compensation the process of correcting for flourescence crosstalk

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Compensation The process of correcting for flourescence crosstalk

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Compensation The process of correcting for flourescence crosstalk. History of compensation by traditional flow cytometry Compensating Image Stream Data Troubleshooting compensation in IDEAS. Why is compensation necessary?. Broad emmision spectra - PowerPoint PPT Presentation

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Page 1: Compensation The process of correcting for flourescence crosstalk

CompensationThe process of correcting for flourescence crosstalk

Page 2: Compensation The process of correcting for flourescence crosstalk

AMNIS CORPORATION-Compensation

• History of compensation by traditional flow cytometry

• Compensating Image Stream Data

• Troubleshooting compensation in IDEAS

Page 3: Compensation The process of correcting for flourescence crosstalk

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Why is compensation necessary?

• Broad emmision spectra

• Imperfections in fluorescence filtering cause leakage into other channels

• Tandem conjugates

Page 4: Compensation The process of correcting for flourescence crosstalk

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The electromagnetic spectrum

Page 5: Compensation The process of correcting for flourescence crosstalk

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Resonance Energy Transfer

Resonance energy transfer is distance dependent and occurs without radiant release from the donor molecule

Page 6: Compensation The process of correcting for flourescence crosstalk

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Spectral overlap

Page 7: Compensation The process of correcting for flourescence crosstalk

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Band Pass Filters

Filters with transmission that is high for a particular band of frequencies, but that falls to low values above and/or below this band

Page 8: Compensation The process of correcting for flourescence crosstalk

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Beam splitter• A beam splitter is an optical device that splits a beam of

light in two.

• A dichroic mirror is a type of beam splitter that is able to split light of different wavelengths.

Page 9: Compensation The process of correcting for flourescence crosstalk

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Traditional flow cytometer flow cell

BD FACSCalibur Optics

Page 10: Compensation The process of correcting for flourescence crosstalk

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The ImageStream® SystemCh1470-

500nm

Ch2400-

470nm

Ch3500-

560nm

Ch4560-

595nm

Ch5595-

660nm

Ch6660-

730nmtdiSynchCW2.mov Frame.mov

Page 11: Compensation The process of correcting for flourescence crosstalk

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Post Mag Lens

Deep Blue Corrector

Spectral Decomposition

Stack

Petzval Lens Sets

Field Lens

Objective &

Quartz Cuvette

Spectral Decomposition6 Spectral Channels 488-505nm Scatter 560-595nm PE 400-470nm DAPI 595-660nm PI, 7-AAD 505-560nm FITC 660-730nm Cy5, DRAQ5

0.3 degree separation per channel

Page 12: Compensation The process of correcting for flourescence crosstalk

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Flourescence Microscopy•The fluorescent microscope utilizes filter cubes that narrow the wavelenth of excitation and emission designed specifically for each fluorochrome.

•Fluorescence microscopes typically do not apply compensation because each color is taken with a different set of optimized filters.

From SemRock

Page 13: Compensation The process of correcting for flourescence crosstalk

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The crosstalk can be quantified and corrected

Givans

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Compensation of flow data during acquisition

Figures from BD FACS Academy

Page 15: Compensation The process of correcting for flourescence crosstalk

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Formula for traditional compensation

D1 = 1F1+ 2F1 +3F1 +…nF1

D2 = 1F2+ 2F2 +3F2 +…nF2

Dn = 1Fn+ 2Fn +3Fn +…nFn

xFn = the amount of signal in detector n that originates from fluorophore x

Dn = the measured signal in detector n

For each detector D=the sum of fluorescence from each fluorophore

A matrix is defined such that each detector measured value is the sum of the peak fluorescence plus the spillover amount from every other fluorochrome.The matrix is used to remove the contribution of the non-peak fluorochrome. This gives you the ‘true’ value for the peak fluorochrome.

Page 16: Compensation The process of correcting for flourescence crosstalk

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Factors affecting matrixes

• Crosstalk is fluorochrome specific

• Tandem conjugates can have dual band fluorescence due to the inefficiency of RET to the acceptor or degradation of the conjugate

• Bright vs Dim fluorescence

• Autofluorescence is cell specific

Page 17: Compensation The process of correcting for flourescence crosstalk

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Compensation of dim to bright cells

Page 18: Compensation The process of correcting for flourescence crosstalk

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BD Fluorescence Spectrum Viewer

Page 19: Compensation The process of correcting for flourescence crosstalk

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BD Fluorescence Spectrum Viewer

Page 20: Compensation The process of correcting for flourescence crosstalk

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BD Fluorescence Spectrum Viewer

Page 21: Compensation The process of correcting for flourescence crosstalk

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Single color control samples used to calculate a 6x6 matrix.Post-acquisition compensation is applied to images on a pixel by pixel basis in IDEAS.

Spectral Compensation

3_Intensity1000 1e4 1e5

1000

1e4

1e5

1e6

3_Intensity

4_In

tens

ity

Un-compensated

5_Intensity1000 1e4 1e5 1e6

01000

1e4

1e5

1e6

5_Intensity

6_In

tens

ity

Un-compensated

3_Intensity-1000 0 1000 1e4 1e5

-10000

1000

1e4

1e5

1e6

3_Intensity

4_In

tens

ity

Compensated

5_Intensity-1000 0 1000 1e4 1e5

-10000

1000

1e4

1e5

1e6

5_Intensity

6_In

tens

ity

Compensated

SSC Brightfield FITC PE PE-Alexa610 Draq-5

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Compensating ImageStream data pixel by pixel• Corrections are applied before spectral compensation.

• ASSIST values are used for:• 1.Darkcurrent correction• 2.Brightfield gain correction• 3.Spatial registration

Brightfield compensation is done using the background around the objects and is automatically computed and applied when the data file is loaded in IDEAS.

