An open-source LabView program that controls the instant FLIM system.
@article {InstantFLIM2020,
author = {Yide Zhang and Ian H. Guldner and Evan L. Nichols and David Benirschke and Cody J. Smith and Siyuan Zhang and Scott S. Howard},
journal = {Optica},
number = {6},
pages = {885--897},
publisher = {OSA},
title = {Instant FLIM enables 4D in vivo lifetime imaging of intact and injured zebrafish and mouse brains},
volume = {8},
month = {Jun},
year = {2021},
url = {http://www.osapublishing.org/optica/abstract.cfm?URI=optica-8-6-885},
doi = {10.1364/OPTICA.426870},
}
Instant-FLIM-Control is an open-source LabView program that permits full control of the instant FLIM hardware system. The program allows users to acquire, analyze, and export FLIM images based on the principle of instant FLIM. The program is fully open-source and highly modularized (see the screenshots of the source code below), so users with LabView programming skills can easily modify the code to customize existing functions or to add new functions.
-
Install LabView 2015 (or newer) on your computer.
-
Download or clone (git clone) this GitHub repository:
https://github.com/yzhang34/Instant-FLIM-Control.git
-
Open the project "Event-driven MPM-FLIM imaging platform.lvproj" in LabView and run the file "Main.vi" to execute the program:
This step is to establish the connection between the LabView software and the instant FLIM hardware. Use the pop-up menus in the "I/O" tab to configurate the input and output ports.
The current implentation of the program requires two NI DAQ cards that support NI-DAQmax.
-
Card 1, e.g., NI PCI-6110, should have at least 4 analog input (AI) channels and 2 ananlog output (AO) channels.
-
Card 2, e.g., NI PCIe-6323, should have at least 1 AI channel and 4 AO channels.
Note:
-
Card 1 and Card 2 should be synchronized using a Real-Time System Integration (RTSI) bus: https://www.ni.com/en-us/support/documentation/supplemental/18/real-time-system-integration--rtsi--and-configuration-explained.html
-
For a complete list of devices that support NI-DAQmx, please check: https://www.ni.com/pdf/manuals/374768ae.html
-
If you do not have cards with 4 AI + 2 AO or 1 AI + 4 AO channels, please contact me at [email protected]. I can provide other versions of the program that would work for your applications. However, you need to make sure that all your cards combined have at least 5 AI channels and 6 AO channels.
The following ports and channels should be configurated before running the program:
-
Mixer AI Channel(s)
- Configurate 4 AI channels of Card 1 (e.g., NI PCI-6110) to read the IF voltages of the four mixers in instant FLIM
-
AIStartTrigger
- Configurate ai/StartTrigger of Card 1 (e.g., NI PCI-6110) to synchronize with Card 2
-
Scan AO Channel(s)
- Configurate 2 AO channels of Card 1 (e.g., NI PCI-6110) to generate the controlling voltages for the galvo scanners (e.g., Thorlabs GVS002); AO1 and AO2 for fast and slow scanning axes, respectively
-
AOStartTrigger
- Configurate ao/StartTrigger of Card 1 (e.g., NI PCI-6110) to synchronize with Card 2
-
DC AI Channel(s)
- Configurate 1 AI channel of Card 2 (e.g., NI PCIe-6323) to read the DC voltage from the bias tee (i.e., the intensity signal) in instant FLIM
-
Bias AO Channel(s)
- Configurate 4 AO channels of Card 2 (e.g., NI PCIe-6323) to generate the bias voltages for the four phase shifters in instant FLIM
-
Stage VISA COM (Optional)
- Configurate the computer's COM port that connects to the motorized stage system (e.g., Prior OptiScan III)
- If not use a stage, uncheck "Use Stage?"
-
DM Resource Name (Optional)
- Configurate the USB resource name assigned to the deformable mirror (e.g., Thorlabs DMP40-P01) used in the optional adaptive optics system
- If not use a deformable mirror, uncheck "Use DM?"
