DUAL-KLAS-NIR

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Product

P700, Plastocyanin, Ferredoxin & Chlorophyll Fluorescence Measuring System

What Does the DUAL-KLAS-NIR Do?

The photosynthetic electron transport chain passes electrons from water through photosystem II, plastoquinone, the cytochrome b6f complex, plastocyanin, P700 (the photosystem I reaction center), and ferredoxin to NADP⁺. Understanding how electrons flow through this chain and where bottlenecks occur is key to understanding photosynthetic regulation, stress responses, and the coordination between the two photosystems. The DUAL-KLAS-NIR is the only instrument that can monitor the redox state of P700, plastocyanin, and ferredoxin simultaneously and in real time. By adding chlorophyll fluorescence data from the integrated PAM fluorometer, the system provides a comprehensive picture of the entire electron transport chain in a single measurement - from PSII to the acceptor side of PSI.

The DUAL-PAM-100 employs one pair of wavelengths in the near-infrared (NIR) to measure absorbance changes related to redox changes of the photosystem I reaction center. Using four wavelength pairs in the NIR (780/820, 820/870, 870/965 and 840/965 nm), the DUAL-KLAS-NIR is capable of unequivocally discriminating redox changes of plastocyanin, P700, and ferredoxin. The software of the DUAL-KLAS-NIR shares many features with that of the DUAL-PAM-100, making the transition straightforward for existing users. Using automated measuring routines, even complex measuring protocols can be easily performed.

How Does the Deconvolution Work?

The redox changes of P700, plastocyanin, and ferredoxin all produce overlapping absorbance changes in the near-infrared. By applying an innovative analytical approach, the DUAL-KLAS-NIR acquires the in vivo spectral characteristics of pure PC, P700, and Fd. This spectral information allows the system to monitor online the redox changes of all three components and to determine PC/P700 and Fd/P700 ratios, thereby providing direct estimates of the relative pool sizes of these electron carriers.

Three graphs demonstrating example of an experiment to scale the deconvoluted ferredoxin, P700 and plastocyanin signals measured with the DUAL-KLAS-NIR
The DUAL-KLAS-NIR can deconvolute signals from ferredoxin, P700 and plastocyanin.

Integrated PAM Chlorophyll Fluorometer

The DUAL-KLAS-NIR includes a full PAM chlorophyll fluorometer with both green and blue measuring light. Green light penetrates deeper into the leaf than blue light - thus, green-excited fluorescence includes information from deeper leaf layers and provides the best match with the NIR absorbance measurements, which always probe the entire leaf. The blue measuring light gives more specific information on the upper or lower leaf side and produces a fluorescence signal that is one order of magnitude larger than the green-excited signal.

Flexible Time Resolution

The system measures in 1, 2, or 6 channel mode with time resolutions of 35 µs, 150 µs, and 1 ms respectively. The pulse modulation technique developed for the DUAL-PAM-100, in which channels are measured as blocks of 50 µs, has been extended for the DUAL-KLAS-NIR to accommodate 6-channel measurements. An extremely wide range of measuring light frequencies (1 Hz to 400 kHz) supports both continuous F0 assessment and high-resolution recording of fast kinetic transients such as the polyphasic fluorescence rise or flash relaxation kinetics.

Versatile Light Sources

Integrated red (635 nm), blue (460 nm), and far-red actinic LEDs provide continuous actinic illumination, multiple turnover pulses, and single turnover flashes. The red LED array serves as the main actinic light source, while the blue LED in the detector unit allows continuous illumination with up to 300 µmol m⁻² s⁻¹ from the detector side of the sample. Both sides of the leaf can be illuminated for homogeneous light distribution or, by removing the LED array cable of the DKN-E emitter unit, only one side. All light sources switch with 2.5 µs time resolution under software control.

Single-Channel High-Resolution Mode

When single-channel measurements are made, a dedicated script allows the different signals to be measured consecutively at high time resolution combining the speed of single-channel mode with the information content of multi-channel measurements.

Automated Measurement Protocols

The software supports automated slow kinetics recordings, pre-programmed triggered runs, online and offline averaging, and operation via automated measuring routines through script file programming. This enables reproducible, multi-step experiments without manual intervention.

The DUAL-KLAS-NIR is unique in providing online deconvoluted signals of the in vivo redox states of P700, PC and Fd in real time. This opens up a whole new research field with applications that may not have come to our minds yet. In particular, for the first time simultaneous kinetic information on the complex interplay between reactions at the PS I donor and acceptor sides can be obtained, including information on cyclic electron transport around PS I.

Some examples of applications, which have been described in Klughammer and Schreiber, Photosynth Res 128 (2016) 195-214, Schreiber and Klughammer, Plant Cell Physiol 57 (2016) 1454-1467 and Schreiber Photosynth Res 134 (2017) 343-360, are given here.

