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Validation

Run 2026-09-29 against version 1.4.1

Every number in the tables below was computed by the app’s own physics code — the same code the iOS, Android and web apps run — and compared with a value from outside it: a handbook table, a textbook identity, or an independent calculation written separately for the test. A check outside its tolerance fails the test suite, and this page is only regenerated when none does.

CHECKS
174
OUTSIDE TOLERANCE
0
AREAS
8decay to reactor physics
VERSION
1.4.12026-09-29

How to read the tables

REFERENCE
Where the comparison value comes from. A handbook, ENSDF, CIAAW or a textbook appendix is a published value. “Definition”, “round trip”, “RK4” and “by hand” are independent calculations: they show that the equations are solved correctly, not that the input data is right. The published-value rows cover the data.
TOLERANCE
How precisely the reference itself is quoted, fixed before the check ran — not how close the app happened to land. A rule of thumb such as Co-60 at 1.32 R/h per curie at 1 m gets ±6 %; an exact definition gets a millionth of a percent.
NOT CLAIMED
Conformance to NQA-1, 10 CFR 50 Appendix B or any software quality programme. If your work requires qualified software, use this app as a cross-check, not as the system of record.

Decay and specific activity 13

Closed-form identities

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
lambda = ln2/T½7.3020 × 10⁻¹⁰7.3020 × 10⁻¹⁰< 0.01 %± 1e-6 %definition
A(1 T½)/A₀0.50.5< 0.01 %± 1e-6 %definition
A(10 T½)/A₀9.7656 × 10⁻⁴9.7656 × 10⁻⁴< 0.01 %± 1e-6 %definition
t(1%) in half-lives6.643866.64386< 0.01 %± 1e-4 %definition
A(−1 T½) back-decay22< 0.01 %± 1e-6 %inverse decay

Specific activity vs published Ci/g

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
specific activity Co-60 (Ci/g)1131.611131+0.05 %± 3 %handbook
specific activity Cs-137 (Ci/g)86.811387−0.22 %± 3 %handbook
specific activity Ra-226 (Ci/g)0.9885590.988+0.06 %± 3 %handbook
specific activity Sr-90 (Ci/g)137.542138−0.33 %± 5 %handbook
specific activity H-3 (Ci/g)9621.249650−0.30 %± 5 %handbook
specific activity Pu-239 (Ci/g)0.06202830.0621−0.12 %± 5 %handbook
specific activity U-235 (Ci/g)2.1605 × 10⁻⁶2.1600 × 10⁻⁶+0.02 %± 5 %handbook
specific activity I-131 (Ci/g)1.2429 × 10⁵1.2400 × 10⁵+0.24 %± 5 %handbook

Decay chains 4

Ra-226 chain reaches secular equilibrium in one year

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
secular equilibrium Rn-222/Ra-2261.000011< 0.01 %± 2 %T½(daughter) ≪ T½(parent)
secular equilibrium Pb-214/Ra-2260.9998071−0.02 %± 2 %T½(daughter) ≪ T½(parent)
secular equilibrium Bi-214/Ra-2260.9998071−0.02 %± 2 %T½(daughter) ≪ T½(parent)

Ba-140 → La-140 reaches TRANSIENT equilibrium, not secular

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
La-140/Ba-140 activity at 30 d1.151581.15157< 0.01 %± 1 %λ_d/(λ_d−λ_p)

Gamma dose and shielding 47

Gamma constants vs published R/h per Ci at 1 m

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
Γ Co-60 (R/h per Ci @1 m)1.290911.32−2.20 %± 6 %handbook
Γ Cs-137 (R/h per Ci @1 m)0.3258460.33−1.26 %± 6 %handbook
Γ Ir-192 (R/h per Ci @1 m)0.503330.48+4.86 %± 12 %handbook
Γ Na-22 (R/h per Ci @1 m)1.183491.2−1.38 %± 8 %handbook
Γ I-131 (R/h per Ci @1 m)0.2201960.22+0.09 %± 15 %handbook
Γ Mn-54 (R/h per Ci @1 m)0.4634210.47−1.40 %± 8 %handbook
Γ Au-198 (R/h per Ci @1 m)0.2382760.23+3.60 %± 20 %handbook
Γ Zn-65 (R/h per Ci @1 m)0.3035710.27+12.43 %± 20 %handbook

