EP3881054A1 - An optical nano-manipulator for particles in a fluid - Google Patents
An optical nano-manipulator for particles in a fluidInfo
- Publication number
- EP3881054A1 EP3881054A1 EP19885440.8A EP19885440A EP3881054A1 EP 3881054 A1 EP3881054 A1 EP 3881054A1 EP 19885440 A EP19885440 A EP 19885440A EP 3881054 A1 EP3881054 A1 EP 3881054A1
- Authority
- EP
- European Patent Office
- Prior art keywords
- plasmonic
- colloidal
- trapping
- nano particles
- tweezers
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Withdrawn
Links
Classifications
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B01—PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
- B01L—CHEMICAL OR PHYSICAL LABORATORY APPARATUS FOR GENERAL USE
- B01L3/00—Containers or dishes for laboratory use, e.g. laboratory glassware; Droppers
- B01L3/50—Containers for the purpose of retaining a material to be analysed, e.g. test tubes
- B01L3/502—Containers for the purpose of retaining a material to be analysed, e.g. test tubes with fluid transport, e.g. in multi-compartment structures
- B01L3/5027—Containers for the purpose of retaining a material to be analysed, e.g. test tubes with fluid transport, e.g. in multi-compartment structures by integrated microfluidic structures, i.e. dimensions of channels and chambers are such that surface tension forces are important, e.g. lab-on-a-chip
- B01L3/502761—Containers for the purpose of retaining a material to be analysed, e.g. test tubes with fluid transport, e.g. in multi-compartment structures by integrated microfluidic structures, i.e. dimensions of channels and chambers are such that surface tension forces are important, e.g. lab-on-a-chip specially adapted for handling suspended solids or molecules independently from the bulk fluid flow, e.g. for trapping or sorting beads or physically stretching molecules
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B01—PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
- B01L—CHEMICAL OR PHYSICAL LABORATORY APPARATUS FOR GENERAL USE
- B01L2200/00—Solutions for specific problems relating to chemical or physical laboratory apparatus
- B01L2200/06—Fluid handling related problems
- B01L2200/0647—Handling flowable solids, e.g. microscopic beads, cells, particles
- B01L2200/0668—Trapping microscopic beads
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B01—PHYSICAL OR CHEMICAL PROCESSES OR APPARATUS IN GENERAL
- B01L—CHEMICAL OR PHYSICAL LABORATORY APPARATUS FOR GENERAL USE
- B01L2400/00—Moving or stopping fluids
- B01L2400/04—Moving fluids with specific forces or mechanical means
- B01L2400/0403—Moving fluids with specific forces or mechanical means specific forces
- B01L2400/0454—Moving fluids with specific forces or mechanical means specific forces radiation pressure, optical tweezers
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y15/00—Nanotechnology for interacting, sensing or actuating, e.g. quantum dots as markers in protein assays or molecular motors
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B82—NANOTECHNOLOGY
- B82Y—SPECIFIC USES OR APPLICATIONS OF NANOSTRUCTURES; MEASUREMENT OR ANALYSIS OF NANOSTRUCTURES; MANUFACTURE OR TREATMENT OF NANOSTRUCTURES
- B82Y20/00—Nanooptics, e.g. quantum optics or photonic crystals
Definitions
- the present disclosure generally relates to the field of optical nanomanipulation.
- the present disclosure relates to a colloidal plasmonic tweezer designed to be used as a remotely controlled nano-manipulator.
- the main feature that makes this technology unique is its ability to remotely control specific colloidal objects as desired, allowing independently controlled manipulation of individual specimens at any preferred location of a fluidic volume.
- Optical tweezers have been used to trap dielectric spheres, viruses, bacteria, living cells, organelles, small metal particles, and even strands of DNA.
- Applications include confinement and organization (e.g. for cell sorting), tracking of movement (e.g. of bacteria), application and measurement of small forces, and altering of larger structures (such as cell membranes).
- traps are created at specific locations of a two- dimensional substrate that needs to be nano-pattemed. Therefore, unlike traditional laser tweezers these devices cannot be operated to selectively trap, dynamically transport and independently control target objects at bulk fluidic volume.
- the primary disadvantages of using plasmonic tweezers for optical manipulation are: (i) method is slow since it relies on diffusion of objects to the small trapping volume; (ii) requires a nanopatterned substrate which is a cumbersome task for scaling up; and iii) it is inefficient for transporting objects due to its static nature.
- the numbers expressing quantities or dimensions of items, and so forth, used to describe and claim certain embodiments of the invention are to be understood as being modified in some instances by the term“about.” Accordingly, in some embodiments, the numerical parameters set forth in the written description and attached claims are approximations that can vary depending upon the desired properties sought to be obtained by a particular embodiment. In some embodiments, the numerical parameters should be construed in light of the number of reported significant digits and by applying ordinary rounding-off techniques. Notwithstanding that the numerical ranges and parameters setting forth the broad scope of some embodiments of the invention are approximations, the numerical values set forth in the specific examples are reported as precisely as practicable.
