Apparatus for determining the position of a trapped object in optical tweezers

Abstract

The invention relates to an apparatus 10 for determining the position of several objects 1 trapped simultaneously by a single laser beam 2, characterized in that the apparatus 10 comprises: a laser source 5 emitting the laser beam 2; actuation systems 13, 14 for three-dimensionally deflecting the laser beam 2 between several trapping points 15; a microscope objective 6 for focusing the laser beam 2 coming from the actuation system 13, 14 onto the trapping points 15; a sample chamber 8 containing the objects 1 to be trapped on the trapping points 15; a light source 11 for illuminating the sample chamber 8; and a camera 16 for determining the position of each of the trapped objects 1, the camera 16 being arranged between the laser source 5 and the actuation system 13, 14 so that the light 20 emitted by the light source 11 passes successively through the sample chamber 8, the microscope objective 6, the actuation system 13, 14 and the camera 16.

Description

[Technical field]

[0001] The present invention relates to a device for determining the position of several objects trapped simultaneously by a single laser beam. In particular, the device according to the invention makes it possible to determine the external forces exerted on the objects. [Background technology]

[0002] Optical tweezers (originally called single-beam gradient force traps) are scientific instruments that use highly focused laser beams to provide attractive or repulsive forces (typically on the order of piconewtons) depending on the relative refractive index between a particle and the surrounding medium. These forces can be used to physically hold and move microscopic objects in a manner similar to tweezers. They can trap and manipulate small particles, typically on the order of microns in size, including dielectric and absorbing particles. Optical tweezers have been particularly successful in recent years in the study of various biological systems.

[0003] As shown in Figures 1 and 2, optical tweezers are capable of manipulating nanometer and micron sized dielectric particles 1 by exerting extremely small forces via a highly focused laser beam 2 extending along an optical axis Z. The beam 2 is typically focused by sending it through a microscope objective. The narrowest point of the focused beam, known as the beam waist, contains a very strong electric field gradient 3. The dielectric particles are attracted along the gradient to the region of strongest electric field, which is the center of the beam. The laser light also tends to exert a force on the particles in the beam along the beam propagation direction. This is due to the conservation of momentum, where photons that are absorbed or scattered by the small dielectric particles impart momentum to the dielectric particles. This is known as the scattering force 4, and results in the particle being displaced slightly downstream from its exact location at the beam waist, as seen in Figure 1.

[0004] In an optical trap, a tightly focused laser beam provides an equilibrium position near the beam waist. When the trapped object 1 is displaced laterally or axially away from the equilibrium position, optical forces act to pull it back towards the equilibrium position. For small displacements, the force exerted on the particle is a linear function and the optical trap can be compared to a simple spring system that obeys Hooke's law. In this model, the restoring optical force F is proportional to its distance from its equilibrium position and the trap stiffness is proportional to the light intensity. Taking into account the range of motion and the trap stiffness, three-dimensional piconewton resolution is achievable.

[0005] This particularity has led to the use of optical traps for quantitative force measurements such as the strength of intermolecular bonds, the stiffness of cell membranes, or intracellular measurements for microrheology.

[0006] Force calibration of any object with reasonable accuracy remains a challenge, since the optical stiffness depends on several factors, such as the material properties, the refractive index of both the object and the environment, the size and shape of the trapped object, etc. For these reasons, silicon or polystyrene microspheres are often used as force probes to indirectly manipulate and sense forces during micromanipulation tasks. By using artificial microbeads with uniform material and shape, the optical forces applied to the microbeads can be obtained.

[0007] For small displacements, the optical forces can be described by a spring model: F=K * (P レーザ -P プローブ ) Here, P レーザ and P プローブ represent the positions of the laser and particle 1, respectively. F is the three-dimensional optical force. K:[K x ,K y ,K z ] is the trap stiffness, where K x , K y , K zrepresent the stiffness in the x, y, and z directions, respectively. The optical force F is therefore obtained by measuring the displacement of the particle from the equilibrium trapping position.

[0008] Well-established methods exist for accurate stiffness calibration, such as the equipartition method and the Stokes resistance method. Thus, force sensing arises directly from the position of the laser and its ability to detect one of the trapped objects.

[0009] This position determination can be done by image-based position detection, where the image of a video camera is used to extract information, or by interferometry, where the beam displacement after the laser has passed through the sample is measured via a quadrant photodiode QDP.