Geometry, linearity, and the HVL/TVL definitions

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
inverse square 1 m → 2 m44< 0.01 %± 0.01 %1/r²
linearity in activity22< 0.01 %± 1e-6 %rate ∝ A
spectrum HVL halves the rate0.50.5< 0.01 %± 1 %definition
spectrum TVL → 10 % of rate0.10.1< 0.01 %± 1 %definition

Narrow-beam HVL equals ln2/µ from the shipped NIST table

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
Cs-137 narrow HVL Pb (cm)0.5499260.5499< 0.01 %± 1 %ln2/µ @662 keV
Co-60 narrow HVL Pb (cm)1.039321.0367+0.25 %± 1 %ln2/µ @1.25 MeV
Buildup ≥ 1 and rising with depth (Pb, 1 MeV)B = 1.367 at 1 mfp, 2.444 at 5 mfppass—physical requirement

H*(10)/Ka lies in the ICRP 74 band

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
H*(10)/Ka for Cs-137ratio 1.2035, band 1.00–1.35pass—ICRP 74 Table A.21
H*(10)/Ka for Co-60ratio 1.1588, band 1.00–1.35pass—ICRP 74 Table A.21
H*(10)/Ka for Ir-192ratio 1.1724, band 1.00–1.35pass—ICRP 74 Table A.21

Solvers reproduce their own targets (round trips)

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
shield Ir-192 in lead: rate at answer2.5000 × 10⁻⁶2.5000 × 10⁻⁶< 0.01 %± 1e-3 %round trip
shield Co-60 in concrete: rate at answer2.5000 × 10⁻⁶2.5000 × 10⁻⁶< 0.01 %± 1e-3 %round trip
shield Pb-212+ in lead: rate at answer2.5000 × 10⁻⁶2.5000 × 10⁻⁶< 0.01 %± 1e-3 %round trip
shield Ba-140+ in iron: rate at answer2.5000 × 10⁻⁶2.5000 × 10⁻⁶< 0.01 %± 1e-3 %round trip
distance Co-60: rate at answer1.0000 × 10⁻⁴1.0000 × 10⁻⁴< 0.01 %± 1e-3 %round trip
distance Tc-99m: rate at answer1.0000 × 10⁻⁴1.0000 × 10⁻⁴< 0.01 %± 1e-3 %round trip
distance F-18: rate at answer1.0000 × 10⁻⁴1.0000 × 10⁻⁴< 0.01 %± 1e-3 %round trip
Co-60 concrete: transmission at HVL0.50.5< 0.01 %± 0.5 %definition
Co-60 concrete: transmission at TVL0.10.1< 0.01 %± 0.5 %definition
Ir-192 tungsten: transmission at HVL0.50.5< 0.01 %± 0.5 %definition
Ir-192 tungsten: transmission at TVL0.10.1< 0.01 %± 0.5 %definition

+progeny entries equal their members summed by hand

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
Γ Pb-212+ = Pb-212 + Bi-212 + Tl-2080.006544720.00654953−0.07 %± 0.3 %ENSDF, by hand
Γ Ba-140+ = Ba-140 + La-1400.01273610.0127358< 0.01 %± 0.3 %ENSDF, by hand
Γ Mo-99+ = Mo-99 + 0.876 Tc-99m0.001259060.00125906< 0.01 %± 0.3 %ENSDF, by hand

ANS-6.4.3 buildup and the coherent-free μ it requires

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
B lead, 1 MeV, 4 mfp2.205772.21−0.19 %± 3 %ANS-6.4.3 Table 3
B lead, 0.5 MeV, 10 mfp2.084712.1−0.73 %± 3 %ANS-6.4.3 Table 3
B water, 1 MeV, 10 mfp26.435326.1+1.28 %± 3 %ANS-6.4.3 Table 3
B water, 0.5 MeV, 5 mfp18.115418.4−1.55 %± 3 %ANS-6.4.3 Table 3
B concrete, 1 MeV, 10 mfp20.718320.7+0.09 %± 3 %ANS-6.4.3 Table 3
B iron, 1 MeV, 10 mfp15.73315.8−0.42 %± 3 %ANS-6.4.3 Table 3
B iron, 0.5 MeV, 5 mfp7.706497.68+0.34 %± 3 %ANS-6.4.3 Table 3
B aluminum, 1 MeV, 10 mfp21.042321+0.20 %± 3 %ANS-6.4.3 Table 3
coherent share of μ, lead, 662 keV (%)6.033385.99455+0.65 %± 5 %NIST XCOM

