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Fission tracks and their application in Geology
Lecture on fission track dating in three parts I The method - what is fission tracks about II Application of the fission track method III Fission tracks and very low-grade metamorphism
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What is the aim of the three courses ?
learn about the physical background of track formation learn how to read and interpret fission track data and evaluate FT data from the literature learn about the potential of this method - and its flaws eventually apply the method in your research
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3 key questions What process creates fission tracks?
How do we measure fission tracks? How are fission track data presented? Part 1 - The method
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The periodic table of elements
Part 1 - The method
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Description of a nuclide
atomic mass (N): amount of protons + neutrons 238 92 U atomic number (Z): amount of protons Part 1 - The method
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yellow nuclides with a decay
The nuclide chart black stable nuclides red nuclides with b+ decay blue nuclides with b- decay green nuclides with spontaneous fission yellow nuclides with a decay last stable element Part 1 - The method
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Radioactive decay Part 1 - The method
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a-decay of Uranium Part 1 - The method
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spontaneous fission of 238U
Part 1 - The method
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The “camel“ curve Part 1 - The method
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Fission on the nuclide chart
Part 1 - The method
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Induced decay of 235-Uranium
Part 1 - The method
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Natural ratios and half life times
a decay 4.47·109 y 7.04·108 y 1.40·1010 y T1/2 spont. fission 8.19·1015 y 1.0·1019 y 1.0·1021 y Nuclide 238U 235U 232Th Element ratio % 0.721 % % Only 238U is important for fission track formation ! Part 1 - The method
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track formation in crystal lattice
track etching to make them visible Part 1 - The method
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Can we see fission tracks without etching ?
TEM image from Yada et al. (1987) Part 1 - The method
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fission track annealing
track length as a second important parameter Part 1 - The method
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Age versus U content Part 1 - The method
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minerals for FT dating: apatite
apatites from the Durango thermal field apatite Ca5(PO4)3(F, CL, OH) U Part 1 - The method
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minerals for FT dating: zircon
ZrSiO4 U Part 1 - The method
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Sample preparation procedure
Part 1 - The method
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Counting the tracks apatite crystal mica print Part 1 - The method
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Not all grains can be counted...
tracks on plane II a, b We only count tracks on grain surfaces II c axis, i.e…. - with blade shaped tracks - with sharp polish scratches - with parallel etch pits - with corresponding geometry tracks on plane II c Part 1 - The method
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Why do we have to irradiate our samples?
Before irradiation, we only observe tracks generated by the spontaneous decay of 238U. These tracks are counted per area unit. The number of tracks are a function of age and U content. For age calculation, we need to know the grain's individual U content. The sample is irradiated with a dosimeter of known U content. During irradiation, the 235U in the grain undergoes a fission decay and produces induced tracks. Part 1 - The method
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What do we count Induced tracks on dosimeter mica (rd): each irradiated sample package has at least two dosimeters (top, bottom) estimation of irradiation gradient Spontaneous tracks on mineral grain (rs) Induced tracks on mica print of the mineral grain (ri) Part 1 - The method
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Induced tracks on white mica
Part 1 - The method
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The FT age equation - 1 dNP/dt = -lNP NP = number of parent atoms
NP = (NP )0e-lt l = decay constant ND = Np (e-lt -1) ND = number of daughter atoms ld= la + lf where ld ≈ la Ns = lf / la238N (e-lat -1) Ns = number of spont. tracks t = 1 / la238ln[(la / lf)(Ns/238N) + 1] Part 1 - The method
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The FT age equation - 2 Ni = 235N s f s = neutron cross section
f = neutron fluence Ni = 238N I s f I = 235U / 238U general age equation t = 1 / la ln[(la / lf)(Ns/Ni) I s f + 1] G = geometry factor = 0.5 (2p/4p geometry) Q = revelation factor = 1 practical age equation t = 1 / la ln[(la / lf)(rs/ri) Q G I s f + 1] Part 1 - The method
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… simplified, for the last 150 m. y
… simplified, for the last 150 m.y., track production has been constant Part 1 - The method
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The zeta (z) age approach
Problem: Many of the factors in the age equation are loosely constrained or not accurately known. It was proposed to use age standards and irridiate the standards together with dosimeter glasses of known U content calibration factor z (zeta) z = Q I s f / (rmlf) rm = density of tracks on dosimeter zeta age equation t = 1 / la ln[(la)(rs/ri) rmG z + 1] Part 1 - The method
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What is the error of a fission track age ?
