Abstract:
The invention relates to an optical substance manipulator capable of continuing to apply a continued force of action to moving substances without being limited by the flowing conditions for the substances yet with a wide manipulation margin and with efficiency, thereby continuously carrying out various manipulations such as separation, concentration, mixing, and deflection. Specifically, the invention provides an optical substance manipulator capable of manipulating microscopic particles dispersed in a flowing fluid by means of light pressure, characterized by comprising an optical system that forms multiple linear light-collective areas simultaneously with respect to a fluid that flows on a subject surface  5,  and further comprising, in optical paths forming the respective linear light-collective areas, means CL 1 , CL 2  adapted to adjust directions of the linear light-collective areas on the subject surface and means M 1 , M 2  adapted to adjust positions of the linear light-collective areas.

Description:
[0001]     This application claims benefit of Japanese Application No. 2006-142315 filed in Japan on May 23, 2006, the contents of which are incorporated by this reference.  
       BACKGROUND OF THE INVENTION  
       [0002]     The present invention relates generally to an optical substance manipulator, and more particularly to an optical substance manipulator harnessing the principles of optical tweezers, which are applied to some fields such as biochemical, molecular mechanics and micro•nanoscale thermofluid engineering fields.  
         [0003]     Optical substance manipulation techniques represented by an optical tweezers device are capable of manipulating a microscale substance in a non-contact, non-destructive fashion. There is an optical tweezers technique extensively put into practical uses, in which light is tightly focused by an objective lens or the like into a medium such as a solution or air, so that a substance (particles) can be picked up near the focus of incident light by virtue of light pressure occurring at the substance interface in the medium (see Non-Patent Publication 1).  
         [0004]     The optical tweezers technique is capable of picking up a substance in a non-contact way, and manipulating the captured subject three-dimensionally with a micrometric order resolving power. For this reason, there has been much achieved through its use as an experimental tool that applies any desired manipulation to a subject of sub-microscopic size such as a single cell or DNA to go deep into what happens chemically and biologically (Non-Patent Publication 2). As one example, there is the result so far reported of using optical tweezers to take hold of and manipulate microscopic particles added to both terminus of a string form of single molecule, thereby making a knot across the molecular and measuring a tension change (Non-Patent Publication 3).  
         [0005]     The optical substance manipulation techniques used so far in the art, for the most part, make use of laser light obtained by entering parallel light in a collective lens such as an objective lens to focus that light onto one point. With this method, strong manipulation force is obtainable because the light is focused with high intensity; however, there is the scope of action narrowing down to a few micrometers for that. Further, the directionality of manipulation force resulting from light pressure is only limited to that of trapping force toward, or repulsive force off, the laser focus. For this reason, a substance of micrometer order is manipulated by a method wherein once that substance has been trapped at the focus, the whole ambient medium or the whole laser irradiation system is moved to transfer the substance. This method works very favorably for moving a single substance to any desired position; however, it renders it difficult to apply extensive manipulation, continuous manipulation, and fast manipulation to a group of massive substances scattered in the medium.  
         [0006]     In recent years, an idea for making up for the narrowness of the range of action of the optical tweezers technique has been proposed: there are a number of laser irradiation areas formed in a medium as by locating a special diffraction grating or the like in a laser light path to split a laser beam into multiple beams, so that multiple substances can be manipulated simultaneously (Non-Patent Publication 4, and Patent Publications 1 and 2). Also, it has been reported that by locating a cylindrical lens or the like in an optical path, the laser focus is so transformed that multiple substances can be trapped linearly (Non-Patent Publication 5). With these methods, it is true that the amount of concurrently manipulatable substances can be increased; however, they are similar to the prior art in terms of light pressure being used as a substance trapping force, and so are used mainly for substance manipulation after trapping.  
         [0007]     To enable continuous manipulation without taking hold of a substance, it is necessary to continue to apply continued force of action to a moving substance. For instance, if a subject group of substances is in a constantly flowing state, continuous manipulation is enabled even with trapping force as light pressure. In this regard, there is a continuous manipulation method proposed, using multi-point optical tweezers using a diffraction grating (Non-Patent Publications 6 and 7, and Patent Publication 1). However, the performance of action would vary largely depending on the flowing conditions for substances. In addition, this method is inefficient because the margin of substance manipulation is narrow relative to the range of substantial light irradiation.  
