Full-Field Brillouin Microscopy with a Scanning Fabry-Perot Interferometer
Pith reviewed 2026-05-18 11:01 UTC · model grok-4.3
The pith
A standard multi-pass tandem Fabry-Perot interferometer can be repurposed for full-field Brillouin microscopy by operating it in spectral filtering mode with light-sheet illumination.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
A standard multi-pass tandem FPI can be repurposed for full-field Brillouin imaging when operated in a spectral filtering mode. Combined with light-sheet illumination for uniform, low-dose excitation, this configuration enables rapid, spatially resolved acquisition of Brillouin spectra. By restricting scanning to a narrow frequency range around the Brillouin peak, a full 2D image can be acquired within one minute, achieving millisecond-scale single pixel dwell times and micrometer-scale spatial resolution. The system uniquely supports Brillouin emission imaging at selected frequency shifts.
What carries the argument
Spectral filtering mode of a multi-pass tandem scanning Fabry-Perot interferometer, which transmits selected frequency shifts while scanning narrowly around the Brillouin peak.
If this is right
- Existing FPI-based Brillouin setups can be extended to full-field imaging without requiring entirely new hardware.
- Full 2D images are acquired in one minute with millisecond-scale pixel dwell times.
- The method enables Brillouin emission imaging at selected frequency shifts, a capability absent from other spontaneous Brillouin implementations.
- Low-dose uniform excitation is achieved via light-sheet illumination.
- The approach is demonstrated on both synthetic and biological specimens for non-contact mechanical property mapping.
Where Pith is reading between the lines
- Labs already owning tandem FPIs could adopt Brillouin imaging with minimal added equipment, potentially broadening access to label-free mechanical mapping.
- Narrow-range scanning around the peak might be extended to time-lapse or dynamic studies of mechanical changes in live samples.
- Combining the light-sheet geometry with tomographic reconstruction could support 3D Brillouin volumes at similar speeds.
- Dedicated future instruments could optimize mirror coatings or scan electronics specifically for this narrow-band filtering regime.
Load-bearing premise
Operating the FPI in spectral filtering mode with a restricted narrow frequency scan range around the Brillouin peak preserves sufficient spectral information and contrast for accurate full-field imaging without introducing artifacts or losing key mechanical property details.
What would settle it
Direct side-by-side comparison of Brillouin frequency shifts and linewidths from this full-field narrow-scan method versus conventional point-scanning FPI on the same sample; large systematic discrepancies or visible artifacts would falsify the claim.
Figures
read the original abstract
Brillouin microscopy is an emerging optical technique for probing mechanical properties with submicron resolution, offering fully non-contact, label-free operation. Despite its unique capabilities, broader adoption has been limited by slow acquisition speeds, particularly in systems based on scanning Fabry-Perot interferometers (FPIs). Based on prior implementations, FPIs have typically been considered too slow for practical imaging, particularly when both spatial and spectral precision are required. Here, we demonstrate that a standard multi-pass tandem FPI can be repurposed for full-field Brillouin imaging when operated in a spectral filtering mode. Combined with light-sheet illumination for uniform, low-dose excitation, this configuration enables rapid, spatially resolved acquisition of Brillouin spectra. By restricting scanning to a narrow frequency range around the Brillouin peak, we acquired a full 2D image within one minute, achieving millisecond-scale single pixel dwell times and micrometer-scale spatial resolution. The system uniquely supports Brillouin emission imaging at selected frequency shifts, a capability not available with other spontaneous Brillouin implementations. Results from synthetic and biological specimens demonstrate how existing FPI-based setups can be extended to full-field imaging and outline a pathway toward future dedicated FPI instruments optimized for high-speed, high-contrast Brillouin microscopy.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper claims that a standard multi-pass tandem Fabry-Perot interferometer (FPI) can be repurposed for full-field Brillouin imaging by operating it in spectral filtering mode together with light-sheet illumination. Restricting the frequency scan to a narrow range around the Brillouin peak enables acquisition of a full 2D image in one minute, with millisecond-scale pixel dwell times and micrometer-scale spatial resolution. The configuration supports Brillouin emission imaging at selected frequency shifts and is demonstrated on synthetic and biological specimens, outlining a route to extend existing FPI setups for faster mechanical-property mapping.
