Sealed beta sources

Feasibility review

Strontium-90 for research

A long-lived beta source: Sr-90 and its yttrium-90 daughter emit betas up to 2.28 MeV.

Half-life
28.91 years
Beta max
545.9 keV; Y-90 2279 keV
Decay
Beta minus to Y-90 (64.05 h), then to Zr-90
Exempt quantity
0.1 µCi
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Request a feasibility review for Sr-90

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How ordering works
Sr-90 at a glanceIAEA evaluated data
aSIMULATED BETA SPECTRUM05001000150020002500Energy (keV)Electrons per keVSr-90, 545.9 keV maxY-90, 2279 keV maxb0204060050100Time (years)Activity (%)T½ 28.91 y
a Energy of the beta particles, calculated from the IAEA data: Sr-90 and its daughter Y-90, in equilibrium (dashed), and the total a source emits. b Activity left after the reference date. Data: IAEA [1]

Research applications

Where Sr-90 does the work.

Figures are simulated examples of each measurement.

  • aSIMULATED050100150Beta dose (Gy)00.51Lx/Tx (rel.)naturalDₑ

    Geochronology and archaeology

    Luminescence dating2, 3, 4

    Sr-90/Y-90 sources in TL and OSL readers give the known doses that luminescence ages are measured against.

    More: Luminescence dating

    A luminescence age is the dose a sample absorbed since it was last exposed to light or heat, divided by the yearly dose rate where it lay buried. The reader gives the sample a series of known beta doses and reads its natural signal against the growth curve they make.

    Risø TL/OSL readers often carry a 1.48 GBq Sr-90/Y-90 source that delivers about 0.1 Gy per second. Many quartz grains saturate with a characteristic dose of 30 to 50 Gy, which limits the oldest ages a sample can give.

  • bSIMULATED0204060Collected charge (ke⁻)EventsMPV 23 ke⁻

    Particle physics instrumentation

    Silicon sensor tests5, 6

    Detector groups test silicon sensors with Sr-90 sources, whose energetic Y-90 electrons deposit charge much as collider particles do.

    More: Silicon sensor tests

    A plastic scintillator behind the sensor triggers only on the most energetic electrons, whose charge in the silicon closely matches that of a minimum-ionizing particle. The CMS tracker group measured charge collection this way on sensors before and after irradiation.

    The collected charge follows a Landau distribution. In 300 µm of silicon its most probable value is about 23,000 electrons.

  • cSIMULATED0204060Distance from source (cm)050100Dose rate (µGy/s)1/d²120 µGy/s6 µGy/s

    Radiation protection dosimetry

    Calibrating beta dosimeters7, 8

    Sr-90/Y-90 is one of the ISO 6980 reference beta sources for calibrating beta dosimeters and dose rate meters.

    More: Calibrating beta dosimeters

    Calibration laboratories place the instrument at a fixed distance from a shuttered source. The PTB beta secondary standard BSS 2, with a 460 MBq Sr-90/Y-90 source, gives a nominal dose rate in tissue at 0.07 mm depth of 120 µGy/s at 11 cm and 6 µGy/s at 50 cm.

  • dSIMULATED012345Aluminium (mm)10⁻³10⁻²10⁻¹1Count rate (rel.)Sr-90Y-90

    Radiation physics

    Beta absorption and thickness gauges9, 10

    Betas stop within a range set by their energy, so the count rate behind an absorber measures its thickness.

    More: Beta absorption and thickness gauges

    Sr-90 betas stop in about 0.7 mm of aluminium and Y-90 betas in about 4 mm, from the Katz and Penfold range-energy relation. A curve of count rate against absorber thickness gives the endpoint energy of each group.

    Industrial nucleonic gauges use Sr-90, among other beta sources, to measure paper, plastic film and aluminium sheet.

  • eSIMULATED0100200300Residue on planchet (mg)02550Efficiency (%)β, Sr-90/Y-90α, Am-241

    Environmental radioanalysis

    Gross beta counting11

    EPA Method 900.0 prescribes Sr-90 in equilibrium with Y-90 for calibrating gross beta counts of drinking water.

    More: Gross beta counting

    Labs add a Sr-90/Y-90 standard to tap water aliquots, dry them on 2-inch planchets with 0 to 300 mg of residue, and plot counting efficiency against residue weight. Each sample's efficiency is read from that curve.

  • fSIMULATED071421Days after separation050100Activity (% of Sr-90)Sr-90Y-90

    Radiochemistry

    Radiostrontium in water1, 12, 13

    Sr-90 in water is measured through its Y-90 daughter, which grows back into purified strontium within two to three weeks.

    More: Radiostrontium in water

    EPA Method 905.0 separates strontium, removes the yttrium, and lets Y-90 grow back in before separating and counting it. Known amounts of Sr-90 standard set the counting efficiencies.

    With its 64.05 hour half-life, Y-90 reaches about 97 percent of the Sr-90 activity two weeks after separation.

