multiphoton deep imaging of the mouse brain€¦ · tissue scattering is the main limitation in...
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![Page 1: Multiphoton Deep Imaging of the Mouse Brain€¦ · Tissue scattering is the main limitation in deep imaging! Scattering decreases the excitation photons at the focal volume (exponential](https://reader030.vdocument.in/reader030/viewer/2022040916/5e8f36ad981a201b686d86e7/html5/thumbnails/1.jpg)
Multiphoton Deep Imaging of the Mouse Brain
Chris Xu School of Applied and Engineering Physics
Cornell University
Deep tissue imaging Multiphoton endoscopy Fiber optics
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Acknowledgments PhD students: !Tianyu Wang!
! !Mengran Wang!! !Evan Yu!! !Fei Xia!! !Kriti Charan!! !Michael Buttolph!! !Najva Akbari!
!MS Student: !Mahailo Rebec!!Senior research associate: Dimitre Ouzounov!
! !post-doc: David Sinefeld!! !post-doc: Bo Li!
!
!!!
!
! ! !! !
Collaborators: Chris Schaffer Nozomi Nishimura Frank Wise Tom Bifano (BU) Charles Lin (Harvard) David Tank (Princeton) Na Ji (Janelia Farm) Andreas Tolias (Baylor) Companies: OFS-Fitel (Denmark) NKT Photonics (Denmark) Calmar Lasers Newport NIH: DARPA:
U01NS090530 W911NF-14-1-0012 R01EB014873 R01EB017274 R21EY026391 R21EB017339
Meyer Cancer Center Cornell CCMR Kavli Foundation
IARPA MICrONS
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E=mc2
a few neurons
108 neurons
1011 neurons
fMRI
?
Need new tools to build the bridge
1 transistor
The difficulty of understanding the brain
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The need for in vivo deep tissue imaging
mouse brain (108 neurons)
10 mm
102 neurons
0.2 mm
105 to 106 neurons
1 mm
High temporal (> 10 Hz) and spatial (< 1 µm) resolution , deep (> 1 mm), and large scale (> 1 mm3) imaging, within scattering brain tissue, is a major scientific challenging.
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TransparentbrainIsrela.velyeasier.
Camera does not work in scattering sample.
tissue scattering and
parallel data acquisition?
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Scattering limits high resolution optical imaging!
Mouse brain in vivo under a regular light microscope Think about looking through Tofu or cheese… Absorption, Scattering, Inhomogeneity
Multiphoton microscopy for deep brain imaging! ! ! !!
Denk, Strickler, and Webb 1990!
with diffuser in front of lens
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Multiphoton fluorescence excitation Excited State f
Ground State i
hv
1hv
hv
Intermediate State j
16 -17 2~ 10 to 10 /if cm photonσ −One-photon cross section:
49 42 ~ 10 / (or 10 GM)ij jf j cm s photonσ σ σ τ −=Two-photon cross section:
Femtosecond pulsed excitation is typically required.
T=1/f
τ1two-photon signal ( )f τ −∝ •
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Multiphoton Fluorescence Microscopy (1) nonlinear and (2) longer wavelength
Fluorescein molecule!
Green fluorescence!
hv!
1-photon blue excitation!
hv!
1-photon excitation
Fluorescence
2-photon excitation
2-photon red excitation!
2hv!
Green fluorescence!
hv!
Fluorescence
Denk, Strickler, and Webb 1990
λ (nm) 400 500 600 700 800
2PE ∝ I 2
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One Photon Two Photon
Fluorescein solution
focal plane focal plane
Signal I∝ 2Signal I∝
3D scanning of the focal spot to form a 3D image.
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Confocal microscopy does not work well in thick scattering sample.!
Non-scattering specimen
Scattering specimen
confocal aperture confocal aperture detector
Multiphoton microscopy works well with scattering sample. Deep tissue, high resolution imaging is the advantage of MPM.
Multiphoton microscopy (MPM) in thick scattering tissue!
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Nonlinear excitation enables a sharp focus in 3D!
in a scattering environment.!
Multiphoton microscopy (MPM) in thick scattering tissue!
No inverse scattering is necessary as long as a sharp focus can
be formed.
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Tissue scattering is the main limitation in deep imaging!
Scattering decreases the excitation photons at the focal volume (exponential decay of S)!
With Scattering
> 105
Exponential decay of signal!
Mouse brain vasculature
Signal ∝ exp(−2 i z / ls )
• Signal-to-noise ratio problem: intrinsic quantum noise of photons • Photon shot noise limit
• Signal-to-background problem: no longer able to form a sharp focus • Inverse scattering problem (want to avoid)
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Signal-to-background ratio in scattering tissue
Theer, P. et al, Opt. Lett., 2003
2~ ~ exp( 2 / )sSignalSBR z z l
Background−
Fluorescence vs depth z
z
Signal
Background
ls = scattering length
Excitation power vs depth z
Scattering specimen
0( ) ~ exp( / )sP z P z l−
z
Strategy: reduce scattering AND increase excitation confinement
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long wavelength for reducing excitation attenuation in brain
400 600 800 1000 1200 1400 1600 1800 2000 Wavelength (nm)
scattering coefficient (1/mm)
0
5
10
(b)
0
5
10
(c)
effective attenuation coefficient (1/mm)
scattering dominate
*
* *
1 1/ 1/a s
effective attenuation lengthl l
=+
/ / a sz l z lexcitation power e e− −∝
1 1/ 1/a s
imaging depthl l
∝+
Optimum wavelength is a trade-off between absorption and scattering.
