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. 2019 Dec 16;20(24):6341. doi: 10.3390/ijms20246341

Table 2.

Definition of the terms and formulas for calculation of the JIP-test parameters from the chlorophyll a fluorescence transient OJIP emitted by dark-adapted leaves.

Quantum Yields and Probabilities
ϕP0 = 1 − F0/FM Maximum quantum yield of primary photochemistry in PSII (at t = 0)
ϕE0 = (1 − F0/FM)(1 − VJ) Quantum yield of electron transport (at t = 0) beyond QA
ϕR0 = (1 − F0/FM)(1 − VI) Quantum yield for reduction of the end of electron acceptors at PSI acceptor side (RE)
ϕD0 = F0/FM Quantum yield (at t = 0) of energy dissipation
δR0 = (1 − VI)/(1 − VJ) The efficiency with which an electron can move
from the reduced intersystem electron acceptors to the PSI
end electron acceptors
ψE0 = 1 − VJ Probability (at t = 0) that a trapped exciton will move an electron into electron transport chain beyond QA
Specific Energy fluxes expressed per active PSII reaction center (RC)
ABS/RC = (1 − γRC)/ γRC = M0 × (1/VJ)/[1 − (F0/FM)] Apparent antenna size of active PSII RC
TR0/RC = Mo(1/Vj) Trapping flux (leading to QA reduction) per RC
DI0/RC = (ABS/RC − TR0/RC) Dissipated energy flux per RC
ET0/RC = M0(1/Vj) ψ0 Electron transport flux per RC (further than QA)
RC/CS0 = FO φP0 Vj/M0 Density of RCs (QA reducing PSII reaction centers)
Performance index per absorption
PIABS = 1 − (F0/FM)/Mo/VJ × FM − F0/F0 × 1 − VJ/VJ Performance index (potential) for energy conservation from exciton to the reduction of intersystem electron acceptors
Phenomenological energy fluxes per excited cross-section (CS)
ABS/CS Absorption energy flux per CS
TR0/CS Trapped energy flux per CS
ET0/CS Electron transport flux per CS
DI0/CS Dissipation energy flux per CS

F0—fluorescence intensity at 50 µs, FM—maximal fluorescence intensity, FJ—fluorescence intentisity at J step (at 2 ms), VJ—relative variable fluorescence at 2 ms calculated as VJ = (FJ − F0)/(FM − Fo), Mo initial slope of fluorescence kinetics which can be derived from equatation Mo = 4 × (F300µs − F0)/(FM − F0).