         [0008]     Patent Publication 1  
         [0009]     JP2005-502482A  
         [0010]     Patent Publication 2  
         [0011]     JP2005-515878A  
         [0012]     Non-Patent Publication 1  
         [0013]     Hiroo Ukita, “Micromechanical Photonics—Applications of Optical Information Systems”, pp. 61 (published by Morikita Shuppan Co., Ltd., 2002, 9)  
         [0014]     Non-Patent Publication 2  
         [0015]     Ashkin, A., IEEE Journal of Selected Topics in Quantum Electronics, Vol. 6, pp. 841-856, (2000)  
         [0016]     Non-Patent Publication 3  
         [0017]     Arai, Y., et al., Nature, Vol. 399, pp. 446-448, (1999)  
         [0018]     Non-Patent Publication 4  
         [0019]     Grier, D. G., Nature, Vol. 424, pp. 810-816, (2003)  
         [0020]     Non-Patent Publication 5  
         [0021]     Dasgupta, R., et al., Biotechnology Letters, 25, Pp. 1625-1628, (2003)  
         [0022]     Non-Patent Publication 6  
         [0023]     Korda, P. T., et al., Physical Review Letters, Vol. 89, No. 12, 128301, (2002)  
         [0024]     Non-Patent Publication 7  
         [0025]     MacDonald, M. P., et al., Nature, Vol. 426, pp. 421-424, (2003)  
       SUMMARY OF THE INVENTION  
       [0026]     The prior art situations being like this, the present invention has for its object the provision of an optical substance manipulator capable of continuing to apply a continued force of action to moving substances without being limited by the flowing conditions for the substances yet with a wide manipulation margin and with efficiency, thereby continuously carrying out various manipulations such as separation, concentration, mixing, and deflection.  
         [0027]     According to the invention, that object is achieved by the provision of an optical substance manipulator capable of manipulating microscopic particles dispersed in a flowing fluid by means of light pressure, characterized by comprising an optical system that forms multiple linear light-collective areas simultaneously with respect to a fluid that flows on a subject surface, and further comprising, in optical path forming the respective linear light-collective areas, means adapted to adjust the directions of the linear light-collective areas on the subject surface and means adapted to adjust the positions of the linear light-collective areas.  
         [0028]     Preferably in this case, that means adapted to adjust the directions of the linear light-collective areas is a cylindrical lens or mirror adjustable in terms of rotation.  
         [0029]     Similarly, it is preferred that the means adapted to adjust the positions of the linear light-collective areas comprises an optical element adjustable in terms of position and angle.  
         [0030]     It is also preferred that the aforesaid optical system works splitting light coming out of one light source into two or more and synthesizing light after passing through the means adapted to adjust the directions of the linear light-collective areas and the means adapted to adjust the positions of the linear light-collective areas.  
         [0031]     It is further preferred that there are two linear light-collective areas formed, and the aforesaid optical system comprises light splitter means adapted to split light coming out of one light source into two, means adapted to adjust the directions of the linear light-collective areas, means adapted to adjust the positions of the linear light-collective areas, and light synthesis means adapted to synthesize the light split into two.  
         [0032]     The optical substance manipulator of the invention provides a non-contact type substance manipulation system that harnesses laser radiation pressure with an improved degree of flexibility in the ability to manipulate subjects. As compared with the prior optical tweezers art, the invention makes it easier to implement a bulk of manipulations for a group of substances scattered over an extensive range: it is possible to manipulate cells and DNAs in large quantities and in continuous fashions. The invention, because of manipulating substances without fixing them to one site, also allows for continued manipulations of substances flowing in a microscopic flowing topology represented by microchemical chips. With the invention harnessing non-destructive laser light, it is further possible to manipulate biological substances while keeping them intact. Furthermore, the invention allows for localized manipulation limited to the laser irradiation range, making a lot of contributions to the development of technology toward the integration of functions on chips for DNA analysis and chemical synthesis. In addition, the optical substance manipulator of the invention can be additionally attached to an optical microscope, and so has high general versatility with sample vessels. Thus, the inventive optical substance manipulator can implement various substance manipulations on the same system without recourse to any exclusive diffraction gratings, etc., and so would have a lot more applications in a lot more fields, and ever higher versatilities as well.  
         [0033]     Still other objects and advantages of the invention will in part be obvious and will in part be apparent from the specification.  