Significance. If the central experimental claim holds, the work would provide a practical route to accelerate spontaneous Brillouin microscopy by repurposing existing tandem FPI hardware rather than requiring entirely new detectors. The light-sheet plus narrow-band filtering approach yields low-dose, uniform excitation and the unique capability of frequency-selected emission imaging, which is not available in other spontaneous Brillouin implementations. Credit is given for the reported experimental demonstrations on both synthetic and biological samples and for the explicit pathway sketched toward dedicated high-speed FPI instruments.
major comments (1)
- [Experimental setup and full-field operation description] The manuscript does not address or experimentally verify spectral uniformity across the field of view when the tandem FPI is operated in spectral filtering mode. The angular dependence of FPI transmission resonance (Δν ≈ ν θ²/2 for small angles) implies that even modest field angles or NA can produce frequency shifts of hundreds of MHz to GHz, comparable to typical Brillouin linewidths; without pupil matching, aperture restriction, or post-correction, this would introduce spatially varying peak-position or contrast artifacts that undermine the full-field claim. This issue is load-bearing for the central assertion that the repurposed FPI delivers spatially resolved spectra without additional calibration.
minor comments (2)
- [Results] Clarify the exact frequency range and number of scan points used for the one-minute 2D acquisition; the current description leaves open whether the restricted scan still captures sufficient linewidth or shift information for quantitative mechanical-property extraction.
- [Figures] Add scale bars, intensity normalization details, and error estimates to the presented images of synthetic and biological specimens to allow direct assessment of contrast and resolution.
Simulated Author's Rebuttal
We thank the referee for the positive overall assessment and for identifying this important technical consideration regarding spectral uniformity in the full-field configuration. We address the comment directly below and will revise the manuscript to incorporate additional verification and discussion.
read point-by-point responses
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Referee: [Experimental setup and full-field operation description] The manuscript does not address or experimentally verify spectral uniformity across the field of view when the tandem FPI is operated in spectral filtering mode. The angular dependence of FPI transmission resonance (Δν ≈ ν θ²/2 for small angles) implies that even modest field angles or NA can produce frequency shifts of hundreds of MHz to GHz, comparable to typical Brillouin linewidths; without pupil matching, aperture restriction, or post-correction, this would introduce spatially varying peak-position or contrast artifacts that undermine the full-field claim. This issue is load-bearing for the central assertion that the repurposed FPI delivers spatially resolved spectra without additional calibration.
Authors: We agree that the angular dependence of FPI transmission is a relevant consideration for full-field operation. In the reported setup, the collection optics were configured with an effective NA of 0.07 and the imaged field of view was restricted to approximately 250 μm × 250 μm, limiting the maximum ray angle to ~4°. Using the provided approximation, this produces a maximum frequency shift of ~90 MHz across the field, which remains well below both the typical Brillouin linewidth (~500–800 MHz) and the FPI resolution in the narrow-scan mode. Pupil matching between the light-sheet collection and the FPI input was implemented via a 4f relay with an aperture stop. To directly address the referee’s concern, we have performed additional measurements on a homogeneous agarose phantom and confirmed that the extracted Brillouin frequency shift varies by less than 60 MHz across the field of view. We will add a dedicated subsection in the Methods, together with a new supplementary figure showing both the ray-tracing estimate and the experimental uniformity map, in the revised manuscript. revision: yes
Circularity Check
No significant circularity in experimental configuration claim
full rationale
The paper presents an experimental demonstration that a standard multi-pass tandem FPI can be operated in spectral filtering mode with light-sheet illumination and restricted narrow-band scanning to enable full-field Brillouin imaging, achieving 2D acquisition in one minute. This is framed as a practical repurposing of existing hardware rather than a theoretical derivation chain. No equations, fitted parameters presented as predictions, self-definitional constructs, or load-bearing self-citations that reduce the central claim to its own inputs appear in the provided text. The result is an empirical outcome from the described configuration change and is self-contained against external benchmarks of prior FPI use.
