Imaging instrument having objective axis and light sheet or light beam projector axis intersecting at less than 90 degrees

Information

  • Patent Grant
  • 11506877
  • Patent Number
    11,506,877
  • Date Filed
    Friday, November 10, 2017
    6 years ago
  • Date Issued
    Tuesday, November 22, 2022
    a year ago
  • Inventors
    • Tomer; Raju (Tenafly, NJ, US)
  • Original Assignees
  • Examiners
    • Dunning; Ryan S
    Agents
    • Potomac Law Group, PLLC
Abstract
Light Sheet Theta (LS-0) Microscopy achieves large sample imaging capabilities without affecting the imaging depth or the image quality. An optical layout places a detection objective normal to the sample surface, while placing the illumination objectives that generate light sheets at an angle (theta) significantly smaller than 90 degrees. In this configuration, the light sheets enter from same side of the sample as the detection objective. The intersection of the light-sheet and the detection focal plane results in a line illumination-detection profile that is discriminated by a camera.
Description
BACKGROUND

There is an increasing need for methods and devices that permit rapid high-resolution imaging of the structure and function of large three-dimensional objects, for example broad slabs of substantial thickness, in particular, fully intact biological samples such as large slices of biological tissues. An example of this is brain tissues the importance of which, to neuroscience research is underscored by the announcement of high profile initiative including White House sponsored BRAIN Initiative for building Neurotechnologies.


In the known technique of light sheet microscopy (LSM), a thin sheet of light illuminates a sample from the side and an orthogonally arranged objective detects the emitted signal from the illuminated plane. FIG. 1A is a figurative illustration of a light sheet microscope. A detection optical system 100 has a camera 110 that receives image light signal through an imaging lens 108 and an objective 104 having a high numerical aperture (NA) for discriminating feature in a relatively thick sample 115. The sample 115 is illuminated by light sheets 114 and 112 which are projected from illumination objectives 102 and 106 into the sample so as to focus a pair of light sheets 114 and 112 on the front focal plane of the imaging system. Three dimensional volumes of samples are acquired by either moving the sample 115 step-wise to image it plane-by-plane or by synchronously moving the aligned light-sheet and detection objective stepwise through the stationary sample. The acquired image “stack” (i.e., the collection of 2D planes) provides three-dimensional information about the sample. Samples larger than the field-of-view of the microscope (i.e. the part of sample visible at one position) are imaged by acquiring tiles of stacks which are then stitched together. Such volumes can also be acquired repeatedly with time delays to allow capturing of the dynamics of living samples.


The configuration of light sheet microscopy provides two key advantages: minimum possible energy load on the sample (therefore minimum photobleaching and phototoxicity) and very high imaging speeds. The imaging depth (i.e., the sample dimension along the imaging axis) is generally determined by the working distance of the detection objective, which puts a physical limit, and the optical scattering properties of biological tissue being imaged. The overall intact sample size that can be imaged is also restricted in one of the two other sample dimensions (i.e., the dimension along the light sheet propagation direction indicated in FIG. 1A at 117 and labeled “limit on sample size”) as the light-sheet needs to penetrate the tissue for illumination.


A commonly used configuration (FIG. 1B) that can address these limitations provides a detection objective 130 and illumination objective 130 whose optical axes are at 45 degrees to sample surface normal. This configuration reduces the imaging depth in the sample as the effective working distance of the detection objective is limited because of the angle. Also because of the geometry constraints of physical size of detection objective 130 (i.e. the objective may physically ram into the sample). The working distance is adversely affected as indicated by the arrowheads. In addition, using an angled detection objective results in aberrations, especially for high resolution detection objectives. Light sheets can also be generated through the detection objective itself (i.e. using of same objective for illumination and detection), as in oblique plane microscopy for example described by Dunsby in US Patent Publication 8582203. This however comes at the cost of reduction in the image quality, imaging depth (as the signal is detected off the native imaging plane) and also high photo damage.


SUMMARY

Presently described are embodiments of a microscope which may be identified as Light Sheet Theta Microscopy (LSTM), also referred to herein as LSTM. The LSTM microscope provides the ability to resolve images in substantial depth as in a light sheet microscopy while providing the ability to scan samples having a large area. Variations also provide faster scanning by imaging on opposite sides of the sample.


Objects and advantages of embodiments of the disclosed subject matter will become apparent from the following description when considered in conjunction with the accompanying drawings.





BRIEF DESCRIPTION OF DRAWINGS

Embodiments will hereinafter be described in detail below with reference to the accompanying drawings, wherein like reference numerals represent like elements. The accompanying drawings have not necessarily been drawn to scale. Where applicable, some features may not be illustrated to assist in the description of underlying features.



FIGS. 1A and 1B illustrate embodiments of prior art light sheet type microscopes.



FIG. 2 illustrates specific features of LSTM, according to embodiments of the disclosed subject matter.



FIG. 3A illustrates a LSTM microscope that employs a single light sheet illuminating a single linear region, according to embodiments of the disclosed subject matter.



FIG. 3B illustrates LSTM that employ double light sheets illuminating a single linear region, according to embodiments of the disclosed subject matter.



FIG. 3C illustrates LSTM microscope that employ double light sheets illuminating respective linear regions, embodiments of the disclosed subject matter.



FIG. 3D illustrates the volume of the sample that is discriminated by the detection arm in combination with the focus, the selection of pixels of the imaging device, and the light sheet intersection with the focal plane, according to embodiments of the disclosed subject matter.



FIGS. 4A and 4B show scanning modes, including a first 4A that scans a light sheet in a single axis perpendicular to an oblique (with respect to the sample surface) optical axis and a second 4B that scans a light sheet in dual axes both oblique and parallel to the sample surface, according to embodiments of the disclosed subject matter.



FIG. 5A shows a LSTM microscope for illustrating various features of the disclosed subject matter.



FIGS. 5B through 5D illustrate optional illumination arms that employ various optical components for providing various features, according to embodiments of the disclosed subject matter.



FIG. 6 illustrates the simultaneous acquisition of illuminated linear regions in separate planes at independent coordinates of the axis that is perpendicular to the illuminated line and parallel to the sample surface, according to embodiments of the disclosed subject matter.



FIGS. 7A through 7E illustrate stages of a scan of a single “tile” of a larger slab which scan is performed optically for one of a matrix of positions of an X-Y-Z-theta stage that positions the slab, according to embodiments of the disclosed subject matter. Note that the line readout in camera and illumination can be synchronously scanned in opposite direction as well.



FIG. 8 illustrates a controller connected to actuators of the various embodiments to permit automated operation of the LSTM system, according to embodiments of the disclosed subject matter.



FIG. 9 shows the compositing of the images of multiple tiles to create a 3D image of slab, according to embodiments of the disclosed subject matter.



FIG. 10 is a block diagram of another embodiment for implementing LSTM.



FIGS. 11A-B depict the physical geometric constraints for the objectives in the FIG. 10 embodiment.



FIGS. 12A-D depict a comparison of the illumination path lengths of the FIG. 10 embodiment and LSM for a sample of the same thickness and width.



FIGS. 13A-B depict the effective light sheet thickness for the FIG. 10 embodiment.



FIGS. 14A-D depict a comparison of energy load on the sample in LSM and the FIG. 10 embodiment.



FIG. 15A depicts a calculation of an effective working distance for an illumination objective.



FIG. 15B depicts the range of allowable angular positions for the objectives in the FIG. 10 embodiment.



FIG. 16 compares LSTM and LSM imaging of a ˜2 cm wide and ˜5 mm thick rat brain slice, stained for vasculature.



FIGS. 17A and 17B illustrate LSTM system with an integrated microtomy apparatus, according to an embodiment of the disclosed subject matter.



FIG. 18 illustrates relationships of angles between features of certain embodiments.



FIG. 19 illustrates GRIN lens embodiments for forming light sheets.



FIGS. 20A-20D illustrate an alternative scanning mechanism suitable for 1D or 2D scanning as described with reference to FIGS. 4A and 4B.





DETAILED DESCRIPTION

Presently described are embodiments of a microscope which may be identified as Light Sheet Theta (LS-θ) Microscopy, also referred to herein as LSTM. LSTM achieves planar imaging by employing obliquely arranged illumination light sheets from the same side of the sample as the detection objective. This configuration alleviates limitations on the lateral dimensions of the sample, while providing similar or better imaging depth, quality, low photo-bleaching and high imaging speed for larger samples. LSTM allows imaging of larger samples with high uniform resolution across the entire sample. In addition, LSTM achieves uniform illumination across the entire imaging field-of-view, in contrast to the non-uniform Gaussian illumination commonly used in LSM, thus enabling quantitative imaging across the entire sample. LSTM allows imaging of large samples including thick slabs of cleared and labelled post-mortem healthy and diseased human brains as well as imaging of large animal intact brains, including rat and primate brains. Moreover, LSTM facilitates in situ detection of thousands of transcripts in expanded tissue samples.


An embodiment is illustrated figuratively in FIG. 2, Illumination beam is formed through illumination objectives 142 in combination with preceding optics which form a sheet of light 144. The preceding optics may include scanning mirrors and electrically tunable lenses for scanning, sheet formation optical elements that may include a cylindrical lens, and a partial block 140 the combined effect of which are to form the light sheets 144 in desired positions traversing across and along each respective optical axis. Note that the effect of the block 140 is to form the light sheet such that it is not blocked by the detection objective. By forming the light sheet through a side of the illumination objective, the light sheet has a central axis that is oblique to the illumination objectives optical axis and is closer to parallel with the sample surface plane and further from the surface normal. This configuration may place the angle of the light sheet (or sheets) between the angles of the light sheets in the prior embodiments FIGS. 1A and 1B.


To provide the ability to scan large samples as in large sample imaging capabilities without affecting the imaging depth or the image quality. The optical layout is summarized in FIG. 2. The basic idea is to place the detection objective normal to the sample surface, while placing the illumination objectives that generate light sheets at an angle (theta) significantly smaller than 90 degrees. In this configuration, the light sheet enters from same side of the sample as the detection objective. The formed light sheets are arranged at an angle relative to the detection plane. The intersection of the light-sheet and the detection focal plane results in an illuminated linear volume discriminated by the detection arm that appears end-on at 219 in FIG. 3A.


Referring momentarily to FIG. 3D, the illuminated linear volume 219 is actually a small volume that is discriminated through not only the high NA detection objective (and other detection optics) which define the front focal plane but also the selection of pixels on the sCMOS camera 110 sensor which exclude out-of-plane light in a manner similar to a slit and also exclude light that is adjacent to the linear volume 219 that is targeted. This detected line 219 can be selected using illumination scanning optics that move the line 219 by moving the region where the light sheet intersects the front focal plane while simultaneously selecting the portion (i.e., the elongate region of pixels) on the sCMOS (or any other scientific camera) camera sensor that are detected. Call this line-by-line detection. This effectively scans the detection optics simultaneously with the illumination optics. That is, the syncing of line-by-line detection of sCMOS camera with the line illumination ensures that only the signal from that particular illuminated linear volume 219 is detected and interference from other sources of scattering or illumination are rejected.


By scanning this illuminated linear volume 219, the entire front focal plane may be illuminated and captured. The scanning on the illumination side may be performed, as later explained, by one or more mirrors, electrically tunable lenses, or alternatives thereto (e.g., rotating prisms, diffraction optics, MEMs pico projectors, electrically controllable spatial light modulators, tunable Acoustic lens (e.g. TAG Lens) and others commended by the state of the art for this purpose. This can also be achieved by synchronously scanning the illumination objective along the light sheet propagation direction alternatively or in conjunction with other scanning mechanisms.). The scanning of the light sheet in combination with the selective sampling of lines on the sCMOS camera imaging plane together may capture a “tile” portion of a larger sample to be imaged in its entirety. By syncing the illuminated linear volume 219 with the line-by-line detection of the sCMOS camera 110, high quality images of the plane are acquired.


According to embodiments, three different modes of detection may be provided with respective embodiments or through a single embodiment with multiple user-selectable modes. Referring to FIG. 3A, in a first mode, a single light sheet 210 is used to generate an illuminated linear volume 219. An exposed pixel line 204 is illustrated schematically to show that it corresponds to a column of pixels (or multiple columns or numerical synthesis of the signals from multiple columns effective to provide the selection of desired optical signal and exclusion of undesired such as scattered light from regions outside the illuminated linear volume 219). The cone of light captured and imaged from the illuminated linear volume 219 is indicated at 218 to indicate a high NA detection objective.