[0010] Displacement in an optical tweezers system can be achieved by either moving the platform or by moving the laser beam, which is called passive or active actuation.

[0011] In passive actuation, the incorporation of a motorized stage allows for dynamic control of the sample chamber while the object to be manipulated remains fixed on the trap.

[0012] In active operation, the laser direction is changed through active optics. Furthermore, it is possible to multiplex the trapping laser beam in order to trap several objects simultaneously using a unique laser source. By rapidly deflecting the laser beam between several trapping positions, it is possible to trap several objects so that the objects do not have time to spread between two laser visits. This method is called the time-sharing method. Alternatively, by using active diffractive optical elements such as spatial light modulators (SLMs), several traps can be dynamically controlled to generate several diffractive spots at different positions, which is called the space-sharing method.

[0013] For quantitative force measurements with optical tweezers, passive methods are usually used, since the optical trap remains fixed and only position information of the trapped object is required. Summary of the Invention

[0014] The present invention is to perform position measurements, and therefore force measurements, for all traps created by a three-dimensional multi-trap actuation system that extends the force measurement capability to several traps.

[0015] To this end, the present invention aims to provide an apparatus for determining the positions of multiple objects simultaneously trapped by a single laser beam.

[0016] The device according to the invention comprises: a laser source emitting a laser beam; an actuation system for three-dimensionally deflecting the laser beam between a number of trapping points; a microscope objective lens for focusing the laser beam coming from the actuation system onto the trapping point; a sample chamber containing an object to be trapped on the trapping point; a light source for illuminating the sample chamber; - an image sensor (camera) for determining the position of each trapped object, said image sensor being positioned between the laser source and the actuation system such that the light emitted by the light source passes successively through the sample chamber, the microscope objective, the actuation system and the image sensor.

[0017] The actuation system controls the three-dimensional position of the object. The image sensor is placed between the laser source and the actuation system, and since the actuation system is reversible, the image acquired by the image sensor is always aligned with the laser spot. Then, by tracking the three-dimensional position of each object, it is possible to obtain three-dimensional force information of several traps, similar to what was performed in the passive actuation method.

[0018] The actuation system may include a deformable mirror for controlling the axial position of the trapping point. The term "axial" refers to the axis of the laser beam. The planar scanning mirror may be a mirror galvanometer.

[0019] The deformable mirror is typically capable of axially focusing or defocusing the laser beam.

[0020] The apparatus may comprise a system for passing the laser beam emitted by the laser source through the deformable mirror several times.

[0021] Thus, by passing the laser beam through the same deformable mirror several times, the focusing (in the case of the converging configuration of the deformable mirror) or defocusing (in the case of the diverging configuration of the deformable mirror) is amplified and thus the angle of the laser beam at the entrance of the microscope objective is increased (in the case of the diverging configuration of the deformable mirror) or decreased (in the case of the converging configuration of the deformable mirror). The axial position of the trapping point can therefore be increased (in the case of the diverging configuration of the deformable mirror) or decreased (in the case of the converging configuration of the deformable mirror). The invention allows for fast motion control of the trapping point in a large working space. As the device is still based only on mirrors, the optical path is bidirectional, i.e. it is independent of the propagation direction and the optical efficiency is maximized. This property allows simultaneous trapping of objects in the axial direction and visualization of the trapped objects in the axial plane, since the illumination light returns along the same path as the manipulation laser.

[0022] The working axis working space can therefore be expanded by using several "virtual" deformable mirrors in series. The idea is to pass the laser beam through the same deformable mirror several times, for example using a set of mirrors. By ensuring that the virtual deformable mirror is located in a conjugate plane of the objective entrance aperture, the working space can be significantly increased, while ensuring that the size of the laser beam diameter at the objective entrance aperture remains the same, regardless of the degree of focusing or divergence of the laser beam.

[0023] The working space, the number of traps that can be generated, and the maximum applicable force are increased. It can be used to simultaneously manipulate or stimulate several biological and synthetic objects in a large 3D working space. This actuation technique is also useful in different applications where 3D orientation of micro-objects (biological or synthetic) is required, such as cell surgery applications (e.g., nuclear transfer, embryo microinjection, polar body biopsy), 3D tomographic imaging of biological samples, or microassembly in microfluidic devices.

[0024] The system for passing the laser beam over the deformable mirror several times may comprise at least one set of two mirrors for guiding the laser beam during two successive passes of the laser beam over the deformable mirror.

