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Reading the fleeting moments of photosynthesis at sunlight intensity… correlated-photon spectroscopy demonstrated

inquantio

Published Aug 26, 2026• 0 citations
Publisher

Abstract

Using the correlations between photon pairs generated by spontaneous parametric down-conversion (SPDC) from a continuous-wave (CW) laser, researchers have performed time- and frequency-resolved fluorescence spectroscopy at illumination intensities comparable to real-world sunlight. By measuring purified light-harvesting complexes (LH2) and intact photosynthetic membranes, they tracked at the single-photon level how excitation energy transfer lifetimes change with the open or closed state of the reaction center (RC). Wavelength-integrated fluorescence lifetime traces were recorded in as little as 0.6 seconds, though the authors state plainly that this is not a demonstration of quantum advantage in the strict sense of using entanglement to break a classical sensitivity limit. [Quantum Biology Society] Ultrafast optical spectroscopy has played a central role in studying the earliest dynamics of processes such as photosynthesis and vision. Conventional pulsed-laser methods, however, pour an enormous number of photons onto a sample in a vanishingly brief instant, a condition far removed from the natural setting of sunlight, where a pigment absorbs single photons only rarely. Spectroscopy using quantum states of light has been put forward as an alternative, but experimental demonstrations have been scarce and have typically demanded measurements running for hours or more, a serious practical barrier. A collaboration between the University of Glasgow in the UK and the Politecnico di Milano in Italy has now reported a way to close that gap, publishing in Nature Communications in September 2025. ■ Pairing a continuous-wave laser with correlated photons The team focused a 413 nm continuous-wave (CW) laser into a nonlinear crystal, periodically poled KTiOPO4 (ppKTP), and used spontaneous parametric down-conversion (SPDC) to generate entangled photon pairs at 800 and 860 nm. The 860 nm photon was detected by a single-photon avalanche diode (SPAD) and served as the heralding photon, while its 800 nm twin was sent to the sample. Because the arrival times of the two photons are correlated, the pair itself can drive a time-correlated single photon counting (TCSPC) unit, and the experiment reaches a time resolution of 100 to 200 ps with no pulsed laser anywhere in the setup. The herald arm also carries a tunable interference filter, so choosing the herald wavelength effectively chooses the excitation wavelength of its partner, and tuning the crystal temperature shifts the pair further, giving excitation tunability from 670 nm to 1100 nm. A birefringent common-path interferometer (TWINS) placed in front of the fluorescence detector adds spectral resolution on the detection side. Unlike a grating spectrometer feeding a detector array, this Fourier-transform approach collects all the light onto a single pixel. On the authors' estimate, based on their own measurements and published specifications for state-of-the-art SPAD cameras, that is worth a factor of roughly 4 to 8 in signal-to-noise ratio (SNR) for the same total acquisition time. ■ Tracking energy flow in intact photosynthetic membranes The technique was then applied to real photosynthetic proteins. LH2 complexes purified from the purple photosynthetic bacterium Rhodoblastus acidophilus, excited one photon at a time, gave a single-exponential fluorescence lifetime of 1.13 ± 0.01 ns, in excellent agreement with the value measured on the same sample using a classical femtosecond pulsed laser. The researchers went on to analyze intact photosynthetic membranes from Rhodobacter sphaeroides, which contain LH2, LH1 and the reaction center (RC) together. With the RCs open and able to carry out charge separation, excitation energy drains rapidly onward to the RC and the fluorescence lifetime is short: 101 ± 3 ps. When the RCs were closed by adding a reducing agent, charge separation was blocked, the RC equilibrated with LH1, which then became the terminal emitter, and the lifetime lengthened to 248 ± 9 ps, with the emission spectrum red-shifting to peak near 875 nm. Taken together, these measurements capture at the single-photon level the cascade that carries light energy from LH2 through LH1 to the RC. The fastest step in that chain, the roughly 1 ps transfer from B800 to B850 within LH2, remains beyond the current time resolution; what the experiment reads out is the excited-state lifetime that the cascade produces. ■ A dramatic cut in measurement