Three graphs of deconvoluted signals of the in vivo redox states of P700, PC and Fd

The effective quantum yield of photosystem I. In all older measurements the P700 signal contained always contributions of Fd and variable amounts of PC, depending on the method used to reduce this contribution. Panel C of the figure illustrates the light intensity dependence of the effective PSI quantum yield Y(I), the effective quantum yield of PSII Y(II) and the effective quantum yield of PSII corrected for PSI fluorescence Y(II)corr of Brassica napus.

The effective antenna size of photosystem I. On a dark-to-light transition, first oxidized PC starts to accumulate and only with some delay oxidized P700. The initial slope of the clean PC signal can now be used as a measure for the effective antenna size of PS I. The second figure zooms in on the initial absorbance changes and shows the large difference in the initial slope of PC (red) and P700 (blue). For a dark-acclimated leaf, with inactive photosystem I acceptor side, the initial slope of Fd-reduction can also be used for this purpose. The figure illustrates the delay in the oxidation kinetics of P700 relative to those of PC for a barley leaf, which has a relatively high PC/P700 ratio.

a graph

The DUAL-KLAS-NIR has a window to visualize the simultaneous changes in the P700 and PC redox states relative to each other. This allows an estimation of the apparent equilibrium constant between PC and P700. The figure gives an example of a P700 versus PC redox plot.

During a saturation pulse given to a well dark-adapted leaf, the Fd-pool becomes reduced and in a subsequent period of darkness slowly re-oxidizes again. When the electron flow on the acceptor side of PSI has become activated the re-oxidation kinetics become much faster. Following activation of the acceptor side of PSI, the dark-inactivation can be followed by monitoring the rate at which Fd becomes re-oxidized following a probe pulse. These kinetics can be fit with an exponential fit routine. Panel A gives examples of the Fd reoxidation kinetics fit with an exponential fit routine and Panel B shows the dark-inactivation kinetics of the acceptor side of PSI for a Hedera helix leaf.

The maximal NIR transmittance changes of PC, P700 and Fd are proportional to the leaf/sample content of these compounds and the ratios of the extinction coefficients of PC, P700 and Fd are constant. This makes it possible to probe the PC/P700 and Fd/P700 ratios and thereby the relative PC and Fd pool sizes in different species or under different conditions (e.g. sun/shade, stressed/non-stressed) on a routine basis with the DUAL-KLAS-NIR. It is observed that high PC/P700 ratios correlate with high ETR values. The figure illustrates that sun and shade leaves of, in this case, Hedera helix have considerably different PC and Fd contents relative to P700.

Scientific Publications using Walz Devices

Source: Google Scholar.
Keywords: (Walz OR Waltz) Effeltrich.
Date: June 22, 2026.

Ʃ = 19642

Per Year

Source: Google Scholar.
Keywords: (Walz OR Waltz) Effeltrich.
Date: June 22, 2026.

Ʃ = 19642

Year

Selected Publications

Effect of the insecticide clothianidin on the photosynthetic electron transport chain in pea.

Volgusheva AA, Hao J, He H, Lovyagina ER, Loktyushkin AV, Parshina EY, Luneva OG, Balzhumanov AA, Khruschev SS, Maksimov GV, Rubin AB

Photochemistry and Photobiology 101: 580-591

Go to publication

Plastocyanin affects photosynthesis and high light acclimation by modulating redox states of electron transport chain in Chlamydomonas reinhardtii

Wu G, Bin S, Chen J, Li J, Yi H, Wei C, Zheng H, Chen C, Lee B, Wang X, Yang W, Hu Z, Li X

Communications Biology 8: 476

Go to publication

Role of plastocyanin in response to photosynthetic electron transport in Solanum nigrum under Cd stress

Xiang J, Fu Z, Xu H, Huang X, Zhu F

Plant Stress 18: 101073

Go to publication

Metabolite-level regulation of enzymatic activity controls awakening of cyanobacteria from metabolic dormancy

Doello S, Sauerwein J, von Manteuffel N, Burkhardt M, Neumann N, Appel J, Rapp J, Just P, Link H, Gutekunst K, Forchhammer K

Current Biology 35: 77-86

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The impact of redox mediators on the electrogenic and physiological properties of Synechocystis sp. PCC 6803 in a biophotovoltaic system

Yuan J, Bai Y, Lenz C, Reilly-Schott V, Schneider H, Lai B, Krömer JO

ChemSusChem 18: e202402543

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Unravelling the physiological and anatomical basis of divergent adaptations in cultivated and wild tomatoes

Ganie SA, Forget G, Amaral J, Wall SA, Singh P, Kromdijk J, Carmo-Silva E, Lawson T

