Automated tissue type imaging with OCT Ton van Leeuwen DJ Faber, DM - - PowerPoint PPT Presentation

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Automated tissue type imaging with OCT Ton van Leeuwen DJ Faber, DM - - PowerPoint PPT Presentation

Automated tissue type imaging with OCT Ton van Leeuwen DJ Faber, DM de Bruin, NM Weiss, DV Nguyen, SM Jansen, M Almasian, AL Post, L Wilk, MCG Aalders, Berrend Muller, A Swaan (AMC), X Attendu (PolyMtl), J Kalkman (TUD) Academic Medical Center,


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Automated tissue type imaging with OCT

Ton van Leeuwen

DJ Faber, DM de Bruin, NM Weiss, DV Nguyen, SM Jansen, M Almasian, AL Post, L Wilk, MCG Aalders, Berrend Muller, A Swaan (AMC), X Attendu (PolyMtl), J Kalkman (TUD) Academic Medical Center, University of Amsterdam, Biomedical Engineering & Physics: T.G.vanLeeuwen@amc.uva.nl www.amc.nl/BMEP

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Gustav Strijkers Ed van Bavel Henk Marquering Maurice Aalders

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  • Physics of

– Interaction of light with tissue – Development of instrumentation

  • Application of light

– Therapeutic – Diagnostic

  • Monitoring / function
  • Imaging / morphology

Optical imaging and sensing of functioning biological systems (cells/organs) Relation between optical properties (µa, µs, g) and status of the tissue or tissue type

introduction dependent scattering multiple scattering conclusion

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SLIDE 4

OCT is the “Harlem Oil” of Biomedical Optics

introduction dependent scattering multiple scattering conclusion

See http://www.haarlemmerolie.nl

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SLIDE 5

One drop of OCT solves all the problems…

introduction dependent scattering multiple scattering conclusion

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SLIDE 6

Velocity (mm/sec)

What kind of tissue are we looking at?

introduction dependent scattering multiple scattering conclusion

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SLIDE 7

One drop of OCT solves all the problems…

introduction dependent scattering multiple scattering conclusion

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SLIDE 8
  • OCT signal dependent on:

– Depth of focus – Position of the focus – Amount of back scattering – Attenuation coefficient

( ) ( )

z P P z h c zn z i

s NA b sample ref med

µ µ g h 2 exp ) ( 2 Re

, det

  • Ä

þ ý ü î í ì ÷ ø ö ç è æ =

DJ Faber, et al.Optics Express 2004, 12: 4353-4365

introduction dependent scattering multiple scattering conclusion

Single scattering approximation

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SLIDE 9
  • OCT signal dependent on:

– Depth of focus – Position of the focus – Amount of back scattering (amplitude of the OCT signal) – Attenuation coefficient

( ) ( )

z P P z h c zn z i

s NA b sample ref med

µ µ g h 2 exp ) ( 2 Re

, det

  • Ä

þ ý ü î í ì ÷ ø ö ç è æ =

800 nm OCT of rat aorta

introduction dependent scattering multiple scattering conclusion

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SLIDE 10
  • OCT signal dependent on:

– Depth of focus – Position of the focus – Amount of back scattering – Attenuation coefficient (‘slope’ of the OCT signal)

( ) ( )

z P P z h c zn z i

s NA b sample ref med

µ µ g h 2 exp ) ( 2 Re

, det

  • Ä

þ ý ü î í ì ÷ ø ö ç è æ =

Kodach et al, Biomedical Optics express 2010, Optics Express 2011

introduction dependent scattering multiple scattering conclusion

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SLIDE 11

Velocity (mm/sec)

application of µtextraction

Van der Meer et al, IEEE TMI, 2005, 24, 1369-1376 Lasers Med Science 2005, 20, 45-51

Cardiovascular tissues

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SLIDE 12
  • OCT signal dependent on:

– Depth of focus – Position of the focus – Amount of back scattering – Attenuation coefficient

( ) ( )

z P P z h c zn z i

s NA b sample ref med

µ µ g h 2 exp ) ( 2 Re

, det

  • Ä

þ ý ü î í ì ÷ ø ö ç è æ =

  • Is it so simple to measure !" (!$%& ≈ !")?
  • How to verify that (e.g. for large !")?

– !"~*+,*-,./0.1+, – !2~*+,*-,./0.1+, – !"~!2 –

34 35 = *+,7.0,.

introduction dependent scattering multiple scattering conclusion

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SLIDE 13

Velocity (mm/sec)

All μOCTfor Intralipid

  • @ 600, 800, 1300 & 1600 nm (single scattering model)

introduction dependent scattering multiple scattering conclusion

Why is the attenuation coefficient saturating for higher concentrations IL?