1300 nm and 1700 nm windows.
J. Biomed. Opt. 16, 106014 (2011) Nature Photonics, 7, 205–209, 2013
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Fluorophores for the long wavelength spectral windows
Fluorophores for 2-photon excitation at 1300 nm and 1700 nm ~ very few!
Excited State f
Ground State i
Long wavelength is not practical for 2-photon excitation.
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Fluorophores for the long wavelength spectral windows
Fluorophores for two-photon excitation at 1300 nm and 1700 nm ~ very few!
Excited State f
Ground State i
What about three-photon excitation (3PE)?
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Fluorophores for the 1300 and 1700 nm spectral windows for 3-photon excitation
Fluorescent proteins 1PE (nm)
Fluorescence emission
Possible 3PE (nm)
Orange (mOrange, mKO) 548 560 1645
tdTomato, Ds-red 555 583 1665
Red (mCherry, J-red) 585 610 1755
Far-red 590 650 1770
All orange and red dyes for 3PE at ~ 1700 nm.
Long wavelength spectral windows
3-photon excitation
3PE of blue and green fluorophores, GFPs, and GCaMPs at 1300 nm.
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22 1/PE z∝
43 1/PE z∝
Axial fluorescence profile in non-scattering sample
3-photon excitation reduces out-of-focus background, and improves the 3D confinement
focal plane
2Signal I∝
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3PE provides better 3D confinement in scattering tissue
22 1/PE z∝
43 1/PE z∝
2PE 3PE
Axial fluorescence profile with tissue scattering
orders of magnitude improvement in SBR.
Better 3D confinement leads to better tissue penetration.
2PE
3PE
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2P at 920 nm 3P at 1300 nm Transgenic mouse with GCaMP6s
2P at 920 nm 3P at 1300 nm
3-photon imaging has vastly improved SBR for deep imaging in non-sparsely labeled brain.
Fluorescein labeled brain vasculature
Between 700 and 800 µm: SBR for 2P < 1.0 At 1060 µm depth (below the white matter): SBR for 3P > 20
2P SBR
3P SBR
Manuscript in preparation
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In vivo 3-photon imaging of red fluorescent protein (RFP) labeled neurons beyond white matter
Maximum power at the sample is ~ 22 mW.
Red: RFP fluorescence Blue: THG
1700 nm
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In vivo 3-photon imaging of RFP neurons beyond white matter
Brainbow mouse
Nature Photonics, 7, 205–209, 2013 CLEO 2012, postdeadline paper, CTh5C.4.
third harmonic generation of myelinated axons
fluorescence of neurons
SP at ~1.1 mm
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In vivo imaging through unthinned, intact mouse skull
Green: THG Red: fluorescence Manuscript in preparation
skull
brain
3-photon imaging at 1700 nm
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In vivo imaging of brain function!
• Ca-imaging for recording neuronal activity in vivo!✦ Organic dyes!✦ Genetically engineered fluorescent protein probes!
✦ Green fluorescence protein Ca-probes (GCaMPs) (3-photon excitation at 1300 nm)!
✦ Red fluorescent protein based Ca-probes (RCaMP) (3-photon excitation at 1700 nm) !!
!
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FOV = 300 µm x 300 µm Frame Rate = 8.49Hz Frame Size = 256 x 256 pixels Mouse: 16 weeks old Power = 36 mW at 800kHz (Newport Spirit-NOPA)
Imaging spontaneous activity of deep L6 neurons GCaMP6 at 1300 nm
(single trial measurement) 10 min movie, sped up by 60x THG + GCaMP fluorescence
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Low pass filtered ΔF/F vs time
Raw data in photons/neuron/frame (recorded at 8.49 frames/s)
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Imaging the brain activity of an entire mouse cortical column (Somatosensory Cortex L1 to L6 of a densely labeled transgenic mouse)
Field-of-view (FOV) 235 µm at 8.49 frames/s Power: 4.1 mW at 130 µm and 20.5 mW at 800 µm Green: Fluorescence Magenta: Third Harmonic Generation (THG)
CamKII-tTA/GCaMP6s Densely labeled transgenic mouse provided by Tolias and Reimer at Baylor Medical College
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1.0 mm
EC
neocortex
hippocamp
us
3-photon imaging of spontaneous activity in hippocampus within an intact mouse brain
Imaging the hippocampus is much harder because the white matter is much more scattering than the grey matter (appears to be ~ 2.5x) !!
