Title: Advanced PhaseBased Segmentation of Multiple Cells from Brightfield Microscopy Images
1Advanced Phase-Based Segmentation of Multiple
Cells from Brightfield Microscopy Images Rehan
Ali Wolfson Medical Vision Laboratory, Department
of Engineering Science, University of Oxford
2Overview
- The case for brightfield image processing
- Considering different forms of spatially variant
phase - Physical Phase
- Image / Local Phase
- Our segmentation framework
- Results
- Limitations and future extensions
3Anatomical vs Functional Imaging
- Medical image processing relies on multi-modal
approach for jointly analysing anatomic and
functional data - This is rare in microscopy image processing! Most
work done directly on fluorescence images - Brightfield offers detailed anatomic information
but suffers from poor contrast - Accurate boundary delineation for quantitative
analysis of intracellular fluorescent data is
best done on anatomic data
CT (left) and PET (right) images from
www.dana-farber.org
Three cells in a brightfield (left) and
fluorescence (right) image
4Improving Contrast
- Manual defocus
- Most common as non-enhanced brightfield is most
widely available form of microscope - Hardware Enhancement
- Zernike Phase Contrast
- Differential Interference Contrast
- Software Enhancement
- Phase Recovery
Digital phase recovery images from
www.iatia.com.au
Image from www.microscopyu.com
Image from www.microscopyu.com
5Effects of Physical Phase when Defocusing
?z - 2µm
?z - 8µm
?z -100µm
?z 0µmIn Focus
?z 2µm
?z 8µm
?z 100µm
6Defocusing Theory
- Transport of Intensity equation can be derived
from the time-independent wave equation - Defines laplacian relation between z-axis
intensity derivative and physical phase
7Phase Recovery
- Quantitative Phase Microscopy (QPM, Iatia)
proposes a FFT-based solution to TIE, to recover
phase (Barty et al, 1998) - Problems
- Low frequency artefacts
- May not recover very thin cell body regions
Brightfield Image
QPM result
8Image / Local Phase
- Intensity-independent feature detector used in
medical imaging - Basis is the analytic signal used in 1D signal
processing - Allows computation of odd and even quadrature
filters - These respond to odd and even features in
bandpassed signals - Local phase is the ratio of filter response to
feature symmetry? describes type of feature - Local energy is the magnitude of filter responses
? describes strength of feature - Monogenic signal representation extends this to
nD by allowing computation of nD-specific QFs
Odd
Even
Blue signal after DoG bandpass filtering Red
signal after filtering with HT of DoG
9Monogenic Signal
Quadrature Filters Odd h1(x,y) Ib(x,y) h2(x,y)
Ib(x,y)
Bandpass Filter Even Ib(x,y) I(x,y)b(x,y)
Not useful in low contrast cases
Diff of Gaussians Bandpass, Spatial
Domain Normally zero-DC
10Monogenic Signal Results w Bandpass Filter
?I/ ?z
Local Phase ? -p to p
Local Orientation F -p to p (points in
direction of max signal variance)
11Results with Non-Zero DC Lowpass Filter
?I/ ?z
Local Phase ? -p to p
Local Orientation F -p to p (points in
direction of max signal variance)
12Level Set
- Use narrowband Level Set framework for multiple
object segmentation - Use local phase and local orientation based terms
in speed function
13Local Orientation Term
14Segmentation Overview
Initialisation
Inputs
I(x,y,dz)
Local Phase
Initial Class Map
?I/ ?z
I(x,y,-dz)
Local Orient
User clicks on cells
Physical Phase
Requires motorised z-axis stage to capture /- z
images Cells must be fixed / stationary during
defocus image acquisition (e.g. adherent)
Monogenic Signal
Split up cells(region growing)
Level Set
15Validation vs Manual Segmentation
AlgorithmManual
16Current Issues
- Automatic Initialisation required for HT analysis
- Use a strongly defocused image
- Use a specific fluorescence image
- Use texture from in-focus image
- Method struggles with ultra-thin cell body
regions - Parameter tuning required to obtain good results
17Summary
- Segmentation of anatomical cell features is
ideally done on an anatomical image (e.g.
brightfield) - Information can be extracted from difficult
images using one or combination of techniques - Physical phase models of image formation
- Image signal analysis with local phase
- Code now available for Windows / Linux at
www.sephace.com
18www.sephace.com
19Acknowledgements
- Wolfson Medical Vision Labs
- Professor Sir Michael Brady FRS FREng
- Dr Mark Gooding
- Dr Weiwei Zhang
- Nathan Cahill
- Gray Cancer Institute
- Dr Martin Christlieb
- Life Sciences Interface Doctoral Training
Centre,University of Oxford - EPSRC UK for funding