5 10 15 20 5 10 15 20 25 30

600 nm 800 nm 1300 nm 1600 nm scattering coefficient (mm

  • 1)

Intralipid concentration (%)

g » 0.8 g » 0.7 g » 0.3 g » 0.4

μOCT (mm-1)

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SLIDE 14

Velocity (mm/sec)

Dependent scattering for all beads

Corrected for dependent scattering with structure factor by Percus-Yevick model

μs for high concentrations

Nguyen et al Optics Express 2013

0.00 0.05 0.10 0.15 0.20 0.25 0.30 5 10 15 20 25 30 35 µs (mm

  • 1)

volume fraction

Æ 1215 nm Æ 906 nm Æ 759 nm Æ 0.376 nm

introduction dependent scattering multiple scattering conclusion

!" ≁ $%&$'&()*(+%&

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OCT signal analysis: amplitude

!" ~ $%&$'&()*(+%& Amplitude Amplitude

M Almasian, et al.J BiomOptics, 2015, 20: 121314

introduction dependent scattering multiple scattering conclusion

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SLIDE 16

OCT signal analysis: amplitude

back scattering coefficient/scattering coefficient

Mitra Almasian et al, Scientific Reports 2017

∅ ≈ # $% 2

introduction dependent scattering multiple scattering conclusion

'( ≁ '*

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Velocity (mm/sec)

  • Picking up multiple scattered light will reduce µOCT using

the single scattering model

  • higher scattering values, deeper into the tissue, dependent
  • n g and NA optics
  • Extended Huygens Fresnel (EHF) model

Effect of multiple scattering…

  • D. Levitz et al., Optics.Express 2004, 12, 249-259

( ) ( ) ( ) ( ) [ ] ( ) [ ]

2 1 2 2 2 2 2

exp 1 1 exp 1 exp 2 2 exp 1 ú û ù ê ë é

  • +

+

  • +
  • µ

s h s h s s s s h d

W W z W W z z z W z i µ µ µ µ

introduction dependent scattering multiple scattering conclusion

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SLIDE 18

Velocity (mm/sec)

OCT: dependent (PY) and multiple (EHF)scattering

Æ = 0.70 µm gMie+PY= 0.71-0.56 Æ = 0.47 µm gMie+PY= 0.39-0.06 Æ = 0.91 µm gMie+PY= 0.79-0.67 Æ = 1.6 µm gMie+PY= 0.91-0.87

introduction dependent scattering multiple scattering conclusion

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SLIDE 19

Velocity (mm/sec)

  • Blood, µOCT measured by 800 nm OCT

Effect of chosen (fixed) g in EHF model g = 0.995 g = 0.8

Spheres, Intralipid, g>0.8, so what?

Faber et al, OL 2009

introduction dependent scattering multiple scattering conclusion

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phantom B-scan plane Flow channel Solid TiO2 phantom Whole blood flow 400 μm channel, 20 mm/sec Solid TiO2 phantom

Forward scattering of blood

  • Whole blood flowing through

static sample: flow on!

SM Jansen et al, Sensors 2018

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Velocity (mm/sec)

  • Fitting both µOCT and g in EHF: no convergence
  • Setting g correctly results in:

Effect of NA (PSF) on µOCT

M Almasian, in progress

introduction dependent scattering multiple scattering conclusion

!" 13%& 20%& 51%& %* (&&,-) g %/01 (&&,-) %/01 (&&,-) %/01 (&&,-) 5.4 0.91 6 7 10 14 0.89 22 23 24 21 0.87 40 33 55

  • Better model needed?
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SLIDE 22

Velocity (mm/sec)

  • Fitted PSF (and Roll-of) for 4 C7 Dragonflytm

Intravascular Imaging Probe (St. Jude Medical,

  • St. Paul, Minnesota, USA)

But NA (PSF) is more or less constant..

introduction dependent scattering multiple scattering conclusion

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SLIDE 23

Velocity (mm/sec)

  • It is not as simple as Harlem Oil

– "# ≁ %&'%(')*+),&' – "- ~ %&'%(')*+),&' – "# ≁ "-

  • correctly fitted PSF (and Roll-of)

– NA can differ between catheters

  • If / ≾ 0.8: "567 ≈ "#

– For larger g, more multiple scattered light contributes to the OCT signal

  • automated tissue type imaging with OCT:

– be carefull – other contrast mechanisms – The eye…

Discussion

introduction dependent scattering multiple scattering conclusion

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SLIDE 24

Velocity (mm/sec)

What kind of tissue are we looking at?

introduction dependent scattering multiple scattering conclusion

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SLIDE 25

Velocity (mm/sec)

What kind of tissue are we looking at?

introduction dependent scattering multiple scattering conclusion

OCT during restauration of Rembrandt painting Marten at Rijksmuseum, see https://www.rijksmuseum.nl/nl/marten-en-oopjen

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SLIDE 26

Velocity (mm/sec)

  • It is not as simple as Harlem Oil

– "# ≁ %&'%(')*+),&' – "- ~ %&'%(')*+),&' – "# ≁ "-

  • correctly fitted PSF (and Roll-of)

– NA can differ between catheters

  • If / ≾ 0.8: "567 ≈ "#

– For larger g, more multiple scattered light contributes to the OCT signal

  • automated tissue type imaging with OCT:

– be carefull – other contrast mechanisms – The eye…

Discussion

introduction dependent scattering multiple scattering conclusion