-
Shutter Line (Optional)
- Configurate the digital output line (e.g., port0/line0) of a DAQ card (e.g., NI PCI-6110) to control a mechanical shutter (e.g., Thorlabs SHB1T)
-
Power Control Direction (Optional)
- Configurate the digital output line (e.g., port0/line0) and the counter (e.g., ctr1) of a DAQ card (e.g., NI PCIe-6323) to control a motor that adjusts the laser power
Prepare lifetime standards, i.e., fluorophore solutions with known fluorescence lifetimes (1, 2). Here are a few examples of lifetime standards:
-
1 mM Coumarin 6 in Methanol:
$\tau$ = 2.3 ns -
1 mM Coumarin 6 in Ethanol:
$\tau$ = 2.4 ns -
1 mM Fluorescein in 0.1M NaOH (pH=13):
$\tau$ = 4.0 ns -
1 mM Rhodamine B in water:
$\tau$ = 1.7 ns
Once a lifetime standard is prepared (in a cuvette, petri dish, or glass slide with cavity), fill in "Target Lifetime (s)" (1) with the expected lifetime of the standard (e.g., 2.3E-9 for 1mM Coumarin 6 in Methanol), place the standard on the stage, open the laser shutter, focus the beam into the fluorophore solution, and click the button "Calibrate" (2) to start the necessary system calibration. The program automatically performs calibration using the lifetime standard. Once the calibration is complete, the coefficients (3) required for instant FLIM measurements are automatically calculated. These coefficients are:
-
Calibrated Bias (V): Bias voltages that are needed for the four mixers to effectively induce phase shifts of 0, 0.5$\pi$,
$\pi$ , and 1.5$\pi$ -
$M/B$ : The ratio between the conversion losses of the mixer (RF to IF ports) and the bias tee (RF&DC to DC ports) -
$O_{B}$ : The DC offset (invariant to PMT signal variations) on the bias tee's DC port -
$d_{13}$ : The difference between the DC offsets of the first and third mixers' IF ports -
$d_{24}$ : The difference between the DC offsets of the second and fourth mixers' IF ports
Because different excitation wavelengths result in different measurement coefficients, the calibration procedure should be performed for each excitation wavelength that will be used. The user can fill in the "Wavelength (nm)" box (4) to record the excitation wavelength currently being calibrated with and, after calibration, click the "Save" button (5) to save the calibrated coefficients to the program's front panel (6).
A total of four calibration results (four different excitation wavelengths) can be stored simultaneously. Before performing real measurements, the user should click the "Load" button to load the calibrated coefficients matching the experimental condition into the program.
To evaluate if the calibration is successful, the user can perform a measurement while the lifetime standard is still under the microscope. Switch to the "Measurement" tab (1) and click the "Measurement" button (2):
Switch to the "Results" tab (1) to check the measurement results. If the calibration is correct, the values in the lifetime image and histogram (2) should match that of the lifetime standard used for calibration:
Meanwhile, on the "Phasors" tab (1), the phasors in the phasor plot (2) should be located at the semicircle. The user can label the pixels corresponding to the phasors by selecting a region of interest (ROI) (3) and then draw the ROI on the phasor plot (4). If the calibration is correct, all image pixels on the left should be labeled with the ROI's color.
In this protocol, we will use a standard biological test slide (FluoCells prepared slide #1, F36924) to demonstrate how to perform an instant FLIM measurement.
After placing the sample on the stage, switch to the "Fast Scan" tab (1) where the program uses crude but fast scans (faster than one frame per second) to help the user find the focal position. Click the "Fast Scan" button (2) to start scanning and change the stage positions (3) while the images are generated in real time. Change the XY and Z step sizes if needed. When a focal position is found, the user should expect not only a clear image (4) but also a high "Mean Pixel Value" of the image (5).
Once a clear image of the sample is obtained, the user can calibrate the pixel width according to the on-screen instructions (6). The pixel width is related to the objective lens used; therefore, the pixel width calibration should be performed each time a new objective lens is used.
Switch to the "Measurement" tab (1) for intensity imaging. Fill in the measurement parameters (2), including the pixel dwell time, pixel size, and XY Factor (obtained from pixel width calibration). Specify the "# of Frames to Average" (3) for each image; the more frames used for averaging, the higher signal-to-noise ratio the resulting image has. Click the "Measure" button to start measurement (4). When the measurement is complete, one can modify the brightness/contrast of the intensity image (5). The mixer images from the four mixers can also be seen (6).