[0025] The system for passing the laser beam through the deformable mirror several times advantageously comprises a system for passing the laser beam through the deformable mirror several times between two successive passes of the laser beam through the deformable mirror. An afocal system is provided for conjugating the two successive passes of the beam.

[0026] The afocal system can include two focusing lenses.

[0027] The actuation system can include a planar scanning mirror for controlling the planar position of the trap point. The term "planar" refers to a plane perpendicular to the axis of the laser beam. The planar scanning mirror can be a mirror galvanometer.

[0028] The apparatus advantageously comprises a first afocal system arranged between the deformable mirror and the planar scanning mirror, and a second afocal system arranged between the planar scanning mirror and the microscope objective lens, for conjugating the deformable mirror and the planar scanning mirror with the entrance opening of the microscope objective lens.

[0029] The apparatus may include a system for calculating the force on each trapped object as a function of the position of each of the trapped objects as determined by the camera.

[0030] The force F on each trapped object can be calculated by the system using an optical force model. F=K * (P レーザ -P プローブ ) Here, P レーザ -P プローブ represents the displacement between the laser position and the position of the trapped object, and K is the stiffness of the trap.

[0031] The force on a trapped object is the sum of all external forces that move the object from its equilibrium position, i.e., the sum of all external forces that move the object excluding the force applied by the laser beam.

[0032] The forces and torques applied to a compound object with several objects attached to its body can be calculated as a function of the force F on each trapped object.

[0033] The trapped objects can be biological objects, such as red blood cells and bacterial cells, or synthetic objects, such as optical robots (especially print-engineered microstructures with different types of end effectors) that can be used to indirectly manipulate and measure forces. Thus, the trapped objects can be biological objects, microspheres or synthetic objects. [Brief description of the drawings]

[0034] Other objects, features and advantages of the present invention will become apparent upon reading the following description, given purely as a non-limiting example, and upon reference to the accompanying drawings, in which: [Figure 1] As mentioned above, a schematic diagram of optical tweezers. [Diagram 2] As mentioned above, FIG. 1 shows the determination of an external force applied to an object trapped in optical tweezers. [Diagram 3] 1 illustrates diagrammatically an apparatus for determining the position of an object trapped in optical tweezers according to the present invention; [Figure 4] FIG. 2 illustrates a haptic interface associated with a device according to the invention. [Diagram 5] 2 shows diagrammatically a mirror galvanometer for use in the device according to the invention; [Figure 6] 2 shows diagrammatically a deformable mirror for use in a device according to the invention; [Figure 7] 2 shows diagrammatically a deformable mirror for use in a device according to the invention; [Figure 8] FIG. 2 shows an optical robot associated with the device according to the invention. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

[0035] FIG. 3 shows the present invention, in which multiple objects are simultaneously trapped by a single laser beam 2. An apparatus 10 for determining the position of a body 1 is shown.

[0036] The apparatus 10 comprises a laser source 5 emitting a laser beam 2. The laser source 5 may be a 1070 nm laser. The stiffness of the trap depends on the laser power, typically used output laser powers may be between 100 mW and 2 W.

[0037] The laser beam 2 passes through an actuation system for deflecting the laser beam 2 between several trapping positions. The generation of several simultaneous trapping points using a single laser source can be achieved using spatial or temporal sharing methods. By rapidly deflecting the laser beam between a set of positions, multiple stable trapping points can be generated. Displacement in an optical trapping system can be achieved by moving the platform or by moving the laser beam, which is called passive or active actuation.

[0038] In passive actuation, the incorporation of a motorized stage allows for dynamic control of the sample chamber while the object to be manipulated remains fixed on the trap.

[0039] In active operation, the laser direction is changed through active optics. Furthermore, it is possible to multiplex the trapping laser beam in order to trap several objects simultaneously using a unique laser source. By rapidly deflecting the laser beam between several trapping positions, it is possible to trap several objects so that the objects do not have time to spread between two laser visits. This method is called the time-sharing method. Alternatively, by using active diffractive optical elements such as spatial light modulators (SLMs), several traps can be dynamically controlled to generate several diffractive spots at different positions. This method is called the space-sharing method.

[0040] A microscope objective 6 is used to focus the laser beam 2 coming from the actuation system onto the trapping point and to image the trapped object 1. The sample 7 object 1 is placed in a sample chamber 8, which is placed on a platform 9 (which can be a 3D nanostage).

[0041] A light source 11 is used to illuminate the sample. The light source can be an LED (light emitting diode).