Journal of Experimental Botany 76: 6548-6566

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Molecular dynamics of photosynthetic electron flow in a biophotovoltaic system

Yuan J, Appel J, Gutekunst K, Lai B, Krömer JO

Environmental Science and Ecotechnology 23: 100519

Go to publication

Towards solar chemicals: Understanding and redesigning photosynthesis

Hubáček M

Thesis University Turku

Moderate temperature reduction changes the high-light acclimation strategy of lettuce plants

Lempiäinen T, Muth-Pawlak D, Vainonen JP, Rintamäki E, Tikkanen M, Aro E-M

Physiologia Plantarum 177: e70298

Go to publication

Sub-optimal temperature leads to tighter coupling between photosynthetic electron transport and CO2 assimilation under fluctuating light in maize

Sales CRG, Arrivault S, Tonetti T, Clapero V, Vath L, Cubas LA, Stitt M, Kromdijk J

The regulation of PSI cyclic electron transport by both plastoquinone and ferredoxin redox states. correlation with the rate of proton motive force utilization

Satoh H, Ohara Y, Hanke G, Ifuku K, Shimakawa G, Suzuki Y, Makino A, Morigaki K, Miyake C

Frontiers in Plant Science 16: 1626163

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PSII photoinhibition as a protective strategy: maintaining an oxidative state of PSI by suppressing PSII activity under environmental stress

Takeuchi K, Harimoto S, Maekawa S, Miyake C, Ifuku K

Physiologia Plantarum 177: e70392

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The protective role of chloroplast NADH dehydrogenase-like complex (NDH) against PSI photoinhibition under chilling stress

Takeuchi K, Harimoto S, Che Y, Kumazawa M, Satoh H, Maekawa S, Miyake C, Ifuku K

New Phytologist 248: 2262-2279

Go to publication

The role of the LysR-type transcriptio factor PacR in regulating nitrogen metabolism in Anabaena sp. PCC7120

Werner E, Huokko T, Santana-Sánchez A, Picossi S, Nikkanen L, Herrero A, Allahverdiyeva Y

Physiologia Plantarum 177: e70248

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Redox state of photosynthetic ferredoxin under heat and light stress.

Pshybytko NL

Journal of Applied Spectroscopy 91: 342-348

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Glycogen synthesis prevents metabolic imbalance and disruption of photosynthetic electron transport from photosystem II during transition to photomixotrophy in Synechocystis sp. PCC 6803.

Ortega-Martinez P, Nikkanen L, Wey LT, Florencio FJ, Allahverdiyeva Y, Díaz-Troya S

New Phytologist 243: 162-179

Go to publication

Dynamics and interplay of the photosynthetic regulatory processes depend on the amplitudes of oscillating light.

Niu Y, Matsubara S, Nedbal L, Lazár D

Plant, Cell & Environment 47: 2240-2257

Go to publication

A mathematical model of photoinhibition: exploring the impact of quenching processes.

Nies T, Matsubara S, Ebenhöh O

in silico Plants 6: diae001

Go to publication

Flavonols do not affect aphid load in green or senescing birch leaves but coincide with a decrease in photosystem II functionality.

Mattila H, Khorobrykh S, Tyystjärvi E

Biology Open 13: bio060325

Go to publication

Strong heterologous electron sink outcompetes alternative electron transport pathways in photosynthesis.

Hubáček M, Wey LT, Kourist R, Malihan-Yap L, Nikkanen L, Allahverdiyeva Y

The Plant Journal 119: 2500-2513

Go to publication

Manganese deficiency alters photosynthetic electron transport in Marchantia polymorpha.

Hani U, Krieger-Liszkay A

Plant Physiology and Biochemistry 215: 109042

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A mathematical model to simulate the dynamics of photosynthetic light reactions under harmonically oscillating light.

Fuente D, Orlando M, Bailleul B, Jullien L, Lazár D, Nedbal L

Plant Physiology and Biochemistry 217: 109138

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Proton gradient regulation 5 is required to avoid photosynthetic oscillations during light transitions.

Degen GE, Pastorelli F, Johnson MP

Journal of Experimental Botany 75: 947-961

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Flv3A facilitates O2 photoreduction and affects H2 photoproduction independently of Flv1A in diazotrophic Anabaena filaments.

Santana-Sánchez A, Nikkanen L, Werner E, Tóth G, Ermakova M, Kosourov S, Walter J, He M, Aro E-M, Allahverdiyeva Y

New Phytologist 237: 126-139

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Evaluating the oxidation rate of reduced ferredoxin in Arabidopsis thaliana independent of photosynthetic linear electron flow: plausible activity of ferredoxin-dependent cyclic electron flow around photosystem I.