A second mode is as that illustrated in FIG. 2 and further described by FIG. 3B where a single illuminated linear volume 219 is generated by a single detection arm and dual light sheets 212. A third embodiment shown in FIG. 3C provides two light sheets 212, one on each side of the detection objective. The two light sheets may independently scan two different portions, for example two halves, of the plane as illustrated by the two image light cones 220A and 220B. (Note, that for detection of a light sheet, the term “wedge” may be more appropriate than “cone”, but it should be clear from context when is being identified by the latter term). As indicated above, the scanning may be done with the sample and the detection and illumination arms in respective fixed positions while the light scanning optics provide motion of the illuminated linear volume 219 and, simultaneously, the exposed pixel lines 205 are selected by sampling of the image plane of the camera chip 206. Note that in the figure the left pixel line 205 may correspond to the right light cone 220B and the right pixel line 205 may correspond to the left light cone 220A if the detection optics flips the image about the optical axis.


Other variant scanning modes are possible for each of the foregoing modes. For example, there are two scanning modes for scanning the illuminated linear volume 219 for planar illumination. Referring to FIG. 4A, a first of these scanning modes is where the light sheet is only displaced laterally (i.e. perpendicular to the light sheet propagation direction) as indicated by laterally displaced light sheets 237 and 239 which defined illuminated linear volumes 240A and 240B (these are positions along a front focal plane of the light sheet (beam waist) that traverses the plane indicated at 241. The latter may be accomplished using a galvo mirror, for example. In this scanning mode, referred to herein as 1-axis scanning (1-AS), the intersection of the light sheet and focal plane happens at different position in the light sheet.


Referring to FIG. 4B, in a second scanning mode, referred to herein as 2-axes scanning (2-AS), the front focal plane of the illumination optics is translated axially as well as transversely. By permitting the focused position of light sheet (i.e. the beam waist) to be scanned along the light sheet propagation direction as well as transversely, particularly in synchrony with the lateral scanning (as in the first mode) so that the thinnest part of the light sheet intersects with the detection plane, the front focal plane of the illumination optics can intersect with the detection front focal plane, resulting in very high image quality. In the latter mode, high-NA illumination objectives, results in much thinner light sheets.


To characterize and compare these modes of illumination and detection, micron scale fluorescent beads and CLARITY-cleared human brain tissue stained with nuclear stain DAPI were imaged. The resulting image volumes revealed that 2-AS allows for much more uniform axial resolution across the entire field-of-view, whereas both 1-AS and conventional LSM imaging produce reduced image quality on the periphery of the field-of-view. Simultaneous two-sided illumination from two symmetrically arranged illumination arms (as seen in FIG. 3B), provided higher signal and reduces the illumination artifacts caused by opaque objects in the illumination path thus improving the uniform planar illumination and detection prerequisite for achieving quantitatively accurate imaging.


The three-dimensional volumes are acquired by either moving the sample across the illuminated sheet in a stepwise manner (or continuously at slow speed, while imaging), or by synchronously moving the effective illumination light-sheet and the exposed pixel line resolved by the detection arm. Imaging speed can be further increased by simultaneously imaging the sample from opposed detection arms on respective opposite faces of the sample. In addition, a continuous motion of the sample may be used to traverse laterally instead of moving the exposed pixel line. The continuous traversal is faster than step-wise motion as linear stages may take significant amount of time for starting and stopping.


The various LSTM system embodiments enable imaging experiments of large sample size with extremely high resolution similar that of light sheet microscopy. In LSTM microscopy the detection objective remains normal to the sample surface, and the illumination objectives are placed at an angle (significantly different from 90 degrees, as close to 90 degrees as allowed by the geometry), thus removing the limitations demonstrated in FIGS. 1A and 1B. The light-sheet intersects with the detection plane of the objective in a line profile, which is then scanned horizontally to create an effective planar illumination upon integration. The synchronization of the line profile and the line-by-line detection of the sCMOS camera results in rejection of any signal other than the line profile. There are three modes that include use of one light-sheet and the modes of using of two light-sheets described above. Also, embodiments permit the use of two sheets independently to simultaneously image the two halves of the plane (resulting in 2 times higher imaging speed.) There are two methods to generate intersected illumination profiles. One where the light-sheet is only displaced laterally FIG. 4A (i.e. perpendicular to its propagation direction) and one where the light-sheet is also displaced axially (i.e. along the direction of propagation, which in combination with lateral displacements allows the generation of much thinner light sheets).


Some application examples include:


Imaging of thick slabs of human brain, or other organs, that are cleared by using any of the tissue clearing procedures including CLARITY, iDISCO, uDISCO, SeeDB, ClearT and Scale. These procedures employ a cocktail of chemicals to render the tissue transparent while preserving structural and molecular content. These tissues can come from normal or diseased states including, but not limited to, various types of cancers, neurological disorders and other diseased biopsies.


Imaging of large animal intact brains, including rat and primate brains. The current state-of-the-art technology has been limited to imaging samples of mouse brain size.


Live imaging applications in imaging mouse brain for functional activity.


Live imaging of 3D cell cultures.


Referring to FIGS. 5A and 5B, an LSTM system configured to image two sides of a slab simultaneously has four illumination arms 303A, 303B, 303C, 303D. A single illumination arm of the current embodiment is shown in FIG. 5B at a larger size. In each illumination arm 303A, 303B, 303C, 303D, a light source 302 applies an input LASER whose diameter is expanded by a beam expander (BE) represented by the pair of lenses 304 and 306. An iris 307 remove the low-intensity peripheral parts of the expanded beams. The beam can be selectively diverted using a pair of flipping mirrors 310 and 316 or permitted to pass directly to a cylindrical lens 318. When the beam passes through the cylindrical lens 318, it is compressed in one dimension to generate a sheet-shaped profile. Thereafter, the beam is scanned by an optical scanning device 320, for example a one or two dimensional galvo mirror scanner. A first dimension of the scanner may scan the emerging sheet beam in a path that is generally perpendicular to the plane of the sheet and the second dimension, if present, may provide a degree of freedom for alignment. The focused sheet is then imaged on the sample via a scan lens 322 (f-theta lens which converts angular motion of Galvos to lateral motion), a tube lens 324 and the illumination objective 330, the stop 326 serving the function previously described with reference to block 140 of FIG. 2. When the flipping mirrors, which may be motorized, are in the divert position, the beam is reflected and routed through a U-shaped path by mirrors 308, 314 and a relay lens system 310. An electrically tunable lens (ETL) 312 can be controlled electrically at high speed to allow axial displacements described in FIG. 1E. The ETL is placed in at the conjugate focal plane by using the lens relay lens system 210. This selectable routing may be controlled by motorized flip mirrors 310, 316. The optical scanning device 320 allows fast lateral displacements of the final sheets as shown in FIGS. 4A and 4B. The detection arm includes the components described above with regard to FIG. 2, including detection objective 338, a tube lens 328 and sCMOS camera 330.


Note that instead of subsystems 300A and 300B being positioned to scan different layers of the sample, they may image the same layer simultaneously, permitting the captured image data to be combined to increase resolution. Variations may also be provided such as illumination arm or arms on one side and detection arm on the opposite side of the sample. Also, the block 140 may be eliminated and also made movable so that it can be adjusted from a range of 0% blockage to a major fraction of the aperture of the illumination objective. Any of the claimed embodiments may be modified to provide additional embodiments with zero or adjustable blockage.


It will be clear that any of the mirror or other deflectors such as optical scanning device 320 may be substituted by equivalent light redirectors. Such may include refracting as well as reflecting components or other types of light manipulation devices. Lenses may be of any suitable type. Wave-guide-based devices including fiber optics may also be substituted for beam reflectors. Devices other than ETLs may be employed to manipulate the axial position of the front focal plane of the illumination arm, including but not limited to, mounting of illumination objective on fast piezo motors for axial motion profile. The camera 330 may also be replaced, for example by a scannable line sensor. Instead of a sheet beam, a scanned pencil beam may be projected over a target illuminated linear volume 219 although such alternatives may have characteristics that are adverse to the functions of speed provided by the illustrated and described embodiments.


A sample 336 may be mounted for translation and rotation movement, for example, mounted on an XYZ-theta motorized stage. This may permit the sample 336 to be scanned over multiple tiles. The illumination arm of FIG. 5B is replicated four times as shown in FIG. 5A. This allows multiple modes of illumination and image detection. FIG. 5A shows an LSTM system 300 with two identical LSTM subsystems 300A and 300B. Each LSTM subsystem has a respective detection arm 301A and 301B, one directed for detection at each face of the sample 336. Each detection arm 301A, 301B has a pair of illumination arms, detection arm 301A having illumination arms 303A and 303B and detection arm 301B having illumination arms 303C and 303D. The sample 336 may be surrounded by immersion liquid according to any relevant techniques. The four LSTM subsystems may scan at each of multiple discrete tile-specific positions of the translation system. Each scan images a layer, indicated at 332. The layer for each tile may be composited by stitching to form a full layer of the sample. In addition, the acquisition of multiple layers may be done for each tile, each layer being composited by stitching, to form a full layer. That is each tile-specific position of the translation system may acquire multiple layers.



FIGS. 5C and 5D show other variations of illumination arms that may be substituted for the illumination arms of FIG. 5A. FIG. 5C shows the illumination arm of FIG. 5B without the U-shaped diverted path, flipping mirrors and relay lens components. This provides the scanning functionality described relative to FIG. 5A but without the flexibility of switching the ETL in and out of the illumination arm. FIG. 5D shows an illumination arm suitable for the scanning mode depicted in FIG. 4A without the axial displacement of the light sheet front focal plane 241. The illumination arm of FIG. 5D has not ETL in the light path.


Referring to FIG. 6, a de-synchronized line- by-line detection mode for simultaneously capturing of the emitted signals is shown. This operating mode can be performed with the LSTM system 300 of FIG. 5A, for example. Illumination sheet beams 353 and 354 are directed toward a first surface of a sample and illumination sheet beams 366 and 362 are directed toward an opposite surface of the sample. The two pairs of illumination beams in concert with the detection arms (not shown explicitly) including camera image detectors that discriminate respective pixel columns 350 and 360 capture illuminated linear volumes 219A and 219B at laterally different positions. This arrangement minimizes light interference between the two offset targets. Thus, by scanning with a phase difference between the two detection arms, two sides of a sample can be scanned simultaneously with minimal mutual interference.


The LSTM system may have a controller to perform a function that automatically performs a calibration by sparsely automatically sampling of the imaging planes at multiple positions in the sample. According to an embodiment, the LSTM system may be controlled to perform a sparse traversal of a large sample in order to extract parameters that affect the positions of the illuminated linear volumes 219 such as surface variations and variations in index of refraction. Thus, a sparse matrix of samples can be captured and analyzed for these variations and stored in order to create a fine traversal itinerary. This ultimately may speed and improve the imaging quality of the acquisition of optical data in a large sample. The traversal itinerary may employ adaptive correction of the detected parameters and interpolation of the parameters from the sparse intervals. The adaptive optics may correct, for example, light sheet displacement relative to the detection focal plane.



FIGS. 7A through 7E illustrate stages of a scan of a single “tile” of a larger slab which scan is performed optically for one of a matrix of positions of an X-Y-Z-theta stage that positions the slab, according to embodiments of the disclosed subject matter. FIG. 8 illustrates a controller connected to actuators of the various embodiments to permit automated operation of the LSTM system, according to embodiments of the disclosed subject matter. FIG. 7A shows illumination sheet beams 353 illuminating illuminated linear volume 219 in an initial position to the right of a tile 370 to be imaged at a fixed position of a slab 372. The slab may be moved by a traversing system 406 (See FIG. 8) that moves an X-Y-Z-theta stage, for example, under control of a controller 410. For a sequence illustrated in FIGS. 7A through 7E, the stage may remain in a fixed position after which it's z position may be changed in steps until an entire volume is scanned and then the stage moved to a different coordinate (See FIG. 9) to sample an array of tiles of a slab. The data may be composited to form an image of the slab, as discussed. In the sequence from FIG. 7A to 7E, the illumination beam is traversed by controlling the optical scanning device 320 with the controller 410. The controller may position the motorized flip mirrors 310, 316 to pass illumination light through the electrically tunable lens (ETL) 312. Thus, the sheet beams 353 will be moved progressively or in stages, a few of which are shown in FIGS. 7A-7E. At each position (progressive and continuous or discrete) the exposed pixel line 204 is sampled thereby selecting a then-current line image of the illuminated linear volume 219. The selection of image data of the camera, storage, and sampling as well as compositing may be performed automatically by the controller 410 connected to the camera 330.



FIGS. 20A through 20D further illustrate what is happening during a scan. 20A and 20B show the projection of the illuminated line on the camera sensor at one end of the cross-axis scan and at an arbitrary intermediate point along the scan to an opposite end for a microscope that does not flip the position of the image across the optical axis. FIGS. 20A and 20B show the projection of the illuminated line on the camera sensor at one end of the cross-axis scan and at an arbitrary intermediate point along the scan to an opposite end for a microscope that does flip the position of the image across the optical axis.