time, and the boundary of quantum advantage The clearest breakthrough in this work is speed. The team reduced the time needed to record a wavelength-integrated TCSPC fluorescence decay to 0.6 seconds while keeping the SNR at about 4, still sufficient to yield a lifetime estimate in line with those from far longer acquisitions. Quantum-light spectroscopy, once a matter of hours, has entered sub-second territory. Full time- and frequency-resolved maps still take longer, since the interferometer must be scanned position by position: 3.3 minutes for the faster LH2 map shown in the paper, and 3.3 hours at the finest sampling. The authors drew a firm line around what the result does and does not show. They state explicitly in the paper that they have not demonstrated quantum advantage in the rigorous sense of using entanglement to surpass a classical bound on sensitivity or resolution. What they do claim is that the correlations of entangled photon pairs make fast, efficient time-resolved fluorescence measurement possible with nothing more than a CW laser, something that cannot be achieved by classical means. The practical implication is that observing photosynthetic machinery under sunlight-like, extremely low-light conditions could settle into a routine laboratory tool rather than remaining a special demonstration. #QuantumBiology #Photosynthesis #SinglePhoton #CorrelatedPhotons #EntangledPhotonPairs #SpontaneousParametricDownConversion #SPDC #FluorescenceLifetime #TCSPC #LH2 #LH1 #ReactionCenter #PurpleBacteria #QuantumLightSpectroscopy #NatureCommunications https://www.nature.com/articles/s41467-025-63830-3

DOI
10.5281/zenodo.22107600

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Using the correlations between photon pairs generated by spontaneous parametric down-conversion (SPDC) from a continuous-wave (CW) laser, researchers have performed time- and frequency-resolved fluorescence spectroscopy at illumination intensities comparable to real-world sunlight. By measuring purified light-harvesting complexes (LH2) and intact photosynthetic membranes, they tracked at the single-photon level how excitation energy transfer lifetimes change with the open or closed state of the reaction center (RC). Wavelength-integrated fluorescence lifetime traces were recorded in as little as 0.6 seconds, though the authors state plainly that this is not a demonstration of quantum advantage in the strict sense of using entanglement to break a classical sensitivity limit. [Quantum Biology Society] Ultrafast optical spectroscopy has played a central role in studying the earliest dynamics of processes such as photosynthesis and vision. Conventional pulsed-laser methods, however, pour an enormous number of photons onto a sample in a vanishingly brief instant, a condition far removed from the natural setting of sunlight, where a pigment absorbs single photons only rarely. Spectroscopy using quantum states of light has been put forward as an alternative, but experimental demonstrations have been scarce and have typically demanded measurements running for hours or more, a serious practical barrier. A collaboration between the University of Glasgow in the UK and the Politecnico di Milano in Italy has now reported a way to close that gap, publishing in Nature Communications in September 2025. ■ Pairing a continuous-wave laser with correlated photons The team focused a 413 nm continuous-wave (CW) laser into a nonlinear crystal, periodically poled KTiOPO4 (ppKTP), and used spontaneous parametric down-conversion (SPDC) to generate entangled photon pairs at 800 and 860 nm. The 860 nm photon was detected by a single-photon avalanche diode (SPAD) and served as the heralding photon, while its 800 nm twin was sent to the sample. Because the arrival times of the two photons are correlated, the pair itself can drive a time-correlated single photon counting (TCSPC) unit, and the experiment reaches a time resolution of 100 to 200 ps with no pulsed laser anywhere in the setup. The herald arm also carries a tunable interference filter, so choosing the herald wavelength effectively chooses the excitation wavelength of its partner, and tuning the crystal temperature shifts the pair further, giving excitation tunability from 670 nm to 1100 nm. A birefringent common-path interferometer (TWINS) placed in front of the fluorescence detector adds spectral resolution on the detection side. Unlike a grating spectrometer feeding a detector array, this Fourier-transform approach collects all the light onto a single pixel. On the authors' estimate, based on their own measurements and published specifications for state-of-the-art SPAD cameras, that is worth a factor of