In instant FLIM, all FLIM data, including lifetime images, phasor plots,
etc., are generated simultaneously with the intensity image; therefore,
once the intensity imaging is complete, the lifetime images and phasor
plots are also ready. Switch to the "Results" tab (1) to view the raw
(gray scale) and composite (HSV mapping: lifetime to hue, intensity to
value) lifetimes images. Both conventional (
Phasor plots are also generated simultaneously with the intensity image. Switch to the "Phasors" tab (1) to view the phasor results. The parameters of the phasor plot, including the ranges of G and S, the number of bins (grids) of each direction of the 2D phasor histogram, and the colormap, can be modified (2). Up to four ROIs can be drawn on the phasor plot and label the corresponding pixels in the raw image. The user can draw ROIs by selecting a ROI (3) and then clicking and holding the mouse on the phasor plot. The drawn ROIs can be enabled or hidden by the checkboxes (4). The pixels corresponding to the ROIs will be labeled/overlapped with the ROIs' colors if the "Phasor Overlap?" box is checked (5).
Switch to the "Z-Stack" tab (1) for 3D stack measurements. Specify the depth of each slice and the total number of slices in the Z-stack (2). Check the "Calculate Lifetimes and Phasors During Image Acquisition?" box (3) if needed; disabling the box can speed up the 3D image acquisition. Start the 3D measurement by clicking the "Z-Stack Measure" button (4).
Once the 3D measurement is complete, the user can view different versions of the 3D stack, such as intensity, lifetime, composite lifetime, and phasor plot (1). Adjust the slider (2) below the image to view different slices in the stack.
The displayed phasor overlap images are labeled according to the ROI configurations in the "Phasors" tab.
Switch to the "Time-Lapse" tab (1) to perform 2D time-lapse or 3D time-lapse (4D) measurements. For 2D time-lapse imaging, specify the time-lapse interval and the number of time points (2), and then start the measurement by clicking the "2D Time-Lapse Measure" button (3). For 3D time-lapse imaging, specify the interval and number of time points (4) and then start the measurement with the "3D Time-Lapse Measure" button (5). As the measurement goes, the imaging data are automatically saved as TIF files in your computer's disk.
The instant FLIM system is compatible with GSOS, a super-resolution frequency-domain FLIM technique (4). To perform GSOS microscopy, two instant FLIM imaging experiments with the same field of view on the same sample are needed. When performing the two experiments, the power of the excitation laser needs to be controlled and recorded (by a power meter) such that the power of the second experiment (P2) is slightly higher than that of the first one (P1). For example, we can set P1=3.5% and P2=4.0% for these two imaging experiments. First, set the power to P1 and perform the instant FLIM measurement as usual:
When the imaging at P1 is complete, switch to the "GSOS Process" tab (1) and click the "Load P1" button to load the instant FLIM data into the GSOS panel (2); the value of P1 should be filled in the "P1 Power (au)" box as the GSOS algorithm requires the values of P1 and P2. Then, change the laser power to P2 and perform another instant FLIM imaging experiment. When that is complete, switch back to the "GSOS Process" tab again, click the "Load P2" button to load the instant FLIM data for P2, and fill in the value of P2 (3). Finally, click the "Two-Step GSOS" button to start the GSOS processing (4), which can be executed instantly.
Switch to the "GSOS Results" tab (1) to view the results of the GSOS processing: the raw and composite lifetimes of the super-resolution FLIM image (2).