  • gSIMULATED010203040Check (day)97100103Counts (% of mean)+2σ−2σ+3σ−3σ

    Laboratory quality control

    Daily instrument checks14

    A long-lived Sr-90/Y-90 check source, counted on each day of use, shows when a counter drifts.

    More: Daily instrument checks

    Labs count the check source at least 20 times to set a central line, then chart each count against warning limits at two standard deviations and control limits at three. A count outside the control limits stops measurements until the problem is found.

    Sr-90/Y-90, with a 2.28 MeV endpoint, is a common beta source for counter calibration. A check source needs a known half-life and enough activity for precise counts, not a traceable certificate.

Forms

Sr-90 forms researchers ask for

Every source is confirmed with its manufacturer before you order.

  • Disk check source

    Sr-90/Y-90 sealed in a thin disk

    Counter and survey meter checks

    Feasibility review
  • Thin-window source

    Deposit in a capsule behind a thin window

    Detector tests and beta absorption

    Feasibility review
  • Wide-area reference source

    Even deposit on a backing plate

    Contamination monitor tests

    Feasibility review
  • Standard solution

    Sr-90/Y-90 in dilute acid, in a sealed vial

    Planchet and counter efficiency standards

    Feasibility review

Activity, certificate and lead time are set with the manufacturer at quote.

Before you order

Plan for decay and licensing.

Plan around decay

Sr-90 has a half-life of 28.91 years. Ask for the activity you need on the day you start using it.

Activity remaining after
  1. 1 year97.6%
  2. 5 years88.7%
  3. 10 years78.7%
  4. 20 years61.9%

Licensing

Exempt quantityNeeds a license100 nCi
Activity of one source, log scale

A single Sr-90 source at or below 0.1 µCi is an exempt quantity under 10 CFR 30.71, Schedule B. Above that, your institution needs a license that covers it.

  • Combining exempt sources to exceed the limit is not covered.
  • Exempt-quantity sources must come from a distributor licensed under 10 CFR 32.18.
  • Agreement States apply equivalent rules. Your RSO reviews the exact source before you order.

Sources: 15, 16, 17

Start a request

Request a feasibility review for Sr-90.

No license file needed to ask. A scientist reads every request and replies with the next step.

  1. Name the instrumentThe counter, reader or sensor setup sets the source form.
  2. Give the window you needA thick window passes only the Y-90 betas.
  3. Plan for decadesActivity falls about 2.4 percent a year. Plan leak tests and disposal with your RSO.
  1. 01Need
  2. 02Details
  3. 03Contact
Where are you starting?

You get Feasibility reply and a candidate supplier path

Decay data

Sr-90 decay data

Decay schemeSr-90 to Y-90 to Zr-90
90Sr28.91 yQ 546 keV90Y90Zr64.05 hβ− 100%β− 100%
Energies in keV, with emission probability per decay. Levels not to scale. Data: IAEA [1]
Half-life
28.91 years ± 0.03
Decay mode
Beta minus (100%)
Daughters
Y-90, then Zr-90
Decay energy (Q)
546 keV
Sr-90 emissions
RadiationEnergy (keV)Per 100 decays
Beta545.9 max, 195.7 mean100
Beta (Y-90)2278.5 max, 932.4 mean100

Sr-90 sources hold Y-90 (half-life 64.05 hours) in equilibrium, so they emit its radiation too; Y-90 lines are per 100 Sr-90 decays.

Source: IAEA LiveChart of Nuclides, ENSDF evaluation by S. K. Basu and E.A. MCCUTCHAN (literature cutoff 1 March 2020), retrieved 25 September 2026 [1]. Reference values; a manufacturer's certificate states the activity of a specific source.

Questions, answered

Sr-90 questions

Why does a Sr-90 source emit two kinds of beta particle?

Sr-90 decays to yttrium-90, which decays in turn with a half-life of 64.05 hours. In a sealed source the two stay in equilibrium, so each Sr-90 decay is matched by a Y-90 decay: betas up to 546 keV from Sr-90 and up to 2.28 MeV from Y-90.

How long does a Sr-90 source last?

Its activity halves every 28.91 years, so about 97.6 percent remains after one year and about 79 percent after ten. The Y-90 activity follows the Sr-90 activity.

Can we buy Sr-90 without a radioactive materials license?

Only very small sources. A single Sr-90 source at or below 0.1 microcurie is an exempt quantity under 10 CFR 30.71, and a distributor licensed under 10 CFR 32.18 can supply it to users without a license. Larger sources need a license that covers them. Your RSO decides how your institution handles each case.

Does Sr-90 emit gamma rays?

Sr-90 and Y-90 decay by beta emission, and the IAEA data list no gamma line from either stronger than one in ten thousand decays. Betas slowing down in the source and its surroundings do make bremsstrahlung X-rays, which your RSO includes in shielding plans.

What activity should we ask for?