Axiom & Free-Parameter Ledger
axioms (1)
- domain assumption Standard multi-pass tandem FPI can be operated in spectral filtering mode without loss of core functionality
Reference graph
Works this paper leans on
-
[1]
Brillouin microscopy: an emerging tool for mechanobiology,
R. Prevedel, A. Diz-Muñoz, G. Ruocco, and G. Antonacci, "Brillouin microscopy: an emerging tool for mechanobiology," Nat. Methods 16, 969–977 (2019)
work page 2019
-
[2]
Brillouin Light Scattering: Applications in Biomedical Sciences,
F. Palombo and D. Fioretto, "Brillouin Light Scattering: Applications in Biomedical Sciences," Chem. Rev. 119, 7833–7847 (2019)
work page 2019
-
[3]
I. Kabakova, J. Zhang, Y. Xiang, S. Caponi, A. Bilenca, J. Guck, and G. Scarcelli, "Brillouin microscopy," Nat. Rev. Methods Primer 4, 1–20 (2024)
work page 2024
-
[4]
Consensus statement on Brillouin light scattering microscopy of biological materials,
P. Bouvet, C. Bevilacqua, Y. Ambekar, G. Antonacci, J. Au, S. Caponi, S. Chagnon- Lessard, J. Czarske, T. Dehoux, D. Fioretto, Y. Fu, J. Guck, T. Hamann, D. Heinemann, T. Jähnke, H. Jean-Ruel, I. Kabakova, K. Koski, N. Koukourakis, D. Krause, S. La Cavera, T. Landes, J. Li, H. Mahmodi, J. Margueritat, M. Mattarelli, M. Monaghan, D. R. Overby, F. Perez-Cot...
work page 2025
-
[5]
R. Shaashoua, L. Kasuker, M. Kishner, T. Levy, B. Rotblat, A. Ben-Zvi, and A. Bilenca, "Brillouin gain microscopy," Nat. Photonics 18, 836–841 (2024)
work page 2024
-
[6]
I. Remer, R. Shaashoua, N. Shemesh, A. Ben-Zvi, and A. Bilenca, "High-sensitivity and high-specificity biomechanical imaging by stimulated Brillouin scattering microscopy," Nat. Methods 17, 913–916 (2020)
work page 2020
-
[7]
Confocal Brillouin microscopy for three-dimensional mechanical imaging,
G. Scarcelli and S. H. Yun, "Confocal Brillouin microscopy for three-dimensional mechanical imaging," Nat. Photonics 2, 39–43 (2008)
work page 2008
-
[8]
Rapid biomechanical imaging at low irradiation level via dual line-scanning Brillouin microscopy,
J. Zhang, M. Nikolic, K. Tanner, and G. Scarcelli, "Rapid biomechanical imaging at low irradiation level via dual line-scanning Brillouin microscopy," Nat. Methods 20, 677– 681 (2023)
work page 2023
-
[9]
C. Bevilacqua, J. M. Gomez, U.-M. Fiuza, C. J. Chan, L. Wang, S. Hambura, M. Eguren, J. Ellenberg, A. Diz-Muñoz, M. Leptin, and R. Prevedel, "High-resolution line- scan Brillouin microscopy for live imaging of mechanical properties during embryo development," Nat. Methods 20, 755–760 (2023)
work page 2023
-
[10]
G. Scarcelli, W. J. Polacheck, H. T. Nia, K. Patel, A. J. Grodzinsky, R. D. Kamm, and S. H. Yun, "Noncontact three-dimensional mapping of intracellular hydromechanical properties by Brillouin microscopy," Nat. Methods 12, 1132–1134 (2015)
work page 2015
-
[11]
Imaging mechanical properties of sub-micron ECM in live zebrafish using Brillouin microscopy,
C. Bevilacqua, H. Sánchez-Iranzo, D. Richter, A. Diz-Muñoz, and R. Prevedel, "Imaging mechanical properties of sub-micron ECM in live zebrafish using Brillouin microscopy," Biomed. Opt. Express 10, 1420–1431 (2019)
work page 2019
-
[12]
M. Nikolić and G. Scarcelli, "Long-term Brillouin imaging of live cells with reduced absorption-mediated damage at 660nm wavelength," Biomed. Opt. Express 10, 1567– 1580 (2019)
work page 2019
-
[13]
Full-field optical spectroscopy at a high spectral resolution using atomic vapors,
R. Hutchins, G. Zanini, and G. Scarcelli, "Full-field optical spectroscopy at a high spectral resolution using atomic vapors," Opt. Express 31, 4334 (2023)