Note that although the drawings of FIGS. 7A-7E suggest that the detection arm does not flip the image about the axis as would typically happen in microscopes. Embodiments in which the line source on one side of the optical axis are imaged on an opposite side are also contemplated in this context.



FIG. 9 shows the compositing of the images of multiple tiles to create a 3D image of slab, according to embodiments of the disclosed subject matter. Each tile may be formed by the sequence illustrated in FIGS. 7A-7E and for each, z-axis slices may be acquired. An array of tiles—multiple ones for each level of depth acquired—may be obtained to image a slab volume. The speed may be doubled by acquiring samples at two depths simultaneously using a system such as described with regard to FIG. 5A.



FIG. 10 depicts another embodiment for implementing LSTM. Each of the illumination arms 500 in this embodiment includes a LASER source 502, collimators 504 (e.g., using ˜10 mm output beam diameter), ETL 508, cylindrical lens 512, galvo scanner 514, scan lens 516, tube lens 520 and illumination objective 530 (e.g., a Olympus Macro 4×/0.28 NA). In this embodiment, a first iris 506 is incorporated after the collimator 504 to remove the peripheral spread of Gaussian beams; a one dimensional slit 510 is incorporated before the cylindrical lens 512, to control the effective numerical aperture of illumination; and a second iris 518 is incorporated at the conjugate plane, between scan lens 516 and the tube lens 520, to control the light sheet height for minimizing unwanted illumination. In some embodiments, a stop (not shown, but similar to the stop 326 in the FIG. 5A embodiment) may be provided just before the illumination objective 530.


In some embodiments, the illumination arms 500 are mounted at an approximately 60° angle relative to the detection arm 550 fixed on an optic table. In alternative embodiments, this angle may vary within the parameters discussed in connection with FIG. 15B. Optionally, to facilitate the optical alignment of the system, all the three optical arms 500, 550 may be mounted on two manual translation stages. Optionally, an open top sample chamber filled with an immersion oil (e.g., with a Refractive Index of 1.454) may be used. Optionally, samples may be mounted in a quartz cuvette attached to the base of the sample chamber.


In this embodiment, two thin light sheets are generated by using two illumination optical arms 500. When the illumination objectives are air objectives, a 3D printed cap with a coverslip (e.g., a 1 inch diameter quartz coverslip) may be used to seal the objective for oil immersion use.


The detection arm 500 in this embodiment includes a detection objective 552 (e.g., Olympus 10×/0.6 NA/8 mmWD or 25×/1.0 NA/8 mmWD), a tube lens 556, and an sCMOS camera 558 (e.g., a Hamamatsu Orca Flash 4.0 V3). In some preferred embodiments, an emission filter (not shown) is disposed between the detection objective 552 and the tube lens 556.


A list of suitable parts and their sources that may be used in this embodiment is provided in Table 1.












TABLE 1





Source
Cat. Number
Qty
Description















Detection unit










Thorlabs
CXY2
1
60 mm Cage System Translating Lens Mount for Ø2″ Optics


Thorlabs
LCP90F
1
60 mm Removable Cage Plate


Thorlabs
SM2A20
1
SM2-M38 ADAPTER FOR NIKON TUBE LENS


Thorlabs
SM2L30-
2
SM2 Lens Tube, 3″ Thread Depth, One Retaining Ring Included



SM2




Thorlabs
LCP09
2
60 mm Cage Plate with Ø2.2″ Double Bore for SM2 Lens





Tube Mounting


Thorlabs
ER10
4
Cage Assembly Rod, 10″ Long, Ø6 mm


Thorlabs
SM1A1
1
Adapter with External SM05 Threads and Internal SM1 Threads


Thorlabs
SM2A31
1
Adapter with External C-Mount Threads and Internal SM2





Threads


Hamamatsu
C13440
1
Digital camera


Custom
ObjAdater
1
Custom made Adapter from SM2 to M34 threading


Thorlabs
SM2V10
1
Ø2″ Adjustable Lens Tube, 0.81″ Travel


Olympus
XlPlan N,
2
Oil immersion Objective



10X




Thorlabs
LCP01B
2
60 mm Cage Mounting Bracket


Thorlabs
RS2
2
Ø1″ Pillar Post, ¼″-20 Taps, L = 2″, 8-32 Adapter Included


Thorlabs
TBB0606
2
Large-Area Translation Stage, 6″ × 7.66″







Two Illumination units










Thorlabs
SM2V10
2
Ø2″ Adjustable Lens Tube, 0.81″ Travel


Custom
ObjAdater
2
Custom made Adapter from SM2 to M34 threading


Olympus
Macro
2
Air Objective



4x/0.28NA/





29.5WD




Thorlabs
SM2A20
2
SM2-M38 ADAPTER FOR NIKON TUBE LENS


Thorlabs
CXY2
2
60 mm Cage System Translating Lens Mount for Ø2″ Optics


Thorlabs
LCP09
2
60 mm Cage Plate with Ø2.2″ Double Bore for SM2 Lens





Tube Mounting


Thorlabs
LCP01B
4
60 mm Cage Mounting Bracket


Thorlabs
RS2
4
Ø1″ Pillar Post, ¼″-20 Taps, L = 2″, 8-32 Adapter Included


Thorlabs
TBB0606
4
Large-Area Translation Stage, 6″ × 7.66″


Thorlabs
ER05
8
Cage Assembly Rod, ½″ Long, Ø6 mm


Thorlabs
LCP02
6
30 mm to 60 mm Cage Plate Adapter, 8-32 Tap


Thorlabs
LJ1695RM-
2
Ø1″, N-BK7 Mounted Plano-Convex Round Cyl Lens



A




Thorlabs
CRM1L
2
Cage Rotation Mount for Ø1″ Optics, Double Bored with





Setscrew, 8-32 Tap


Thorlabs
CP20S
2
30 mm Cage System Iris, Ø20.0 mm Maximum Aperture


Thorlabs
CP90F
2
30 mm Removable Cage Plate, Front and Back Plate, Internal





SM1 Threading


Thorlabs
CXY1
2
30 mm Cage System, XY Translating Lens Mount for Ø1″





Optics


Thorlabs
CP12
2
30 mm Cage Plate, Ø1.2″ Double Bore for SM1 Lens





Tube Mounting


Thorlabs
LCP01
4
60 mm Cage Plate, SM2 Threads, 0.5″ Thick, 8-32 Tap





(Two SM2RR Retaining Rings Included)


Thorlabs
CLS-SL
2
Scan Lens with Large Field of View, 400 to 750 nm, EFL = 70





mm


Thorlabs
ER18
6
Cage Assembly Rod, 18″ Long, Ø6 mm


Thorlabs
LCP50S
2
60 mm Cage System Iris, Ø50.0 mm Maximum Aperture


Optotune
EL-16-40-
2
Electrically Tunable Lens



TC-VIS-





5D-C




Thorlabs
ER4
18 
Cage Assembly Rod, 4″ Long, Ø6 mm


Thorlabs
VA100C
2
30 mm Cage System Adjustable Slit, 8-32 Tap, Imperial





Micrometer


Thorlabs
GVS001
2
1D Galvo System, Silver-Coated Mirror, PSU Not Included


Thorlabs
GCM001
2
1D Galvo 30 mm Cage System Mount


Omicron
Custom
2
Collimator with ~10 mm bead diameter output


Omicron
SOLE-6
1
LASER engine with 4 lines: 405, 488, 561, 647 nm







Mounting Base










Thorlabs
MB1236
1
Aluminum Breadboard 12″ × 36″ × ½″, ¼″-20 Taps


Thorlabs
RS12
4
Ø1″ Pillar Post, ¼″-20 Taps, L = 12″, 8-32 Adapter Included


Thorlabs
C1001
4
Post Mounting Clamp for Ø1″ Post







Motorized XYZ Stage and sample mounting










Thorlabs
LNR50S
3
50 mm (1.97″) TravelMax Translation Stage, ¼″-20 Taps


Thorlabs
LNR50P3
1
XY Adapter Plate for LNR50 TravelMax Stages, Imperial





Hole Spacings



LNR50P2
2
Right-Angle Bracket for LNR50 TravelMax Stages, Imperial





Threads


Custom
Sample
1
Custom made 3D printed sample chamber



chamber









Controls & electronics










National
PXIe-
1
Control PCIe card for PXI chasis


Instruments
PCIe8381




National
NI PXIe-
1
PXI express chasis


Instruments
1028




National
7852R
1
FPGA card


Instruments





National
7842R
2
FPGA card


Instruments





Thorlabs
GPS011
1
Galvo System Linear Power Supply


Thorlabs
LEDD1B
2
T-Cube LED Driver with Trigger Mode, 1200 mA


Thorlabs
BSC203
1
BSC203-Three-Channel APT ™ Benchtop Stepper Motor





Controller


Markettech
SOLE-6
1
6 Laser Light Engine with 4 wavelengths


Serversdirect
Custom
1
Custom workstation with Supermicro





X10DRHCT Motherboard, 24 TB SSD Hard Disks (EVO





850), 256 GB RAM (Crucial RDIMM





DDR4), Quadro K4200 Graphics card.









Because LSTM involves scanning of a line illumination-detection profile generated by the intersection of the light sheet and the detection plane, some preferred embodiments use static sheets (generated by the use of a cylindrical lens and associated optics), instead of a dynamic sheet (generated by rapid scanning of a pencil beam) to maximize imaging speeds. But some alternative embodiments can use dynamic sheets.


A galvo scanner 514 is used to achieve rapid translation of light sheets perpendicular to their propagation direction. For the 2-AS mode, rapid translation of the thinnest part of the sheet along the propagation direction is required. This may be accomplished using a variety of approaches including but not limited to using fast piezo motors to translate the illumination objectives, using holographic spatial light modulators or an electrically tunable lens (ETL) 508 to induce divergence and convergence of a collimated beam. The use of piezo motors for rapid scanning of objective often results in vibrations and require additional settling time, and the spatial light modulators are limited in modulation speed because of slower refresh rates. ETLs, on the other hand, can achieve high frequency modulation of focal plane position without the need for moving optics of significant mass. Accordingly, some preferred embodiments use ETLs 508. In practice, an ETL based approach has proven to be highly effective for achieving uniform simultaneous 2-axes scanning.


One way to optically align the LSTM assembly is to place a prism mirror (e.g., with fine scratches in the center) in the focal plane of detection optics, to visualize the location and cross- section of the light sheet relative to the detection focal plane. The light sheet positioning parameters can then optimized such that the thinnest part was in alignment with the center of the field-of-view of the detection plane. Next, the mirror can be replaced with a high concentration (>2%) agarose gel containing fluorescent beads (Note. The high concentration of agarose may be used to ensure that only the surface plane of the agarose gel is visible during the alignment optimization.). By examining the extent and quality of the illuminated beads located on the surface, optimal galvo scanner and ETL parameters for achieving uniform planar illumination across the entire field-of-view can be identified.


A series of calculations was used to assess and compare various properties of the FIG. 10 embodiment. The results of these calculations are summarized in FIGS. 15A and 15B. First, the physical geometric constraints of arranging a given set of detection and illumination objectives in a non-orthogonal configuration were calculated (FIGS. 15A-B). The main physical parameters used in the calculations are the working distances and the diameters of both the illumination objectives 530 and detection objectives 552. Next, the range of physically-allowable, relative angular arrangements that enable light sheets to intersect the detection focal plane at their thinnest parts (while also ensuring that illumination objectives remain above the physical extent of the detection objective) were calculated. For instance, when an Olympus Macro 4×/0.28 NA/29.5 mmWD is used as the illumination objective and an Olympus 10×/0.6 NA/8 mmWD is used as the detection objective, only angular configuration of 43.3° to 62.3° are possible. This can be calculated from the physical geometric constraints on the arrangement of illumination objectives by analyzing the two opposite bounds (FIGS. 11A-B and 15B): the illumination objective not to touch the detection objective (FIG. 11A) and the illumination objective not going below the physical extent of the detection objective (FIG. 11B). The range of allowable angular positions can be calculated by taking the effective working distances and the objective diameters into account as shown in the schematics of FIG. 15B, resulting in the following relationships:







W





2
*

sin


(

θ





i

)



=



D





1

2

+

D





2
*


cos


(

θ





i

)


2










W





2
*

cos


(

θ





f

)



=


W





1

+

D





2
*


sin


(

θ





f

)


2







where W1 and W2 are the working distances of the detection and illumination objectives respectively, D1 and D2 are the diameters of the detection and illumination objectives respectively, and θi and θf are the boundary angular positions. When the objectives are designed to be used in air, Snell's law may be used to calculate the approximate effective working distance (e.g., in a refractive index liquid of 1.454, as shown in FIG. 15A), resulting in ˜44 mm, and the objective diameter (lowest part of the tapered ending) was measured to be ˜28 mm. For many experiments values of W1=8, and D1=40 were used.