State the activity you need at a reference date close to first use, the instrument or measurement it serves, and any window limit. We confirm a matching source and certificate with the manufacturer before you order.

Can a decayed or unused source be returned?

Some manufacturers take back their own sealed sources. A return is a separate shipment with its own RSO and shipping review, so ask us before you need it.

More isotopes

Sources

References

  1. IAEA Nuclear Data Section. LiveChart of Nuclides, Sr-90 and Y-90 decay data (ENSDF evaluations). Retrieved 25 September 2026. www-nds.iaea.org/relnsd/vcharthtml/VChartHTML.html
  2. Duller GAT. Luminescence Dating: Guidelines on Using Luminescence Dating in Archaeology. Swindon: English Heritage; 2008. users.aber.ac.uk/ggd/duller_english_heritage_luminescence_dating.pdf
  3. Osunkwor E, DeWitt R. Beta dose rate reduction for the built-in 90Sr/90Y sources of Risø TL/OSL automated readers. Ancient TL. 2021;39(2):18-27. doi.org/10.26034/la.atl.2021.553
  4. Hu Y, Li B, Jacobs Z. Single-grain quartz OSL characteristics: testing for correlations within and between sites in Asia, Europe and Africa. Methods Protoc. 2020;3(1):2. doi.org/10.3390/mps3010002
  5. Adam W, Bergauer T, Blöch D, et al. (Tracker Group of the CMS Collaboration). Experimental study of different silicon sensor options for the upgrade of the CMS Outer Tracker. J Instrum. 2020;15(4):P04017. doi.org/10.1088/1748-0221/15/04/P04017
  6. Kramberger G, Wermes N. Semiconductor detectors. In: Particle Data Group, Review of Particle Physics. Int J Mod Phys A. 2026;41(22):2630011. pdg.lbl.gov/2026/reviews/rpp2026-rev-particle-detectors-accel.pdf
  7. Ambrosi P, Buchholz G, Helmstädter K. The PTB beta secondary standard BSS 2 for radiation protection. J Instrum. 2007;2(11):P11002. doi.org/10.1088/1748-0221/2/11/P11002
  8. International Atomic Energy Agency. Calibration of Radiation Protection Monitoring Instruments. Safety Reports Series No. 16. Vienna: IAEA; 2000. www-pub.iaea.org/MTCD/Publications/PDF/P074_scr.pdf
  9. Katz L, Penfold AS. Range-energy relations for electrons and the determination of beta-ray end-point energies by absorption. Rev Mod Phys. 1952;24(1):28-44. doi.org/10.1103/RevModPhys.24.28
  10. International Atomic Energy Agency. Technical Data on Nucleonic Gauges. IAEA-TECDOC-1459. Vienna: IAEA; 2005. www-pub.iaea.org/MTCD/Publications/PDF/te_1459_web.pdf
  11. U.S. Environmental Protection Agency. Method 900.0: Gross alpha and gross beta radioactivity in drinking water. In: Prescribed Procedures for Measurement of Radioactivity in Drinking Water. EPA-600/4-80-032. Cincinnati: EPA; 1980. www.epa.gov/sites/default/files/2015-06/documents/epa-900.0.pdf
  12. U.S. Environmental Protection Agency. Method 905.0: Radioactive strontium in drinking water. In: Prescribed Procedures for Measurement of Radioactivity in Drinking Water. EPA-600/4-80-032. Cincinnati: EPA; 1980. www.epa.gov/sites/default/files/2015-06/documents/epa-905.0.pdf
  13. U.S. EPA, NRC, DOE, et al. Multi-Agency Radiological Laboratory Analytical Protocols Manual (MARLAP), Volume II, Chapter 14: Separation techniques. NUREG-1576, EPA 402-B-04-001B. 2004. www.epa.gov/sites/default/files/2015-05/documents/402-b-04-001b-14-final.pdf
  14. U.S. EPA, NRC, DOE, et al. Multi-Agency Radiological Laboratory Analytical Protocols Manual (MARLAP), Volume III, Chapter 18: Laboratory quality control. NUREG-1576, EPA 402-B-04-001C. 2004. www.epa.gov/sites/default/files/2015-05/documents/402-b-04-001c-18-final.pdf
  15. U.S. Nuclear Regulatory Commission. 10 CFR 30.71, Schedule B (exempt quantities). eCFR, current as of 23 September 2026. www.ecfr.gov/current/title-10/section-30.71
  16. U.S. Nuclear Regulatory Commission. 10 CFR 30.18, Exempt quantities. eCFR, current as of 23 September 2026. www.ecfr.gov/current/title-10/section-30.18
  17. U.S. Nuclear Regulatory Commission. 10 CFR 32.18, Manufacture, distribution and transfer of exempt quantities of byproduct material. eCFR, current as of 23 September 2026. www.ecfr.gov/current/title-10/section-32.18

Technical review by ConductScience, 25 September 2026. Next review 25 September 2027.

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