Scattering length in mouse brain at 1700 nm
le ~ 366 µm for grey matter le ~ 140 µm for white matter
le ~ 310 µm for hippocampus
white matter
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In vivo imaging of hippocampal neurons within an intact mouse brain
Using 3-photon excitation of GCaMP6s at 1300 nm
Purple = Third harmonic generation Green = GCaMP6s fluorescence FOV = 400 µm x 400 µm (Newport Spirit-NOPA)
SP layer
Nature Methods (2017) doi:10.1038/nmeth.4183
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17-week old mouse FOV = 200 µm x 200 µm Frame rate = 8.49 Hz power ~ 50 mW at 800 KHz repetition rate
Imaging spontaneous activity in hippocampus within an intact mouse brain (Single trial measurement)
3-photon excitation of GCaMP6s at 1300 nm
15-minute movie segment of 48-min total recording, sped up by 60x
Watch mouse thinking, deeply Depth = 984 µm
20 µm
Imaged the same mouse multiple times over a period of several weeks.
20 µm
Nature Methods (2017) doi:10.1038/nmeth.4183
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Raw data in photons/neuron/frame (recorded at 8.49 frames/s)
Activity imaging of mouse hippocampus (single trial measurement)
Watch mouse thinking, deeply and quantitatively
.
.
Nature Methods, in press
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Activity imaging in hippocampus High spatial resolution and contrast: nucleus exclusion is clearly visible
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How to go forward from here?
(1) Excitation source (2x to 3x) (2) Adaptive optics (3) Other possibilities
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perfect focus
tissue heterogeneity
Adaptive optics (AO) may be the low hanging fruit.
AO should have larger impact for 3-photon imaging. AO should have larger impact for deep imaging.
spatial light modulator (SLM) wavefront engineering plane wave input
aberration
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Impact of adaptive optics (AO) on multiphoton imaging AO correction for the same 2-m focal length cylindrical lens at objective back pupil
2-photon
4-photon
3-photon
AO has order(s) of magnitude more impact for higher-order excitation! Opt. Exp., Vol. 23, pp. 31472-31483, 2015
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Correc(onPhasemap
10μm
10μm
Phase error ∝ Δn
λ
(a)
(b)
AO for in vivo 3-photon imaging of RFP-labeled neurons at 1000 µm depth
10μm
10μm
(1)
(2)
(1)
(2)
ratio=1.8899 Signal=0.036137 Iteration=195
5 10 15 20 25 30
5
10
15
20
25
30
Low-order correction provides a large field-of-view.
With AO
Without AO
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Correction phase maps at different imaging depths ratio=1.8899 Signal=0.036137 Iteration=195
5 10 15 20 25 30
5
10
15
20
25
30
1000μm
ratio=1.7719 Signal=0.054501 Iteration=195
5 10 15 20 25 30
5
10
15
20
25
30
200μm
ratio=2.2177 Signal=0.10351 Iteration=195
5 10 15 20 25 30
5
10
15
20
25
30
400μm
ratio=1.528 Signal=0.088564 Iteration=195
5 10 15 20 25 30
5
10
15
20
25
30
600μm
Correcting aberration caused by brain tissue, not by imaging system.
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10!m 10!m
We are pushing the depth limit using AO for 3P.
No AO correction After AO correction (gain ~ 5x)
AO should have larger impact for deep imaging. AO should have larger impact for 3-photon imaging. But longer wavelength reduces the AO impact…
1700 nm 3PE of RFP-labeled neurons in Brainbow mouse at 1530 µm depth.
Manuscript in preparation
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But what are we compensating?
RFP fluorescence from Brainbow mouse
Aberration scattering
Perhaps easier and more practical.
x x
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Depth = 984 µm
~ 2 orders of magnitude improvement seems possible. (~ within a few years)
With the optimized laser, AO, smart scanning,
What else?
Only imaging the neurons (~ 10x)
But how to do it?
What about motion in vivo?
20 µm
100x more neurons OR another ~ 400 µm in depth.
How to go beyond ~ 2 mm in mouse brain???
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Really difficult:
increase excitation cross sections of fluorescent probes Need chemist and protein engineers, but have been tried for the last 20 years
Brave new world:
Tissue clearing of living brain with adaptive illumination
Tissue clearing of living brain using clearing materials
The dream
µeff = 3µa (µs' + µa ) ≈ 3µaµs
'Absorption limit: > 0.5 mm-1
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PushingtheLimitsofOp.calBrainImaging • Long wavelength and 3-photon imaging is superior for
deep penetration. – 3-photon microscopy of hippocampal structure and function – Through skull imaging Particularly suited for deep and densely labeled volume imaging
• Improvement of orders magnitude may be possible
– Optimization of excitation source (2x to 3x) – Adaptive optics (~ 5x) – Smart scanning (~10x)
– Increase probe performance (cross section, wavelength, etc.), tissue clearing with chemical or with smart light…
Increasing difficulty
Chris Xu