The DOI matches its Crossref record; 2 of the 2 references it cites were found in a registry or an index.
The Dependence of Quantum Yield on Wavelength and Growth Irradiance
Abstract
The wavelength dependence of photosynthetic quantum yield was measured in a leaf disc oxygen electrode using narrow-band interference filters. Photorespiration was suppressed by measuring oxygen evolution in air containing ~ 1% CO2. Rates of oxygen evolution were determined as a function of absorbed irradiances between 0 and 100 µmol quanta m-2 s-1 and the slope was taken as the quantum yield. The wavelength-dependence previously observed in many species was confirmed for pea and spinach leaves. The maximum quantum yields obtained here and by others are close to 0.111 mol O2 mol-1 quanta for red light. Given the wavelength dependence of quantum yield and the spectral distribution of light, the quantum yields for various white lights were calculated to be around 85% of the red maximum. The quantum yields in white light were the same for plants grown at different irradiances. It is argued that the wavelength dependence of quantum yield reflects the distribution of quanta between the two photosystems with the quantum yield dropping at wavelengths strongly absorbed by chlorophyll b as this is mainly associated with photosystem II.
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Citations
Cites
Comparative photosynthesis of sun and shade plants
Boardman, N. K. (1977) · Annual Review of Plant Physiology · doi:10.1146/annurev.pp.28.060177.002035 · Cited by 1,826 · cited 1×
“The independence of quantum yield and growth irradiance supports the conclusion of Boardman (1977) and Bjtjrkman (1981).”
ResultThe action spectrum, absorptance and quantum yield of photosynthesis in crop plants
McCree, K. J. (1971) · Agricultural Meteorology · doi:10.1016/0002-1571(71)90022-7 · Cited by 1,278 · cited 1×
“The three curves shown have been calculated for clover (McCree 1972), the mean of 26 herbaceous plants (Inada 1976) and Chlorella (Emerson and Lewis 1943) by solving the following equations: cu + = 1, cu = +re1 / 2 for X < 690 nm or /3=+,,1/2 for X > 690 nm (Fig.”
Method
Cited by
Evans, J. R., & Poorter, H. (2001) · Plant, Cell & Environment · doi:10.1046/j.1365-3040.2001.00724.x · Cited by 1,229
Self-citationHIKOSAKA, K., & TERASHIMA, I. (1995) · Plant, Cell & Environment · doi:10.1111/j.1365-3040.1995.tb00562.x · Cited by 420
Comparative ecophysiology of leaf and canopy photosynthesis
TERASHIMA, I., & HIKOSAKA, K. (1995) · Plant, Cell & Environment · doi:10.1111/j.1365-3040.1995.tb00623.x · Cited by 417
Thylakoid Membrane Organisation in Sun/Shade Acclimation
Anderson, J., Chow, W., & Goodchild, D. (1988) · Australian Journal of Plant Physiology · doi:10.1071/pp9880011 · Cited by 357
Photosynthetic light-response curves: I. The influence of CO2 partial pressure and leaf inversion
�gren, E., & Evans, J. R. (1993) · Planta · doi:10.1007/bf00195075 · Cited by 351
Self-citation
Metadata
- Authors
- Evans, Jr.
- Venue
- Australian Journal of Plant Physiology
- Publisher
- CSIRO Publishing
- Published
- 1987-02-01
- Volume
- 14
- Issue
- 1
- Pages
- 69-79
- ISSN
- 0310-7841 (ISSN-L)
- 1446-5655
- OpenAlex
- W2324107639
- Cited by
- 243
- References
- 2
- FWCI
- 1.72
- Type
- journal article
- Language
- en
- Open access
- closed
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Contains information from the Semantic Scholar Academic Graph Datasets, made available under the ODC Attribution License (ODC-BY 1.0).
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