FIG. 15A shows approximate calculations of the effective working distance (EWD) for an Olympus Macro 4×/0.28 NA/29.5 WD air illumination objective when used in an immersion liquid with refractive index 1.454. Original working distance (OWD) is the working distance in air according to the objective specifications. A thin quartz coverslip and a 3D printed cap were used to seal the illumination objectives. EWD was estimated to be 43.84 mm.


12 depicts the influence of angular separation of the illumination arms 500 and the detection arms 550 in the FIG. 10 embodiment on the resulting image volumes and a comparison of the illumination path length of LSTM vs. LSM. In LSM, the illumination light sheet needs to penetrate the entire width (w) of the sample (FIG. 12B), whereas in LSTM the effective illumination path length depends on the angular arrangement and tissue thickness(t): t/cos(θ) where t is the sample thickness to be imaged and θ is the angle between the illumination propagation direction and the detection axis (FIG. 12A). Thus, from an illumination path length stand point, minimizing the angular separation will increase illumination penetration.


The graph in FIG. 12C plots the dependence of illumination depth of LSTM on θ. Each curve represents a different tissue thickness(t), as marked by the arrow in the direction of increase in thickness. When the effect of θ on the effective light sheet thickness (approximated as b/sin(θ), which determines the axial resolution, is measured, an inverse relationship is found: increasing θ provides better the axial resolution. Because illumination is provided via a low NA objective for which the light scattering has much smaller effect on the illumination side, some embodiments maximize the angular separation at ˜60° to achieve higher axial resolution. The experiments discussed herein were performed using this configuration.


The graph in FIG. 12D compares the illumination depth required to image a sample of given width and thickness. The ratio of the LSTM and LSM illumination path was converted into a binary representation by thresholding at 1, and plotting the results as a heat map to summarize the parameters ranges where LSTM (the region on the right) and LSM (the region on the left) need smaller illumination depth, and hence which approach will provide better image quality.


The imaging performances of LSTM and LSM was compared using a thick (˜5 mm deep and ˜2 centimeters wide) cleared rat brain section stained for vasculature, with a highly transparent sample with bright uniformly distributed signal. LSTM enabled imaging of the entire sample with uniform high-resolution, whereas the lack of penetration of the illumination light sheets in LSM resulted in progressively poorer image quality towards the center of the tissue. These and other experiments help demonstrate the suitability of LSTM for quantitative high-resolution imaging of large samples, without any limits on lateral sizes.


The use of lower NA illumination in LSTM 1-AS configuration in a large sample was tested in a CLARITY-cleared thick coronal section of Thyl-eYFP transgenic mouse brain. Low numerical aperture illumination was used to generate a large field-of-view (and hence thicker light sheets). While, the LSTM 1AS mode allowed for high-quality imaging of the section, image quality was reduced for peripheral portions of the field-of-view. This result was similar to the imaging performance of a LSM system employing Gaussian beams for illumination.


Next, the imaging performance of LSTM in simultaneous 2-AS mode was assessed using a thick (˜9.6 mm×13.5 mm×5.34 mm) coronal section of CLARITY-cleared Thyl-eYFP transgenic mouse brain, with 10×/0.6 NA/8 mmWD and 25×/1.0 NA/8 mm objectives. A larger input beam diameter was used to employ full NA (0.28) of the illumination objective. With this configuration, LSTM provided rapid high-resolution quantitative imaging of these large samples without any reduction in the image quality across the sample dimensions.


As a follow up to these experiments, an entire intact cleared mouse brain (with connected spinal cord) of Thyl-eYFP transgenic mouse was successfully imaged. A detailed high-resolution 3D rendering was performed and it demonstrated uniform, high quality imaging. One can therefore conclude that LSTM allows high-resolution quantitative imaging of large intact biological systems with no limitations on the lateral dimensions. Sample thickness that can be imaged remains limited by the working distance of the detection objective and also by level of tissue transparency and penetration of labelling reagents.


Due to the non-orthogonal incidence of the light sheet on the detection plane, the effective light sheet thickness can be approximated as the projection of the original thickness on to the detection direction, resulting in b/sin(θ), where b is the original light sheet thickness at the most focused position, and θ is the angle of incidence relative the detection axis. FIGS. 13A-B depict this relationship, and shows that effective planar illumination thickness can be approximated as b/sin(θ). More specifically, FIG. 13A shows the geometry and FIG. 13B plots the effective light sheet thickness as a function of θ for different values of b (the arrow points in the direction of increasing b value).



FIG. 14 depicts a comparison of energy load on the sample in LSTM and LSM. The two rows compare the time-accumulated energy load in LSTM and LSM for imaging a single plane (FIGS. 14A and 14C, respectively) and a single image stack tile (FIGS. 14B and 14D, respectively). The energy load in LSTM is dependent on the sample thickness, and in LSM on the sample width. For larger samples LSTM energy load is similar to LSM.



FIG. 16 compares the normalized mean intensity for LSTM and LSM imaging of a ˜2 cm wide and ˜5 mm thick rat brain slice, stained for vasculature. The images used for the FIG. 16 comparison were maximum intensity z-projections, and were acquired using 10×/0.6 NA objective. FIG. 16 profiles the mean (in the vertical direction) intensity across the region of interest (ROI). Due to the scattering of the illumination light sheet, the image signal in LSM is degraded towards the interior of the sample, whereas LSTM allows uniform quality imaging across the entire sample.



FIG. 18 shows the relative angles formed by illumination optical axes 650 (one for each of two illumination objectives or one alone for a single illumination objective), major plane or axis 652 and 654 of the illumination beams such as when emitted from the perimeter of the objective so as to be at a shallower angle than the illumination objective optical axis 650. The angle 658 between the illumination objective axes 658 is smaller than the angle 656 between the major plan or axes 652 and 654. The drawing shows a range of angles for each that is constrained to avoid interference between a detection objective (optical axis indicated at 651) and the illumination objectives.


Throughout the specification, reference to embodiments includes those defined by the claims. Thus, any proposed modifications to embodiments contemplates corresponding variations of the claims and such variations are considered to be disclosed in the present application.


Many of the disclosed embodiments contemplate the use of one or more movable stages carrying specimens, optical components, or both. The details of such devices and technology which are sufficient to implement the disclosed embodiments and variations thereof are in the public domain and are therefore not disclosed.


Motion stage-driven microtome may also be combined with the disclosed LSTM microscope embodiments. The microtome may be controlled automatically, in synchrony with a tile-wise scan of a sample, to remove a layer of the sample after an outer layer has been scanned into memory. Once a layer is removed, the traversing system can move the excitation and detection arms to scan the exposed deeper layer automatically. A microtome may be provided for opposite surfaces of a sample, for example, separate microtomes may be provided for the opposing sample faces of the embodiment of FIG. 5A. FIG. 17A illustrates figuratively illustrates the embodiment of FIG. 5A with microtomes 610 positioned with respect to opposing faces of a sample 602 to shave, in steps, outer surfaces of the sample 602. A traversing attachment including a movable stage may provide X-Y, and or Z positioning of a knife 611 relative to the sample 602. The detection and excitation optics are indicated as outlines at 618 and 616 respectively. A main support is indicated at 606. The automatic sequential positioning of the knife may be accomplished using a very short traverse to remove a tile-sized layer at a time, or regions the size of multiple tiles may be removed at a time. At least part of the traversal of the knife may be accomplished using the traversing system used for relative positioning of the optics and 616, 618 and sample 602 during scanning.


In any of the embodiments, further processing such as compression, may be performed on acquired data in parallel with scanning. For example, as the optical data are acquired for a tile, the data from a previous tile may be further processed to reduce the data volume, for example, by algorithms such as JPEG2000 2D or JPEG2000 3D. The further processing may also include other image processing tasks such as image segmentation, feature recognition or other data reduction procedures.


It will be understood that although a camera is shown for each detection arm, in alternative embodiments, a single camera can receive light, with a suitable optical arrangement, from both sides of a slab to be imaged.


Note that in any of the embodiments employing an electrically tunable lens, any other suitable mechanism configured to move the sheet beam waist along an axis of the illumination objective may instead, or additionally—as feasible may be employed. These include, but are not limited to, alone or in combination, acousto-optics tunable lenses, spatial light modulators, digital micromirror devices or mounting of illumination objective on a piezo motor, gradient-index (GRIN) lenses, micro electromechanical machines (MEMS) carrying fibers, beam redirectors, for example a GRIN lens at the end of a fiber driven by a MEMS motor. See, for example, “Multimode fibre: Light-sheet microscopy at the tip of a needle by Ploschner at al, (http://dx.doi.org/10.1038/srep18050). Those of skill in the art will recognize that other equivalent or similar mechanisms may also be used. FIG. 19 illustrates a fiber 670 carrying a GRIN focusing element 672 that forms a light sheet 674. To implement the scanning mode of FIG. 4A, a motor such as a piezo motor, MEMS motor, servo, stepping or any other type of motor and drive 678 may drive the GRIN lens as illustrated. A light source is not shown but is understood to be provided. To implement the scanning mode of FIG. 4B, a similar type of motor and drive 678 and 680 may be used to move the GRIN lens as illustrated in concert to move a line of maximum intensity light of a resulting sheet beam along a path normal to a detection objective optical axis or a single motor and drive 676 may be used to scan across the same path. The dashed coupling line between the motor and GRIN lens indicate mechanical coupling.


Suitable mechanisms such as stage on tracks, linkages, or flexible composite structures can be used to maintain the orientation of the GRIN lens throughout the sweep of the scan. Note that other sweep paths may be implemented other than those shown in FIGS. 4A and 4B as well as FIG. 19 such as an arc sweep or combinations of the illustrative modes.


In any embodiment described as including an sCMOS camera, other suitable imaging devices may be substituted, including, but not limited to CCD or line detectors.


As used in the current specification and in the claims, the term “objective” may refer to any lens or set of lens capable of being used as an objective or a part thereof. So, for example, the excitation arm is described, in embodiments, as using an objective to form a sheet beam. In this role it is not used for forming an image but the optical element itself may have features of an objective including characterizing features such as a numerical aperture.


In any of the embodiments, provisions may be made to alter the depth of field of the microscope and to select a number of depths to scan for a given tile in order to increase the speed of throughput for live imaging of tissue samples, for example. The depth of field may be selected by any suitable mechanism such as an objective turret selector or replaceable objectives.


According to first embodiments, an optical imaging apparatus includes a first illumination arm having optical components arranged for forming a first sheet beam. A first detection arm has a front focal plane and having optical components for imaging a linear volume where the sheet beam intersects the front focal plane. The first illumination arm and first detection arm optical components each include a respective illumination objective and detection objective, the angle of the first sheet beam is oblique to the optical axis of the illumination objective, and the first detection arm front focal plane is perpendicular to the detection objective.


The first embodiments include variants in which the first illumination arm optical components include scanning components that cause a beam waist of the sheet beam to traverse the first detection arm front focal plane. The first embodiments include variants that include a controller connected to a first camera to read image data therefrom, wherein the first detection arm includes a two-dimensional image detector of the camera, the controller reading and storing selected pixels of the image detector responsively to positions of the sheet beam waist, thereby causing the selected pixels to follow the traversal of the beam waist. The first embodiments include variants in which the controller controls the scanning components. The first embodiments include variants in which the scanning components include an electrically tunable lens configured to move the sheet beam waist along an axis of the illumination objective. The first embodiments include variants that include a traversing system, the controller configured to control the scanning components and to form an image slice from successive samples of the linear volume. The first embodiments include variants that include a second illumination arm identical to the first and configured to form a second sheet beam that intersects the first sheet beam. The first embodiments include variants in which the first and second illumination arm illumination objective optical axes each forms an angle to the surface of the first detection arm front focal plane. The first embodiments include variants in which each of the illumination arms includes a partial beam block which causes the sheet beam to be formed using a side portion of the illumination objective. The first embodiments include variants in which the angles of the sheet beams are responsive to the position of the beam block. The first embodiments include variants that include a controller connected to a traversal system, the controller is programmed to optically scan portions of a degree of freedom of the traversing system such that the traversing system can move in steps along an axis corresponding to the degree of freedom whose size is responsive to a dimension of the optical scan, to permit the capture of a sample larger than the dimension of the optical scan. The first embodiments include variants that include a second illumination arm and a second detection arm, both identical, respectively, to the first illumination and detection arms, the second illumination and detection arms is positioned on opposite sides of a movable stage. The first embodiments include variants that include cameras on each of the first and second illumination arms, a controller connected to first and second image detectors to read image data therefrom, wherein the first detection arms each includes a two-dimensional image detector of the camera, the controller reading and storing selected pixels of the image detector responsively to positions of the sheet beam waist, thereby causing the selected pixels to follow the traversal of the beam waist. The first embodiments include variants in which the controller is configured to control the sheet beams of the first and second illumination arms to maintain a distance between the intersections of the sheet beams and the front focal planes of the detection arms. The first embodiments include variants in which the controller is configured to control the sheet beams of the first and second illumination arms to maintain a distance between the intersections of the sheet beams and the front focal planes of the detection arms by maintain a phase difference between the scan cycling of the two sheet beams.