roughly 4 to 8 in signal-to-noise ratio (SNR) for the same total acquisition time. ■ Tracking energy flow in intact photosynthetic membranes The technique was then applied to real photosynthetic proteins. LH2 complexes purified from the purple photosynthetic bacterium Rhodoblastus acidophilus, excited one photon at a time, gave a single-exponential fluorescence lifetime of 1.13 ± 0.01 ns, in excellent agreement with the value measured on the same sample using a classical femtosecond pulsed laser. The researchers went on to analyze intact photosynthetic membranes from Rhodobacter sphaeroides, which contain LH2, LH1 and the reaction center (RC) together. With the RCs open and able to carry out charge separation, excitation energy drains rapidly onward to the RC and the fluorescence lifetime is short: 101 ± 3 ps. When the RCs were closed by adding a reducing agent, charge separation was blocked, the RC equilibrated with LH1, which then became the terminal emitter, and the lifetime lengthened to 248 ± 9 ps, with the emission spectrum red-shifting to peak near 875 nm. Taken together, these measurements capture at the single-photon level the cascade that carries light energy from LH2 through LH1 to the RC. The fastest step in that chain, the roughly 1 ps transfer from B800 to B850 within LH2, remains beyond the current time resolution; what the experiment reads out is the excited-state lifetime that the cascade produces. ■ A dramatic cut in measurement time, and the boundary of quantum advantage The clearest breakthrough in this work is speed. The team reduced the time needed to record a wavelength-integrated TCSPC fluorescence decay to 0.6 seconds while keeping the SNR at about 4, still sufficient to yield a lifetime estimate in line with those from far longer acquisitions. Quantum-light spectroscopy, once a matter of hours, has entered sub-second territory. Full time- and frequency-resolved maps still take longer, since the interferometer must be scanned position by position: 3.3 minutes for the faster LH2 map shown in the paper, and 3.3 hours at the finest sampling. The authors drew a firm line around what the result does and does not show. They state explicitly in the paper that they have not demonstrated quantum advantage in the rigorous sense of using entanglement to surpass a classical bound on sensitivity or resolution. What they do claim is that the correlations of entangled photon pairs make fast, efficient time-resolved fluorescence measurement possible with nothing more than a CW laser, something that cannot be achieved by classical means. The practical implication is that observing photosynthetic machinery under sunlight-like, extremely low-light conditions could settle into a routine laboratory tool rather than remaining a special demonstration. #QuantumBiology #Photosynthesis #SinglePhoton #CorrelatedPhotons #EntangledPhotonPairs #SpontaneousParametricDownConversion #SPDC #FluorescenceLifetime #TCSPC #LH2 #LH1 #ReactionCenter #PurpleBacteria #QuantumLightSpectroscopy #NatureCommunications https://www.nature.com/articles/s41467-025-63830-3
Classical time-resolved optical spectroscopy experiments are performed using sequences of ultrashort light pulses, with photon fluxes incident on the sample which are many orders of magnitude higher than real-world conditions corresponding to sunlight illumination. Spectroscopy and microscopy schemes that use quantum states of light have been widely described theoretically with fewer experimental demonstrations that typically require very long measurements that can extend for hours or more. Here, we show that time-resolved spectroscopy with quantum light can be performed without compromising measurement time or wavelength tunability, recording a fluorescence lifetime trace in biological samples in less than a second with acceptable signal-to-noise ratio. Starting from spontaneous parametric down-conversion driven by a continuous-wave laser, we exploit the temporal correlation between randomly generated signal/idler pairs to obtain temporal resolution, and their spectral correlation to select the excitation frequency. We also add spectral resolution in detection, using a 'photon-efficient' Fourier transform approach which employs a common-path interferometer. We demonstrate the potential of this approach by resolving, at the single-photon level, excitation energy transfer cascades from LH2 to LH1 in the photosynthetic membrane and disentangling the lifetimes of two dyes in a mixture. Our results provide a new approach to ultrafast optical spectroscopy, where experiments are performed under illumination intensity conditions comparable to real-world sunlight illumination.