Behind a wall the point kernel stays at or above a slab Monte Carlo

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
Cs-137, 20 cm of concrete, 1 m behind: app at or above slab Monte Carloapp/MC = 1.55 (transmission 1.84e-1 vs 1.19e-1)pass—Klein–Nishina slab Monte Carlo
Co-60, 30 cm of concrete, 1 m behind: app at or above slab Monte Carloapp/MC = 1.36 (transmission 1.05e-1 vs 7.77e-2)pass—Klein–Nishina slab Monte Carlo
Cs-137, 40 cm of water, 1 m behind: app at or above slab Monte Carloapp/MC = 1.66 (transmission 2.64e-1 vs 1.58e-1)pass—Klein–Nishina slab Monte Carlo
Cs-137, 5 cm of lead, 1 m behind: app at or above slab Monte Carloapp/MC = 1.13 (transmission 5.53e-3 vs 4.88e-3)pass—Klein–Nishina slab Monte Carlo
Ir-192, 2 cm of lead, 1 m behind: app at or above slab Monte Carloapp/MC = 1.08 (transmission 2.74e-2 vs 2.55e-2)pass—Klein–Nishina slab Monte Carlo
Co-60, 10 cm of lead, 1 m behind: app at or above slab Monte Carloapp/MC = 1.19 (transmission 4.82e-3 vs 4.05e-3)pass—Klein–Nishina slab Monte Carlo

Metastable isomers 20

Decay law and published half-lives

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
isomer T½ Tc-99m (s)21625.921625.9< 0.01 %± 3 %IAEA/ENSDF
isomer T½ Ba-137m (s)153.12153.12< 0.01 %± 3 %IAEA/ENSDF
isomer T½ Ag-110m (s)2.1585 × 10⁷2.1585 × 10⁷< 0.01 %± 3 %IAEA/ENSDF
isomer T½ In-113m (s)5968.565968.56< 0.01 %± 3 %IAEA/ENSDF
isomer T½ Kr-83m (s)65886588< 0.01 %± 3 %IAEA/ENSDF
isomer T½ Sr-87m (s)1013410134< 0.01 %± 5 %IAEA/ENSDF
Tc-99m A(1 T½)/A₀0.50.5< 0.01 %± 1e-6 %definition
Ba-137m excitation = 661.66 keV line661.659661.657< 0.01 %± 0.1 %ENSDF

Branching ratios are physical

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
isomers reporting 0 % for every branch00exactexactconversion rule

Delayed channels are not counted as competing branches

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
Rb-98m primary branches100100< 0.01 %± 0.01 %NUBASE2020 §2.4
Rb-98m β-delayed channels held apartdelayed: B-2N,B-Npass—NUBASE2020 §2.4
delayed channels leaked into decayModes00exactexactNUBASE2020 §2.4

Isomer gamma sources are reachable in the Dose tab

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
Tc-99m selectable as a dose source4 linespass—IAEA decay_rads
Ba-137m selectable as a dose source6 linespass—IAEA decay_rads
Ag-110m selectable as a dose source35 linespass—IAEA decay_rads
Xe-135m selectable as a dose source6 linespass—IAEA decay_rads
Kr-85m selectable as a dose source7 linespass—IAEA decay_rads
Tc-99m dominant γ (keV)140.511140.511< 0.01 %± 0.1 %ENSDF
Tc-99m dominant γ intensity (%)8989< 0.01 %± 5 %ENSDF
Ba-137m dominant γ (keV)661.657661.657< 0.01 %± 0.1 %ENSDF