Ohnishi M, Maekawa S, Wada S, Ifuku K, Miyake C

International Journal of Molecular Sciences 24: 12145

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Plants cope with fluctuating light be frequency-dependent nonphotochemical quenching and cyclic electron transport.

Niu Y, Lazár D, Holzwarth AR, Kramer DM, Matsubara S, Fiorani F, Poorter H, Schrey SD, Nedbal L

New Phytologist 239: 1869-1886

Go to publication

Eukaryote-specific assembly factor DEAP2 mediates an early step of photosystem II assembly in Arabidopsis.

Keller J-M, Frieboes MJ, Jödecke L, Kappel S, Wulff N, Rindfleisch T, Sandoval-Ibanez O, Gerlach I, Thiele W, Bock R, Eirich J, Finkemeier I, Schünemann D, Zoschke R, Schöttler MA, Armbruster U

Plant Physiology 193: 1970-1986

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The photosystem I supercomplex from a primordial green alga Ostreococcus tauri harbors three light-harvesting complex trimers.

Ishii A, Shan J, Sheng X, Kim E, Watanabe A, Yokono M, Noda C, Song C, Murata K, Liu Z, Minagawa J

eLife12: e84488

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Enhanced function of non-photoinhibited photosystem II complexes upon PS II photoinhibition.

Gunell S, Lempiäinen T, Rintamäki, Aro E-M, Tikkanen M

BBA-Bioenergetics 1864: 148978

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Higher reduced state of Fe/S-signals, with the suppressed oxidation of P700, causes PS I inactivation in Arabidopsis thaliana.

Furutani R, Wada S, Ifuku K, Maekawa S, Miyake C

Antioxidants 12: 21

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High cyclic electron transfer via the PGR5 pathway in the absence of photosynthetic control.

Degen GE, Jackson PJ, Proctor MS, Zoulias N, Casson SA, Johnson MP

Plant Physiology 192: 370-386

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Scrutinizing the impact of alternating electromagnetic fields on molecular features of the model plant Arabidopsis thaliana.

Schmidtpott SM, Danho S, Kumar V, Seidel T, Schöllhorn W, Dietz K-J

International Journal of Environmental Research and Public Health 19: 5144

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Determining Photosynthetic Control, a probe for the balance between electron transport and Calvin-Benson cycle activity, with the DUAL-KLAS-NIR.

Schansker G

Photosynthesis Research 153: 191-204

Go to publication

CP12 fine-tunes the Calvin-Benson cycle and carbohydrate metabolism in cyanobacteria.

Lucius S, Theune M, Arrivault S, Hildebrandt S, Mullineaux CW, Gutekunst K, Hagemann

Frontiers in Plant Science 13: 1028794

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Insight on the regulation of photosynthesis in pea leaves exposed to oscillating light.

Lazár D, Niu Y, Nedbal L

Journal of Experimental Botany 73: 6380-6393

Go to publication

Plants acclimate to photosystem I photoinhibition by readjusting the photosynthetic machinery.

Lempiäinen T, Rintamäki E, Aro E-M, Tikkanen M

Plant, Cell & Environment 10: 2954-2971

Go to publication

Synechocystis sp. PCC 6803 requires the bidirectional hydrogenase to metabolize glucose and arginine under oxic conditions.

Burgstaller H, Wang Y, Caliebe J, Hueren V, Appel J, Boehm M, Leitzke S, Theune M, King PW, Gutekunst

Frontiers in Microbiology 13: 896190

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Evidence for electron transfer from the bidirectional hydrogenase to the photosynthetic complex I (NDH-1) in the Cyanobacterium Synechocystis sp. PCC 6803.

Appel J, Craig S, Theune M, Hüren V, Künzel S, Forberich B, Bryan S, Gutekunst K

Microorganisms 10: 1617

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Flv3A facilitates O2 photoreduction and affects H2 photoproduction independently of Flv1A in diazotrophic Anabaena filaments.

Santana-Sanchez A, Nikkanen L, Toth G, Ermakova M, Kosourov S, Walter J, He M, Aro E-M, Allahverdiyeva Y

Pyruvate:ferredoxin oxidoreductase and low abundant ferredoxins support aerobic photomixotrophic growth in cyanobacteria.

Wang Y, Chen X, Spengler K, Terberger K, Boehm M, Appel J, Barske T, Timm S, Battchikova N, Hagemann M, Gutekunst K

Photosynthetic linear electron flow drives CO2 assimilation in maize leaves.

Shimakawa G, Miyake C

International Journal of Molecular Sciences 22: 4894

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PGRL2 triggers degradation of PGR5 in the absence of PGRL1.

Rühle T, Dann M, Reiter B, Schünemann D, Naranjo B, Penzler J-F, Kleine T, Leister D

Nature Communications 12: 3941

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Singlet oxygen, flavonols and photoinhibition in green and senescing silver birch leaves.

