>
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