- a general object of the present disclosure is to provide a system and method for optical manipulation that does not suffer from drawbacks of known systems and methods for optical manipulation.
- An object of the present disclosure is to provide a system and method for optical manipulation that uses low power optical illumination and yet do not suffer from drawbacks of plasmonic trapping.
- An object of the present disclosure is to provide a system and method that uses low power optical illumination for plasmonic trapping of nano particles, and yet allows mobility.
- An object of the present disclosure is to provide a system and method for nano manipulation that integrates plasmonic and optical trapping to use low power optical illumination to trap nano particles as well as provide mobility for the trapped nano particles.
- An object of the present disclosure is to provide a system and method for nano manipulation that does not require a specialized substrate.
- An object of the present disclosure is to provide a system and method for nano manipulation that allows use of multiple laser beams
- Another object of the present disclosure is to provide a system and method for nano manipulation that provides flexibility in antenna design at different illumination.
- Another object of the present disclosure is to provide a system and method for nano manipulation that remote and independent control of movement of the trapped nano particles.
- Yet another object of the present disclosure is to provide a system and method for nano manipulation that allows selective manipulate of few or multiple nanoparticles
- Yet another object of the present disclosure is to provide a system and method for nano manipulation that is compatible for in-vivo applications.
- Yet another object of the present disclosure is to provide a system and method for nano manipulation that can be used in ionic fluids such as some of thebiofluids.
- Still another object of the present disclosure is to provide a system and method for nano manipulation that allows can be seamlessly integrated with existing optical tweezer equipment.
- aspects of the present disclosure relate to optical manipulation of nano particles.
- the present disclosure provides a tweezer, a system and a method for optical manipulation using the disclosed tweezer.
- the disclosed tweezer for trapping and moving the nano particles integrates plasmonic and optical trapping, wherein plasmonic trapping is used for trapping of the nano particles to the tweezer, and the optical trapping uis used to trap the tweezer along with the nano particles trapped to the tweezer to the light beam.
- the disclosed plasmonic tweezer can be used in a colloidal solution containing the nano particles of interest and does not require any specialized substrate to manipulate the nano particles, therefore referred to as colloidal plasmonic tweezer.
- the plasmonic tweezer for trapping and manipulatingnano particles in a colloidal solution, includes a nanorod made of a dielectric material; and a disc made of a plasmonic material. The disc is coupled to one end of the nanorod.
- the disc is configured to work as a plasmonic antenna to trap the nano particles using a plasmonic gradient force of localized and enhanced electromagnetic intensity in optical near field generated by the discs as a result of a light beam focussed on the colloidal plasmonic tweezer.
- the dielectric nanorod is configured such that the colloidal plasmonic tweezer is trapped to the light beam on account of far field optical forces acting on the dielectric nanorod as a result of the light beam, thereby enabling movement of the colloidal plasmonic tweezer by steering the light beam.
- the disc may be made of a plasmonic material selected from a group comprising Silver, Gold, Aluminium-doped Zinc Oxide, and Titanium nitride
- Diameter of the disc may be in the range of 200 to 300nm, and thickness of the disc may be the range of 40-60nm. In a preferred embodiment, the diameter of the disc is kept 250nm and the thickness of the disc is kept as 50nm.
- the nanorod may be made of Silicon dioxide, and its length and diameter may be in the range of 2.00-3.00 pmand 40-60nm respectively. In a preferred embodiment, the length of the nanorod is kept 2.5 pm and the diameter of the nanorod is kept as 50 nm.
- An aspect of the present disclosure relates to a method for trapping and manipulatingnano particles using the disclosed colloidal plasmonic tweezer.
- the disclosed method allows use of multiple light beams, remote and independent control of movement of the trapped nano particles, and allows selective manipulate of few or multiple nano particles
- the disclosed method for trapping and manipulating nano particles includes the steps of: (a) providing a plurality of colloidal plasmonic tweezers in a colloidal solution that contains the nano particles to be manipulated; (b) focussing one or more light beams on one or more of the plurality of colloidal plasmonic tweezers Trapping one or more of the nano particles that are of interest by moving the one or more of the plurality of colloidal plasmonic tweezers close to the one or more nano particles of interest by steering the corresponding light beams; (c) moving each of the one or more of the plurality of colloidal plasmonic tweezers along with the trapped nano particles of interest to corresponding desired locations by steering the corresponding light beams; and (d) releasing the trapped nano particles at the desired location;
- the colloidal plasmonic tweezers include a disc of a plasmonic material coupled to one end of a long dielectric nanorod.