According to second embodiments, the disclosed subject matter includes a method of imaging an elongate volume within a sample. The method includes forming a sheet beam by passing a beam of light through a side of a first objective such that the beam is blocked from passing through a portion to a side of an optical axis of the first objective. The method includes detecting light from a linear volume illuminated by the sheet where the sheet intersects the focal plane of the first objective or a second objective. The forming includes scanning the illumination beam such that the linear volume traverses an axis that is perpendicular to an axis of the linear volume.


The second embodiments include variants in which the detecting includes sampling a line of pixels of a two-dimensional image plane of a camera, the line of pixels coinciding with an image of the linear volume. The second embodiments include variants in which the first objective or a second objective is the first objective. The second embodiments include variants in which the first objective or a second objective is a second objective. The second embodiments include variants in which the scanning includes traversing an axial position of the linear volume along an axis of the first objective. The second embodiments include variants in which the traversing an axial position includes actuating an electrically tunable lens. The second embodiments include variants that include repeating the forming and detecting on an opposite side of a single sample. The second embodiments include variants that include mechanically traversing a sample after each of the steps of scanning and repeating the forming and detecting at each position of the mechanically traversing and compositing the images corresponding to each scan to form a three-dimensional image of a sample.


According to third embodiments, the disclosed subject matter includes a microscope. A detection objective has optical axis is at a normal to a predefined plane defined by two axes of a traversing system. One or more illumination objectives are positioned and oriented to generate one or more light sheets at an angle oblique to the normal such that the light sheets enter the sample from the same side of the predefined plane as the detection objective.


The third embodiments include variants that include a detection arm that conveys light from the detection objective to a two-dimensional image sensor. The third embodiments include variants in which the image sensor is a sCMOS type sensor. The third embodiments include variants that include illumination arms that form beams that pass through the illumination objectives. The third embodiments include variants in which the illumination arms are configured to pass light asymmetrically through the illumination objectives such that the light sheets form an angle relative to the illumination objective optical axes. The third embodiments include variants in which the illumination arms each block a beam applied to a respective one of the illumination objectives. The third embodiments include variants that include a controller and scanning optics controlled by the controller in the illumination arms to cause an intersection between the light sheets and a front focal plane of the detection objective to traverse the front focal plane. The third embodiments include variants that include the controller captures a line of pixels of an imaging device corresponding to an image of an illuminated region located at the intersection.


According to embodiments, the disclosed subject matter includes a microscope. An imaging component has an imaging objective. A first light sheet projector is located on a same side of a sample region as the imaging component. The imaging component itself can include all the part of a conventional microscope, for example. The imaging objective and first light sheet projector have respective optical axes that intersect in the sample region. This occurs because of the way they are positioned and oriented in a common mounting with the microscope. A sample support is positioned and oriented with respect to the imaging objective such that, when a sample is placed on the sample support, the imaging objective optical axis is perpendicular to a surface of the sample.


In variations of the above microscope, the sample support is a generally flat element has a major plane and shaped to hold a slab-shaped sample, the imaging objective optical axis is perpendicular to the major plane. In further variations, which may be combined with the preceding variations, a second light sheet projector is also provided. The second light sheet projector has an optical axis forming an angle with the imaging objective optical axis equal to an angle formed by the first sheet projector optical axis with the imaging objective optical axis.


According to further embodiments, the disclosed subject matter includes a microscope with an imaging component, has an imaging objective, and a first light sheet projector located on a same side of a sample region. The imaging objective and first light sheet projector have respective axes that intersect in the sample region. A sample support is positioned to hold a sample in the sample region. The light sheet projector has light scanning and focusing optics to permit the selection of an axial position of a light sheet beam waist and the selection of a position of the light sheet along an axis perpendicular to the light sheet propagation direction. A controller is connected to control the light scanning and focusing optics to translate the beam waste along a linear path. The imaging objective optical axis are perpendicular to the linear path.


In variations of the foregoing microscope, the focusing optics include an electrically tunable lens (ETL). In further variations, the sample support is a generally flat element shaped to hold a slab-shaped sample. In further variations, a second light sheet projector has an optical axis forming an angle with the imaging objective optical axis equal to an angle formed by the first sheet projector optical axis with the imaging objective optical axis.


In still further variations, one or more further light sheet projectors and an imaging component are arranged on an opposite side of the sample region such that two opposite faces of a sample can be scanned. In still further variations, a translating stage is connected to move the sample support to permit the sequential scanning of portions of a sample.


According to embodiments, the disclosed subject matter includes a microscope with an imaging objective and a first light sheet projector located on a same side of a sample region. The imaging objective and first light sheet projector have respective optical axes that intersect in the sample region. A sample support is provided on a translating stage that translates the sample support along at least one linear axis. The translating stage is positioned and oriented with respect to the imaging objective such that the imaging objective optical axis is perpendicular to the at least one linear axis.


The sample support may be a generally flat element has a major plane and shaped to hold a slab-shaped sample, the imaging objective optical axis is perpendicular to the major plane. A second light sheet projector may be provided having an optical axis forming an angle with the imaging objective optical axis equal to an angle formed by the first sheet projector optical axis with the imaging objective optical axis.


Any of the microscope embodiments may include one or more further light sheet projectors and an imaging component arranged on an opposite side of the sample region such that two opposite faces of a sample can be scanned and/or a translating stage connected to move the sample support to permit the sequential scanning of portions of a sample.


According to embodiments, the disclosed subject matter includes an imaging instrument including a microscope with an objective has an optical axis. A first light beam projector has imaging optics separate from the microscope positioned to direct a beam of light that crosses the optical axis. The first light beam projector forms a sheet has a beam waist in the form of a line of maximum intensity. The first light beam projector has a scanning mechanism that scans the line of maximum intensity through a range of positions along a scan direction perpendicular to the line of maximum intensity. The microscope objective optical axis is perpendicular to the scan direction.


In the imaging instrument, the objective and the light beam projector are located on a same side of a sample volume such that an extended slab-shaped sample can be scanned by moving the sample relative to the objective and the light beam projector. In the imaging instrument and any variations thereof, a traversing system may be connected to one or both of the microscope and a sample support to move them such that a slab-shaped sample can be scanned. In the imaging instrument and any variations thereof, the traversing system is an X-Y traversing system. In the imaging instrument and any variations thereof, the traversing system is an X-Y traversing system, where X and Y axes are perpendicular to the optical axis. In the imaging instrument and any variations thereof, a controller may be connected to the traversing system and scanning mechanism to scan each of multiple tile segments of a sample using the scanning mechanism and to shift the sample support relative to the microscope to scan additional tile segment. In the imaging instrument and any variations thereof, the scanning mechanism includes electrically tunable lens (ETL). In the imaging instrument and any variations thereof, the ETL may change a position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet.


In the imaging instrument and any variations thereof, the scanning mechanism includes a light redirector that scans the sheet such that the line of maximum intensity traverses an axis perpendicular to a direction of propagation of the sheet. In the imaging instrument and any variations thereof, the scanning mechanism may include a light redirector that scans the sheet such that the line of maximum intensity traverses an axis perpendicular to a direction of propagation of the sheet. In the imaging instrument and any variations thereof, the scanning mechanism may include a light redirector that scans the sheet such that the line of maximum intensity traverses an axis perpendicular to a direction of propagation of the sheet.


In the imaging instrument and any variations thereof, the light redirector may include a galvo-motor. In the imaging instrument and any variations thereof, the light redirector may include a galvo-mirror. In the imaging instrument and any variations thereof, the scanning mechanism may scan in two axes, one to changes a position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet and one to change the position of the line of maximum intensity along an axis perpendicular to the direction of propagation of the sheet. In the imaging instrument and any variations thereof, the scanning mechanism may scan in two axes, one to changes a position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet and one to change the position of the line of maximum intensity along an axis perpendicular to the direction of propagation of the sheet. In the imaging instrument and any variations thereof, the scanning mechanism may include an electrically tunable lens (ETL) to change the position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet.


According to embodiments, the disclosed subject matter includes an imaging instrument that includes a microscope with an objective. A first light beam projector has imaging optics separate from the microscope positioned to direct a beam of light that crosses the optical axis. The first light beam projector forms a sheet that has a beam waist in the form of a line of maximum intensity. The first light beam projector has a scanning mechanism that scans the line of maximum intensity through a range of positions along a scan direction perpendicular to the line of maximum intensity.


In variations, the objective and the light beam projector are located on a same side of a sample volume such that an extended slab-shaped sample can be scanned by moving the sample relative to the objective and the light beam projector. According to embodiments, the disclosed subject matter includes the microscopes include a traversing system connected to one or both of the microscope and a sample support to move them such that a slab-shaped sample can be scanned. In variations, the traversing system is an X-Y traversing system. In variations, the traversing system is an X-Y-Z traversing system, where X and Y axes are parallel to a major plane of the sample volume and the Z axis is perpendicular thereto. In variations, a controller is connected to the traversing system and scanning mechanism to scan each of multiple tile segments of a sample using the scanning mechanism and to shift the sample support relative to the microscope to scan additional tile segment. In variations, the scanning mechanism includes electrically tunable lens (ETL). In variations, the ETL changes a position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet. In variations, the scanning mechanism includes a light redirector that scans the sheet such that the line of maximum intensity traverses an axis perpendicular to a direction of propagation of the sheet. In variations, the scanning mechanism includes a light redirector that scans the sheet such that the line of maximum intensity traverses an axis perpendicular to a direction of propagation of the sheet. In variations, the scanning mechanism includes a light redirector that scans the sheet such that the line of maximum intensity traverses an axis perpendicular to a direction of propagation of the sheet. In variations, the light redirector includes a galvo-motor. In variations, the light redirector includes a galvo-mirror. In variations, the scanning mechanism scans in two axes, one to changes a position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet and one to change the position of the line of maximum intensity along an axis perpendicular to the direction of propagation of the sheet. In variations, the scanning mechanism scans in two axes, one to changes a position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet and one to change the position of the line of maximum intensity along an axis perpendicular to the direction of propagation of the sheet. In variations, wherein the scanning mechanism includes electrically tunable lens (ETL) to change the position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet.


According to embodiments, the disclosed subject matter includes a method of acquiring a three-dimensional image of a sample. The method includes projecting a beam of light into a sample, the beam has a line of maximum intensity perpendicular to a direction of propagation of the beam and scanning the beam to scan the line of maximum intensity along a path oblique to both the direction of propagation and perpendicular to it. The method may include capturing images of the line on respective portions of an imaging transducer. The method may be such that, additionally or alternatively, such that the imaging transducer includes a camera sensor. The method may be such that, additionally or alternatively, such that the capturing includes imaging light from the line using a microscope. The method may be such that, additionally or alternatively, such that the capturing includes receiving and imaging secondary light induced by the line of maximum intensity. The method may be such that, additionally or alternatively, such that the capturing includes receiving and imaging a region of fluorescence induced by the line of maximum intensity. The method may be such that, additionally or alternatively, such that the scanning includes mechanically moving the end of a wave guide. The method may include, additionally or alternatively, moving the sample relative to the microscope and the beam of light and repeating the scanning and capturing for a different region of the sample. The method may include, additionally or alternatively, creating two-dimensional images from the capturing and stitching them together to form larger composite images by matching features of the edges of the images. The method may be such that, additionally or alternatively, such that the moving includes moving in one or all of three orthogonal directions. The method may be such that, additionally or alternatively, such that the moving includes moving in all of three orthogonal directions to traverse a three-dimensional volume of positions.


The method may include, additionally or alternatively, changing the focus of an imaging device to optically discriminate multiple depths of the sample after each scan of the scanning. The method may be such that, additionally or alternatively, such that the light sheet projector includes a GRIN lens as an objective.


According to embodiments, the disclosed subject matter includes a microscopy method that includes positioning a detection objective oriented with its optical axis perpendicular to a facing surface of a sample slab. The method further includes positioning an excitation objective oriented to form an acute angle with the detection objective optical axis. The positioning a detection objective and the positioning an excitation objective is such that the detection and excitation objectives is on a same side of the sample slab. The method further includes applying light off-center to the back aperture of the excitation objective such that a beam emerges at an angle with respect to an optical axis of the excitation objective and with a major axis parallel to its direction of propagation that forms a larger angle than the acute angle.


The method may be such that, additionally or alternatively, such that the applying includes partially optically blocking the back aperture. The method may be such that, additionally or alternatively, such that the major axis forms a more acute angle with the facing surface than the detection objective optical axis.