         [0034]     The invention accordingly comprises the features of construction, combinations of elements, and arrangement of parts which will be exemplified in the construction hereinafter set forth, and the scope of the invention will be indicated in the claims. 
     
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0035]      FIG. 1  is illustrative in schematic of the construction of one embodiment of the optical substance manipulator according to the invention.  
         [0036]      FIG. 2  is a taken-apart view of an optical path through the optical substance manipulator of  FIG. 1 .  
         [0037]      FIG. 3  is illustrative in schematic of the behavior of microscopic particles dispersed in a fluid that flows through a flow path in the case where light is collected at one linear light-collective area.  
         [0038]      FIG. 4  is illustrative in schematic of the behavior of microscopic particles dispersed in a fluid that flows through a flow path in the case where light is collected by the optical substance manipulator of  FIG. 1  at two linear light-collective areas. 
     
    
     DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0039]     The optical substance manipulator of the invention is now explained with references to one preferred embodiment.  FIG. 1  is illustrative in schematic (perspective) of the construction of one embodiment of the optical substance manipulator. For a better understanding of explanation, coordinate axes X, Y and Z are determined as shown. Linearly polarized laser light oscillated from a light source laser  1  (e.g., a near infrared Nd:YAG laser of 1,064 nm in wavelength) is expanded in beam diameter at a beam expander made up of a negative lens L 1  and a positive lens L 2  cofocal with each other, incident on a half-wave plate λ/2 at which its direction of polarization is rotated in a given direction. Then, the light enters the first polarization beam splitter BS 1  at which it is split into two components: a component polarized in the Z direction (hereinafter called p-polarized light) and a component polarized in the XY direction (similarly s-polarized light). The p-polarized light component travels toward a mirror M 1  through the first polarizing beam splitter BS 1  while the s-polarized light propagates toward a mirror M 2  upon reflection at the first polarizing beam splitter BS 1 . The respective beams go from the first polarizing beam splitter BS 1  through cylindrical lenses CL 1  and CL 2  located before the mirrors M 1  and M 2  in an optical path, and are reflected at the mirrors M 1  and M 2 , arriving at the second polarizing beam splitter BS 2 . Here, the s-polarized light component alone is reflected while the p-polarized light component passes through; both the beams travel in the Y-axis direction. Two such beams are expanded in beam diameter by positive lenses L 3  and L 4  cofocal with each other, arriving at a mirror M 3 ; however, a quarter-wave plate λ/4 interposed between the positive lenses L 3  and L 4  turns them into circularly polarized light. The laser light reflected by the mirror M 3  in the X-axis direction enters a filter box  2  built in an inverted microscope. The two beams are reflected in the Z-axis direction by the first dichroic mirror DM 1  located in the filter box  2  and has the property of transmitting visible light and reflecting light in the near infrared range. The two beams then enter an infinity correction oil immersion objective lens Ob mounted on the microscope where they are collected, entering a subject in a flow passage  5  through a microchannel MC via an oil immersion oil. Note here that there is a mercury lamp  3  located to illuminate the subject in the flow passage  5  through the microchannel MC; that is, illumination light from that mercury lamp  3  is reflected off the second dichroic mirror DM 2  located on a viewing side with respect to the first dichroic mirror DM 1 , and enters the objective lens Ob through the first dichroic mirror DM 1  where it is collected to illuminate the subject. A fluorescent image of the subject in the flow passage through the micro-channel MC, magnified by the objective lens Ob, is taken by a photographic camera  4  through the first and second dichroic mirrors DM 1  and DM 2 . That image is displayed, and recorded.  
         [0040]     The half-wave plate λ/2 here is adjustable in terms of rotation about the optical axis (X-axis) so that the direction of linearly polarized light oscillated from the laser  1  is adjustable. By that adjustment, it is possible to adjust the proportion of the p- and s-polarized light components incident on the first polarizing beam splitter BS 1 .  
         [0041]     Why the two beams are turned by the quarter-wave plate λ/4 into circularly polarized light for incidence on the subject is to hold back the generation of unwanted interference fringes.  