- the disc is configured to generate a plasmonic gradient force when illuminated with light thereby working as a plasmonic antenna to trap the nano particles;
- the one or more nano particles of interest are trapped by localized and enhanced electromagnetic intensity in optical near field generated by the discs of the one or more of the plurality of colloidal plasmonic tweezers as a result of the one or more light beams focussed thereon.
- the one or more of the plurality of colloidal plasmonic tweezers is moved by trapping the one or more of the plurality of colloidal plasmonic tweezers to the corresponding light beams based on the far field optical forces acting on the corresponding dielectric nanorods as a result of the corresponding light beams focussed on the colloidal plasmonic tweezers.
- the method may further include the step of providing a microfluidic chamber to hold the colloidal solution containing the nano particles to be manipulated and the plurality of colloidal plasmonic tweezers.
- the method may further include the step of providing one or more polarised laser sources to generate one or more light beams, the one or more polarised laser sources being coupled to an optical microscope.
- the method may further include the step of providing at least one galvo-mirror in paths of the light beams emanating from the one or more polarised laser sources to steer the light beams, wherein the at least one galvo-mirror enables steering the corresponding light beam remotely.
- the method may further include the step of sonicating the colloidal solution to distribute the plurality of colloidal plasmonic tweezers in the colloidal solution.
- Another aspect of the present disclosure relates to a system for trapping and manipulatingnano particles of interest, the system.
- the disclosed system allows remote and independent control of movement of the trapped nano particles, and is compatible for in-vivo applications.
- the system can be seamlessly integrated with existing optical tweezer equipment.
- the disclosed system for trapping and manipulating nano particles of interest includes: (a) a plurality of colloidal plasmonic tweezers suspended in a colloidal solution; and (b) one or more elliptically polarised laser sources to generate one or more elliptically polarized light beams.
- the one or more polarised laser sources are coupled to an optical microscope.
- the colloidal plasmonic tweezers includes a disc made of a plasmonic material coupled to one end of a long nanorod made of a dielectric material; wherein the disc is configured to generate a plasmonic gradient force when illuminated by a light beam thereby working as a plasmonic antenna to trap the nano particles.
- the nano particles of interest are trapped by localized and enhanced electromagnetic intensity in optical near field generated by the discs of the one or more of the plurality of colloidal plasmonic tweezers as a result of the one or more light beams focussed thereon.
- the one or more of the plurality of colloidal plasmonic tweezers are moved by trapping the one or more of the plurality of colloidal plasmonic tweezers to the corresponding light beams based on the far field optical forces acting on the corresponding dielectric nanorods as a result of the corresponding light beams focussed on the colloidal plasmonic tweezers.
- the system may further include at least one galvo-mirror in path of each of the light beams emanating from the one or more polarised laser sources to remotely steer the light beams to remotely move of the one or more colloidal plasmonic tweezers trapped by the corresponding light beams.
- the one or more elliptically polarized laser light beams may be low power infrared lasers.
- the colloidal solution may be an ionic biofluid.
- the colloidal solution may be an in vivo biofluid.
- the colloidal solution may be based on any or a combination of hyaluronic gel and vitreous humour, and the trapping and manipulating nano particles of interest may be done in ex-Vivo conditions.
- the system may include a microfluidic chamber to hold the colloidal solution containing the nano particles to be trapped and manipulated.
- FIG. 1A illustrates an exemplary representation of trapping of nano particles for nanomanipulation using by a plasmonic tweezer.
- FIG. IB illustrates an exemplary graph of localised surface plasmon resonance (LSPR) wavelength as a function of disk diameter and associated temperature rise due to light absorption.
- LSPR localised surface plasmon resonance
- FIG. 1C illustrates thermal diffusivity (Brownian sensitivity) of a nanorod as a function of its length.
- FIG. ID illustrates an exemplary structure of the proposed Colloidal Plasmonic Tweezer (CPT), integrating the plasmonic nanodisc with a dielectric nanorod, and an SEM image of a plurality of CPTs attached to a substrate, in accordance with embodiments of the present disclosure.
- CPT Colloidal Plasmonic Tweezer
- FIG. 2 illustrates an exemplary setup for the system for trapping and manipulating nano particles using the proposed CPT, in accordance with embodiments of the present disclosure.
- FIG. 3A illustrates anextinction cross section of plasmonic nanodisc in vertical and horizontal configurations, in accordance with an embodiment of the present disclosure.
- FIG. 3B illustrates differential orientation of CPT with respect to laser illumination, in accordance with an embodiment of the present disclosure.
- FIG. 3C illustrates trapping of polystyrene particles in plasmonic near-field for vertical and horizontal configurations, in accordance with an embodiment of the present disclosure.