Mattila H, Sotoudehnia P, Kuuslampi T, Stracke R, Mishra KB, Tyystjärvi E

Trees 35: 1267–1282

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Dynamic thylakoid stacking and state transitions work synergistically to avoid acceptor-side limitation of photosystem I.

Hepworth C, Wood WHJ, Emrich-Mills TZ, Procter MS, Casson S, Johnson MP

Nature Plants 7: 87-98

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Developmental acclimation of the thylakoid proteome to light intensity in Arabidopsis.

Flannery SE, Hepworth C, Wood WHJ, Pastorelli F, Hunter CN, Dickman MJ, Jackson PJ, Johnson MP

The Plant Journal 105: 223–244

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Differences in ionic, enzymatic, and photosynthetic features characterize distinct salt tolerance in eucalyptus species.

Balti H, Abassi M, Dietz K-J, Kumar V

Plants 10: 1401

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In-vivo quantification of electron transport makes up about 35% in a cyanobacterium.

Theune ML, Hildebrant S, Steffen-Heins A, Bilger W, Gutekunst K, Appel J

Biochimica et Biophysica Acta 1862: 148353

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redundancy and crosstalk between flavodiiron proteins and NDH-1 in Synechocystis sp. PCC 6803.

Nikkanen L, Santana Sánchez A, Ermakova M, Rögner M, Cournac L, Allahverdiyeva Y

Redox regulation by peroxiredoxins is linked to their thioredoxin-dependent oxidase function.

Telman W, Liebthal M, Dietz K-J

Photosynthesis Research 145: 31-41

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Near-infrared in vivo measurements of photosystem I and its luminal electron donors with a recently developed spectrophotometer.

Shimakawa G, Sétif P, Krieger-Liszkay A

Photosynthesis Research 144: 63-72

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Identification of the electron donor tot flavodiiron proteins in Synechocystis sp. PCC 6803 by in vivo spectroscopy.

Sétif P, Shimakawa G, Krieger-Liszkay A, Miyake C

Biochimica et Biophysica Acta 1861: 148256

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Functional redundancy between flavodiiron proteins and NDH-1 in Synechoscystis sp. PCC 6803.

Nikkanen L, Santana Sánchez S, Ermakova M, Rögner M, Cournac L, Allahverdiyeva Y

The Plant Journal 103: 1460-1476

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Intrinsic fluctuations in transpiration induce photorespiration to oxidize P700 in photosystem I.

Furutani R, Makino A, Suzuki Y, Wada S, Shimakawa G, Miyake C

Plants 9: 1761

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A commonly used photosynthetic inhibitor fails to block electron flow to Photosystem I in intact systems.

Fitzpatrick D, Aro E-M, Tiwari A

Frontiers in Plant Science 11: 382

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Interference between arsenic-induced toxicity and hypoxia.

Kumar V, Vogelsang L, Seidel T, Schmidt R, Weber M, Reichelt M, Meyer A, Clemens S, Sharma SS, Dietz K-J

Plant, Cell & Environment 42: 574-590

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Oxidation of P700 induces alternative electron flow in photosystem I in wheat leaves.

Kadota K, Furutani R, Makino A, Suzuki Y, Wada S, Miyake C

Plants 8: 152

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Consequences of photosystem-I damage and repair on photosynthesis and carbon use in Arabidopsis thaliana.

Lima-Melo Y, Gollan PJ, Tikkanen M, Silveira JAG, Aro E-M

Plant Journal 97: 1061-1072

Go to publication

Multilevel regulation of non-photochemical quenching and state transitions by chloroplast NADPH-dependent thioredoxin reductase.

Nikkanen L, Guinea Diaz M, Toivola J, Tiwari A, Rintamäki E

Physiologia Plantarum 166: 211-225

Go to publication

Near-infrared in vitro measurements of photosystem I cofactors and electron-transfer partners with a recently developed spectrophotometer.

Sétif P, Boussac A, Krieger-Liszkay A

Photosynthesis Research 142: 307-319

Go to publication

Regulation of cyclic electron flow by chloroplast NADPH-dependent thioredoxin system.

Nikkanen L, Toivola J, Trotta A, Guinea Diaz M, Tikkanen M, Aro E-M, Rintamäki E

Plant Direct 2: e00093

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Changing frequency of fluctuating light reveals the molecular mechanism for P700 oxidation in plant leaves.

Shimakawa G, Miyake C

Plant Direct 2: e00073

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PROTON GRADIENT REGULATION 5 supports linear electron flow to oxidize photosystem I.

Takagi D, Miyake C

Physiologia Plantarum 164: 337–348

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The chloroplast 2-cysteine peroxiredoxin functions as thioredoxin oxidase in redox regulation of chloroplast metabolism.

