Altair ALSM/CTASLM Baseplate
Overview
For the second iteration of our Altair baseplate system, we set out to make a number of different updates/upgrades from our first baseplate system design.
- For starters, the second iteration of our Altair LSFM baseplate incorporates 3 different microscope configurations:
Traditional Sample-Scanning SPIM
Sample-Scanning Axially-Swept Light Sheet Microscope (ASLM)
Sample-Scanning Cleared-Tissue ASLM (CTASLM)
Where each of these microscope paths incorporate as many of the same elements as possible between them, such that switching or upgrading between these modes is as accessible as possible and doesn’t require repurchasing all components along their respective illumination paths.
The primary distinction between ASLM/CTASLM and our SPIM paths is the incorporation of a remote focusing objective (RFO) system into the illumination path itself. The RFO system essentially allows the light sheet focus to be swept across the full field of view (FoV) of your imaging sensor, in comparison to the traditional SPIM system which is limited to a thin line profile on the imaging sensor. More information on ASLM can be found here. Figure 1 below details the ASLM process, where on the left a schematic of how the focus of the light sheet is swept and synced with the rolling shutter of an associated camera system in ASLM is shown. On the right is two different images taken where the top image is taken without utilizing the RFO and the bottom is utilizing the RFO, where when it’s utilized the beam is able to be swept across the full FoV of the image.
Figure 1: Introduction to the features of ASLM.
Another notable update for these microscope systems are that they also are fully optimized via simulation for three different illumination wavelengths (488 nm, 560 nm, and 640 nm), whereas our first baseplate design was optimized specifically for 488 nm. This should improve the overall quality of imaging between the different excitation wavelengths used in various fluorescent tags.
In addition to the aforementioned upgrades, this iteration of Altair also utilizes a Powell lens instead of a cylindrical lens as the element that forms our light sheet profile itself. Powell lenses are a specialized variant of lenses that are known to produce line profiles with consistent and uniform intensity. When utilized in light-sheet imaging, these lenses essentially help provide a more uniform intensity of illumination across the full FoV of the imaging sensor when compared to cylindrically formed light-sheets which feature more of a gaussian intensity distribution associated with them. More information on Powell lenses can be found at `Laserline Optics <https://www.laserlineoptics.com/powell_primer.html`_.
Zemax Simulation Setup Process
Similarly to our methods used for designing our first iteration of our baseplate (link to page), we first start by using basic magnification equations to select theoretical focal lengths of lenses that would be needed along our illumination path to form a light sheet with our desired physical characteristics. A basic schematic of what one of these powell-lens-based ALSM systems would look like is shown below in Figure (2).
Figure 2: Schematic of the ASLM illumination path design.
Of note in the design process is the careful considerations in abberation-prevention in a remote focusing system is to ensure mapping the magnification of the remote focus objective (RFO) to that of the illumination objective (ILO). In our case our chosen illumination objective is the Thorlabs TL20X-MPL and our remote focus objective is the Thorlabs TL15X-2P.
Because our RFO and ILO utilize different immersion media (n = 1 for the RFO, n = 1.33 for the ILO), we rely on our lens choices for L6 and L7 to ensure the magnification from sample space to remote space is equal to the ratio of these two refractive indices for our immersion media:
Where using our values for our chosen objectives this becomes:
Leaving us with the relation between the focal lengths of L6 and L7 as
With that relationship solidified, we then moved forward with selecting our lenses in our illumination path as follows:
Lens # |
Lens Description |
Link |
|---|---|---|
L1 |
Powell Lens LOCP-8.9R20-2.0 |
|
L2 |
Achromatic Doublet f = 30 mm |
https://www.thorlabs.com/thorproduct.cfm?partnumber=AC254-030-A |
L3 |
Achromatic Doublet f = 80 mm |
https://www.thorlabs.com/thorproduct.cfm?partnumber=AC254-080-A |
L4 |
Achromatic Doublet f = 75 mm |
https://www.thorlabs.com/thorproduct.cfm?partnumber=AC254-075-A |
L5 |
Achromatic Doublet f = 300 mm |
https://www.thorlabs.com/thorproduct.cfm?partnumber=AC254-300-A |
L6 |
Tube Lens f = 200 mm |
https://www.thorlabs.com/thorproduct.cfm?partnumber=TTL200-A |
L7 |
Tube Lens f = 200 mm |
https://www.thorlabs.com/thorproduct.cfm?partnumber=TTL200-A |
RFO |
Remote Focus Objective TL15X-2P, EFL = 13.3 mm |
https://www.thorlabs.com/thorproduct.cfm?partnumber=TL15X-2P |
ILO |
Illumination Objective TL20X-MPL, EFL = 10 mm |
https://www.thorlabs.com/thorproduct.cfm?partnumber=TL20X-MPL |
With the lenses selected, we then moved forward with the simulation and optimization of our illumination path in Zemax Opticstudio. Due to the way in which the blackbox files we utilize associated with the objective in our system are designed, we structured our simulation in a way that essentially unfurled the forward and reverse paths of our system to all be in a single direction, where our reverse path is essentially mirrored with respect to our forward path. This setup is shown below in Figure 3.
Figure 3: Conceptual setup of the ASLM-based Zemax simulations.
We optimized our system similar in method to how we optimized our first system (link to page), where the general process is placing in each component individually into the simulation and optimizing for either collimation or focusing in a particular direction before adding in the subsequent element. In this first optimization process, the offset of the RFO was set to be 0, such that the reverse path reflection point was the exact focus position of the RFO. After this optimization process, the resulting full-width half-maximums (FWHMs) of our light sheet widths were found to be:
Wavelength |
FWHM |
|---|---|
\(\lambda\) = 488 nm |
~392 nm |
\(\lambda\) = 560 nm |
~422 nm |
\(\lambda\) = 640 nm |
~468 nm |
In order to account for the
Adapting for CT-ASLM
In order to allow for a wider variety of biological structures to be studied in our systems, we adapted aspects of our ASLM design detailed above to be for
Our illumination and detection objectives for our CT-ASLM system are changed to both be ASI 54-12-8 Multi-immersion objectives, which are designed to be able to withstand being immersed in media like refractive-index matching media such as BABB. The illumination objective has a different effective focal length than that of the TL20X-MPL objective used in our standard ASLM configuration, so we need to revisit our choice of lenses for L6 and L7:
Where our new relationship between L6 and L7 becomes:
Based on this relationship, we chose L7 to be f = 180 mm and L6 to be f = 200 mm, and used the equivalent tube lenses from Thorlabs that match these (TTL180-A and TTL200-A, respectively).
Re-optimizing the system with our new illumination objective and L7 with a sample immersion media of n = 1.56 yielded the following FWHM of our end light sheet widths:
Custom sample chamber for CTASLM
Wavelength |
FWHM |
|---|---|
\(\lambda\) = 488 nm |
~300 nm |
\(\lambda\) = 560 nm |
~324 nm |
\(\lambda\) = 640 nm |
~356 nm |
Incorporating SPIM
Wavelength |
FWHM |
|---|---|
\(\lambda\) = 488 nm |
~390 nm |
\(\lambda\) = 560 nm |
~416 nm |
\(\lambda\) = 640 nm |
~454 nm |