- FIG. 3D illustrates a beam profile of the diffraction limited laser spot showing the region inaccessible by the trapped particle, in accordance with an embodiment of the present disclosure.
- FIG. 3E illustrates electric field intensity enhancement for the nanodisc in vertical configuration and horizontal configuration, in accordance with an embodiment of the present disclosure.
- FIG. 3F illustrates a histogram of fluctuations of the proposed CPT when trapped with a focused laser (vertical configuration) and defocussed laser (horizontal configuration), in accordance with an embodiment of the present disclosure.
- FIG. 4A illustrates a graph of minimum illumination intensity required to trap, as a function of bead size for vertical and horizontal configurations of the proposed CPT, in accordance with an embodiment of the present disclosure.
- FIG. 4B illustrates an exemplary plasmonic gradient force on a 200 nm polystyrene particle as a function of distance from the proposed nanodisc, in accordance with an embodiment of the present disclosure.
- FIG. 4C illustrates a calculated temperature rise as a function of laser intensity for 400 nm and 1064 nm wavelength, in accordance with an embodiment of the present disclosure.
- FIG. 5A illustrates trapping and releasing of 100 nm fluorescent nano-diamonds in an ultra-low-density solution, in accordance with an embodiment of the present disclosure.
- FIG. 5B illustrates trapping, transporting and releasing of 300 nm fluorescent magnetic particles using two traps parallelly and independently, in accordance with an embodiment of the present disclosure.
- FIG. 6 illustrates an exemplary method flow diagram for the disclosed method for trapping and manipulating nano particles in a colloidal solution, in accordance with embodiments of the present disclosure.
- the present disclosure provides a colloidal plasmonic tweezer) that can be moved by integrating it with laser tweezers for remote and independent control in nanomanipulation at similar power levels as current state of art plasmonic tweezers.
- FIG. 1A is a representation of trapping of nano particles for nanomanipulationby a plasmonic tweezer shown therein as a disc.
- a plasmonic gradient force of localized and enhanced electromagnetic intensity in optical near field is generated, which causes the plasmonic tweezer to work as a plasmonic antenna to trap the nano particles.
- such nanomanipulation requires a suitable antenna where plasmonic enhancements are strong enough to support trapping, and the resonance wavelength of the antenna falls under the biological transparency window where absorption of light in biological matter is minimal.
- the nanodisc geometry can be used where the localised surface plasmon resonance wavelength can be tuned with its size.
- FIG. IB illustrates an exemplary graph of localised surface plasmon resonance (LSPR) wavelength as a function of disk diameter.
- LSPR localised surface plasmon resonance
- the plasmonic antenna in order to overcome the above stated issue, can be combined with a bigger dielectric object which can be trapped with relative ease and steered inside a closed microfluidic chamber using a single beam optical tweezer without any detrimental effects to the plasmonic part.
- FIG. 1C illustrates thermal diffusivity (Brownian sensitivity) of a nanorod as a function of its length.
- the rod has a fixed diameter of about 250 nm. It can be observed that there is an exponential dependence of thermal diffusivity with length of the rod.
- FIG. ID illustrates an exemplary structure of the proposed CPT, integrating the plasmonic nanodisc 102 with a dielectric nanorod 104. Also shown alongside is an SEM image showinga plurality of CPTs attached to a substratel08.As can be seen, the disc 102 is coupled to one end of the nanorod 104.
- the disc 102 may be configured to work as a plasmonic antenna to trap the nano particles, as shown in FIG. 1A, using a plasmonic gradient force of localized and enhanced electromagnetic intensity in optical near field generated by the discs as a result of a light beam focussed on the colloidal plasmonic tweezer.
- Suitable materials areSilver Gold, Aluminium-doped Zinc Oxide, and Titanium nitride etc.
- disc 102 is made of Silver.
- the dielectric nanorod is configured such that the colloidal plasmonic tweezer is trapped to the light beam on account of far field optical forces acting on the dielectric nanorod as a result of the light beam, thereby enabling movement of the colloidal plasmonic tweezer by steering the light beam.
- a suitable dielectric material for making the nanorod 104 is, but not limited to Silicon dioxide.
- the diameter of the disc 102 may be in the range of 200 to 300 nm, and thickness of the disc 102 may be the range of 40-60 nm.
- Length and diameter of the nanorod 104 may be in the range of 2.00-3.00 pm and 40-60 nm respectively.
- the length and diameter of the nanorodl04 are kept 2.5 pm and 50 nm respectively, and the diameter and thickness of the disc is kept 250 nm and 50 nm respectively.
- a bottom-up approach is employed to design a hybrid metal - dielectric geometry consisting of a silver (Ag) nanodisc of about 250 nm diameter and 50 nm thickness integrated to a 2.5 pm long rod of diameter 250 nm, made of Silicon dioxide (Si02).