According to embodiments, the disclosed subject matter includes a microscopy method that includes arranging a detection objective of a microscope with its optical axis normal to a surface of a sample slab and injecting light along directions forming equal and opposite angles with the detection objective optical axis. The method includes imaging light resulting from the injecting using the microscope. The method may be such that, additionally or alternatively, such that the light resulting from the injecting includes fluorescence. The method may be such that, additionally or alternatively, such that the injecting results in a single line-shaped region of maximum light intensity in the sample. The method may include, additionally or alternatively, scanning the region perpendicular to a major axis thereof to trace out a planar segment of the sample while sampling the light resulting from the injecting using a light sensor.


The method may be such that, additionally or alternatively, such that the sensor includes a camera. The method may be such that, additionally or alternatively, such that the imaging includes receiving the resulting slight through a microscope. The method may be such that, additionally or alternatively, such that the detection objective is an objective of a microscope.


The method may, additionally or alternatively, include scanning the region perpendicular to a major axis thereof to trace out a planar segment of the sample that is parallel to the sample surface while sampling the light resulting from the injecting using a light sensor.


According to embodiments, the disclosed subject matter includes a microscope with at least two excitation optical elements arranged to form and direct respective sheets of light such that they intersect to form an illuminated line of intersection in a sample region, the sheets has major planes that form angles of at least 75 degrees. A detection optical element is arranged with respect to the excitation optical elements with an optical axis forming equal angles with the major planes of the sheets.


In variations of the microscope, at least two excitation optical elements include objective lenses. In further variations of the microscope, at least two excitation optical elements include objective lenses each has an adjustable partial beam block to cause the sheet beam to be emerge from a side portion of the objective. In further variations of the microscope at least two excitation optical elements include GRIN lenses. In further variations of the microscope the two excitation optical elements include scanning optical elements arranged to cause the illuminated line to traverse the sample region. In further variations of the microscope the two excitation optical elements include scanning optical elements arranged to cause the illuminated line to traverse the sample region along a focal plane of the detection optical element. In further variations of the microscope a traversing system is provided and the controller is configured to control scanning components and to form an image slice from successive detections of the sample region.


According to embodiments, the disclosed subject matter includes a microscope. First and second imaging components, each have an imaging objective, and first and second light sheet projectors each located on a same side of a sample region as a respective on of the first and second imaging components. Each imaging objective and each light sheet projector has respective axes that intersect in the sample region. A sample support is positioned to hold a sample in the sample region. Each light sheet projector has light scanning and focusing optics to permit the selection of an axial position of a light sheet beam waist and the selection of a position of the light sheet along an axis perpendicular to the light sheet propagation direction. A controller is connected to control the light scanning and focusing optics to translate the beam waste of each light sheet projector independently along a respective linear path.


In variations, the imaging objective optical axes are perpendicular to a respective one of the linear paths. In variations, the imaging objective optical axes are perpendicular to a both of the linear paths. In variations, the focusing optics include an electrically tunable lens (ETL). In variations, the sample support is a generally flat element shaped to hold a slab-shaped sample. It will be appreciated that the modules, processes, systems, and sections described above can be implemented in hardware, hardware programmed by software, software instruction stored on a non-transitory computer readable medium or a combination of the above. For example, a method for capturing three dimensional optical images can be implemented, for example, using a processor configured to execute a sequence of programmed instructions stored on a non-transitory computer readable medium. For example, the processor can include, but not be limited to, a personal computer or workstation or other such computing system that includes a processor, microprocessor, microcontroller device, or is comprised of control logic including integrated circuits such as, for example, an Application Specific Integrated Circuit (ASIC). The instructions can be compiled from source code instructions provided in accordance with a programming language such as Java, C++, C#.net or the like. The instructions can also comprise code and data objects provided in accordance with, for example, the Visual Basic™ language, LabVIEW, or another structured or object-oriented programming language. The sequence of programmed instructions and data associated therewith can be stored in a non-transitory computer-readable medium such as a computer memory or storage device which may be any suitable memory apparatus, such as, but not limited to read-only memory (ROM), programmable read-only memory (PROM), electrically erasable programmable read-only memory (EEPROM), random-access memory (RAM), flash memory, disk drive and the like.


Furthermore, the modules, processes, systems, and sections can be implemented as a single processor or as a distributed processor. Further, it should be appreciated that the steps mentioned above may be performed on a single or distributed processor (single and/or multi-core). Also, the processes, modules, and sub-modules described in the various figures of and for embodiments above may be distributed across multiple computers or systems or may be co-located in a single processor or system. Exemplary structural embodiment alternatives suitable for implementing the modules, sections, systems, means, or processes described herein are provided below.


The modules, processors or systems described above can be implemented as a programmed general purpose computer, an electronic device programmed with microcode, a hard-wired analog logic circuit, software stored on a computer-readable medium or signal, an optical computing device, a networked system of electronic and/or optical devices, a special purpose computing device, an integrated circuit device, a semiconductor chip, and a software module or object stored on a computer-readable medium or signal, for example.


Embodiments of the method and system (or their sub-components or modules), may be implemented on a general-purpose computer, a special-purpose computer, a programmed microprocessor or microcontroller and peripheral integrated circuit element, an ASIC or other integrated circuit, a digital signal processor, a hardwired electronic or logic circuit such as a discrete element circuit, a programmed logic circuit such as a programmable logic device (PLD), programmable logic array (PLA), field-programmable gate array (FPGA), programmable array logic (PAL) device, or the like. In general, any process capable of implementing the functions or steps described herein can be used to implement embodiments of the method, system, or a computer program product (software program stored on a non-transitory computer readable medium).


Furthermore, embodiments of the disclosed method, system, and computer program product may be readily implemented, fully or partially, in software using, for example, object or object-oriented software development environments that provide portable source code that can be used on a variety of computer platforms. Alternatively, embodiments of the disclosed method, system, and computer program product can be implemented partially or fully in hardware using, for example, standard logic circuits or a very-large-scale integration (VLSI) design. Other hardware or software can be used to implement embodiments depending on the speed and/or efficiency requirements of the systems, the particular function, and/or particular software or hardware system, microprocessor, or microcomputer being utilized. Embodiments of the method, system, and computer program product can be implemented in hardware and/or software using any known or later developed systems or structures, devices and/or software by those of ordinary skill in the applicable art from the function description provided herein and with a general basic knowledge of control systems, kinematic design, optics, microscopy and/or computer programming arts.


Moreover, embodiments of the disclosed method, system, and computer program product can be implemented in software executed on a programmed general purpose computer, a special purpose computer, a microprocessor, or the like.


It is, thus, apparent that there is provided, in accordance with the present disclosure, optical imaging systems, devices, and methods. Many alternatives, modifications, and variations are enabled by the present disclosure. Features of the disclosed embodiments can be combined, rearranged, omitted, etc., within the scope of the invention to produce additional embodiments. Furthermore, certain features may sometimes be used to advantage without a corresponding use of other features. Accordingly, Applicants intend to embrace all such alternatives, modifications, equivalents, and variations that are within the spirit and scope of the present invention.

Claims
  • 1. An microscope comprising: an imaging component, with an imaging objective, and a first light sheet projector located on a same side of a sample region;the imaging objective and first light sheet projector having respective axes that intersect in the sample region at an angle of less than 90 degrees;a sample support positioned to hold a sample in said sample region;the first light sheet projector having light scanning and focusing optics to permit the selection of an axial position of a light sheet beam waist and the selection of a position of the light sheet along an axis perpendicular to the light sheet propagation direction;a controller connected to control the light scanning and focusing optics to translate the beam waist along a linear path;the imaging objective optical axis being perpendicular to said linear path.
  • 2. The microscope of claim 1, wherein the focusing optics include an electrically tunable lens (ETL).
  • 3. The microscope of claim 1, wherein the sample support is a generally flat element shaped to hold a slab-shaped sample.
  • 4. The microscope of claim 1, further comprising a second light sheet projector with an optical axis forming an angle with said imaging objective optical axis equal to an angle formed by said first light sheet projector optical axis with said imaging objective optical axis.
  • 5. The microscope of claim 1, further comprising one or more further light sheet projectors and an imaging component arranged on an opposite side of the sample region such that two opposite faces of a sample can be scanned.
  • 6. The microscope of claim 1, further comprising a translating stage connected to move said sample support to permit the sequential scanning of portions of a sample.
  • 7. An imaging instrument, comprising: a microscope with an objective having an optical axis;a first light beam projector with imaging optics separate from said microscope positioned to direct a beam of light that crosses said optical axis at an angle of less than 90 degrees, wherein the objective and the light beam projector are located on a same side of a sample volume; andthe first light beam projector forming a sheet having a beam waist in the form of a line of maximum intensity;the first light beam projector having a scanning mechanism that scans the line of maximum intensity through a range of positions along a scan direction perpendicular to the line of maximum intensity.
  • 8. The imaging instrument of claim 7, wherein the microscope objective has an optical axis that is perpendicular to the scan direction.
  • 9. The imaging instrument of claim 7, wherein the objective and the light beam projector are positioned such that an extended slab-shaped sample can be scanned by moving the sample relative to the objective and the light beam projector.
  • 10. The imaging instrument of claim 7, wherein the scanning mechanism scans in two axes, one to change a position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet and one to change the position of the line of maximum intensity along an axis perpendicular to the direction of propagation of the sheet.
  • 11. The imaging instrument of claim 7, wherein the angle of less than 90 degrees is as close to 90 degrees as allowed by the geometry.
  • 12. The imaging instrument of claim 7, wherein the angle of less than 90 degrees is between 37.5 and 75 degrees.
  • 13. The imaging instrument of claim 7, further comprising a traversing system connected to one or both of the microscope and a sample support to move them such that a slab-shaped sample can be scanned.
  • 14. The imaging instrument of claim 13, wherein the traversing system is an X-Y traversing system.
  • 15. The imaging instrument of claim 13, wherein the traversing system is an X-Y-Z traversing system, where X and Y axes are parallel to a major plane of the sample volume and the Z axis is perpendicular thereto.
  • 16. The imaging instrument of claim 13, further comprising a controller connected to the traversing system and scanning mechanism to scan each of multiple tile segments of a sample using the scanning mechanism and to shift the sample support relative to the microscope to scan additional tile segment.
  • 17. The imaging instrument of claim 7, wherein the scanning mechanism includes electrically tunable lens (ETL).
  • 18. The imaging instrument of claim 17, wherein the ETL changes a position of the line of maximum intensity along a length of the sheet in the direction of propagation of the sheet.
  • 19. The imaging instrument of claim 18, wherein the scanning mechanism includes a light redirector that scans the sheet such that the line of maximum intensity traverses an axis perpendicular to a direction of propagation of the sheet.
  • 20. The imaging instrument of claim 17, wherein the scanning mechanism includes a light redirector that scans the sheet such that the line of maximum intensity traverses an axis perpendicular to a direction of propagation of the sheet.
  • 21. The imaging instrument of claim 20, wherein the light redirector includes a galvo-motor.
CROSS REFERENCE TO RELATED APPLICATIONS

This Application is a US national stage filing under 35 U.S.C. § 371 of International Application No. PCT/US2017/061165, filed Nov. 10, 2017, which claims the benefit of U.S. Provisional Application 62/420,349 filed Nov. 10, 2016, and U.S. Provisional Application 62/473,944, filed Mar. 20, 2017, each of which is incorporated herein by reference in its entirety.