Classical time-resolved optical spectroscopy experiments are performed using sequences of ultrashort light pulses, with photon fluxes incident on the sample which are many orders of magnitude higher than real-world conditions corresponding to sunlight illumination. Here we overcome this paradigm by exploiting quantum correlations to perform time-resolved spectroscopy with entangled photons. Starting from spontaneous parametric down-conversion driven by a continuous-wave laser, we exploit the temporal entanglement between randomly generated signal/idler pairs to obtain temporal resolution, and their spectral entanglement to select the excitation frequency. We also add spectral resolution in detection, using a Fourier transform approach which employs a common-path interferometer. We demonstrate the potential of our entangled-photon streak camera by resolving, at the single-photon level, excitation energy transfer cascades from LH2 to LH1 in the photosynthetic membrane and disentangling the lifetimes of two dyes in a mixture. We show that time-resolved spectroscopy with quantum light can be performed without compromising measurement time, recording a fluorescence time trace in less than a minute even for samples with low quantum yield, which can be reduced to sub-second times with acceptable signal-to-noise ratio. Our results provide a new approach to ultrafast optical spectroscopy, where experiments are performed under conditions comparable to real-world sunlight illumination.
We have used photon pair correlations generated via spontaneous parametric downconversion (SPDC) to measure the fluorescence lifetime of the organic dye rhodamine 6 G, demonstrating that fluorescence lifetime measurements can be achieved using a continuous wave (CW) laser, without pulsed or modulated lasers. Our entangled photon method, quantum fluorescence lifetime (Q-FL) measurements, uses one photon to excite fluorescence and the resulting fluorescence photon is timed and referenced to the arrival time of the other entangled photon. Thus, we can exploit the short timescale of photon pair correlations to conduct experiments that are typically carried out with pulsed lasers and we show that the inherent timing of the photons is fast enough to resolve the nanosecond scale fluorescence lifetime of the sample. This measurement paves the way towards using the time correlations of entangled photons for fluorescence imaging; capitalizing on the presence of fast, sub-100 ps correlations that have not been demonstrated classically.
Researchers at the University of Colorado Boulder and the National Institute of Standards and Technology (NIST) built a single apparatus that illuminates a sample alternately with a classical laser and with entangled photon pairs from SPDC, and used it to test two-photon absorption efficiency in six fluorophores. Entangled pair excitation produced no fluorescence signal above the noise floor in any of the samples, and the resulting upper bounds on the entangled two-photon absorption (E2PA) cross section fall as much as five orders of magnitude below previously reported values. The team argues that the claims of a ten-order-of-magnitude quantum advantage in the literature may rest on reading a simple linear dependence on photon flux as proof while leaving the spatio-temporal correlations of the source unspecified, and their evidence indicates that E2PA efficiency lies far below current detection limits. [Quantum Biology Society] Two-photon absorption (2PA) microscopy is a central tool for looking deep inside living tissue. The classical pulsed-laser approach carries a serious cost, however: concentrating an enormous number of photons into a small spot generates heating and other forms of damage. As an alternative, the idea that spatially and temporally correlated entangled photon pairs generated by spontaneous parametric down-conversion (SPDC) could maximize 2PA efficiency even at extremely low light levels, the process known as E2PA, has attracted considerable attention. A series of recent experimental studies reported that E2PA delivers a quantum advantage over classical 2PA of as much as ten orders of magnitude, and expectations across the field rose accordingly. A collaboration between the University of Colorado Boulder and NIST, with Ralph Jimenez as corresponding author, challenged those enormous numbers head-on in a paper published in Physical Review Applied in 2021. The group built a precision apparatus capable of comparing a classical laser and entangled photon pairs under essentially identical optical conditions, and used it to test the inflated claims experimentally. ■ Mismatched yardsticks: what goes wrong when entangled cross sections are compared The classical 2PA cross section (σC) is an intrinsic property of a molecule. The E2PA cross section (σE), by contrast, depends strongly on how tight a time window (the entanglement time, Te) and how small a spatial region (the entanglement area, Ae) the two photons of a pair arrive in together. The team points out that earlier reports either did not specify Te and Ae, or estimated