- the silver nanodisc plays a crucial role in generating plasmonic gradient force when illuminated with light, which acts as a plasmonic trap, whereas the dielectric part only facilitates optical confinement of the plasmonic tweezer itself.
- the long dielectric nanorod 104 helps in reducing the optical power requirement by minimizing Brownian diffusion.
- the power requirement can be further reduced by combining a plasmonic element with the dielectric nanorod 104 as the effective optical volume increases due to increase in polarizability.
- metal nanoparticles can be captured more strongly than similar sized dielectric particle due to their higher polarizability. Therefore, the hybrid geometry allows the CPT 100 to be operated at low optical power.
- FIG. 2 illustrates an exemplary system for trapping and manipulating nano particles in a colloidal solution, using the proposed CPT, in accordance with embodiments of the present disclosure.
- the system 200 may comprise a microfluidic chamber 202 to hold a colloidal solution containing a plurality of the colloidal plasmonic tweezers 100 and nano particles 204 to be trapped and manipulated, and a laser source206 to generate an elliptically polarized light beam 212.
- the laser source 206 may be coupledan optical microscope 208.
- the system 200 may also comprise at least one galvo-mirror 210 in path of the light beam212 emanating from the laser source 206 to remotely steer the light beam 212.
- the elliptically polarized laser light beam212 can be a low power infrared laser to enable in vivo use of the system 200.
- the colloidal solution can be an in vivo biofuel, such as an ionic biofluid.
- the colloidal solution may be based on any or a combination of interesting fluids such as hyaluronic gel and vitreous humour, and the trapping and manipulating nano particles of interest may be done in ex- Vivo conditions.
- the experiments wereperformed using an elliptically polarised laser source (Nd:YAG; 1064 nm) 206 coupled to a standard optical microscope 208 using a 100X, 1.4NA oil immersion objective.
- the laser spot size can be externally controlled using a telescopic lens assembly 214.
- the focused laser/light beam 212 serves two purposes - simultaneously exciting and holding the CPT 100, which is designed in such a way that dielectric rod 104 acts as a passive element and does not affect the surrounding colloids.
- the CPT 100 held at the laser focus can be manoeuvred precisely by moving the computer-controlled stage. Inside the laser focus, the CPT 100 can have two possible orientations - parallel and perpendicular, with respect to light propagation direction.
- FIG. 3A illustrates a scattering and absorption cross section of plasmonic nanodisc showing plasmon resonances at around 980 nm for in-plane polarisation .
- multiple resonance modes are possible.
- high energy (lower wavelength) modes are not used as silver becomes highly absorbing in that regime, and because of which low energy mode at infrared regime is preferred, which shows large electric field intensity enhancement.
- the use of low power, infra-red lasers makes it compatible for delicate use such as for in-vivo applications.
- FIG. 3B illustrates differential orientation of CPT with respect to laser illumination.
- the laser wavelength is chosen such that it lies to the slightly red-detuned side of the LSPR wavelength, resulting in attractive pulling force on the plasmonic disc towards the laser focus.
- metallic polarizability is higher compared to dielectric, the attraction is stronger on the metallic side. This brings a preferential vertical orientation of the CPT where the plasmonic nanodisc always stays at laser focus and the light polarization is in-plane to the nanodisc orientation.
- any illumination with blue- detuned laser will repel the plasmonic part out of the focus and in that case dielectric part may be trapped in the laser focus.
- the nanomanipulation is performed for both vertical and horizontal configurations inside a standard microfluidic chamber 202 made of glass.
- the microfluidic chamber 202 contains a suspension of CPTs and cargo in the form of colloidal particles.
- the CPTs are fabricated in large numbers and can be released by sonicating the substrate in a fluid.
- FIG. 3C illustrates trapping of polystyrene particles in plasmonic near-field for vertical and horizontal configurations.
- the particles are trapped around the CPT, which is held at a diffraction limited laser focus with a fraction of a milliwatt, corresponding to an intensity 80 kW/cm2.
- the elliptically polarized light enhances the electric field around the nanodisc, imparting an attractive gradient force on the surrounding colloids and trapping is achieved without any need for substrate engineering.
- FIG. 3D illustrates a beam profile of the diffraction limited laser spot showing the region inaccessible by the trapped particle. It can be observed that the CPT stays at the centre of the laser focus, and therefore, peak intensity is forbidden to the tracer particles, which results in about 10 times reduction in total laser power falling on any individual colloid(for 400 nm particle).
- the defocused illumination is distributed on an area, with intensity equivalent to 20 kW/cm2. It can be noticed that particles again get captured around the nanodisc, but no trapping is observed along the direction of light propagation (z- axis), which can be attributed to zero field enhancement in that direction.
- FIG. 3E illustrates electric field intensity enhancement for the nanodisc in vertical configuration and horizontal configuration.