Neutron cross sections and activation 30

Literature anchors and internal identities

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
σ₀ B-10 (n,α) (b)38373837< 0.01 %± 1 %Lamarsh App. II
σ₀ Li-6 (n,α) (b)940940< 0.01 %± 1 %Lamarsh App. II
σ₀ He-3 (n,p) (b)53305330< 0.01 %± 1 %Lamarsh App. II
σ₀ H-1 (n,γ) (b)0.33260.3326< 0.01 %± 1 %Lamarsh App. II
σ₀ Cd-113 (n,γ) (b)2060020600< 0.01 %± 1 %Mughabghab 2006
σ₀ Gd-157 (n,γ) (b)2.5400 × 10⁵2.5400 × 10⁵< 0.01 %± 1 %Mughabghab 2006
σ₀ Sm-149 (n,γ) (b)4014040140< 0.01 %± 1 %D&H Ch. 15
σ₀ U-235 (n,f) (b)582582< 0.01 %± 1 %Lamarsh App. II
σ₀ U-238 (n,γ) (b)2.682.68< 0.01 %± 1 %Lamarsh App. II
σ₀ Pu-239 (n,f) (b)748748< 0.01 %± 1 %Lamarsh App. II
σ₀ Au-197 (n,γ) (b)98.6598.65< 0.01 %± 1 %Mughabghab 2006
U-235 σ_f+σ_γ = σ_a (b)681681< 0.01 %± 0.01 %definition
Pu-239 σ_f+σ_γ = σ_a (b)10171017< 0.01 %± 0.01 %definition
σ_Xe cross_sections vs xenon.ts (b)2.6500 × 10⁶2.6500 × 10⁶< 0.01 %± 0.01 %internal consistency
U-235 α = σ_γ/σ_f0.1701030.169+0.65 %± 3 %Lamarsh §4
U-235 η = ν·σ_f/σ_a2.068192.068+0.01 %± 2 %Lamarsh §4 (η ≈ 2.07)
H weighted sigma_a (b)0.3325520.3326−0.01 %± 3 %Lamarsh & Baratta 3rd ed., App. II
C weighted sigma_a (b)0.00350710.0035+0.20 %± 3 %Lamarsh & Baratta 3rd ed., App. II
N weighted sigma_a (b)1.897771.9−0.12 %± 3 %Lamarsh & Baratta 3rd ed., App. II
Fe weighted sigma_a (b)2.56412.56+0.16 %± 3 %Mughabghab (2006), elemental value
Pb weighted sigma_a (b)0.1742080.171+1.88 %± 3 %Mughabghab (2006), elemental value

Høgdahl rate for gold, by hand

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
Au saturation, thermal 1e123.0162 × 10¹¹3.0162 × 10¹¹< 0.01 %± 1 %Mughabghab σ₀
Au saturation, φₑ = φ_th/304.5958 × 10¹¹4.5958 × 10¹¹< 0.01 %± 1.5 %Høgdahl, Mughabghab I₀

IRDFF-II averages and an independent fission spectrum

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
σ̄ Fe-54(n,p), U-235 fission (mb)76.63576.66−0.03 %± 1 %IAEA IRDFF-II
σ̄ Ni-58(n,p), U-235 fission (mb)105.16105.19−0.03 %± 1 %IAEA IRDFF-II
σ̄ Al-27(n,α), U-235 fission (mb)0.686890.6872−0.05 %± 1 %IAEA IRDFF-II
σ̄ S-32(n,p), U-235 fission (mb)66.82666.846−0.03 %± 1 %IAEA IRDFF-II
fission neutrons above 0.5 MeV (fraction)0.86850.871544−0.35 %± 2 %Watt spectrum
fission neutron mean energy (MeV)22.03084−1.52 %± 2.5 %Watt spectrum
Ni-58(n,p) saturation, 1 g (Bq)4.2288 × 10⁷4.2152 × 10⁷+0.32 %± 3 %IRDFF-II σ̄ + Watt, by hand

Reactor physics 14

Equilibrium poisoning saturates and is Σf-independent

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
[Xe] saturation ratio 1e13→1e141.662761.66276< 0.01 %± 1 %φ/(λ_Xe+σ_Xe·φ)
Xe-135 reactivity saturates with flux-1517 pcm at 1e13 → -2523 pcm at 1e14pass—φ/(λ_Xe+σ_Xe·φ)
[I] linear in flux1010< 0.01 %± 1 %I has no burnup term

Transients agree with an independent RK4 of the same equations

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
startup 1e14: Xe at 10 h7.2284 × 10¹⁴7.2284 × 10¹⁴< 0.01 %± 0.01 %RK4
startup 1e14: Xe at 48 h1.1488 × 10¹⁵1.1488 × 10¹⁵< 0.01 %± 0.01 %RK4
step 100→50 %: Xe at 5 h1.7603 × 10¹⁵1.7603 × 10¹⁵< 0.01 %± 0.01 %RK4
step 100→50 %: Xe at 30 h1.1319 × 10¹⁵1.1319 × 10¹⁵< 0.01 %± 0.01 %RK4
iodine pit peak after 1e14 shutdown (h)10.1510.147+0.03 %± 1 %closed form, D&H §15