         [0042]     The positions of mirrors M 1  and M 2  are adjustable in the direction of propagation of the respective beams (the mirror M 1  for the X-axis direction, and the mirror M 2  for the Y-axis direction), and the angles of mirrors M 1  and M 2  are adjustable about the Z-axis and the direction of propagation of each beam (the mirror M 1  about the X-axis and the mirror M 2  about the Y-axis), respectively. Further, the position of mirror M 3  is adjustable in the direction of propagation of the beam (the Y-axis direction), and the rotation of cylindrical lenses CL 1  and CL 2  about the X- and Y-axes, respectively, is adjustable as well.  
         [0043]      FIG. 2  is a taken-apart view of one optical path from the laser  1  of the optical substance manipulator of  FIG. 1  via the first polarizing beam splitter BS 1 , the cylindrical lens CL 1  and the second polarizing beam splitter BS 2  as far as a focal plane F (subject surface) in the flow passage through the microchannel MC, and the same applies to another optical path through the cylindrical lens CL 2 , too. To be more specific,  FIG. 2 ( a ) is a taken-apart view of the optical path in a section along the generator of the cylindrical lens CL 1 , and  FIG. 2 ( b ) is a taken-apart view of the optical path in a section orthogonal to that generator. In FIGS.  2 ( a ) and  2 ( b ), the focal length of each lens and inter-lens distances are given in mm.  
         [0044]     In the section of  FIG. 2 ( a ) where the refracting power of the cylindrical lens CL 1  (CL 2 ) does not work, parallel light oscillated from the laser  1  is expanded in beam diameter by the beam expander made up of the negative lens L 1  and the positive lens L 2 . The parallel light with an expanded beam diameter goes through the half-wave plate λ/2, the first polarizing beam splitter BS 1 , the cylindrical lens CL 1  (CL 2 ), the mirror M 1  (M 2 ) and the second polarizing beam splitter BS 2 , and is expanded in beam diameter through the positive lenses L 3  and L 4  cofocal with each other with the quarter-wave plate λ/4 interposed between them. The parallel light goes through the mirror M 3  and enters as such the infinity correction objective lens Ob, focusing on the focal plane F.  
         [0045]     In the section of  FIG. 2 ( b ) where the refracting power of the cylindrical lens CL 1  (CL 2 ) works, on the other hand, a light beam through the cylindrical lens CL 1  (CL 2 ) turns under its positive refracting power into convergent light that converges in front of the positive lens L 3 . In the rear of the point of convergence, that convergent light turns into divergent light that is then incident on the positive lens L 3 . That divergent light again turns under the positive refracting powers of the positive lenses L 3  and L 4  into convergent light that converges in front of (on the viewing side) the objective lens Ob. In the rear of the point of convergence, the light, divergent one this time, enters the objective lens Ob, and focuses at a minute distance A off the focal plane F under the positive refracting power of the objective lens Ob.  
         [0046]     For this reason, the laser light is incident on the focal plane (subject surface) F: it is incident on a point in the section where the refracting power of the cylindrical lens CL 1  does not work while it is incident on a certain width in the section where the refracting power of the cylindrical lens CL 1  works, so that it can focus on the focal plane (subject surface) F in a linear or elliptic form. In other words, the laser light focuses on the focal plane (subject surface) F in two linear areas extending in the direction orthogonal to the generator of the cylindrical lens CL 1 , CL 2 .  
         [0047]     And then, the position of each linear light-collective area is arbitrarily adjustable within the focal plane (subject surface) F by the adjustment of the position and angle of the mirror M 1 , M 2  in the optical path, respectively. Further, the direction of that area is adjustable by the adjustment of the angle of each cylindrical lens CL 1 , CL 2  about the optical axis.  
         [0048]     In such arrangement, a shutter was mounted on the s-polarized beam optical path (running from the first polarizing beam splitter BS 1  to the mirror M 2  and the second polarizing beam splitter BS 2  via the cylindrical lens CL 2 ) while light made its way through only the p-polarized beam path (running from the first polarizing beam splitter BS 1  to the mirror M 1  and the second polarizing beam splitter BS 2  via the cylindrical lens CL 1 ). Then, the photographic camera  4  was used to pick up the behavior of microscopic particles dispersed in a fluid flowing in the flow passage  5  in the case where one linear light-collective area was positioned in the flow passage  5  through the microchannel MC. Consequently, such results as shown in  FIG. 3  were obtained.  