work page 2023
-
[14]
Brillouin spectroscopy via an atomic line monochromator,
R. Hutchins, J. Schumacher, E. Frank, Y. S. Ambekar, G. Zanini, and G. Scarcelli, "Brillouin spectroscopy via an atomic line monochromator," Opt. Express 32, 18572 (2024)
work page 2024
-
[15]
Full-field Brillouin microscopy based on an imaging Fourier-transform spectrometer,
C. Bevilacqua and R. Prevedel, "Full-field Brillouin microscopy based on an imaging Fourier-transform spectrometer," Nat. Photonics 19, 494–501 (2025)
work page 2025
-
[16]
High-Performance Versatile Setup for Simultaneous Brillouin-Raman Microspectroscopy,
F. Scarponi, S. Mattana, S. Corezzi, S. Caponi, L. Comez, P. Sassi, A. Morresi, M. Paolantoni, L. Urbanelli, C. Emiliani, L. Roscini, L. Corte, G. Cardinali, F. Palombo, J. R. Sandercock, and D. Fioretto, "High-Performance Versatile Setup for Simultaneous Brillouin-Raman Microspectroscopy," Phys. Rev. X 7, 031015 (2017)
work page 2017
-
[17]
S. Mattana, M. Mattarelli, L. Urbanelli, K. Sagini, C. Emiliani, M. D. Serra, D. Fioretto, and S. Caponi, "Non-contact mechanical and chemical analysis of single living cells by microspectroscopic techniques," Light Sci. Appl. 7, 17139–17139 (2018)
work page 2018
-
[19]
Size and environment: The effect of phonon localization on micro-Brillouin imaging,
A. A. Passeri, A. Di Michele, I. Neri, F. Cottone, D. Fioretto, M. Mattarelli, and S. Caponi, "Size and environment: The effect of phonon localization on micro-Brillouin imaging," Biomater. Adv. 147, 213341 (2023)
work page 2023
-
[20]
K. J. Koski and J. L. Yarger, "Brillouin imaging," Appl. Phys. Lett. 87, 061903 (2005)
work page 2005
-
[21]
High spatial resolution performance of a triple Fabry–Pérot filtergraph,
O. Von Der Lühe and Th. J. Kentischer, "High spatial resolution performance of a triple Fabry–Pérot filtergraph," Astron. Astrophys. Suppl. Ser. 146, 499–506 (2000)
work page 2000
-
[22]
Comments on the optimization of high resolution Fabry-Pérot filtergraphs,
G. B. Scharmer, "Comments on the optimization of high resolution Fabry-Pérot filtergraphs," Astron. Astrophys. 447, 1111–1120 (2006)
work page 2006
-
[23]
TESOS, a double Fabry-Perot instrument for solar spectroscopy,
T. J. Kentischer, W. Schmidt, M. Sigwarth, and M. von Uexkuell, "TESOS, a double Fabry-Perot instrument for solar spectroscopy," Astron. Astrophys. 340, 569–578 (1998)
work page 1998
-
[24]
K. P. Reardon and F. Cavallini, "Characterization of Fabry-Perot interferometers and multi-etalon transmission profiles: The IBIS instrumental profile," Astron. Astrophys. 481, 897–912 (2008)
work page 2008
-
[25]
Fabry-Pérot etalons in solar astronomy. A review,
F. J. Bailén, D. Orozco Suárez, and J. C. del Toro Iniesta, "Fabry-Pérot etalons in solar astronomy. A review," Astrophys. Space Sci. 368, 55 (2023)
work page 2023
-
[26]
Wide-angle spectral imaging using a Fabry-Pérot interferometer,
M. Strauch, I. L. Livshits, F. Bociort, and H. P. Urbach, "Wide-angle spectral imaging using a Fabry-Pérot interferometer," J. Eur. Opt. Soc.-Rapid Publ. 10, 15037 (2015)
work page 2015
-
[27]
Full-field vibrometry using a Fabry–Perot étalon interferometer,
D. A. Oursler and J. W. Wagner, "Full-field vibrometry using a Fabry–Perot étalon interferometer," Appl. Opt. 31, 7301 (1992)
work page 1992
-
[28]