Inhour periods satisfy the six-group equation

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
inhour ρ = 0.05$ → T 226.9 s0.050.05< 0.01 %± 0.1 %inhour eq.
inhour ρ = 0.1$ → T 98.5 s0.10.1< 0.01 %± 0.1 %inhour eq.
inhour ρ = 0.25$ → T 25.4 s0.250.25< 0.01 %± 0.1 %inhour eq.
inhour ρ = 0.5$ → T 5.7 s0.50.5< 0.01 %± 0.1 %inhour eq.
inhour ρ = 0.8$ → T 0.9 s0.80.8< 0.01 %± 0.1 %inhour eq.
small ρ: T·ρ[$] → Σaᵢ/λᵢ (s)12.998513.03−0.24 %± 1 %Keepin mean delay

Mixtures and enrichment 31

4.5 % LEU cascade vs the textbook case

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
SWU per kg product (4.5 % LEU)6.871116.9−0.42 %± 6 %value function
feed per kg product (4.5 % LEU)9.219099.2+0.21 %± 6 %mass balance
mass balance F − P − W-1.7764 × 10⁻¹⁵0-1.7764 × 10⁻¹⁵ abs± 1e-6 %conservation

Elemental fractions vs IUPAC atomic weights

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
H₂O hydrogen (wt%)11.190111.19< 0.01 %± 1 %IUPAC masses
UO₂ uranium (wt%)88.149888.15< 0.01 %± 1 %IUPAC masses
H2O wt% sums to 100100100< 0.01 %± 0.01 %conservation
UO2 wt% sums to 100100100< 0.01 %± 0.01 %conservation
Ca(OH)2 wt% sums to 100100100< 0.01 %± 0.01 %conservation

Atomic weights and molar masses vs IUPAC/CIAAW 2021

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
atomic weight H1.007971.008< 0.01 %± 0.02 %CIAAW 2021
atomic weight B10.813510.81+0.03 %± 0.1 %CIAAW 2021
atomic weight C12.010612.011< 0.01 %± 0.02 %CIAAW 2021
atomic weight N14.006914.007< 0.01 %± 0.02 %CIAAW 2021
atomic weight O15.999415.999< 0.01 %± 0.02 %CIAAW 2021
atomic weight Na22.989822.99< 0.01 %± 0.02 %CIAAW 2021
atomic weight Al26.981526.982< 0.01 %± 0.02 %CIAAW 2021
atomic weight Cl35.452135.45+0.01 %± 0.02 %CIAAW 2021
atomic weight Ca40.07840.078< 0.01 %± 0.02 %CIAAW 2021
atomic weight Fe55.845155.845< 0.01 %± 0.02 %CIAAW 2021
atomic weight Cu63.54663.546< 0.01 %± 0.02 %CIAAW 2021
atomic weight Zr91.223691.224< 0.01 %± 0.02 %CIAAW 2021
atomic weight Cd112.414112.41< 0.01 %± 0.02 %CIAAW 2021
atomic weight Gd157.252157.25< 0.01 %± 0.02 %CIAAW 2021
atomic weight W183.842183.84< 0.01 %± 0.02 %CIAAW 2021
atomic weight Pb207.217207.2+0.01 %± 0.1 %CIAAW 2021
atomic weight Th232.038232.04< 0.01 %± 0.02 %CIAAW 2021
atomic weight U238.029238.03< 0.01 %± 0.02 %CIAAW 2021
molar mass UO₂ (g/mol)270.028270.03< 0.01 %± 0.03 %from CIAAW weights
molar mass UF₆ (g/mol)352.019352.02< 0.01 %± 0.03 %from CIAAW weights
molar mass B₄C (g/mol)55.264755.255+0.02 %± 0.1 %from CIAAW weights
Pu (no stable isotope) = Pu-244 mass244.064244.064< 0.01 %± 0.01 %AME2020
Ra (no stable isotope) = Ra-226 mass226.025226.025< 0.01 %± 0.01 %AME2020

Counting statistics and units 15

Currie critical level and detection limit

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
Currie L_c (B=100)23.263823.3−0.16 %± 1 %Currie 1968
Currie L_d (B=100)49.233749.21+0.05 %± 1 %Currie 1968
Currie L_c (B=400)46.527646.6−0.16 %± 1 %Currie 1968
Currie L_d (B=400)95.761395.71+0.05 %± 1 %Currie 1968
Currie L_c (B=2500)116.319116.5−0.16 %± 1 %Currie 1968
Currie L_d (B=2500)235.344235.21+0.06 %± 1 %Currie 1968

