Miyasaka Lab. ARAI Yuhei 1. Ⅰ. Introduction ・ Single-Molecule Measurements (SMM) ・ Microscope Ⅱ. Applications of single molecule fluorescence imaging.

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Miyasaka Lab. ARAI Yuhei 1

Ⅰ. Introduction ・ Single-Molecule Measurements (SMM) ・ Microscope Ⅱ. Applications of single molecule fluorescence imaging Ⅲ. My work Motivation Method Result and Discussion Ⅳ. Summary 2

3 Each guest molecule is in different environment. Spectrum Spectrum of ensemble Spectrum of a single molecule Trajectory Trajectory of a single molecule

Wide-fieldConfocal Time resolution30 fpm(16.7μm×16.7μm)200 s(15 μm×15 μm) Spatial resolution(x-y plane)250 nm Spatial resolution(z axis)3 μm900 nm Advantage ・ Measure many molecules at one time ・ High spatial resolution about z axis Disadvantage ・ Background light from out of focus ・ Long measurement time ・ Measure few molecules at one time 4 Confocal microscope Wide-field microscope

θ ~ λ/2 ・ sinθ Diffraction-limit Conventional optical microscope Spatial Resolution is limited by “diffraction-limit ” ~ about a half of wavelength ( > 200nm) Super resolution microscopy Beyond the diffraction-limit ~ from several to tens of nm PhotoActivated Localization Microscopy (PALM) Using localization method and photo switchable fluorescent molecule ・ Stochastic Optical Reconstruction Microscopy (STORM) ※ diffraction-limit : 回折限界

Stefan W. Hell, et al, Science,316 (2007) Fluorescent ON state partly hv (activation) Localization High spatial resolved image (several nm ~ ten-odd nm) hv (excitation) OFF state Localization Super resolution microscopy(PALM : Photo-Activated Localization Microscopy)

X : ±0.06 pix. Y : ±0.06 pix. Single-Molecule Tracking : SMT sX, sY : Width of Gauss function Θ : Rotation angle bg : background noise I 0 : Fluorescence intensity X 0, y 0 : Center of Gauss function

Ⅰ. Introduction ・ Single-Molecule Measurements (SMM) ・ Microscope Ⅱ. Applications of single molecule fluorescence imaging Ⅲ. My work Motivation Method Result and Discussion Ⅳ. Summary 8

Evaluating microscopic inhomogeneity of polymer film by using Single-molecule tracking Polymer chain is dense Polymer chain is sparse Microscopic structure of polymer Lithographic nanofabrication Diffusional motion is fast Diffusional motion is slow Nano imprinting S.Takei et al, JJAP, 46(2007)

10 Vis. (Φ co << ) UV (Φ oc =0.21) (Φ F =0.78) DAE2 Poly(2-hydroxyethyl acrylate) [PolyHEA] T g : 17 ℃ →Guest molecules show diffusional motion at room tempature( 21±2 ℃ ) ( Mn : 6,050 、 Mw : 9,800 ) Fluorescence off stateFluorescence ON state UV irradiation time UV irradiation time

11 Difficult to excute accurate SMT if guest molecules spacially overlap Difficult to fit

12 Difficult to excute accurate SMT if guest molecules spacially overlap UV Photobleach Swtiching times 1 2 3 4 ・・

13 UV light intensity : High Overlap, photobleach UV light intensity : Low Long measurement time Optimize UV light intensity 3 μm UV

14 3 mW 1 mW 100 μW 2 μW 3 μm Lack of SMT molecules →Impossible to evaluate inhomogeneity of polymer film Need to develop new switching method