Vaseghi M-J, Chibani K, Telman W, Liebthal MF, Gerken M, Schnitzer H, Müller SM, Dietz K-J

eLife 7: e38194

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Redox changes of ferredoxin, P700, and plastocyanin measured simultaneously in intact leaves.

Schreiber U

Photosynthesis Research 134: 343–360

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Deconvolution of ferredoxin, plastocyanin, and P700 transmittance changes in intact leaves with a new type of kinetic LED array spectrophotometer.

Klughammer C, Schreiber U

Photosynthesis Research 128: 195–214

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Analysis of photosystem I donor and acceptor sides with a new type of online-deconvoluting kinetic LED-array spectrophotometer.

Schreiber U, Klughammer C

Plant and Cell Physiology 57: 1454-1467

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DUAL-KLAS-NIR

General design
Microcontroller: 4 x AVR-RISC (8 MHz) + 4 MB SRAM; 256 000 data points with 12 bit resolution can be stored
Communication
PC interface: USB 1.1, 2.0 and 3.0 compatible
User interface

Windows computer (Windows 7/8/10/11) with KLAS-100 software

Power supply
Rechargeable sealed lead-acid battery 12 V/2 Ah; Battery Charger MINI-PAM/L (100 to 240 V AC)
Power consumption
During basic operation 350 mA
Sockets
6 ports for heads (power for single wavelength (2 channels) and double wavelength (4 channels) modulated measuring light, power for 2 actinic LED arrays (one in DKN-E and one in DKN-D) and 1 NIR measuring light LED array (in DKN-E), input for 2 detectors (the photodiode detector of DKN-D is connected to detector 1), socket for stirrer (plus speed controller and standby switch), AUX (for Spherical Micro Quantum Sensor US-SQS/WB or Cosine-Corrected Mini Quantum Sensor US-MQS/WB), USB (for USB cable), TRIGGER OUT (output of 5 V rectangular signals to trigger external devices), 2 EXT. SIGNALS (input for external DC signals. Range 0-1 V or 0-5 V), and CHARGE (for MINI-PAM/L charger).
Dimensions
36 cm x 16 cm x 26.5 cm (W x H x D), with carrying handle
Weight
5.8 kg
Measuring light
Chip-On-Board LED array for pulse-modulated 780, 820, 840, 870 and 965 nm NIR measuring light, pulse modulated green, fluorescence measuring light (540 nm).
Actinic light
Chip-On-Board LED array (635 nm) for continuous red actinic illumination (max. ~3400 µmol photons m-2 s-1 PAR), which can also be used for single turn over flashes (max. >28000 µmol photons m-2 s-1 PAR, length 5-50 µs), and multiple turnover pulses (MT and SP) (max. 25000 µmol photons m-2 s-1 PAR, length 1-1000 ms).
Dimensions
5.5 cm x 9 cm x 4 cm (W x H x D)
Weight
560 g (incl. cables, 1.4 m long)
Measuring light
pulse modulated blue fluorescence measuring light (460 nm).
Actinic light
Blue light (460 nm) for continuous blue illumination (max. ~400 µmol m-2 s-1 PAR), Chip-On-Board LED array (635 nm) for continuous red illumination (max. ~3400 µmol m-2 s-1 PAR), which can also be used for saturating single turnover flashes (max. >28000 µmol m-2 s-1 PAR, length 5-50 µs), and multiple turnover pulses (MT and SP) (max. 25000 µmol photons m-2 s-1 PAR, length 1-1000 ms), far-red light (740 nm) for continuous far-red illumination (max. 400 µmol photons m-2 s-1).
Signal detection
Photodiode and pulse preamplifier to measure four dual wavelength NIR-transmission difference signals (780-820, 820-870, 870-965 and 840-965 nm) and two fluorescence signals. Time resolution of a single channel measurement is 35 µs, of a two channel measurement is 150 µs and of a 6 channel measurement is 1 ms. The same detector (protected by the same set of filters) is used for fluorescence and NIR transmission measurements. The filter set passes wavelengths > 750 nm.
Dimensions
5.5 cm x 9 cm x 4 cm (W x H x D)
Weight
540 g (including cables, 1.4 m long)
Design
Aluminum box with custom foam packing for DUAL-KLAS-NIR and accessories
Dimensions
60 cm x 40 cm x 34 cm (L x W x H)
Weight
5 kg
Design
Consisting of black anodized aluminum baseplate with gear rack on which one measuring head holder is mounted on a movable stage which can be precisely positioned along the gear rack by a lateral adjustment knob. Includes a 13 cm lab stand rod, which can be fixed (screwed) to the bottom of the baseplate, and a 3 mm Allen wrench
Dimensions
18.5 cm x 11.5 cm x 12 cm (L x W x H, max. without lab stand rod)
Weight
1050 g
Achievable temperatures
12 K below ambient temperature, 15 K above ambient temperature (Quartz cuvette placed in Optical Unit for Suspensions ED-101US/MD with 1.5 mL water and stirrer PHYTO-MS on)
Size
ø 55 mm, 110 mm height
Cable length
130 cm
Weight
0.29 kg (including cable)
Design
Cosine-response mini quantum sensor for selective measurement of photosynthetically active radiation (PAR, 400 – 700 nm) with Perspex diffuser disk as light entrance and signal amplifier box
Signal detection
High stability silicone photovoltaic detector with filter set providing equal response to photon fluxes across the PAR spectral range. The typical signal output of the detector is 2 μA / (1000 μmol m‑2 s‑1)
Temperature coefficient of photodiode
0.01 %/K
Absolute calibration
± 5 %
Angular dependence
error < 4 % between angles from -80° to +80° from normal axis
Immersion coefficient
Typically 1.32
Cable length
3 m
Size: Height
16 mm; diameter: 14 mm; Diffuser diameter: 5.5 mm
Weight
32 g
Amplifier box
Two amplification ranges (0 to 1000 and 0 to 20,000 μmol m‑2 s‑1, each range corresponding to 0 to 2.5 V DC). To be connected to the Leaf Clip Holder 2030-B port of the PAM-CONTROL unit. Power provided by the PAM-CONTOL unit. Dimensions: 5 cm x 3 cm x 5 (W x H x D). Weight: 200 g.
Dimensions