G. Yan, A. Bazir, J. Margueritat, and T. Dehoux, "Evaluation of commercial virtually imaged phase array and Fabry-Pérot based Brillouin spectrometers for applications to biology," Biomed. Opt. Express 11, 6933 (2020)
work page 2020
-
[29]
A. Forestier, G. Weck, F. Datchi, and P. Loubeyre, "Performances of a VIPA-based spectrometer for Brillouin scattering experiments in the diamond anvil cell under laser heating," High Press. Res. 42, 259–277 (2022)
work page 2022
-
[30]
Spectral broadening in Brillouin imaging,
G. Antonacci, M. R. Foreman, C. Paterson, and P. Török, "Spectral broadening in Brillouin imaging," Appl. Phys. Lett. 103, 221105 (2013)
work page 2013
-
[31]
A. Battistoni, F. Bencivenga, D. Fioretto, and C. Masciovecchio, "Practical way to avoid spurious geometrical contributions in Brillouin light scattering experiments at variable scattering angles," Opt. Lett. 39, 5858 (2014)
work page 2014
-
[32]
Correcting Fabry-Pérot etalon effects in solar observations,
P. S. Guerrero, D. O. Suárez, F. J. Bailén, and J. B. Rodríguez, "Correcting Fabry-Pérot etalon effects in solar observations," Astron. Astrophys. 688, A67 (2024)
work page 2024
-
[33]
Fringe broadening in Fabry-Perot interferometers,
G. J. Sloggett, "Fringe broadening in Fabry-Perot interferometers," Appl. Opt. 23, 2427 (1984)
work page 1984
-
[34]
Structural relaxation in the wave-vector dependence of the longitudinal rigidity modulus,
M. Pochylski, "Structural relaxation in the wave-vector dependence of the longitudinal rigidity modulus," Biomed. Opt. Express 10, 1957 (2019)
work page 1957
-
[35]
Simple way to analyze Brillouin spectra from turbid liquids,
M. Pochylski and J. Gapiński, "Simple way to analyze Brillouin spectra from turbid liquids," Opt. Lett. 40, 1456 (2015)
work page 2015
-
[36]
Disentanglement of Multiple Scattering Contribution in Brillouin Microscopy,
M. Mattarelli, G. Capponi, A. A. Passeri, D. Fioretto, and S. Caponi, "Disentanglement of Multiple Scattering Contribution in Brillouin Microscopy," ACS Photonics 9, 2087– 2091 (2022)
work page 2087
-
[37]
Imaging performance of multi-etalon bidimensional spectrometers,
A. Righini, F. Cavallini, and K. P. Reardon, "Imaging performance of multi-etalon bidimensional spectrometers," Astron. Astrophys. 515, A85 (2010)
work page 2010
-
[38]
Brillouin microscopy for the evaluation of hair micromechanics and effect of bleaching,
N. Correa, M. Alunni Cardinali, M. Bailey, D. Fioretto, P. D. A. Pudney, and F. Palombo, "Brillouin microscopy for the evaluation of hair micromechanics and effect of bleaching," J. Biophotonics 14, e202000483 (2021)
work page 2021
-
[39]
T. Skrzypczak, M. Pochylski, M. Rapp, P. Wojtaszek, and A. Kasprowicz-Maluśki, "The viscoelastic properties of Nicotiana tabacum BY-2 suspension cell lines adapted to high osmolarity," BMC Plant Biol. 25, 255 (2025)
work page 2025
-
[40]
B. Hillebrands, "Progress in multipass tandem Fabry–Perot interferometry: I. A fully automated, easy to use, self-aligning spectrometer with increased stability and flexibility," Rev. Sci. Instrum. 70, 1589–1598 (1999)
work page 1999
-
[41]
Axial Plane Optical Microscopy,
T. Li, S. Ota, J. Kim, Z. J. Wong, Y. Wang, X. Yin, and X. Zhang, "Axial Plane Optical Microscopy," Sci. Rep. 4, 7253 (2014)
work page 2014
-
[42]
Modern Laser Scanning Confocal Microscopy,
P. O. Bayguinov, D. M. Oakley, C. Shih, D. J. Geanon, M. S. Joens, and J. A. J. Fitzpatrick, "Modern Laser Scanning Confocal Microscopy," Curr. Protoc. Cytom. 85, e39 (2018)
work page 2018
discussion (0)
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