Single fluorochrome compensation control files are used for fluorescence crosstalk compensation.

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Pixelated Imagery

0

25

35

40

Dark Current

SpectralOverlap

Signal

Green Channel Orange Channel Red Channel

Read Out 1023 1023 1023500 500 800 700 800 500 800 5007001023

1000 1000 1000475 475 775 675 775 475 775 475675

SpectralOverlap

Signal

950 950 950425 425 725 625 725 425 725 425625

Signal

Dark Current Correction Spectral Compensation

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Darkcurrent correction

• Each pixel on a CCD detector has a characteristic baseline output known as dark current offset.

Page 25: Compensation The process of correcting for flourescence crosstalk

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Brightfield gain correction

• Each pixel on a CCD detector has a characteristic responsivity to light exposure, known as the pixel gain.

Page 26: Compensation The process of correcting for flourescence crosstalk

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Spatial registration

• Spatial registration errors between image channels is measured by imaging the same object (SpeedBead) in all 6 channels simultaneously and comparing the location of the images.

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IDEAS Tools

• The corrections are available to the user in IDEAS during data analysis.

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Spectral Compensation: Matrix Development Cross talk matrix is determined by calculating best fit linear regression for each dye into

each channel. Slope of linear regression is matrix coefficient. A 6x6 martix of linear equations is solved for each pixel in every image to remove cross talked light.

5_Intensity1000 1e4 1e5 1e6

01000

1e4

1e5

1e6

5_Intensity

6_In

tens

ity

Un-compensated

3_Intensity1000 1e4 1e5

1000

1e4

1e5

1e6

3_Intensity

4_In

tens

ity

Un-compensated

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Potential pitfalls to watch for

• Saturation• Mis-alignment• Coefficients calculated on poorly fit lines• Autoflourescence• Camera staging

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Misalignment

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Saturation

• Saturation occurs when the pixel can no longer quantify the available light.

• The 10 bit detector provides 1024 bins and once 1023 is reached the pixel can no longer quantify the signal and compensation becomes impossible.

• • It is therefore critical that events with saturated pixels be eliminated

• During data acquisition the laser power, camera sensitivity and cell classifiers are used to reduce saturation

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Saturation

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Undercompensation due to saturated pixels…

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Staging the camera

z

128 FWD Stage Selection

32 FWD Stage Selection8 Stage Selection

Active Channel96 pixels wide by

512 tallX6

Inactive Region12 pixels wide by

512 tallX6

Single or multitap readout register suitable for 50KHz line rate18 tap register suitable for 400KHz line rate

Active Channel96 pixels wide

by512 pixels tall

X6

Inactive area12 pixels wide

byX6

256 FWD Stage Selection

• Charged Coupled Device

Page 35: Compensation The process of correcting for flourescence crosstalk

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Properly compensated single color controls

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Mis-compensated single color controls

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Compensation variation with laser power

• Jurkat cells stained with NFkB FITC were run in the absence of brightfield and a 1000 images were collected with 488 laser excitation ranging from 20mw to 200mw at 20mw increments. Compensation values were calculated in IDEAS graphed over changing laser power. Compensation variation with increasing laser power shows little to no correlation to changing laser power.

Compensation Variation with Laser power

-0.05

0.25

0.55

0.85

20 40 60 80 100 120 140 160 180 200

488 excitation in mw

% C

ompe

nsat

ion FITC into Channel 1

FITC into Channel 2

FITC into Channel 3

FITC into Channel 4

FITC into Channel 5

FITC into Channel 6

Page 38: Compensation The process of correcting for flourescence crosstalk

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20 mw positive 20 mw Blank

100 mw positive 100 mw Blank

200 mw positive 200 mw Blank

Compensation variation with laser power

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Two methods for calculating the matrix

• The Means method is used for uniform objects like beads.

• The Best Fit is used for objects that have a varied level of fluorescence.

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Coefficient error

• Check the matrix

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IDEAS Compensation

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Workflow• Collect files of single color fluorescent controls with brightfield turned off

• Open IDEAS and start a New Matrix under compensation

• Add the single color control files to the analysis (open and load files)

• Select the single cells using the scatter area vs. aspect ratio dot plot to use as the compensation population

• Assign the positive populations to the appropriate channels

• Create the compensation matrix

• Validate the matrix

• Save the matrix

• Use the matrix to open data files

Page 43: Compensation The process of correcting for flourescence crosstalk

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Go forth and compensate!

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Page 46: Compensation The process of correcting for flourescence crosstalk

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• Two channels of interest X and Y• Compute the variance of X (VarX), variance of Y (VarY) and the

covariance of X and Y (CovXY). CovXY measures the degree to which 2 values vary together

• Define a 2 x 2 matrix:

• Eigen Value =

• The major Eigen value is the positive value• Slope =

Calculating the compensation matrix

VarYCovXYCovXYVarX

Eigen values can be found for square symmetric matrices. There are as many eigen values as there rows (or columns) in the matrix. Conceptually they can be considered to measure the strength (relative length) of an axis (dervied from the square symmetric matrix). Each eigen value has an associated eigen vector. An eigen value is the length of an axis, the eigen vector determines its orientation in space.

4

)(*2

22 VarYVarXCovXYVarYVarXVarYVarX

CovXYVarXvalueeigenmajor )(

Page 47: Compensation The process of correcting for flourescence crosstalk

AMNIS CORPORATION-Compensation

Pixelated Imagery

1023

0

25

35

40

Dark Current

SpectralOverlap

Signal

Green Channel Orange Channel Red Channel

Read Out 1023 1023 1023500 500 800 700 800 500 800 500700