Units, isomer specific activity, detection decision, optimum tails

CHECKAPPREFERENCEDEVIATIONTOLERANCESOURCE
1 Ci in Bq3.7000 × 10¹⁰3.7000 × 10¹⁰< 0.01 %± 1e-9 %definition
1 R in C/kg2.5800 × 10⁻⁴2.5800 × 10⁻⁴< 0.01 %± 1e-9 %definition
1 MeV in J1.6022 × 10⁻¹³1.6022 × 10⁻¹³< 0.01 %± 1e-9 %SI 2019 exact e
1 Gy in rad100100< 0.01 %± 1e-9 %definition
1 Sv in rem100100< 0.01 %± 1e-9 %definition
1 y in s (Julian)3.1558 × 10⁷3.1558 × 10⁷< 0.01 %± 1e-9 %IAEA half_life_sec
Tc-99m specific activity (Ci/g)5.2744 × 10⁶5.2700 × 10⁶+0.08 %± 1 %handbook
Currie decision at the boundary, B = 100net 24 → detected, net 23 → not; L_c = 23.26pass—Currie 1968
optimum tails assay (cost ratio 0.5)0.003024620.003025−0.01 %± 0.1 %brute-force scan

Corrections

Errors found by earlier audits, and the release that fixed them. If you used one of these calculations in an earlier version, recompute it.

1.4.1 · HIGH
Shielding behind lead, tungsten and iron. Buildup came from Taylor fits that stopped at 0.5 MeV and borrowed other materials’ data, and the attenuation counted coherent scattering as removal. Now: the ANSI/ANS-6.4.3 standard buildup factors for every material, 15 keV–15 MeV, with the coherent-free attenuation the standard requires. Dose behind thick lead was low: Cs-137 behind 10 cm of lead read about half the corrected value, and a third below an independent slab Monte Carlo that itself leaves out lead fluorescence; behind 5 cm about 25 % below the corrected value. A low-energy source immersed in water read up to 2× low.
1.4.1 · MEDIUM
Fast-neutron activation. Threshold cross sections were order-of-magnitude estimates, applied to every source as if it emitted fission neutrons. They are now IAEA IRDFF-II averages over each source’s own spectrum. Reactor results were 9–43 % low (O-16(n,p), the N-16 source, most); Fe-54(n,p) with Am-Be was 3.4× low; the D-D generator reported activation for reactions a 2.45 MeV neutron cannot cause.
1.4.1 · LOW
Activation data consistency. Four product half-lives and two abundances now match the NUBASE2020 data the tab cites (W-187 was 0.8 % long). The on-screen formula still showed the epithermal factor 0.45 retired in 1.4.0; the calculation already used 1.
1.4.0 · HIGH
Dose and shielding, ten parent nuclides. Pb-212, Bi-212, Ba-140, Np-237, Zr-95, Ce-144, Mo-99, Ra-228, Pb-214 and Ba-131 were offered without the short-lived progeny that carry most of their gamma dose. An aged Pb-212 source read about 10× low, and the shield solver asked for 0.32 cm of lead where 9.95 cm is needed. Each now has a “+progeny” entry at transient-equilibrium activity.
1.4.0 · MEDIUM
Reactor period. The one-group stable period was 2.3× too long at +$0.50. It now solves the six-group inhour equation (Keepin U-235 thermal groups).
1.4.0 · MEDIUM
Decay Chain tab. The followed branch was credited with every decay (Po-212 1.56× high). Activities now come from the full branching solution, with the other branches and any truncation shown.
1.4.0 · MEDIUM
Neutron activation. The epithermal term used a factor matching no published convention; Au-197 read 24 % and Mo-98 40 % low. It now follows the Høgdahl convention with φe per unit lethargy.
1.0.5 · HIGH
Bateman chains. Members below a short-lived one were starved: Ra-226 over one year reported Bi-214 about 104× low. The integrator was replaced with a closed-form solution, checked above against secular and transient equilibrium.
1.0.5 · LOW
H*(10) above 1.5 MeV. The conversion from air kerma fell away where ICRP 74 Table A.21 plateaus, so ambient dose equivalent for high-energy photons read low. All 25 rows now match the printed table.

Known limitations

Stated because a validation page that lists only strengths is marketing.

Found a number that disagrees with your reference? Email [email protected] with the inputs and units you used, the value the app showed, and the value you expected with its source. Accuracy reports are looked at first, and a confirmed one is added to this page.