Base plate, 40 cm x 30 cm

Height

73.5 cm, diameter 1.5 cm

Weight

2.8 kg

Accessories

Design

Black-anodized aluminum body with central 10 x 10 mm glass cuvette; for attachment of Measuring Heads and Miniature Magnetic Stirrer PHYTO-MS; additional ports for attachment of two additional measuring heads

Weight

750 g

Temperature Control Block ED-101US/T
Sectioned block with central 10 x 10 mm opening to be mounted on top of the ED-101US/MD unit; to be connected to external flow-through water bath (not included), weight: 250 g
Miniature Magnetic Stirrer PHYTO-MS

Based on a device manufactures by h+p (type Variomag-Mini); featuring adapter to be mounted in the bottom port of the Optical Unit ED-101US/MD; powered and controlled by the Power-and-Control-Unit

Spherical Micro Quantum Sensor US-SQS/WB

3.7 mm Ø diffusing sphere coupled to integrated PAR sensor via 2 mm diameter fiber; compact amplifier unit and special holder for mounting on Optical Unit ED-101US/MD; to be connected tot the Power-and-Control Unit

Temperature Control Block ED-101US/T
Sectioned block with central 10 x 10 mm opening to be mounted on top of the ED-101US/MD unit; to be connected to external flow-through water bath (not included), weight 250 g
Miniature Magnetic Stirrer PHYTO-MS
Based on device manufactured by h+p (type Variomag-Mini); featuring adapter to be mounted in bottom port of the Optical Unit ED-101US/MD; powered and controlled by the Power-and-Control-Unit DKN-C
Spherical Micro Quantum Sensor US-SQS/WB
3.7 mm ø diffusing sphere coupled to integrated PAR sensor via 2 mm diameter fiber; compact amplifier unit and special holder for mounting on Optical Unit ED-101US/MD; to be connected to the Power-and-Control Unit DKN-C
Design
Quartz glass cuvette, cross section: 10 mm x 10 mm, external dimensions: 12.5 mm x 12.5 mm x 26 mm (L x W x H). Special cuvette holder to position the cuvette between two measuring heads. U-shaped black-anodized aluminum shields to screen out external light. Three sealing gaskets to protect lower measuring head from spills
Design

Magnetic stirrer driven by a rotating magnetic field; the PHYTO-MS is connected to Power-and-Control Unit PHYTO-II-C; a special adapter plug allows the insertion in the bottom port of the Optical Unit ED-101US/MP

Weight
16 g
Display
Three line LCD display
Control range
0 °C to 50 °C at 0.1 K steps
Operating voltage
11 V – 14 V DC
Maximum Peltier current
1 A
Size
105 mm x 90 mm x 130 mm (W x H x D)
Weight
0.57 kg

Power-and-Control Unit US-T/DR

Display
Three line LCD display
Control range
0 °C to 50 °C at 0.1 K steps
Operating voltage
11 V - 14 V DC
Maximum Peltier current
1 A
Size
105 mm x 90 mm x 130 mm (W x H x D)
Weight
0.57 kg