- the polarization is in X-Y plane and the light propagation is along the Z-axis.
- FIG. 3F illustrates a histogram of fluctuations of the proposed CPT a focused laser (vertical configuration) and defocussed laser (horizontal configuration).
- vertical configuration is advantageous for manipulation at micron-scale spatial resolution with greater control such as to move and collect target colloids.
- FIG. 4A illustrates a graph of minimum illumination intensity required to trap, as a function of bead size for vertical and horizontal configurations of the proposed CPT.
- the minimum intensity to trap a particle with CPT increases as the bead size is decreased.
- minimum trapping intensity required in vertical configuration with focused laser is nearly same for different size of particles and is also higher compared to the horizontal configuration. This is because minimum optical power required for laser trapping of CPTs is higher than the threshold intensity required for plasmonic trapping of the tracer colloids. Therefore, no size dependence can be observed on trapping intensity for vertical configuration.
- 4B illustrates an exemplary plasmonic gradient force on a 200 nm polystyrene particle as a function of distance from the proposed nanodisc.
- the intensity is kept constant at 30 kW/cm2 and this simulation is performed for both vertical and horizontal configurations along the X and Y directions.
- the spatial extent of the trap becomes negligible beyond 50 nm from the CPT surface.
- FIG. 4C illustrates a calculated temperature rise as a function of intensity of wavelength.
- plasmon induced heating is an additional side-effect and can play a critical role in the trapping mechanism.
- temperature is estimated to rise just a few degrees, up to an intensity of 100 kW/cm2 with 1064 nm laser.
- the intensity level at 400 nm wavelength can cause at least 10 times higher temperature rise because of intrinsic loss in material.
- FIG. 5A illustrates trapping and releasing of 100 nm fluorescent nano-diamonds in an ultra-low-density solution.
- the CPT was moved close to catch the nano-diamond without waiting for it to diffuse into the trap.
- a collection of nano diamond is subsequently trapped, manoeuvred and released with a CPT in horizontal configuration.
- the sample stage is moved to take the plasmonic tweezer and the nano-diamonds in and out of illumination for subsequent trapping and releasing without modulating the trapping intensity.
- FIG. 5B illustrates trapping, transporting and releasing of 300 nm fluorescent magnetic particles.
- the laser beam is focused using a fast scanning galvo- mirror 210, at two spots with each spot holding a CPT. Two magnetic particles are first captured in each of them. The tweezers are then independently manoeuvred to two different locations that are about 100 microns apart, where the particles are released one-by-one by turning the illumination off.
- FIG. 6 is an exemplary method flow diagram for the disclosed method for trapping and manipulating nano particles in a colloidal solution using the disclosed colloidal plasmonic tweezers.
- the disclosed method 600 may at step 602 include providing a plurality of colloidal plasmonic tweezers, such as colloidal plasmonic tweezers 100 shown at FIG. ID, in a colloidal solution that contains the nano particles to be manipulated.
- the method 600 may include focussing one or more light beams, such as light beam 212 shown in FIG.
- Step 606 of the method 600 may involve trapping of one or more of the nano particles, such as nono particles 204 shown in FIG. 2, that are of interest by moving the one or more of the colloidal plasmonic tweezers 100 close to the nano particles of interest 204 by steering the corresponding light beams 212.
- Step 608 of the method 600 may involve moving the one or more olloidal plasmonic tweezers 100 along with the trapped nano particles 204 of interest to corresponding desired locations by steering the corresponding light beams 212.
- Step 610 of the method 600 may involve releasing the trapped nano particles 204 at the desired location.
- the method 600 may further include a step of providing a microfluidic chamber, such as microfluidic chamber 202 shown in FIG. 2, to hold the colloidal solution containing the nano particles 204 to be manipulated and the plurality of colloidal plasmonic tweezers 100.
- a microfluidic chamber such as microfluidic chamber 202 shown in FIG. 2, to hold the colloidal solution containing the nano particles 204 to be manipulated and the plurality of colloidal plasmonic tweezers 100.
- the method 600 may further include a step ofproviding one or more polarised laser sources, such as laser source 206 shown in FIG. 2, to generate one or more light beams 212.
- the one or more polarised laser sources 206 may be coupled to an optical microscope, such as the optical microscope 206 shown in FIG. 2.
- the method 600 may further include a step ofproviding at least one galvo-mirror, such as galvo-mirror 210, in paths of the light beams 212 emanating from the one or more polarised laser sources 206 to steer the light beams 212.
- the galvo- mirror 210 may enable steering the corresponding light beam remotely.
- the method 600 may further include a step ofsonicating the colloidal solution to distribute the plurality of colloidal plasmonic tweezers 100 in the colloidal solution.
