---
title: "Gallium experiments: opening the Sun’s low-energy window | Sandbox Physics"
description: "Gallium’s low capture threshold let GALLEX, GNO and SAGE reach the Sun’s most abundant neutrinos, by recovering a few germanium atoms and counting their decays."
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language: "en"
page_type: "story"
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  zh-CN: "https://sandboxphysics.com/zh/stories/neutrinos/gallium-low-energy-solar-neutrinos/"
last_modified: "2026-10-09"
---

[2026 Nobel Prize in Physics](https://sandboxphysics.com/nobel/2026/physics/)

# Gallium experiments: opening the Sun’s low-energy window

The Sun’s most abundant neutrinos had too little energy to trigger the chlorine reaction at Homestake. GALLEX and SAGE reached them with gallium, by recovering a few germanium atoms.

Sandbox Physics · 2026-10-09 · Instruments and methods

## The chlorine detector missed the most common solar neutrinos

Homestake’s chlorine experiment could not see the Sun’s most numerous neutrinos. It detected solar neutrinos through a nuclear capture reaction with a threshold of about 814 keV, above the endpoint of the ordinary pp neutrino spectrum.

Gallium-71 offered a different reaction. An electron neutrino with enough energy could turn it into germanium-71 and an electron. The threshold was about 233 keV, low enough to catch part of the pp spectrum, which extends to about 420 keV.

A lower threshold let researchers ask a new question. If a measurement disagreed with the solar prediction, they could now compare reactions that sample different parts of the spectrum. Gallium mattered because it was sensitive to a new part of the spectrum, not because it gave more events.

$$
{}^{71}\mathrm{Ga}+\nu_e\longrightarrow{}^{71}\mathrm{Ge}+e^-
$$

When gallium-71 captures an electron neutrino, it becomes radioactive germanium-71. The threshold of about 233 keV lets in part of the pp spectrum; gallium also captures higher-energy solar neutrinos.

Sources: [1] · [2] · [3] · [4]

## Two underground laboratories, two target materials

The two collaborations used the same capture reaction with different targets and chemistry. GALLEX, beneath Gran Sasso in Italy, used gallium dissolved in a chemical solution. SAGE, at Baksan in the Caucasus, used metallic gallium.

SAGE began its solar runs in 1990; GALLEX measured solar neutrinos from 1991 to 1997. GNO, the Gallium Neutrino Observatory, continued the Gran Sasso program from 1998 to 2003. These are the years the measurements ran; they say nothing about the facilities today.

The work crossed laboratory and political lines. SAGE began as a Soviet–American collaboration and continued as a Russian–American one. GALLEX and GNO joined several European institutions with other partners. Because the materials and teams were independent, results they shared carried more weight.

Sources: [2] · [5] · [6] · [7]

1. 01 **Expose gallium**

   Neutrino captures build up germanium-71

2. 02 **Extract the atoms**

   Measure how many are recovered and move them to counters

3. 03 **Count their decays**

   Fit the decays over time, allowing for efficiency and background

The recovered atoms give the total number of captures over the exposure. A single atom does not reveal the neutrino’s energy, its direction or the solar reaction that made it.

## Let a few atoms accumulate, then recover them

A radiochemical experiment did not catch each interaction as it happened. It left the target exposed for weeks while neutrino captures built up a tiny number of germanium-71 atoms. The team then extracted the germanium and placed it in small, low-background counters.

Germanium-71 is radioactive. Its decay signals, and the way their rate falls off over time, helped separate the recovered atoms from background. The analysis had to allow for atoms that decayed during the exposure, losses in extraction, counting efficiency and unrelated events.

The method gives up information about single events in exchange for a long, cumulative count. It cannot tell the arrival direction or energy of any captured neutrino. The chemical extraction and the counting are as central to the detector as the large target.

Sources: [2] · [5] · [6]

## Calibration is another measurement with its own assumptions

Researchers checked chemical recovery with carrier material and other procedures, measured counter efficiencies and exposed the gallium to intense artificial neutrino sources. A source of known activity tests more of the process at once: neutrino production, capture, extraction and counting.

A source test does not prove every prediction right, because it rests on assumptions too. Its prediction depends on the nuclear capture cross section, which is the probability of interaction, and on the energy lines of the source. Later reanalysis changed some of the GALLEX efficiencies and results.

The source measurements became a research question of their own. In 2022, BEST reported rates below the prediction for its source, strengthening the gallium anomaly. That result is not a confirmed discovery of sterile neutrinos. Nor have all calibration tests agreed perfectly.

Sources: [5] · [1] · [8] · [9]

## Gallium sees pp neutrinos, but not only pp neutrinos

Gallium also captures neutrinos from beryllium, boron, pep and CNO reactions whenever their energy is above threshold. The total rate is a weighted sum: each component has its own interaction probability and its own electron-flavor flux at the detector.

To pull out the pp part, an analysis needs other measurements or model assumptions about the other components. The low threshold is a major advantage, but no recovered germanium atom can be traced to a particular reaction inside the Sun.

Alongside chlorine, water detectors, SNO and reactor measurements, the gallium programs broadened the evidence on solar neutrinos. They asked whether the puzzle held up in a different energy window and with a different technique. The answer helped turn one detector’s disagreement into a problem that several experiments could test.