Peltier Heat-Transfer Head US-T/DS

Achievable temperatures
12 K below ambient temperature, 15 K above ambient temperature (Quartz cuvette placed in Optical Unit for Suspensions ED-101US/MD with 1.5 mL water and stirrer PHYTO-MS on)
Size
⌀ 55 mm, 110 mm height
Cable length
130 cm
Weight

0.29 kg (including cable)

AC Adapter

Input

100 V - 240 V AC 1.5 A 50-60 Hz

Output
12 V DC 5.5 A
Size

130 mm x 56 mm x 30 mm (L x W x H)

Weight
0.50 kg (including cable)
Design
Cuvette is a sandwich of two 2 x 2 cm aluminum frames, each holding the end part of a Walz standard Perspex rod to connect various measuring heads of the DUAL-PAM-100 or DUAL-KLAS-NIR. Distance between Perspex rod and leaf: ca. 1 mm on each leaf side.
Pneumatically separated upper and lower cuvette halves. Controlled by a regulator unit with sockets for cable connections to the Control Unit 3000 C of the GFS-3000 and a trigger input line.
Cuvette temperature
Pt 100 type A (located near the Peltier elements), range -10 to 50 °C, accuracy ±0.1 °C
Temperature control
Set point value for cuvette temperature. Cuvette temperature ranging from 10 degrees below ambient to max. +50 °C
Leaf temperature measurement
Thermocouple, range -10 to 50 °C, accuracy ±0.2 °C
External miniature quantum sensor
Mini Quantum Sensor MQS-B/GFS: Selective PAR measurement, range 0 to 2500 μmol m-2 s-1 PAR, accuracy ±5%, cosine corrected
Leaf area
1.3 cm2
Trigger in
Triggers at 5 V → 0 V signal change
Operating temperature
-5 to 45 °C
Dimensions
Assembled cuvette: 10 cm x 4 cm x 12 cm (L x W x H), electronics box : 7 cm x 7 cm x 15 cm (L x W x H)
Weight
Cuvette, electronics box, cables, and mounting frame: 1.7 kg; Mounting Stand ST-101: 2 kg

General Features and Graphical User Interface

The KLAS-100 software used for DUAL-KLAS-NIR measurements is written in the tradition of the DUAL-PAM-100 software. It allows the user to make the sample quickly ready for online signal deconvolution and the measurements the user has in mind via a fixed sequence of steps. A script is provided to determine the maximum P700, PC and Fd signal amplitudes (comparable to the Pm determination of the DUAL-PAM-100). Four NIR wavelength pairs are measured and the P700, PC and Fd contributions to these NIR signals are determined using so-called differential model plots or DMPs. Differential Model Plots for Hedera helix are included in the software for reference. In practice, separate sets of DMPs have to be determined for individual plant species. Via a fixed sequence of steps, making use of the scripts included in the software for the determination of each DMP (P700, PC and Fd), the user can make his or her own set of DMPs for the photosynthetic organism that is studied.

The software has a window for saturation pulse analysis and one for light curves, just like in the DUAL-PAM-100 software, but then including an analysis of the PC and Fd redox states. Like for the DUAL-PAM-100, the software automatically calculates classical fluorescence ratio parameters as well as more recently suggested parameters. In a new window it is possible to plot the P700 and PC redox states against each other, which gives an idea about the redox-equilibrium between the two. Trigger files can be created and Script files written that in combination allow the reproducible execution of complex experimental protocols. Whereas some background knowledge is required for programming Trigger files and Scripts, even very sophisticated protocols can be reliably executed by non-experts. The software gives the user the flexibility to create almost any experimental protocol that can be imagined for the analysis of electron transport related processes.

Differential Model Spectra (DMPs) for the deconvolution of the NIR-signals

The absorption spectra of P700, plastocyanin (PC) and ferredoxin (Fd) are broad and show few features in the near infrared (NIR). A further complication is that the extinction coefficient of P700 is much higher than that of PC, which is higher again than the extinction coefficient of Fd. By choosing specific wavelength pairs it is only possible to get NIR-signals enriched in Fd (780-820 nm), or P700 (820-870 nm) or PC (870-950 nm). To get from there to a clean deconvolution, the software makes use of the differential model plot (DMP) approach, which does not require knowledge of difference spectra and the wavelength dependence of differential extinction coefficients. Christof Klughammer first developed this method for the KLAS-100, a kinetic LED array spectrophotometer for the 510-570 nm wavelength range.

We know the behavior of PC, P700 and Fd under standard conditions quite well and we can, on the basis of that knowledge, design experiments in which, for a short period of time, only redox changes of one of the three components (PC, P700 or Fd) occur. By normalization of the values determined for the 4 difference signals a “spectral fingerprint” for each component is obtained under the given experimental conditions. It should be noted here as well that the FA and FB iron-sulfur centers located on the acceptor side of photosystem I may also contribute to the Fd-signal.