- the present disclosure provides a system for optical manipulation integrating a plasmonic tweezer with a conventional laser tweezer.
- Proposed colloidal plasmonic tweezer bears a hybrid metal-dielectric design comprising a silver (Ag) nanodisc coupled to a Si02 nanorod.
- the proposed CPT can work in different configurations (vertical, horizontal) based on the type of illumination (red detuned, blue detuned), and can be used to trap and transport various nanomaterials such as nanoparticles, absorbing particles, fluorescent particles, magnetic particles etc.
- the hybrid dielectric -metal design results in minimal heating during operation of the CPT, allowing the CPT to be used for biofluids which are generally susceptible to photodamage. Further, the proposed CPT can be used with remote and independent control.
- the first light beam can be used to manipulate the CPTs while the other one is used to trap colloids.
- the second light beam can be used to heat the CPT so as to use thermophoretic attraction to bring the colloids close to CPT.
- the plasmonic effect can be obtained by alternate plasmonic materials, such as but not limited to TiN and AZO.
- the CPTs can be operated in natural environments, including living biological cells, animals and plants.
- the present disclosure provides a system and method for optical manipulation that does not suffer from drawbacks of known systems and methods for optical manipulation.
- the present disclosure provides a system and method for optical manipulation that uses low power optical illumination and yet do not suffer from drawbacks of plasmonic trapping.
- the present disclosure provides a system and method that uses low power optical illumination for plasmonic trapping of nano particles, and yet allows mobility.
- the present disclosure provides a system and method for nano manipulation that integrates plasmonic and optical trapping to use low power optical illumination to trap nano particles as well as provide mobility for the trapped nano particles.
- the present disclosure provides a system and method for nano manipulation that does not require a specialized substrate.
- the present disclosure provides a system and method for nano manipulation that allows use of multiple laser beams
- the present disclosure provides a system and method for nano manipulation that provides flexibility in antenna design at different illumination.
- the present disclosure provides a system and method for nano manipulation that remote and independent control of movement of the trapped nano particles.
- the present disclosure provides a system and method for nano manipulation that allows selective manipulate of few or multiple nano particles
- the present disclosure provides a system and method for nano manipulation that is compatible for in-vivo applications.
- the present disclosure provides a system and method for nano manipulation that can be used in ionic fluids such as some of the biofluids.
- the present disclosure provides a system and method for nano manipulation that allows can be seamlessly integrated with existing optical tweezer equipment.
Landscapes
- Chemical & Material Sciences (AREA)
- Health & Medical Sciences (AREA)
- General Health & Medical Sciences (AREA)
- Dispersion Chemistry (AREA)
- Fluid Mechanics (AREA)
- Analytical Chemistry (AREA)
- Physics & Mathematics (AREA)
- Hematology (AREA)
- Clinical Laboratory Science (AREA)
- Chemical Kinetics & Catalysis (AREA)
- Microscoopes, Condenser (AREA)
- Physical Or Chemical Processes And Apparatus (AREA)
- Investigating, Analyzing Materials By Fluorescence Or Luminescence (AREA)
Abstract
Description
Claims
Applications Claiming Priority (2)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| IN201841042881 | 2018-11-14 | ||
| PCT/IB2019/059782 WO2020100077A1 (en) | 2018-11-14 | 2019-11-14 | An optical nano-manipulator for particles in a fluid |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| EP3881054A1 true EP3881054A1 (en) | 2021-09-22 |
| EP3881054A4 EP3881054A4 (en) | 2022-08-17 |
Family
ID=70731342
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| EP19885440.8A Withdrawn EP3881054A4 (en) | 2018-11-14 | 2019-11-14 | An optical nano-manipulator for particles in a fluid |
Country Status (2)
| Country | Link |
|---|---|
| EP (1) | EP3881054A4 (en) |
| WO (1) | WO2020100077A1 (en) |
Families Citing this family (4)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7728342B2 (en) | 2020-11-26 | 2025-08-22 | ディーエスエム アイピー アセッツ ビー.ブイ. | Enhancement of virucidal activity of benzoic acid in feed |
| WO2022178902A1 (en) * | 2021-02-28 | 2022-09-01 | 浙江大学 | Method and apparatus for manipulating tiny object |
| CN114390764A (en) * | 2021-12-21 | 2022-04-22 | 桂林电子科技大学 | Electrically-tuned graphene disc nanoparticle plasma optical tweezers |
