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Fundamentals in and

NIF Optical Seminar Jan 16th 2019 - Aurelien Breakdown

Detections

Illuminations

Magic

NIF Optical Seminar Jan 16th 2019 - Aurelien Illumination: What is light ?

Wave Particle

NIF Optical Seminar Jan 16th 2019 - Aurelien Light as a wave: properties

Intensity I α A2 Wavelength (λ) Frequency ν=λ/c Amplitude (A) z direction of propagation

Phase (φ) π/2 z0 t1203 π 0 z

3π/2

NIF Optical Seminar Jan 16th 2019 - Aurelien Light as a wave: properties

LINEAR POLARIZATION CIRCULAR POLARIZATION ELLIPTICAL POLARIZATION Polarization becomes crucial for techniques such as DIC or if you use lasers as an illumination source.

NIF Optical Seminar Jan 16th 2019 - Aurelien Light as a particle: why ?

"It seems as though we must use sometimes the one theory and sometimes the other, while at times we may use either. (…) We have two contradictory pictures of reality; separately neither of them fully explains the phenomena of light, but together they do"

PHOTOELECTRIC EFFECT

Frequency threshold : below this threshold, no electrons are emitted, even if intensity is increased e e e BUT

METAL Light propagates as discrete packets of energy called PHOTONS: Wave theory of light: increasing either the frequency or the intensity of light would increase electron Energy = hν h: Plank’s constant emission rate NIF Optical Seminar Jan 16th 2019 - Aurelien Light interactions

Law of reflection: θ1 θ1' θ = θ ’ Reflection 1 1

n1

n2

θ2

n1 < n2

Law of refraction (Snell’s law):

n1 sinθ1 = n2 sinθ2 Multicolor Refraction (n is dependent on

n1 = c/v1, n2=c/v2 λ) is called dispersion

Refraction NIF Optical Seminar Jan 16th 2019 - Aurelien Diffraction

π/2

π 0

3π/2 constructive interference 0-2π destructive interference π intermediate interference π/2

Superposition of light waves generates interference patterns.

NIF Optical Seminar Jan 16th 2019 - Aurelien Absorption (visible and fluorescence)

NIF Optical Seminar Jan 16th 2019 - Aurelien NIF Optical Seminar Jan 16th 2019 - Aurelien UPRIGHT

camera

epifluorescence eyepiece/occulars pathway

Tube fluorescence lamphouse

objective

condenser turret trans-illumination (condenser lens, lamphouse diaphragm)

field diaphragm

NIF Optical Seminar Jan 16th 2019 - Aurelien Illuminations

• Uniform illumination of the sample (widefield): • Trans illumination: white light (LED or incandescent) or can add filters if needed (i.e. optogenetics experiments). • Fluorescence lightpath source can be an arc lamp (older systems) or LED-based to tune specific wavelengths.

• Other systems use lasers as illumination. Generally those are used in point scanning illumination (confocal in the core) or more complex schemes (beam shaping methods).

NIF Optical Seminar Jan 16th 2019 - Aurelien Detectors

• Chip sensors such as CCD, cMOS. Takes a snapshot of a plane, holds spatial location, usually monochromatic (except for histology), has a certain pixel size (spatial resolution constraint) and refresh rate (kHz or less), needs brighter signal . Used for widefield imaging.

• Photodiodes and PMTs: no intrinsic spatial location, very sensitive (can detect single photons) and fast (MHz/GHz). Used in confocal and multiphoton microscopes.

NIF Optical Seminar Jan 16th 2019 - Aurelien

• Many different types of lenses: convex, concave, plano-, bi- …. • In microscopes, lenses are used to collect and optimize light transmission through distances by relaying important spatial planes (meaning the plane where your sample lies) • For simplicity, we will only consider convex lenses.

1 1 1 = + 푓 표 푖

NIF Optical Seminar Jan 16th 2019 - Aurelien Ray Diagram

a-levelphysicstutor.com

NIF Optical Seminar Jan 16th 2019 - Aurelien “4f” system and magnification

M= f2/f1

NIF Optical Seminar Jan 16th 2019 - Aurelien Trans illumination/ Brightfield

CRITICAl ILLUMINATION KÖHLER ILLUMINATION sample plane f CO condenser lens resolution f contrast aperture CO aperture diaphragm diaphragm

fF

field lens determine the filling of the condenser aperture fF PROBLEM OF CRITICAL field contrast (preventing ILLUMINATION: diaphragm glare) an image of the light source is fCL formed at the sample plane collector lens collimate light fCL

NIF Optical Seminar Jan 16th 2019 - Aurelien Objectives: the critical and expensive part of the microscope

4 1 2

3

NIF Optical Seminar Jan 16th 2019 - Aurelien Objectives:

D pupil plane (back focal plane)

objective

α

f n focal plane

Angular aperture: sin α Numerical aperture: NA = n sin α Pupil diameter: D = 2 f NA = 2 n f sin α NIF Optical Seminar Jan 16th 2019 - Aurelien Objectives: point spread function (PSF)

NIF Optical Seminar Jan 16th 2019 - Aurelien Diffraction

π/2

π 0

3π/2 constructive interference 0-2π destructive interference π

Superposition of light waves generates interference patterns.

