STED Nanoscale 3 D Optical Imaging Digvijay Raorane

  • Slides: 19
Download presentation
STED: Nanoscale 3 D Optical Imaging Digvijay Raorane & Arun Majumdar Department of Mechanical

STED: Nanoscale 3 D Optical Imaging Digvijay Raorane & Arun Majumdar Department of Mechanical Engineering Department of Materials Science University of California, Berkeley Materials Sciences Division Lawrence Berkeley National Laboratory

Outline • • Motivation Introduction: Conventional Optics Near Field Imaging STED - Theory -

Outline • • Motivation Introduction: Conventional Optics Near Field Imaging STED - Theory - Previous experimental work • On-going experiments

Biological Imaging • Virus TMV 16. 5 nm • Microtubules Microtubule 25 nm •

Biological Imaging • Virus TMV 16. 5 nm • Microtubules Microtubule 25 nm • Cell Organelle ER canaliculi dia. 40 -60 nm

Need for High Resolution Optical Technique • Biomolecules that require imaging are typically 1

Need for High Resolution Optical Technique • Biomolecules that require imaging are typically 1 - 50 nm in size • Far-field optics (e. g. confocal) limited to resolution > 200 nm, which cannot directly resolve molecular-scale phenomena • Atomic Force Microscopy cannot be used inside a cell • Optical/fluorescence imaging is most-widely used approach for real-time intracellular visualization • NSOM (Near-field Scanning Optical Microscope)

Optical Imaging at a Glance Far-Field Optics Near-Field Scanning Optical Microscope (NSOM) d Diffraction-limited

Optical Imaging at a Glance Far-Field Optics Near-Field Scanning Optical Microscope (NSOM) d Diffraction-limited spatial resolution ~ λ/2*NA Aperture-limited spatial resolution d ~ 50 nm

NSOM Limitations • Single fiber is limited to the field of view to ~

NSOM Limitations • Single fiber is limited to the field of view to ~ 50 nm. • It is difficult to maintain the tip at the constant distance from the sample within few nms. • Tip can get damaged by thermal stress due to the light. • Scanning a whole cell area (10 mm x 10 mm) takes time. • Multi-location imaging and dynamics cannot be observed. • Fiber-drawing and aperture fabrication is not repeatable, producing different imaging conditions each time. • Tip may get clogged when biological sample is in its buffer medium. Tip Profile http: //micro. magnet. fsu. edu Tip Damage Rosa et al. , Appl. Phys. Lett. 67, (18), 2597 -2599 (1995)

What is Stimulated Emission Depletion (STED) Microscopy?

What is Stimulated Emission Depletion (STED) Microscopy?

Spontaneous Emission Fluorescence Absorption Spontaneous Vibrational ex Relaxation Emission Absorption ~10 ns Emission ex

Spontaneous Emission Fluorescence Absorption Spontaneous Vibrational ex Relaxation Emission Absorption ~10 ns Emission ex Vibrational Relaxation Wavelength, sp-em

Fluorescence Imaging Diffraction-limited spatial resolution ~ λ/2*NA

Fluorescence Imaging Diffraction-limited spatial resolution ~ λ/2*NA

Stimulated Emission Absorption ex st Vibrational Relaxation Absorption st Emission ex Vibrational Relaxation Wavelength,

Stimulated Emission Absorption ex st Vibrational Relaxation Absorption st Emission ex Vibrational Relaxation Wavelength, st

Physical Realization • Conceptual Set-up STED Spot Avalanche Photodiod e λ/2 Phase Plate Fluorescence

Physical Realization • Conceptual Set-up STED Spot Avalanche Photodiod e λ/2 Phase Plate Fluorescence 645 -715 nm Excitation Spot Fluorescence Imaging Spot, d<< /2*(NA) Hell S. et al. , Nature Biotech. , 21(11), 2003

Point Spread Function Engineering • Non Linear Optical Effect - STED laser quenches tail

Point Spread Function Engineering • Non Linear Optical Effect - STED laser quenches tail of PSF due to excitation laser => reduction in FWHM of resultant focal spot incident on fluorescence sample Weiss S. et al. , PNAS, 97 (16), pg. 8747– 8749, 2000

Resolution • Resolution (FWHM) dependence on Intensity FWHM (Δr) • For typical experiment,

Resolution • Resolution (FWHM) dependence on Intensity FWHM (Δr) • For typical experiment,

STED Imaging Absorption ex img st Vibrational Relaxation Absorption st Emission ex Vibrational Relaxation

STED Imaging Absorption ex img st Vibrational Relaxation Absorption st Emission ex Vibrational Relaxation Wavelength, st

Proof of Concept Al 2 O 3 matrix wetted by Polymethyl Methacrylate Westphal et

Proof of Concept Al 2 O 3 matrix wetted by Polymethyl Methacrylate Westphal et al, APL, 82(18), 3125 - 3127 (2003) Westphal et al, PRL 94, 143903 (2005)

Experimental Set up Ti: Sa Laser st OPO Delay LPC PS ex CH st

Experimental Set up Ti: Sa Laser st OPO Delay LPC PS ex CH st SAMPLE Fluorescence img Detector DC 1 DC 2

Collaboration: Prof. Costas Grigoropoulos (ME Dept, UCB)

Collaboration: Prof. Costas Grigoropoulos (ME Dept, UCB)

On-Going Work • Quantum dot as substitute to fluorescent tags - To test compatibility

On-Going Work • Quantum dot as substitute to fluorescent tags - To test compatibility of Q Dots with STED microscopy to overcome photobleaching of fluorescent labels Nucleus with actin fibres Hines et al, Advanced Materials, 15, 1845, 2003 Alivisatos et al, Nature Biotech. , 22, 47 – 52, 2004

Advantages of STED Microscopy • • • High resolution can be achieved routinely (

Advantages of STED Microscopy • • • High resolution can be achieved routinely ( < 50 nm) No need of probe/tip Signal can be collected at far-field Better than confocal microscope in terms of resolution Multiple areas can be probed by forming multiple spots on the sample Resolution depends on the laser intensity ( FWHM = f( Intensity)) Incorporates most widely used fluorescence technique by biologists Can image live biological sample Optical system is simple to understand Can scan the sample in z direction for 3 D image 3 D Image Yeast Mammalian Mitochondria Golgi Hell et al, J. Opt. Soc. Am. A , 9(12), 2159 – 2166, 1992