PCT Information
Filing Document Filing Date Country Kind
PCT/US2017/061165 11/10/2017 WO
Publishing Document Publishing Date Country Kind
WO2018/089839 5/17/2018 WO A
US Referenced Citations (486)
Number Name Date Kind
4149074 Schliepe et al. Apr 1979 A
4181436 Wasmund et al. Jan 1980 A
4218112 Ruker Aug 1980 A
4284897 Sawamura et al. Aug 1981 A
4349242 Ogura Sep 1982 A
4446548 Bouwhuis et al. May 1984 A
4537477 Takagi et al. Aug 1985 A
4604523 Knowles et al. Aug 1986 A
4627730 Jungerman et al. Dec 1986 A
4631581 Carlsson Dec 1986 A
4691103 Poole et al. Sep 1987 A
4700298 Palcic et al. Oct 1987 A
4732473 Bille et al. Mar 1988 A
4733063 Kimura et al. Mar 1988 A
4734578 Horikawa Mar 1988 A
4745270 Horikawa et al. May 1988 A
4791288 Kinameri et al. Dec 1988 A
4800269 Horikawa Jan 1989 A
4806004 Wayland Feb 1989 A
4812748 Brust et al. Mar 1989 A
4824229 Narita et al. Apr 1989 A
4845552 Jaggi et al. Jul 1989 A
4861982 Smid et al. Aug 1989 A
4873434 See et al. Oct 1989 A
4914293 Hayashi et al. Apr 1990 A
4954722 Fine et al. Sep 1990 A
4972258 Wolf et al. Nov 1990 A
4987303 Takase et al. Jan 1991 A
5033834 Corder et al. Jul 1991 A
5038035 Nishimura et al. Aug 1991 A
5043570 Takabayashi Aug 1991 A
5081349 Iwasaki Jan 1992 A
5081350 Iwasaki et al. Jan 1992 A
5086222 Shibuya Feb 1992 A
5103095 Elings et al. Apr 1992 A
5168157 Kimura Dec 1992 A
5172002 Marshall Dec 1992 A
5184012 Yamamoto Feb 1993 A
5204531 Elings et al. Apr 1993 A
5214279 Hakamata May 1993 A
5218195 Hakamata Jun 1993 A
5225923 Montagu Jul 1993 A
5225929 Ulanowski Jul 1993 A
5250965 Abe et al. Oct 1993 A
5260562 Bearden et al. Nov 1993 A
5276324 Ohtaki et al. Jan 1994 A
5276325 Todokoro et al. Jan 1994 A
5306919 Elings et al. Apr 1994 A
5343038 Nishiwaki et al. Aug 1994 A
5355252 Haraguchi Oct 1994 A
5376790 Linker et al. Dec 1994 A
5450501 Smid Sep 1995 A
5508517 Onuki et al. Apr 1996 A
5535052 Jorgens Jul 1996 A
5617500 Shionoya et al. Apr 1997 A
5621532 Ooki et al. Apr 1997 A
5672816 Park et al. Sep 1997 A
5693938 Marchman et al. Dec 1997 A
5777732 Hanninen et al. Jul 1998 A
5790710 Price et al. Aug 1998 A
5828459 Silberberg Oct 1998 A
5835228 Okazaki et al. Nov 1998 A
5835265 Mammone Nov 1998 A
5929439 Fodokoro et al. Jul 1999 A
5930033 Inoue et al. Jul 1999 A
5945669 Arai Aug 1999 A
5978155 Suenaga Nov 1999 A
6034815 Shimada Mar 2000 A
6037583 Moehler et al. Mar 2000 A
6043932 Kusunose Mar 2000 A
6049421 Raz et al. Apr 2000 A
6094300 Kashima et al. Jul 2000 A
6104539 Togino Aug 2000 A
6127681 Sato et al. Oct 2000 A
6144028 Kley Nov 2000 A
6147797 Lee Nov 2000 A
6166385 Webb et al. Dec 2000 A
6167173 Schoeppe et al. Dec 2000 A
6184535 Kashima et al. Feb 2001 B1
6222961 Engelhardt et al. Apr 2001 B1
6262423 Hell et al. Jul 2001 B1
6269206 Simon et al. Jul 2001 B1
6278555 Stock et al. Aug 2001 B1
6320174 Tafas et al. Nov 2001 B1
6337474 Morizono Jan 2002 B1
6337479 Kley Jan 2002 B1
6356088 Simon et al. Mar 2002 B1
6381074 Koshida Apr 2002 B2
6426834 Braunecker et al. Jul 2002 B1
6433929 Sasaki Aug 2002 B1
6441356 Mandella et al. Aug 2002 B1
6449039 Bouzid Sep 2002 B1
6466040 Simon et al. Oct 2002 B1
6521899 Wolleschensky Feb 2003 B1
6525812 Hartmann et al. Feb 2003 B1
6555802 Osipchuk et al. Apr 2003 B2
6567164 Birk et al. May 2003 B2
6573500 Yeremin et al. Jun 2003 B2
6580554 Engelhardt et al. Jun 2003 B2
6594074 Wolleschensky et al. Jul 2003 B1
6608294 Nikitin et al. Aug 2003 B2
6608295 Engelhardt Aug 2003 B2
6608717 Medford et al. Aug 2003 B1
6611643 Birk et al. Aug 2003 B2
6617761 Ando et al. Sep 2003 B2
6628385 Osipchuk et al. Sep 2003 B1
6642504 Cathey, Jr. Nov 2003 B2
6654166 Birk et al. Nov 2003 B2
6657187 Engelhardt Dec 2003 B2
6674573 Suzuki Jan 2004 B2
6686587 Nikitin et al. Feb 2004 B2
6693742 Winterot et al. Feb 2004 B1
6693945 Shimada Feb 2004 B1
6703621 Wolleschensky Mar 2004 B2
6710316 Mandella et al. Mar 2004 B2
6710337 Engelhardt et al. Mar 2004 B2
6710918 Birk et al. Mar 2004 B2
6711283 Soenksen Mar 2004 B1
6717723 Arai Apr 2004 B2
6717726 Boehm et al. Apr 2004 B2
6721690 Olschewski Apr 2004 B2
6754000 Engelhardt et al. Jun 2004 B2
6771417 Wolleschensky et al. Aug 2004 B1
6788456 Knebel Sep 2004 B2
6796699 Birk et al. Sep 2004 B2
6813050 Chen et al. Nov 2004 B2
6824056 Karin Nov 2004 B1
6848825 Simon et al. Feb 2005 B1
6850363 Wendenburg et al. Feb 2005 B1
6852964 Engelhardt et al. Feb 2005 B2
6853455 Dixon et al. Feb 2005 B1
6856391 Garab et al. Feb 2005 B2
6882470 Bloedom et al. Apr 2005 B2
6900435 Lewis May 2005 B1
6900935 Engelhardt et al. May 2005 B2
6906312 Engelhardt Jun 2005 B2
6909542 Sasaki Jun 2005 B2
6914236 Hoffmann Jul 2005 B2
6927902 Schoeppe Aug 2005 B2
6934020 Shimada Aug 2005 B2
6940649 Dowski, Jr. Sep 2005 B2
6943332 Suzuki Sep 2005 B2
6952006 Moellmann Oct 2005 B2
6958858 Engelhardt et al. Oct 2005 B2
6963398 Sasaki et al. Nov 2005 B2
6967725 Denk et al. Nov 2005 B2
6967772 Harris Nov 2005 B2
6978215 Nikitin Dec 2005 B2
6987274 Street et al. Jan 2006 B1
7002739 Awamura Feb 2006 B2
7009171 Sasaki Mar 2006 B2
7009763 Wolleschensky Mar 2006 B1
7015485 Kitagawa Mar 2006 B2
7034317 Olszak et al. Apr 2006 B2
7035478 Crandall et al. Apr 2006 B2
7050208 Overbeck May 2006 B2
7057806 Atkinson Jun 2006 B2
7079256 Li Jul 2006 B2
7088517 Spiecker Aug 2006 B2
7092086 Knebel Aug 2006 B2
7098447 Moellmann Aug 2006 B2
7110118 Ünlü et al. Sep 2006 B2
7115885 Hell Oct 2006 B2
7116437 Weinstein et al. Oct 2006 B2
7123790 Rosman et al. Oct 2006 B2
7129486 Spizig et al. Oct 2006 B2
7130115 Olszak et al. Oct 2006 B2
7141802 Takeyama et al. Nov 2006 B2
7142308 Somekh et al. Nov 2006 B2
7151633 Storz et al. Dec 2006 B2
7154084 Hara Dec 2006 B2
7158224 Montagu Jan 2007 B2
7184610 Weinstein et al. Feb 2007 B2
7187493 Sasaki et al. Mar 2007 B2
7187494 Nishiwaki et al. Mar 2007 B2
7193775 Olszak et al. Mar 2007 B2
7202953 Mueller et al. Apr 2007 B1
7212337 Lange et al. May 2007 B2
7212338 Weyh et al. May 2007 B2
7218762 Olschewski May 2007 B2
7233437 Hirata et al. Jun 2007 B2
7253420 Motomura Aug 2007 B2
7253950 Araya Aug 2007 B2
7257289 Dlschewski Aug 2007 B2
7260253 Rahn et al. Aug 2007 B2
7271382 Engelmann et al. Sep 2007 B2
7271952 Suzuki et al. Sep 2007 B2
7274446 Wolleschensky et al. Sep 2007 B2
7283297 Knebel Oct 2007 B2
7298461 Cremer et al. Nov 2007 B2
7301696 Wolleschensky Nov 2007 B2
7304790 Kawano et al. Dec 2007 B2
7339148 Kawano et al. Mar 2008 B2
7342219 Araya et al. Mar 2008 B2
7385165 Aikawa Jun 2008 B2
7385709 Plamann et al. Jun 2008 B2
7388714 Liang et al. Jun 2008 B2
7394482 Olschewski Jul 2008 B2
7397601 Laudo Jul 2008 B2
7411166 Wolleschensky et al. Aug 2008 B2
7450243 Marks et al. Nov 2008 B2
7457331 Riedmann et al. Nov 2008 B2
7468834 Wolleschensky Dec 2008 B2
7477449 Knebel et al. Jan 2009 B2
7485856 Kley Feb 2009 B2
7489828 Asad et al. Feb 2009 B2
7508582 Lauer Mar 2009 B2
7511890 Ulrich et al. Mar 2009 B2
7518652 Olson et al. Apr 2009 B2
7518764 Osborne et al. Apr 2009 B2
7518790 Sase et al. Apr 2009 B2
7535640 Totzeck et al. May 2009 B2
7542597 Rahn et al. Jun 2009 B2
7547874 Liang Jun 2009 B2
7551350 Iketaki et al. Jun 2009 B2
7554669 Buckland et al. Jun 2009 B2
7556968 Ando et al. Jul 2009 B2
7560709 Kimura et al. Jul 2009 B2
7561327 Riedmann Jul 2009 B2
7564621 Kawano et al. Jul 2009 B2
7580185 Haisch et al. Aug 2009 B2
7589891 Kawasaki Sep 2009 B2
7630113 Sase et al. Dec 2009 B2
7633053 Wolleschensky et al. Dec 2009 B2
7643155 Marks et al. Jan 2010 B2
7659991 Seitz Feb 2010 B2
7660035 Böhm et al. Feb 2010 B2
7668362 Olson et al. Feb 2010 B2
7696996 Hattori et al. Apr 2010 B2
7728270 Wolleschensky et al. Jun 2010 B2
7733565 Hattori et al. Jun 2010 B2
7742213 Potsaid et al. Jun 2010 B2
7755841 Christenson et al. Jul 2010 B2
7773278 Chu et al. Aug 2010 B2
7796149 Steinert Sep 2010 B2
7802027 Schek Sep 2010 B2
7804642 Nagasawa et al. Sep 2010 B2
7820958 Ishihara et al. Oct 2010 B2
7843572 Tearney et al. Nov 2010 B2
7865007 Yamada Jan 2011 B2
7869039 Akao et al. Jan 2011 B2
7872799 Wolleschensky Jan 2011 B2
7873241 Storz et al. Jan 2011 B2
7885448 Bartels Feb 2011 B2
7903329 Yoshida et al. Mar 2011 B2
7915575 Yokoi Mar 2011 B2
7918555 Sverdrup et al. Apr 2011 B2
7943889 Vogt May 2011 B2
7957057 Sase et al. Jun 2011 B2
7973927 Raicu et al. Jul 2011 B2
7978405 Laudo Jul 2011 B2
7978894 Soenksen Jul 2011 B2
7986456 Frekers et al. Jul 2011 B2
8049873 Hauger et al. Nov 2011 B2
8055042 Soenksen Nov 2011 B2
8085402 Ichimura et al. Dec 2011 B2
8094303 Denney et al. Jan 2012 B2
8094902 Crandall et al. Jan 2012 B2
8115164 Netz et al. Feb 2012 B2
8119960 Fukuyama Feb 2012 B2
8139288 Osborne et al. Mar 2012 B2
8159744 Tsurumune Apr 2012 B2
8164622 Crandall Apr 2012 B2
8175452 Staker et al. May 2012 B1
8189201 Haisch et al. May 2012 B2
8237797 Hayashi et al. Aug 2012 B2
8238387 Yamazoe Aug 2012 B2
8254020 Holy et al. Aug 2012 B2
8254023 Watson et al. Aug 2012 B2
8263946 Gugel Sep 2012 B2
8275226 Berman Sep 2012 B2
8284483 Beaurepaire et al. Oct 2012 B2
8362448 Wolleschensky et al. Jan 2013 B2
8368035 Seibel et al. Feb 2013 B2
8384901 Yudakov et al. Feb 2013 B2
8385619 Soenksen Feb 2013 B2
8440969 Moore et al. May 2013 B2
8441633 Truong et al. May 2013 B2
8450674 Yang et al. May 2013 B2
8456725 Toomre et al. Jun 2013 B2
8526091 Ito et al. Sep 2013 B2
8558998 Feldkhun et al. Oct 2013 B2
