δ13C
In geochemistry, paleoclimatology, archaeology, and paleoceanography δ13C (pronounced "delta thirteen c") is a normalized ratio of the two stable isotopes of carbon—13C and 12C—reported in parts per thousand (per mille, ‰).[1]
The definition is, in per mille:
where the standard is an established reference material.
The δ13C of a given compound can vary based on the sources of the precursor material and the biogeochemical processes it has undergone. For example, carbon dioxide derived from ecosystem respiration can be differentiated from carbon dioxide formed from the combustion of fossil fuels using δ13C, as the precursor materials (modern organic matter and petroleum, respectively) have different isotopic values—the basis of the "Seuss Effect". In the case of photosynthesis, two plants grown adjacently with the same source of carbon dioxide may be isotopically distinguishable due to differing biochemical mechanisms and physiologies preferentially selecting for a given isotope—a process known as "isotopic fractionation".
Reference standard
Reference standards are used for verifying the accuracy of isotope ratio measurements, which are typically performed via isotope ratio mass spectrometry, cavity ring down spectroscopy, tunable laser absorption spectroscopy, or nuclear magnetic resonance.
The initial reference material used to standardize carbon isotope ratios "Pee Dee Belemnite" (PDB) —a Cretaceous marine fossil, Belemnitella americana, originating from the Peedee Formation in South Carolina. This material had an anomalously high 13C/12C ratio (0.0112372[2]), and was established as δ13C value of zero.
Due to the high demand of PDB standard, the supply was ultimately exhausted. Other standards calibrated to the same ratio, including one known as VPDB (for "Vienna PDB"), have replaced the original.[3] The 13C/12C ratio for VPDB, which the International Atomic Energy Agency (IAEA) defines as a δ13C value of zero is 0.011113.[4] The use of different primary reference standards will result in isotope ratios that are incomparable due to the difference in scales. To avoid confusion, isotope ratio measurements typically include a subscript denoting the reference material it was corrected to, such as δ13CPDB or δ13CVPDB.
To prevent the depletion of the supply of VPDB, secondary reference materials with isotope ratios determined in direct comparison to VPDB, such as NBS-19 (available from the National Institute of Standards and Technology, δ13CVPDB= 1.95‰),[5] are commonly used in the laboratory setting for standardizing measurements.
Causes of δ13C variations
Methane has a very light δ13C signature: biogenic methane of −60‰, thermogenic methane −40‰. The release of large amounts of methane clathrate can affect global δ13C values, as at the Paleocene–Eocene Thermal Maximum.[6]
More commonly, the ratio is affected by variations in primary productivity and organic burial. Organisms preferentially take up light 12C, and have a δ13C signature of about −25‰, depending on their metabolic pathway. Therefore, an increase in δ13C in marine fossils is indicative of an increase in the abundance of vegetation.
An increase in primary productivity causes a corresponding rise in δ13C values as more 12C is locked up in plants. This signal is also a function of the amount of carbon burial; when organic carbon is buried, more 12C is locked out of the system in sediments than the background ratio.
Geologic significance
C3 and C4 plants have different signatures, allowing the abundance of C4 grasses to be detected through time in the δ13C record.[7] Whereas C4 plants have a δ13C of −16 to −10‰, C3 plants have a δ13C of −33 to −24‰.[8]
Positive and negative excursions
Positive δ13C excursions are interpreted as an increase in burial of organic carbon in sedimentary rocks following either a spike in primary productivity, a drop in decomposition under anoxic ocean conditions or both.[9] For example, the evolution of large land plants in the late Devonian led to increased organic carbon burial and consequently a rise in δ13C.[10]
Major excursion events
- Lomagundi-Jatuli event (2,300–2,080 Ma) Paleoproterozoic - Positive excursion
- Shunga-Francevillian event (2,080 Ma) Paleoproterozoic - Negative excursion
- Shuram-Wonoka excursion (570–551 Ma) Neoproterozoic - Negative excursion
- Steptoean positive carbon isotope excursion (494.6-492 Ma) Paleozoic - Positive excursion
- Ireviken event (433.4 Ma) Paleozoic - Positive excursion
- Mulde event (427 Ma) Paleozoic - Positive excursion
- Lau event (424 Ma) Paleozoic - Positive excursion
- Cenomanian-Turonian boundary event (93.9 Ma) Mesozoic - Positive excursion
- Paleocene–Eocene Thermal Maximum (55.5 Ma) Cenozoic - Negative excursion
See also
- δ18O
- δ15N
- δ34S
- Isotopic signature
- Isotope analysis
- Isotope geochemistry
- Isotopic labeling
References
- ^ Libes, Susan M. (1992). Introduction to Marine Biogeochemistry, 1st edition. New York: Wiley.
- ^ Craig, Harmon (1957-01-01). "Isotopic standards for carbon and oxygen and correction factors for mass-spectrometric analysis of carbon dioxide". Geochimica et Cosmochimica Acta. 12 (1): 133–149. Bibcode:1957GeCoA..12..133C. doi:10.1016/0016-7037(57)90024-8. ISSN 0016-7037.
- ^ Miller & Wheeler, Biological Oceanography, p. 186.
- ^ Meyers, Fabienne (2024-12-23). "The isotopic composition of VPDB". IUPAC | International Union of Pure and Applied Chemistry. Retrieved 2026-01-06.
- ^ Brand, Willi A.; Coplen, Tyler B.; Vogl, Jochen; Rosner, Martin; Prohaska, Thomas (2014-03-20). "Assessment of international reference materials for isotope-ratio analysis (IUPAC Technical Report)". Pure and Applied Chemistry. 86 (3): 425–467. doi:10.1515/pac-2013-1023. hdl:11858/00-001M-0000-0023-C6D8-8. ISSN 1365-3075. S2CID 98812517.
- ^ Panchuk, K.; Ridgwell, A.; Kump, L.R. (2008). "Sedimentary response to Paleocene-Eocene Thermal Maximum carbon release: A model-data comparison". Geology. 36 (4): 315–318. Bibcode:2008Geo....36..315P. doi:10.1130/G24474A.1.
- ^ Retallack, G.J. (2001). "Cenozoic Expansion of Grasslands and Climatic Cooling". The Journal of Geology. 109 (4): 407–426. Bibcode:2001JG....109..407R. doi:10.1086/320791. S2CID 15560105.
- ^ O'Leary, M. H. (1988). "Carbon Isotopes in Photosynthesis". BioScience. 38 (5): 328–336. doi:10.2307/1310735. JSTOR 1310735.
- ^ Canfield, Donald E.; Ngombi-Pemba, Lauriss; Hammarlund, Emma U. (15 October 2013). "Oxygen dynamics in the aftermath of the Great Oxidation of Earth's atmosphere". Proceedings of the National Academy of Sciences of the United States of America. 110 (42): 16736–16741. Bibcode:2013PNAS..11016736C. doi:10.1073/pnas.1315570110. PMC 3801071. PMID 24082125.
- ^ Joachimsk, M.M.; Buggisch, W. "THE LATE DEVONIAN MASS EXTINCTION – IMPACT OR EARTH-BOUND EVENT?" (PDF). Lunar and Planetary Institute.
Further reading
- Miller, Charles B.; Patricia A. Miller (2012) [2003]. Biological Oceanography (2nd ed.). Oxford: John Wiley & Sons. ISBN 978-1-4443-3301-5.
- Mook, W. G., & Tan, F. C. (1991). Stable carbon isotopes in rivers and estuaries. Biogeochemistry of major world rivers, 42, 245–264.