Chinese Journal of Lasers, Volume. 51, Issue 21, 2107101(2024)

Research Progress and Prospects of Low‑Power Stimulated Emission Depletion Microscopy

Haoxian Zhou, Luwei Wang, Renlong Zhang, Fangrui Lin, Liwei Liu, and Junle Qu*
Author Affiliations
  • Key Laboratory of Optoelectronic Devices and Systems of Ministry of Education/Guangdong Province, College of Physics and Optoelectronic Engineering, Shenzhen University, Shenzhen 518060, Guangdong , China
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    Figures & Tables(6)
    Schematic diagrams of STED. (a) Imaging principle diagram; (b) simplified Jablonski energy level diagram for a typical STED process; (c) Atto 647N dye spectra
    Schematic diagrams of low-power STED imaging methods based on single molecular localization. (a) MINFLUX[83];
    Schematic diagrams of low-power STED imaging methods based on image signal processing. (a) DE-STED[92]; (b) mSTED[93]; (c) FM-STED[94]
    Schematic diagrams of low-power STED imaging methods based on time-resolved detection. (a) Time-gating[101]; (b) SPLIT[97]; (c) phasor plot analysis[98]; (d) ratiometric photon reassignment[99]
    • Table 1. Parameters and imaging indexes of STED probes (λex: excitation wavelength; λem: emission wavelength; Isat: saturation intensity; Psat: STED power; τ: fluorescence lifetime)

      View table

      Table 1. Parameters and imaging indexes of STED probes (λex: excitation wavelength; λem: emission wavelength; Isat: saturation intensity; Psat: STED power; τ: fluorescence lifetime)

      TypeOriginal name

      λex & λem /

      nm

      Isat PsatτPhotostability

      Resolution /

      nm

      Organic dyesAbberior STAR 48834503 & 5243.9 ns110
      Atto 53276532 & 5523.8 ns~20
      Atto 647N16644 & 6699 mW3.5 ns52
      MitoPB-Yellow41480 & 5701.3 MW/cm27.5 nsOver 390 s<60
      MitoESq-63542635 & 6704.37 MW/cm21.7 nsOver 50 min35.2
      520R43521 & 5464.0 ns40
      Complex1+[45488 & 660180 nsOver 1000 s

      35(XY

      120‒150(Z

      AIE dotsTPA-T-CyP56480 & 684~50 mWOver 17.5 s74
      Red-AIE-OXE57405 & 6404.5 ns95
      TTF@SiO258510 & 66040 mW1.29 nsThe fluorescence intensity decreased by 30% after one and a half hours of imaging30.7
      PDsPDFDP60403 & 633~0.4 mWThe fluorescence intensity decreased by 30% after two hours of imaging71
      CNPPV77455 & 604~0.5 mWThe fluorescence intensity decreased by 44% after two hours of imaging78
      Other types of organic nano-particlesCSONPs61500 & 6500.0085 MW/cm2Over 600 s60
      Organosilica nanohybrids75470 & 5200.188 MW/cm24.37 nsThe fluorescence intensity decreased by 50% after 100 scans43.6
      DBTBT-4C862496 & 65511.9 mW3.85 nsOver 25 min100
      QDsQdots70578445 & 705~50 mW8 nsThe fluorescence intensity decreased by 50% after 1300 scans~50
      CsPbBr364488 & 5200.126 MW/cm215.5 nsOver 200 min20.6
      UCNPs

      8%Tm3++

      20% Yb3+[65

      980 & 4550.19 MW/cm2Tens of μs to msOver 200 min28

      10% Tm3++

      18% Yb3+[66

      975 & 4550.849 MW/cm2Over 3000 scans66
      CDsFNCDs70466 & 5130.226 MW/cm24.89 nsThe fluorescence intensity decreased by 12% after 1000 scans22.1
      CPDs-372465 & 5150.23 MW/cm24009 psThe fluorescence intensity decreased by 30% after 200 scans92
      FNDsNV center79550 & 68513 ns4.1
      NVN center80480 & 5302.5 MW/cm227 nsOver 100 scans90
      LPR hybridsAuNRs73610 & 640~15 MW/cm23.5 ns±0.2 nsUp to 50% increase
      Gold nanospheres81500 & 5254.6‒5.8 MW/cm20.95 nsThe fluorescence intensity decreased by 50% after 20 scans75
    • Table 2. Imaging performance comparison of STED and its derivative techniques