An adaptive optics (AO) setup consisting of a deformable mirror (Thorlabs DMP40-P01) can be used in instant FLIM to correct wavefront distortions and thus improve the imaging quality. Three adaptive optics optimization algorithms are included in this program to configurate the wavefront correction elements:
-
Simple Max Search Algorithm
- This algorithm iterates through all possible Zernike coefficients, one by one, until a maximal metric is found
-
Quadratic Search Algorithm (5)
- This algorithm assumes that the optimization metric (e.g., the
mean pixel value) is a quadratic function of the Zernike
coefficients of the deformable mirror; the algorithm requires
$2N + 1$ measurements to correct for$N$ Zernike coefficients
- This algorithm assumes that the optimization metric (e.g., the
mean pixel value) is a quadratic function of the Zernike
coefficients of the deformable mirror; the algorithm requires
-
Stochastic Parallel Gradient Descent Algorithm (6, 7)
- This algorithm stochastically variates the Zernike coefficients in parallel; every time the metric changes, the algorithm uses the gradient of the change to update the coefficients until a maximal metric is obtained or the specified steps of iterations are reached
The AO optimization is based on the image metric obtained from the "Fast Scan" module (1). Switch to the "Adaptive Optics" tab (2) to perform AO related operations. The sliders (3) can directly control each one of the Zernike coefficients of the deformable mirror. The user may manually adjust these sliders, instead of using the optimization algorithms, to improve the imaging quality. The optimization algorithms mentioned above can be performed by clicking the "Quadratic Search Algorithm" (4), the "Simple Max Search Algorithm" (5), or the "SPGD Algorithm" (6) buttons. Regardless of the algorithm used, the metric (7) should increase as the optimization proceeds. The optimization is complete when the metric no longer increases.
All the data acquired or generated by the program can be exported.
The 2D images (intensity, mixer, raw/composite lifetime, phasor, overlap) can be exported using the "Save 2D Images" button in the "File Operation for 2D Images" tab. It is essential to save the "Intensity", "G", and "S" images because all other images (except for the mixer ones) can be recovered from these three images. In practice, we recommend the users to only save these three images to save the computer's disk space.
The 3D images can be exported using the "Save 3D Stacks" button in the "Z-Stack" tab. To save disk space, the program only saves the "Intensity", "G", and "S" stacks.
The time-lapse images are exported automatically according to the directory and file name defined in the "Z-Stack" tab.
This program is fully open-source and highly modularized so users with LabView program skills can easily add new functions to the program. New functions can be added as new event cases so they will not interfere with existing functions:
-
N. Boens, W. Qin, N. Basarić, J. Hofkens, M. Ameloot, J. Pouget, J.-P. Lefèvre, B. Valeur, E. Gratton, M. VandeVen, N. D. Silva, Y. Engelborghs, K. Willaert, A. Sillen, G. Rumbles, D. Phillips, A. J. W. G. Visser, A. van Hoek, J. R. Lakowicz, H. Malak, I. Gryczynski, A. G. Szabo, D. T. Krajcarski, N. Tamai, A. Miura, Fluorescence Lifetime Standards for Time and Frequency Domain Fluorescence Spectroscopy. Anal. Chem. 79, 2137--2149 (2007).
-
A. S. Kristoffersen, S. R. Erga, B. Hamre, Ø. Frette, Testing Fluorescence Lifetime Standards using Two-Photon Excitation and Time-Domain Instrumentation: Rhodamine B, Coumarin 6 and Lucifer Yellow. J. Fluoresc. 24, 1015--1024 (2014).
-
Y. Zhang, A. A. Khan, G. D. Vigil, S. S. Howard, Super-sensitivity multiphoton frequency-domain fluorescence lifetime imaging microscopy. Opt. Express. 24, 20862 (2016).
-
Y. Zhang, D. Benirschke, O. Abdalsalam, S. S. Howard, Generalized stepwise optical saturation enables super-resolution fluorescence lifetime imaging microscopy. Biomed. Opt. Express. 9, 4077 (2018).
-
D. Debarre, M. J. Booth, T. Wilson, Image based adaptive optics through optimisation of low spatial frequencies. Opt. Express. 15, 8176 (2007).
-
M. A. Vorontsov, V. P. Sivokon, Stochastic parallel-gradient-descent technique for high-resolution wave-front phase-distortion correction. J. Opt. Soc. Am. A. 15, 2745 (1998).7. G. Palczewska, Z. Dong, M. Golczak, J. J. Hunter, D. R. Williams, N. S. Alexander, K. Palczewski, Noninvasive two-photon microscopy imaging of mouse retina and retinal pigment epithelium through the pupil of the eye. Nat. Med. 20, 785--789 (2014).
© 2019 Yide Zhang, University of Notre Dame
Licensed under the Apache License 2.0