Te at the output of the nonlinear crystal while neglecting the group delay dispersion (GDD) accumulated in the optics along the way, so that the value at the sample can be smaller by orders of magnitude. They also note that the linear dependence of signal on photon flux, offered in previous work as evidence of entangled absorption, appears equally in ordinary one-photon processes such as scattering, one-photon absorption, or fluorescence from the coating of an optic in the beam path. Working backwards, they find a physical contradiction: to justify the large cross sections previously reported, the light would have to be confined to a region 10⁻⁶ to 10⁻¹⁰ times the diffraction-limited spot size. ■ Cross-checking in one controlled apparatus: a signal below the noise floor The apparatus splits an 810 nm pulsed laser into two paths, one used directly for classical excitation, the other frequency-doubled to 405 nm and sent into a type-0 ppKTP crystal to generate entangled photon pairs by SPDC. The two beams are combined on a polarizing beam splitter and sent along essentially the same path to a focus inside a single cuvette, with an optical chopper providing on-the-fly background subtraction. Across six fluorophores including AF455, quantum dot 605 and fluorescein, classical laser excitation produced a clear 2PA signal scaling with the square of the photon flux, with fitted exponents between 1.95 and 2.05, and the derived classical cross sections agreed closely with published values, confirming the integrity of the instrument. Under SPDC excitation, however, all six samples stayed at the noise floor, below the instrument's detection limit of 0.22 counts per second, despite an incident SPDC rate of 8.9 × 10⁹ photons per second, which is part of what makes the resulting sensitivity so high. ■ An upper bound a hundred thousand times lower With no signal to measure, the team substituted its measurable fluorescence lower bound to calculate upper bounds on σE. These run from 1.0 ± 0.2 × 10⁻²⁵ cm² per fluorophore for fluorescein to 4.8 × 10⁻²³ cm² for quantum dot 605. For 9R-S and rhodamine 6G (Rh6G) in particular, two molecules previously reported to show strong E2PA, the bounds established here fall five orders of magnitude and four orders of magnitude respectively below the published values. Converted into a quantum advantage of E2PA over classical 2PA, the upper bounds come out at 410 to 7000, against prior claims approaching 10¹⁰. ■ Significance and outlook The paper does not prove that E2PA does not exist. When the team fed its measured σC together with its estimates of Te and Ae into the simple probabilistic model, the theoretically expected σE landed three to five orders of magnitude below this experiment's detection limit. Their Te at the sample was about 1620 fs, against roughly 17 fs for a transform-limited pulse, and Ae could only be constrained to somewhere between 2.1 and 13,700 µm². In other words, entangled two-photon absorption may simply be too faint to capture with present sensitivity, and the enormous quantum advantages in the existing literature are, on this evidence, likely to be experimental artefacts or overstated interpretation. The authors are careful to add that they do not expect this simple model to give an exact answer. They also set out a methodological standard: any report of E2PA results should quantify Te and Ae at the sample position. The vision of low-light biological imaging built on quantum optics remains attractive, but opening that door will require stepping back from expectations inflated by several orders of magnitude and taking a cool second look at the limits of the instruments and the correlations of the source. #QuantumBiology #EntangledTwoPhotonAbsorption #E2PA #TwoPhotonMicroscopy #SpontaneousParametricDownConversion #SPDC #QuantumAdvantage #UpperBounds #Fluorophores #Rhodamine6G #EntanglementTime #EntanglementArea #Reproducibility #NIST #PhysRevApplied https://arxiv.org/abs/2008.02664
Fluorescence lifetime experiments are a standard approach for measuring excited-state dynamics and local environmental effects. Here, we show that entangled photon pairs produced from a continuous-wave (CW) laser diode can replicate pulsed laser experiments without phase modulation. As a proof of principle, picosecond fluorescence lifetimes of indocyanine green are measured in multiple environments. The use of entangled photons has three unique advantages. First, low-power CW laser diodes and entangled photon source design lead to straightforward on-chip integration for a direct path to distributable fluorescence lifetime measurements. Second, the entangled pair's wavelength is easily tuned by adjusting the temperature or electric field, allowing a single source to cover octave bandwidths. Third, femtosecond temporal resolutions can be reached without requiring major advances in source technology or external phase modulation. Entangled photons could therefore provide increased accessibility to time-resolved fluorescence while also opening new scientific avenues in photosensitive and inherently quantum systems.