| CN116682591A (en) * | 2023-04-04 | 2023-09-01 | 哈尔滨工业大学(深圳)(哈尔滨工业大学深圳科技创新研究院) | A method to control particle motion in glassy colloidal systems using optical tweezers |
Family Cites Families (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| WO2009018183A2 (en) * | 2007-07-27 | 2009-02-05 | President And Fellows Of Harvard College | System and method for near-field optical tweezers |
-
2019
- 2019-11-14 WO PCT/IB2019/059782 patent/WO2020100077A1/en not_active Ceased
- 2019-11-14 EP EP19885440.8A patent/EP3881054A4/en not_active Withdrawn
Also Published As
| Publication number | Publication date |
|---|---|
| EP3881054A4 (en) | 2022-08-17 |
| WO2020100077A1 (en) | 2020-05-22 |
Similar Documents
| Publication | Publication Date | Title |
|---|---|---|
| Ghosh et al. | All optical dynamic nanomanipulation with active colloidal tweezers | |
| WO2020100077A1 (en) | An optical nano-manipulator for particles in a fluid | |
| US10603685B2 (en) | Methods and systems for assembly of particle superstructures | |
| Zhou et al. | Recent progress on optical micro/nanomanipulations: structured forces, structured particles, and synergetic applications | |
| Roxworthy et al. | Application of plasmonic bowtie nanoantenna arrays for optical trapping, stacking, and sorting | |
| Shoji et al. | Permanent fixing or reversible trapping and release of DNA micropatterns on a gold nanostructure using continuous-wave or femtosecond-pulsed near-infrared laser light | |
| Quidant | Plasmonic tweezers—The strength of surface plasmons | |
| US7696473B2 (en) | Method of optical manipulation of small-sized particles | |
| Cuche et al. | Brownian motion in a designer force field: dynamical effects of negative refraction on nanoparticles | |
| Zhong et al. | Oscillations of absorbing particles at the water-air interface induced by laser tweezers | |
| Lin et al. | Efficient optical trapping and detection of nanoparticle via plasmonic bowtie notch | |
| Sharma et al. | Optothermal pulling, trapping, and assembly of colloids using nanowire plasmons | |
| Xiang et al. | Optical trapping with focused surface waves | |
| Mishra et al. | Nature of trapping forces in optically induced electrothermal vortex based tweezers | |
| Shalin et al. | Optical forces in plasmonic nanoantennas | |
| Samadi et al. | Thermophoresis suppression by graphene layer in tunable plasmonic tweezers based on hexagonal arrays of gold triangles: numerical study | |
| Numata et al. | Manipulation of metal nanoparticles using fiber-optic laser tweezers with a microspherical focusing lens | |
| Kotsifaki et al. | Giant optical forces using an array of asymmetric split-ring plasmonic nanostructures | |
| Chen et al. | Plasmon-Enhanced Optothermal Manipulation | |
| Iyengar et al. | Trapping characterization of semi metallic magnetic beads in optical tweezers | |
| Chen et al. | Optical trapping with pillar bowtie nanoantennas | |
| Tinguely et al. | Nanostructured fibre tip for trapping of nanoparticles | |
| Villangca et al. | Photothermal heating in metal-embedded microtools for material transport | |
| Toussaint Jr et al. | Plasmonic nanotweezers based on Au bowtie nanoantenna arrays for manipulation of nano-to-macroscopic objects | |
| Park et al. | Influence of laser power and beam path under nonuniform AC electric fields on 3D microvortex flow |
Legal Events
| Date | Code | Title | Description |
|---|---|---|---|
| STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE INTERNATIONAL PUBLICATION HAS BEEN MADE |
|
| PUAI | Public reference made under article 153(3) epc to a published international application that has entered the european phase |
Free format text: ORIGINAL CODE: 0009012 |
|
| STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: REQUEST FOR EXAMINATION WAS MADE |
|
| 17P | Request for examination filed |
Effective date: 20210611 |
|
| AK | Designated contracting states |
Kind code of ref document: A1 Designated state(s): AL AT BE BG CH CY CZ DE DK EE ES FI FR GB GR HR HU IE IS IT LI LT LU LV MC MK MT NL NO PL PT RO RS SE SI SK SM TR |
|
| DAV | Request for validation of the european patent (deleted) | ||
| DAX | Request for extension of the european patent (deleted) | ||
| A4 | Supplementary search report drawn up and despatched |
Effective date: 20220715 |
|
| RIC1 | Information provided on ipc code assigned before grant |
Ipc: B82Y 20/00 20110101ALI20220711BHEP Ipc: B82Y 15/00 20110101ALI20220711BHEP Ipc: B01L 3/00 20060101ALI20220711BHEP Ipc: H05H 3/04 20060101ALI20220711BHEP Ipc: B82Y 30/00 20110101ALI20220711BHEP Ipc: G01N 1/00 20060101ALI20220711BHEP Ipc: G01N 21/00 20060101AFI20220711BHEP |
|
| STAA | Information on the status of an ep patent application or granted ep patent |
Free format text: STATUS: THE APPLICATION HAS BEEN WITHDRAWN |
|
| 18W | Application withdrawn |
Effective date: 20240604 |