error(age) = error(rs) + error(ri) + error (rd) + SD(z) Poissonian statistics: error (n) = n-0.5 Generally, errors for fission track ages are large compared to other radiologic dating methods, in the range of 5-10%. Part 1 - The method
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The partial annealing zone
Part 1 - The method
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Crossing the partial annealing zone
Part 1 - The method
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Track length histogram
Part 1 - The method
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How can we observe tracks in full length ?
Part 1 - The method
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Confined fission tracks under the microscope
TINCLE = track in cleavage TINT = track in track Part 1 - The method
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Long and short tracks, gaps
(from Barbarand et al. 2003) Part 1 - The method
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The shape of the time-temperature path
Part 1 - The method
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data production: age length
Part 1 - The method
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final data for each locality
Part 1 - The method
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What rocks are suitable for FT dating?
Well suitable: granites, pegmatites, syenites, granodiorites, orthogneisses from these lithologies. Less suitable: sandstones, greywackes, paragneisses, andesites, basalts Not suitable: very pure qtz or cal sandstones, limestones, silt- and claystones, ultramafics Part 1 - The method
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Rules of thumb for sample collection:
Well suitable: granites, pegmatites, syenites, granodiorites, orthogneisses from these lithologies. Less suitable: sandstones, greywackes, paragneisses, andesites, basalts Not suitable: very pure qtz or cal sandstones, limestones, silt- and claystones, ultramafics Part 1 - The method
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Cl content of apatite Ca5(PO4)3(F, CL, OH) Part 1 - The method
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Zircon FT annealing and radiation damage
young or U poor zircon strong retentivity for FT high closure temperature old or U rich zircon lower retentivity for FT low closure temperature Part 1 - The method
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Closure temperature and PAZ
Part 1 - The method
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Annealing studies annealing experiments under laboratory conditions:
field studies and comparison with other indicators for time and temperature temperature: °C time: minutes to years ( s) bore holes contact aureoles around intrusive bodies areas with regional metamorphic gradients Part 1 - The method
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Laboratory annealing studies
Part 1 - The method
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Combining laboratory and field information
Part 1 - The method
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What does a fission track age mean?
It dates a fast to very fast cooling event (with complete crossing of the partial annealing zone) It dates a moment during cooling across the partial annealing zone It forms a mixed age between an old and a young age component It provides an age information about the detrital origin the single grains in a sample Part 1 - The method
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When does the FT method fail to provide an age information
if the time-temperature history is very complex (e.g. contains short-term hydrothermal events) if the sample has been heat treated after cooling (e.g. gem quality zircons in Sri Lanka) if a sample contains many different age populations or age origins if apatite grains in a sample are very variable in Cl content if zircon grains are very variable in U content and therefore accumulated radiation damage Part 1 - The method
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Data presentation - I: maps
Part 1 - The method
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Data presentation: vertical profiles
apatite FT ages along bore hole (Wagner et al. 1989) PAZ Part 1 - The method
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Data presentation: horizontal profiles
Part 1 - The method
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Data presentation: Radial plot - I
Part 1 - The method
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Data presentation: Radial plot - II
Part 1 - The method
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Data presentation: Boomerang plot - I
Part 1 - The method
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Data presentation: Boomerang plot - II
Part 1 - The method
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Data presentation: Boomerang plot - examples
(from Gleadow et al. 2002) Part 1 - The method
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Thank you for your attention !
Part 1 - The method
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