Efficient Generation of Entangled Photon-Pairs The first experiments with correlated photons have been performed in the context of EPR-Bell experiments on the realistic and local properties of quantum mechanics. The source used there produced pairs of polarization entangled photons from a 2-photon decay of Calcium atoms. The technical requirements of these experiments were high (vacuum systems, stronge dye-lasers, etc.) whereas the efficiency of the source was quite low. An important step forward was the introduction of spontaneous parametric down conversion (SPDC), which has become the most common source in quantum optics for generating correlated or entangled photon pairs. In this process photons of an intense pump laser convert to photon pairs in an optical nonlinear crystal. Conservation of energy and momentum leads to strong correlations between the generated photons. With this kind of two-photon source it was possible to realize or improve many experiments on the foundations of quantum mechanics addressing the EPR-Paradoxon and in the new field of quantum information. But again, more advanced experiments and applications suffer from the limited ef- ficiency of the fluorescence process. Many photon pairs are lost by spatial and spectral filtering, which is necessary to achieve polarization entanglement and long coherence times. Different techniques have been implemented to increase the number of photon pairs using two-crystal arrangements, focusing techniques or periodically poled crystals. Most of these methods have the disadvantage that no entangled photons have been observed. It is the aim of this work to increase the yield and to improve the mode definition of entangled photon pairs generated by resonant enhancement of the pump mode and the fluorescence modes. As a first step a linear cavity for the pump mode was realized. Since the conversion probability is proportional to the pump power it was possible to increase the photon pair count rate by factor of 7 over the previous source. Besides the possibility of further improvement on already established pair correlation experiments, such an enhancement allows to build a compact source for photon pairs, in which an expensive argon-ion laser is replaced by a cheap diode laser. Among other applications such sources are of strong interest for quantum cryptography. 3 In many quantum information experiments optical fibers are use to carry the photons over long distance. Therefore, light from the parametric down-conversion source has to be efficiently coupled into fibers. In the second part we report on a new method to optimize collection efficiency by matching the angular distribution of the parametric fluorescence to the spatial mode of an optical fiber. By using this technique, we detected 366500 polarization-entangled photon pairs per second in the near-infrared region in single-mode optical fibers for 465 mW pump power (at 351.1 nm) with a 2 mm BBOcrystal. The entanglement of the photon pairs was verified by measuring polarization correlations of more than 96% in a HV-basis and in a ±45◦-basis. To our knowledge, such enormous count rates of highly entangled photon pairs have not been reached yet with any other technique. In the third part of this thesis we investigated the process of parametric downconversion in a cavity which is resonant to certain longitudinal down-conversion modes only. The idea of placing the parametric down-conversion source inside a cavity is not new. Such a device is usually referred to as a single or double resonant optical parametric oscillator (OPO) and is mainly used to generate squeezed quantum states. In that kind of application the system is operating close to but still under the threshold of oscillation. In our application the situation is quite different. The system is operating far below threshold so that mainly spontaneous emission occurs. In that mode correlations between single photons can still be observed. But bouncing the light back and forth inside the cavity increases the interaction length and hence enhances the signal levels of the down-conversion fields. Further, by resonating two certain modes only, the bandwidth is reduced by orders of magnitude and the coherence time is found to be inverse proportional to the bandwidth. A similar experiment has already been realized with a type-I parametric down-converter in the resonator. We have tried to realize a compact double resonant OPO far below threshold with a type-II parametric down-converter in a high-finesse cavity to realize a bright source of entangled photon pairs with extremely narrow bandwidth.