8565499 Zhao et al. Oct 2013 B2
8575570 Choi et al. Nov 2013 B2
8643924 Okada Feb 2014 B2
8654441 Jalali et al. Feb 2014 B2
8711211 Betzig Apr 2014 B2
8711473 Hirata Apr 2014 B2
8743195 Najmabadi et al. Jun 2014 B2
8755579 Soenksen Jun 2014 B2
8759745 Klose et al. Jun 2014 B2
8773760 Gmitro et al. Jul 2014 B2
8786693 Kihara et al. Jul 2014 B2
8792156 Kieu et al. Jul 2014 B1
8830573 Cui et al. Sep 2014 B2
8841591 Wilde et al. Sep 2014 B2
8878923 Henderson et al. Nov 2014 B2
8896918 Dixon Nov 2014 B2
8908270 Murayama et al. Dec 2014 B2
8948846 Pan Feb 2015 B2
8958148 Honda Feb 2015 B2
8964020 Hersee Feb 2015 B2
8964288 Cooper Feb 2015 B2
8965196 Staker et al. Feb 2015 B2
8982206 Raicu et al. Mar 2015 B2
8982455 Redford Mar 2015 B2
9001321 Fujita et al. Apr 2015 B2
9030548 Zhou et al. May 2015 B2
9036232 Birk et al. May 2015 B2
9041793 Bugge et al. May 2015 B2
9057879 Knebel et al. Jun 2015 B2
9063335 Sommer et al. Jun 2015 B2
9081173 Vizi et al. Jul 2015 B2
9091861 Kishimoto Jul 2015 B2
9103721 Raicu et al. Aug 2015 B2
9104030 Kieu et al. Aug 2015 B2
9110301 Lippert et al. Aug 2015 B2
9122070 Suzuki Sep 2015 B2
9134519 Berman Sep 2015 B2
9149180 Muto et al. Oct 2015 B2
9153928 Fermann et al. Oct 2015 B2
9170151 Kuwabara et al. Oct 2015 B2
9201008 Thériault et al. Dec 2015 B2
9201231 Honda Dec 2015 B2
9223125 Betzig Dec 2015 B2
9250061 Lorbeer et al. Feb 2016 B2
9261689 Shimada et al. Feb 2016 B2
9268133 Takahashi Feb 2016 B2
9285575 Xie et al. Mar 2016 B2
9304308 Goruganthu Apr 2016 B2
9304309 Okada Apr 2016 B2
9335253 Ode May 2016 B2
9347871 Fujinuma et al. May 2016 B2
9360660 Yi et al. Jun 2016 B2
9383565 Shi et al. Jul 2016 B2
9386211 Soenksen Jul 2016 B2
9404857 Popescu et al. Aug 2016 B2
9429740 Winterot et al. Aug 2016 B2
9448395 Betzig Sep 2016 B2
9464995 Edelmann et al. Oct 2016 B2
9477074 Betzig Oct 2016 B2
9478393 Potocek et al. Oct 2016 B2
9494777 Rumyantsev et al. Nov 2016 B2
9507136 Cooper et al. Nov 2016 B2
9509956 Piestun et al. Nov 2016 B2
9519127 Matsumoto et al. Dec 2016 B2
9541750 Bouzid Jan 2017 B2
9551568 Zhou et al. Jan 2017 B2
9551862 Mizuta Jan 2017 B2
9563046 Hohng et al. Feb 2017 B2
9564291 Own et al. Feb 2017 B1
9581497 Mikami Feb 2017 B2
9594237 Schwedt et al. Mar 2017 B2
9625694 Dohi Apr 2017 B2
9625696 Hashimoto et al. Apr 2017 B2
9632301 Damaskinos et al. Apr 2017 B2
9634454 Kieu et al. Apr 2017 B1
9645376 Fischer et al. May 2017 B1
9645378 Hilbert et al. May 2017 B2
9645380 Wartmann May 2017 B2
9690974 Obrien et al. Jun 2017 B2
9696531 Hersee Jul 2017 B2
9696532 Kitagawa Jul 2017 B2
9696536 Nobis Jul 2017 B2
9709786 Fukutake Jul 2017 B2
9709789 Dam et al. Jul 2017 B2
9720218 Cui et al. Aug 2017 B2
9721326 Piché et al. Aug 2017 B2
9726878 Krattiger Aug 2017 B2
9915519 Wu et al. Mar 2018 B2
9939243 Brotman Apr 2018 B2
20010015411 Ohdaira et al. Aug 2001 A1
20020018291 Fukuyama Feb 2002 A1
20020159146 Leimbach et al. Oct 2002 A1
20020176076 Bouzid et al. Nov 2002 A1
20030058530 Kawano Mar 2003 A1
20030214707 Engelhardt Nov 2003 A1
20040051030 Olszak et al. Mar 2004 A1
20040080818 Olschewski Apr 2004 A1
20040115683 Medford et al. Jun 2004 A1
20040133112 Rajadhyaksha Jul 2004 A1
20040218263 Brugal Nov 2004 A1
20040238730 Langowski et al. Dec 2004 A1
20050024718 Sase et al. Feb 2005 A1
20050058372 Engelmann et al. Mar 2005 A1
20050072913 Lange et al. Apr 2005 A1
20050078362 Borlinghaus Apr 2005 A1
20050099682 Lauer May 2005 A1
20050207005 Kawano Sep 2005 A1
20060011812 Wolleschensky et al. Jan 2006 A1
20060012864 Funk et al. Jan 2006 A1
20060012891 Goelles et al. Jan 2006 A1
20060018013 Suzuki et al. Jan 2006 A1
20070047071 Honda et al. Mar 2007 A1
20070081222 Bartzke et al. Apr 2007 A1
20070109633 Stelzer May 2007 A1
20070121198 Suzuki et al. May 2007 A1
20070121200 Suzuki et al. May 2007 A1
20070121473 Lange et al. May 2007 A1
20070159689 Schau et al. Jul 2007 A1
20070171433 Tearney et al. Jul 2007 A1
20070183029 Iketaki Aug 2007 A1
20070238955 Tearney et al. Oct 2007 A1
20070246659 Bloos et al. Oct 2007 A1
20080013166 Haisch et al. Jan 2008 A1
20080158668 Ouchi et al. Jul 2008 A1
20080180790 Tafas et al. Jul 2008 A1
20080204766 Uhl Aug 2008 A1
20090174935 Szulczewski et al. Jul 2009 A1
20090303584 Pacholik et al. Dec 2009 A1
20100014156 Iketaki Jan 2010 A1
20100053743 Galimberti et al. Mar 2010 A1
20100265575 Lippert et al. Oct 2010 A1
20110025837 Vossen et al. Feb 2011 A1
20110122488 Truong et al. May 2011 A1
20110134254 Hulsken et al. Jun 2011 A1
20110194174 Laudo Aug 2011 A1
20110216401 Curry Sep 2011 A1
20120050733 Takimoto Mar 2012 A1
20120206798 Knop et al. Aug 2012 A1
20120287244 Bennett et al. Nov 2012 A1
20120320438 Knebel et al. Dec 2012 A1
20130057953 Yokoi Mar 2013 A1
20130229663 Yang et al. Sep 2013 A1
20130286181 Betzig et al. Oct 2013 A1
20140099659 Keller Apr 2014 A1
20140118529 Zheng et al. May 2014 A1
20140126046 Shroff et al. May 2014 A1
20140192406 Bathe Jul 2014 A1
20150098126 Keller Apr 2015 A1
20150116822 Mori Apr 2015 A1
20150253560 Otte et al. Sep 2015 A1
20150286042 Hilbert et al. Oct 2015 A1
20150338625 Sieckmann et al. Nov 2015 A1
20150370060 Williams et al. Dec 2015 A1
20160041200 Fine Feb 2016 A1
20160048014 Knebel et al. Feb 2016 A1
20160054226 Gandolfi et al. Feb 2016 A1
20160103318 Du et al. Apr 2016 A1
20160123812 Kyogaku May 2016 A1
20160123813 Kyogaku May 2016 A1
20160139387 Virk et al. May 2016 A1
20160139394 Taniguchi et al. May 2016 A1
20160154236 Siebenmorgen et al. Jun 2016 A1
20160170193 Ue Jun 2016 A1
20160195705 Betzig et al. Jul 2016 A1
20160209588 Steinert et al. Jul 2016 A1
20160209646 Hattori et al. Jul 2016 A1
20160220120 Kim et al. Aug 2016 A1
20160259163 Hoegele et al. Sep 2016 A1
20160282596 Ciobota et al. Sep 2016 A1
20160299326 Eggert et al. Oct 2016 A1
20160341668 Gupta et al. Nov 2016 A1
20160363538 Dutertre et al. Dec 2016 A1
20160363563 Fukushima Dec 2016 A1
20160370570 Foelling Dec 2016 A1
20170038291 Chen Feb 2017 A1
20170038575 Pretorius Feb 2017 A1
20170059840 Tamano Mar 2017 A1
20170059841 Trulson et al. Mar 2017 A1
20170168280 Schumann et al. Jun 2017 A1
20170184830 Akahane Jun 2017 A1
20170199362 Schwedt et al. Jul 2017 A1
20170219809 Wald et al. Aug 2017 A1
20170254749 Yun Sep 2017 A1
20170261736 Abe Sep 2017 A1
20170285315 Amano et al. Oct 2017 A1
20170299553 Fukushima et al. Oct 2017 A1
20170301101 Stoppe et al. Oct 2017 A1
20170307864 Daugela Oct 2017 A1
20170315339 Schwedt et al. Nov 2017 A1
20170322408 Iguchi Nov 2017 A1
20170350763 Shafer et al. Dec 2017 A1
20170351111 Jeong et al. Dec 2017 A1
20170356884 Hu et al. Dec 2017 A1
20180031816 Shimada Feb 2018 A1
20180039059 Kondo et al. Feb 2018 A1
20180120550 Boccara et al. May 2018 A1
20180125360 Högele et al. May 2018 A1
20180136451 Soenksen May 2018 A1
20180149673 Huo et al. May 2018 A1
20180195963 Imoto Jul 2018 A1
20180196246 Bares et al. Jul 2018 A1
20180210184 Betzig Jul 2018 A1
20180231416 Roscher et al. Aug 2018 A1
20190064493 Truong et al. Feb 2019 A1
Foreign Referenced Citations (5)
Number Date Country
2012122027 Sep 2012 WO
2013150273 Oct 2013 WO
2015109323 Jul 2015 WO
2015184124 Dec 2015 WO
2019161048 Aug 2019 WO
Non-Patent Literature Citations (12)
Entry
Gao, “Extend the field of view of selective plan illumination microscopy by tiling the excitation light sheet”, Optical Society of America, published Feb. 26, 2015, Optics Express pp. 6102-6111 (Year: 2015).
Bouchard et al., “Swept confocally-aligned planar excitation (SCAPE) microscopy for high-speed volumetric maging of behaving organisms”, Nature Photonics, Jan. 19, 2015, vol. 9(2), pp. 113-119.
Chhetri et al., “Whole-animal functional and developmental imaging with isotropic spatial resolution”, Nature Methods, Dec. 2015, vol. 12(12), pp. 1171-1178.
Holy, “Calcium imaging in populations of olfactory neurons by planar illumination microscopy”, Cold Spring Harb Protoc, Mar. 1, 2014, 2014(3), pp. 317-323.
International Search Report and Written Opinion for International Application No. PCT/US2017/061165 dated Mar. 9, 2018.
Tomer et al., “Advanced CLARITY for rapid and high-resolution imaging of intact tissues”, Nat Protoc, Jul. 2014, vol. 9(7): pp. 1682-1697.
Tomer, “Shedding light on the system: studying embryonic development with light sheet microscopy”, Curr Opin Genet Dev, Oct. 2011, 21(5), pp. 558-565.
Vettenburg et al., “Light-sheet microscopy using an Airy beam”, Nature Methods, May 2014, vol. 11(5), pp. 541-544.
Wu et al., “Inverted selective plane illumination microscopy (iSPIM) enables coupled cell identity lineaging and Teurodevelopmental imaging in Caenorhabditis elegans”, Proceedings of the National Academy of Sciences, Oct. 25, 2011, vol. 108(43), pp. 17708-17713.
Wu et al., “Spatially isotropic four-dimensional imaging with dual-view plane illumination microscopy”, Nat Biotechnol, Nov. 2013, 31(11), pp. 1032-1038.
Extended European Search Report dated May 18, 2020 for European Patent Application No. 17868760.4.
Hedde et al., “Selective plane illumination microscopy with a light sheet of uniform thickness formed by an electrically tunable lens,” Microscopy Research and Technique, vol. 81(9), Sep. 2018, pp. 924-928.
Related Publications (1)
Number Date Country
20190310451 A1 Oct 2019 US
Provisional Applications (2)
Number Date Country
62473944 Mar 2017 US
62420349 Nov 2016 US