[0042] Light 20 is focused in an axial direction Z onto the sample 8 via a lens 12 .

[0043] The actuation system controls the three-dimensional position of the object 1, i.e. in the Z axial direction and in the planar X, Y directions. It includes a deformable mirror 13 and a galvanometer 14, which are used to control the axial Z position and the planar X, Y position, respectively, of the trapping point.

[0044] On the Z axis a deformable mirror 13 is used that can focus or defocus the laser beam 2. The deformable mirror 13 and the galvanometer 14 are placed in a conjugate plane on the entrance aperture of the microscope objective 6. Thus the laser beam 2 pivots around the entrance aperture of the microscope objective 6, maintaining the same degree of overfill and producing an equally stable trap, independent of the angle or degree of collimation of the incident beam 2.

[0045] The deformable mirror 13 can be a microelectromechanical component with 111 actuators and 37 piston tip tilt segments with an update rate of over 2 kHz. Each segment has a diameter of 700 μm, while the array has an aperture of 3.5 mm and a maximum dynamic range (stroke) of 5.8 μm. Electrostatic actuation allows precise positioning of each segment with nanometer and microradian resolution (wavefront resolution <15 nm rms). The mechanical step response speed is less than 200 μs (10-90%) and it has a high reflectivity (>99.9%).

[0046] The segmented deformable mirror 13 can effectively generate smooth shapes and is used to control the degree of collimation of the laser beam 2. By synchronizing the orientation of the mirror galvanometer 14 with the movement of the deformable mirror 13, it is possible to displace the focal spot laterally and axially while maintaining diffraction-limited performance. This axial scanning implies very low mechanical inertia and therefore a Z-bandwidth compatible with the galvanometer 14. The overall switching speed between 3D trap positions is of the same order of magnitude as a comparable 2D system in the prior art. It is therefore possible to obtain a very stable trap without introducing significant aberrations.

[0047] A Gaussian laser beam (1070 nm) is guided via a galvanometer 14, a deformable mirror 13 and standard optical elements into an inverted microscope 6. Two afocal systems f1, f2 and f3, f4 are preferably used to conjugate the two actuators 13, 14 with the entrance aperture of the microscope objective 6 and expand the laser beam 2. This is expanded to overfill (20%) the objective entrance to improve trapping efficiency.

[0048] FIG. 5 shows how, for small movements of the mirror galvanometer 14, the laser beam 2 pivots around the entrance aperture of the microscope objective lens, generating an optical trap movement in the optical plane and thus several trap points 15.

[0049] Shown is the effect of focusing (Figure 6) or defocusing (Figure 7) the deformable mirror 13 to change the Z position of the trap point 15. The size of the beam 2 at the entrance aperture of the objective lens remains the same regardless of the degree of collimation of the incident beam.

[0050] According to the invention, an image sensor 16 for determining the position of each of the trapped objects 1 is arranged between the laser source 5 and the actuation system 13, 14, more precisely between the laser source 5 and the deformable mirror 13, so that the light emitted by the light source 11 passes successively through the sample 7, the microscope objective 6, the actuation system 13, 14 and then is guided via a dichroic mirror 21 to the camera 16. The image sensor can be an event-based camera.

[0051] Due to the fact that the actuation system 13, 14 uses only mirrors, the passage of light is bidirectional, i.e. the path is independent of the propagation direction. Using this property, and thanks to the specific position of the camera 16, it is possible to track the position of the trapped object 1 by looking at one trapping point 15 at a time, as it is a three-dimensional position and the object 1 is always kept in the center of the field of view of the camera 16.

[0052] If the camera 16 is placed between the laser source 5 and the actuation system 13, 14, the white light 20 reaches and passes through the actuation system 13, 14 in exactly the opposite direction to the laser beam 2. In this way, the image on the sensor 16 is always scanned over the laser spot. In this configuration, only one sensor receives measurements of all scanning points. By synchronizing the multi-trap actuation technique with the event-based camera 16 (or other camera), it becomes possible to distinguish between events (or frames) coming from different traps 15. This solution is advantageous in that it is possible to distinguish between events (or frames) coming from different traps 15 without the need for a multi-trap actuation technique. This avoids the problem of determining the center of the moving laser in multi-trap force measurements. Since the whole pixel is used to determine the position of each trapped object, a trade-off between spatial and temporal resolution may remain, but the time to make the measurement depends on the number of generated traps and the scanning frequency. In this way, it is possible to position, for example, three different traps arbitrarily in space, and the sensor receives information from all scanned points, thus measuring the position of each trapped object relative to the laser and, finally, extracting the information of the external force on each trap.