      View table

      Table 2. Imaging performance comparison of STED and its derivative techniques

      MethodType of STEDResolutionAdvantageDisadvantage

      Conventional

      STED

      pSTED98109

      40 nm fluorescent beads:

      52 nm/24 mW;

      endoplasmic reticulum (PTK2): 52 nm/36 mW

      Higher peak power compared to CW-STED for the same resolution at lower depletion powerHigh cost and complexity; need pulse synchronization
      CW-STED16

      20 nm fluorescent beads:

      34 nm/812 mW; neurofilaments:

      52 nm/432 mW

      Low cost and complexity; wide wavelength coverageThe average power is 4‒5 times higher compared to pSTED, increasing the probability of photobleaching and re-excitation
      MINFLUXpSTED83

      ~1 nm precision;

      ~5 nm resolution

      The localization precision and imaging resolution are greatly improvedComplex controls and algorithms are required
      LocSTEDCW-STED84Single molecules of Alexa 555: ~15 nmOffer a more relaxed requirement for STED beam to achieve high-resolutionRequire specialized imaging buffers for the reversible blinking of fluorophores and careful control to achieve optimal results
      MINSTEDpSTED87Ångström range precision; ~4 nm resolutionHigher resolution and more efficient particle discovery compared to MINFLUXThe high depletion power for precise localization causes anti-Stokes background noise
      On-line time-gated STEDCW-STED102

      40 nm fluorescent beads:

      35 nm/250 mW;

      microtubule (PtK2):

      89 nm/300 mW

      Simple operation, effective resolution improvement (better resolution improvement for CW-STED)Require precise time synchronization; reduce the SNR (signal to noise ratio) of image
      pSTED102

      Microtubule (PtK2):

      89 nm/45 mW

      Off-line time-gated STEDCW-STED100

      Microtubule (astrocytes):

      70 nm/85 mW

      Reduce system costs and flexibly set time gatesReduce the SNR of image

      SPLIT

      CW-STED97

      Microtubule (HeLa):

      ~100 nm/40 mW;

      Improve resolution without affecting the SNRThe separation criteria required to improve resolution is not quantified; the accuracy of photon separation is affected by discrete noise
      pSTED107

      60 nm fluorescent beads:

      69 nm±4 nm/25 mW

      PPApSTED98

      100 nm fluorescent beads:

      118 nm/10 mW;

      HeLa: 86 nm/20 mW

      The resolution improvement effect is better than the time-gatingTCSPC is required for PPA, complicating the system
      RPR-STEDpSTED99

      40 nm fluorescent beads:

      96 nm/60 mW;

      microtubule (HeLa):

      108 nm/50 mW

      Improve the resolution without affecting the SNR; TCSPC is not required for PPA, simplifying the systemThe resolution improvement effect is not obvious compared to time-gating
      DE-STEDpSTED92

      23 nm fluorescent beads:

      30 nm±8 nm/3.6 mW;

      microtubule (BSC-1):

      82 nm/1.4 mW

      The depletion power is greatly reducedAn image mismatch may arise owing to sample drift
      mSTEDpSTED93

      23 nm fluorescent beads:

      41.2 nm±8 nm/1.95 mW;

      microtubule (HeLa):

      90 nm/1.8 mW

      Solve the pixel mismatch problemSusceptible to aberration
      FM-STEDpSTED94

      23 nm fluorescent beads: 140 nm / 10 mW; microtubule (BSC-1):

      108 nm / 10 mW

      Effectively improve resolution and remove background signalsThe fluorescence intensity decreased after treatment
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    Haoxian Zhou, Luwei Wang, Renlong Zhang, Fangrui Lin, Liwei Liu, Junle Qu. Research Progress and Prospects of Low‑Power Stimulated Emission Depletion Microscopy[J]. Chinese Journal of Lasers, 2024, 51(21): 2107101

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    Paper Information

    Category: Biomedical Optical Imaging

    Received: Jun. 13, 2024

    Accepted: Jul. 4, 2024

    Published Online: Oct. 31, 2024

    The Author Email: Qu Junle (jlqu@szu.edu.cn)

    DOI:10.3788/CJL240959

    CSTR:32183.14.CJL240959

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