Sources: [2] · [1] · [10] · [11]

## What we learned

Gallium’s lower capture threshold brought pp solar neutrinos within reach. GALLEX, GNO and SAGE measured the total capture rate over long exposures, which complemented other detectors. Reading that rate required chemical recovery, decay counting, source calibration and allowance for neutrinos from other solar reactions.

## Primary sources & revision

1. [John Bahcall · Gallium Solar Neutrino Experiments (1997)](https://arxiv.org/abs/hep-ph/9710491)
2. [SAGE Collaboration · Solar neutrino capture rate with gallium metal (1999)](https://arxiv.org/abs/astro-ph/9907113)
3. [GALLEX Collaboration · Solar neutrinos observed at Gran Sasso (1992)](https://doi.org/10.1016/0370-2693(92%2991521-A)
4. [Brookhaven National Laboratory · Raymond Davis Jr. and solar neutrinos](https://www.bnl.gov/bnlweb/history/nobel/2002.php)
5. [Kaether et al. · Reanalysis of GALLEX solar and source experiments (2010)](https://arxiv.org/abs/1001.2731)
6. [GNO Collaboration · Solar Neutrino Observations: GNO I (2000)](https://arxiv.org/abs/hep-ex/0006034)
7. [Brookhaven National Laboratory · Neutrino research and the GALLEX/SNO collaborations](https://www.bnl.gov/science/neutrinos.php)
8. [Barinov et al. · Results from the Baksan Experiment on Sterile Transitions (2022)](https://arxiv.org/abs/2109.11482)
9. [Particle Data Group · Neutrino Masses, Mixing, and Oscillations (2024)](https://pdg.lbl.gov/2024/reviews/rpp2024-rev-neutrino-mixing.pdf)
10. [Bahcall, Gonzalez-Garcia & Peña-Garay · Solar Neutrinos Before and After KamLAND (2003)](https://arxiv.org/abs/hep-ph/0212147)
11. [SNO Collaboration · Direct Evidence for Neutrino Flavor Transformation (2002)](https://arxiv.org/abs/nucl-ex/0204008)

First published 2026-10-09; last revised 2026-10-09. Original explanatory text and diagrams by Sandbox Physics. Illustrations are schematic; no experimental event records are reproduced here. This is an independent educational publication, not an official Nobel or experiment collaboration publication.

[← Previous: The Sun’s missing neutrinos: a tank, a calculation and a long disagreement](https://sandboxphysics.com/stories/neutrinos/homestake-solar-neutrino-problem/) [Next: How do you know those neutrinos came from the Sun? →](https://sandboxphysics.com/stories/neutrinos/kamiokande-real-time-solar-neutrinos/)

## Keep reading

Neutrinos · Reading path

### What happened to the Sun’s neutrinos?

1. [Article **Which reactions in the Sun make neutrinos?**](https://sandboxphysics.com/stories/neutrinos/solar-fusion-neutrino-sources/)
2. [Article **The Sun’s missing neutrinos: a tank, a calculation and a long disagreement**](https://sandboxphysics.com/stories/neutrinos/homestake-solar-neutrino-problem/)
3. [You are here **Gallium experiments: opening the Sun’s low-energy window**](https://sandboxphysics.com/stories/neutrinos/gallium-low-energy-solar-neutrinos/)
4. [Article **How do you know those neutrinos came from the Sun?**](https://sandboxphysics.com/stories/neutrinos/kamiokande-real-time-solar-neutrinos/)
5. [Article **SNO: where did the Sun’s missing neutrinos go?**](https://sandboxphysics.com/stories/neutrinos/sno-flavor-transformation/)
6. [Article **Why does passing through the Sun change a neutrino’s flavor?**](https://sandboxphysics.com/stories/neutrinos/solar-matter-msw-effect/)
7. [Article **Borexino: how do you hear the Sun inside a radioactive world?**](https://sandboxphysics.com/stories/neutrinos/borexino-low-background-solar-neutrinos/)
8. [Article **After the missing neutrinos were explained, what could they tell us about the Sun?**](https://sandboxphysics.com/stories/neutrinos/solar-neutrinos-and-solar-models/)

Neutrinos · Topic

### Unexpected results and sterile neutrinos

Gallium, reactor and timing experiments have all reported surprises. Which ones held up, and could a fourth kind of neutrino explain the rest?

1. [Article **How does a faint signal become a neutrino discovery?**](https://sandboxphysics.com/stories/neutrinos/neutrino-discovery-evidence-chain/)
2. [You are here **Gallium experiments: opening the Sun’s low-energy window**](https://sandboxphysics.com/stories/neutrinos/gallium-low-energy-solar-neutrinos/)
3. [Article **Why can a neutrino change flavor?**](https://sandboxphysics.com/stories/neutrinos/neutrino-flavor-oscillations/)
4. [Article **The reactor anomaly and the spectrum bump ask different questions**](https://sandboxphysics.com/stories/neutrinos/reactor-anomaly-and-spectrum-bump/)
5. [Article **Short reactor baselines: look for a change with distance**](https://sandboxphysics.com/stories/neutrinos/short-baseline-reactor-sterile-tests/)
6. [Article **OPERA: tau appearance and a corrected clock anomaly**](https://sandboxphysics.com/stories/neutrinos/opera-tau-appearance-and-timing-correction/)
7. [Article **Sterile neutrinos: an explanation must pass several tests**](https://sandboxphysics.com/stories/neutrinos/sterile-neutrinos-anomalies-and-tests/)