[0053] This ability to simultaneously measure forces at multiple 3D positions is important in many biomechanical studies, such as characterizing the membrane stiffness of cells at multiple points during the fusion phase or measuring stiffness simultaneously on different cells. Multitrap force measurements are also useful in mechanotransduction studies, e.g., the adaptation of cells to repetitive stimuli, revealing how cells change shape and control their migratory behavior.

[0054] The optical robot 22 is in particular a print-designed microstructure with different types of end effectors that are actuated in 6DoF (six degrees of freedom) by optical tweezers via a spherical handle attached to its body (Figure 8).

[0055] By measuring the 3-dimensional forces for each handle of the robot, 6-axis force / torque measurements can be made by combining the information for each trap. These 6-DoF Optobots with 6-axis force sensors will enable the study of novel biological interactions, such as the mechanics of Toxoplasma gondii. This latter requires mechanical work of translational and rotational-torsion movements to complete cell invasion and can therefore only be characterized with 6-axis force / torque sensors.

[0056] A haptic interface 17 can be used, as shown in Figure 4. The user controls the three-dimensional position of the microrobot and senses the three-dimensional external force F applied to the microrobot via a force sensor 18, which determines the applied force as described above. A computer 19 allows to provide the operator with visual perception and environmental information.

Claims

1. An apparatus (10) for determining the positions of multiple objects (1) trapped simultaneously by a single laser beam (2), said apparatus (10) comprising: a laser source (5) emitting a laser beam (2), - an actuation system (13, 14) for three-dimensional deflection of said laser beam (2) between several trapping points (15); - a microscope objective (6) for focusing the laser beam (2) coming from the actuation system (13, 14) onto the trapping point (15); - a sample chamber (8) containing said object (1) to be trapped on said trapping point (15); a light source (11) for illuminating said sample chamber (8); an image sensor (16) for determining the position of each of the trapped objects (1), the image sensor (16) being arranged between the laser source (5) and the actuation system (13, 14) such that the light (20) emitted by the light source (11) passes successively through the sample chamber (8), the microscope objective (6), the actuation system (13, 14) and the image sensor (16); An apparatus (10), comprising:

2. 2. The device (10) according to claim 1, characterized in that the actuation system (13, 14) comprises a deformable mirror (13) for controlling the axial (Z) position of the trapping point (15).

3. 3. Apparatus (10) according to claim 2, characterized in that the deformable mirror (13) is capable of axially focusing or defocusing the laser beam.

4. 3. An apparatus (10) according to claim 2, characterized in that it comprises a system for steering the laser beam (2) emitted by the laser source (5) onto the deformable mirror (13) several times.

5. The device (10) according to any one of claims 1 to 4, characterized in that the actuation system (13, 14) comprises a planar scanning mirror (14) for controlling the planar (X, Y) position of the trapping point (15).

6. The actuation system (13, 14) comprises a planar scanning mirror (14) for controlling a planar (X, Y) position of the trap point (15), and a first afocal system (f) arranged between the deformable mirror (13) and the planar scanning mirror (14) for conjugating the deformable mirror (13) and the planar scanning mirror (14) with an entrance opening of the microscope objective lens (6). １ , f ２ ), and a second afocal system (f) arranged between the plane scanning mirror (14) and the microscope objective lens (6). １ , f ２ 3. The device (10) according to claim 2, further comprising:

7. The device (10) according to any one of claims 1 to 6, characterized in that it comprises a system (18) for calculating a force (F) on each trapped object (1) as a function of the position of each of the trapped objects (1) determined by the image sensor (16).

8. The force F on each trapped object is expressed by the optical force model: F = K ＊ (P レーザ -P プローブ ) calculated by the system (18) using the formula: レーザ -P プローブ 8. The apparatus (10) of claim 7, wherein θ represents the displacement between the position of the laser beam and the position of the trapped object, and K is the stiffness of the trap.

9. 9. An apparatus (10) according to claim 7 or 8, characterized in that the forces and torques applied to a composite object (22) having several objects (1) attached to a body are calculated as a function of the force (F) on each trapped object (1).

10. Device (10) according to any one of the preceding claims, characterized in that the object (1) to be trapped is a biological object, a microsphere or a synthetic object.

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