NIF Optical Seminar Jan 16th 2019 - Aurelien PSF: why do you care ?

NIF Optical Seminar Jan 16th 2019 - Aurelien Two point sources are resolved if the distance between the two maxima of the PSFs is equal or bigger than the distance between the maximum of a PSF with the first minimum

NIF Optical Seminar Jan 16th 2019 - Aurelien Objectives: why you don’t put oil on certain objectives…. Numerical aperture Snell’s law

NA = n sin α n1 sinθ1 = n2 sinθ2

n2 ~ 1 n2 ~ 1.5

n1 ~ 1.5 n1 ~ 1.5

NIF Optical Seminar Jan 16th 2019 - Aurelien Objectives: coverslips choice. Spoiler alert should be #1.5 (170 μm)

correction ring

The index of refraction of glass and oil is not equal. The thicker the glass the more aberrations. Most objectives are designed for 170 μm glass and you can play with the correction collar to improve the contrast of your image.

NIF Optical Seminar Jan 16th 2019 - Aurelien Objectives: working distance for in vivo and ephys people.

α working distance f n (w.d.) (f)

f = nominal tubelens focal length / nominal magnification Ex: Olympus LUMPlanFln, W f = 180 / 40 = 4.5 mm w.d. = 3.3 mm

NIF Optical Seminar Jan 16th 2019 - Aurelien Objectives: aberrations

Planapochromat: max degree of aberration correction – spherical and chromatic- correction (4 colors) - Planapo The tubelens might Planfluorite: less corrected (4 colors) - PlanFl contribute to aberration compensation Planoachromat: less corrected (3 colors) - Plan NIF Optical Seminar Jan 16th 2019 - Aurelien Objectives: chromatic and spherical aberrations.

NIF Optical Seminar Jan 16th 2019 - Aurelien Objective and Tube lens

f fT M  T fO

Changing fT, M changes too!

http://www.microscopyu.com/articles/optics/cfintro.html fO http://www.olympusmicro.com/primer/anatomy/tubelength.html

NIF Optical Seminar Jan 16th 2019 - Aurelien Trans illumination through eye piece

S sample plane S S

fCL fCL fF fF fCO fCO fO ∞ fT fE

? eyepiece fieldlens objective tube lens tube lightsource collectorlens condenserlens fielddiaphragm aperture diaphragmaperture final image in the retinaimage finalthe in intermediateimagingplane NIF Optical Seminar Jan 16th 2019 - Aurelien Trans illumination with a camera

S sample plane S

fCL fCL fF fF fCO fCO fO ∞ fT fieldlens objective tube lens tube lightsource collectorlens condenserlens fielddiaphragm aperture diaphragmaperture intermediateimagingplane NIF Optical Seminar Jan 16th 2019 - Aurelien Fluorescence

NIF Optical Seminar Jan 16th 2019 - Aurelien Fluorescence scales

Glutamate Ribosome PSD-95 actin

NIF Optical Seminar Jan 16th 2019 - Aurelien Fluorescence: parameter space

Efficiency of fluorophores depend on 2 main parameters: • Extinction coefficient: how much light can be absorbed at a wavelength • Quantum yield: how many photons are emitted vs how many are absorbed

Those two factors will determine the fluorophore’s brightness. Other parameters such as pH, temperature can also influence the brightness observed.

Excitation from ground state to an excited state can happen in a single step or multiple steps (single or multi photon excitation)

NIF Optical Seminar Jan 16th 2019 - Aurelien Pros and cons of fluorescence

• Excellent SNR (theoretically) • Large number of fluorophores available • Usually up to 4 lines/colors at the same time • Can use the properties for more specialized microscopy such as FRET, FLIM, FRAP….

• No correlation between fluorophore intensities • Bleaching and dark state. • Phototoxicity • Autofluorescence (especially in tissue)

NIF Optical Seminar Jan 16th 2019 - Aurelien Bleaching

NIF Optical Seminar Jan 16th 2019 - Aurelien Fluorescence selection in a microscope

A filter set is composed of: • Excitation filter: to limit the wavelengths reaching your sample. • Emission filter: to only collect the emitted wavelengths you’re interested in • Dichroic mirror that reflects certain wavelengths and let others pass through

NIF Optical Seminar Jan 16th 2019 - Aurelien Fpbase and filter choices

Created and maintained by Talley Lambert To help you choose filters for your here at HMS fluorophores www.fpbase.org www.semrock.com

NIF Optical Seminar Jan 16th 2019 - Aurelien Beyond the tube lens: detection

NIF Optical Seminar Jan 16th 2019 - Aurelien Ressources: • microscopyU • Olympus microscopy resource center • Leica Science lab

Next week: • comparison between scopes • discussion of specific illuminators and detectors • Scan heads

NIF Optical Seminar Jan 16th 2019 - Aurelien