         [0049]      FIG. 3 ( a ) is illustrative in schematic of how microscopie particles  11  dispersed in the fluid behaves in the case where the angle of the cylindrical lens CL 1  is adjusted to form a linear light-collective area  10  with its direction lying in the Y-axis direction orthogonal to the direction (X-axis direction) of a flow in the flow passage  5 . The laser light oscillated from the laser  1  is Gaussian distribution one with an intensity peak at the center: the linear light-collective area  10  has the highest intensity at the center. Accordingly, the microscopic particles  11  flowing at right angles with the linear light-collective area  10  under the radiation pressure of laser light go in the linear light-collective area  10 , and once the microscopic particles  11  enter the linear light-collective area  10 , they move from both its sides, gathering together in the central direction.  
         [0050]      FIG. 3 ( b ) is illustrative, as in  FIG. 3 ( a ), of the case where an almost half of the Gaussian distribution beam focusing on the focal plane F is blocked off halfway down in the optical path to bring the position of the linear light-collective area  10  having the highest intensity to near the right end of the drawing. In this case, the microscopic particles  11  flowing at right angles with the linear light-collective area  10  under the radiation pressure of laser light go into the linear light-collective area  10 , and once the microscopic particles  11  enter the linear light-collective area  10 , they move from the left to the right end of the drawing. The microscopic particles  11  gathering near that right end are saturated, leaving that right end in the flowing direction.  
         [0051]      FIG. 3 ( c ) is a schematic view illustrative of how microscopic particles  11  dispersed in the fluid behaves in the case where the angle of the cylindrical lens CL 1  is adjusted to form a linear light-collective area  10  with its direction lying obliquely at an angle with the direction of a flow in the flow passage  5  (the X-axis direction). In this case, the microscopic particles  11  flowing at an angle with the linear light-collective area  10  under the radiation pressure of laser light go into the linear light-collective area  10 , and once the microscopic particles  11  enter the linear light-collective area  10 , they move a direction along the flow, or from the upper left to the lower right of the drawing when the linear light-collective area  10  tilts as shown. Then, the microscopic particles gathering together at that lower right end are saturated, leaving the lower right end in the direction of the flow.  
         [0052]     Reference is then made to a modification to the inventive arrangement of  FIG. 1  wherein light of almost equal intensity goes along both the p- and s-polarized beam paths: an account is given of how microscopic particles  11  dispersed in a fluid flowing in the flow passage  5  behaves where two linear light-collective areas  101  and  102  are located in the flow passage  5  through microchannel MC.  
         [0053]     As shown in  FIG. 4 ( a ), the angles of cylindrical lenses CL 1  and CL 2  are adjusted with their refracting powers acting in the same direction to form two light-collective areas  101  and  102  at the same position in the direction of a flow within the flow passage  5  and with their directions lying orthogonal to that direction; as shown in  FIG. 3 ( b ), the left linear light-collective area  101  is positioned such that there is the highest intensity at the right end, and the right linear light-collective area  102  is positioned such that there is the highest intensity at the left end; and between the left  10   1  and the right linear light-collective area  10   2 , there is a gap formed by the adjustment of the position and angle of the mirror M 1  at the p-polarized light beam path and by the adjustment of the position and angle of the mirror M 2  at the s-polarized light beam path. Then, the microscopic particles  11  flowing at right angles with the linear light-collective areas  10   1  and  10   2  under the radiation pressure of laser light go into the respective linear light-collective areas  10   1  and  10   2 , and once they enter the linear light-collective areas  10   1  and  10   2 , they move from the left to the right end of the area  10   1  and from the right to the left end of the area  10   2 : they pass through the gap between the left  10   1  and the right linear light-collective area  10   2  as if focused or concentrated on that gap.  
         [0054]     As shown in  FIG. 4 ( b ), the angles of cylindrical lenses CL 1  and CL 2  are separately adjusted such that at the same position in a direction of a flow within the flow passage  5 , the left linear light-collective area  10   1  lies in an obliquely lower right direction and the right linear light-collective area  10   2  lies in an obliquely lower left direction, as shown in  FIG. 3 ( c ), and between the lower right end of the left  10   1  and the lower left end of the right linear light-collective area  10   2 , there is a gap formed by the adjustment of the position and angle of mirrors M 1  and M 2  in the respective optical paths. Then, microscopic particles  11  flowing at angles with the linear light-collective areas  10   1  and  10   2  under the radiation pressure of laser light go into the respective linear light-collective areas  10   1  and  10   2 , and once they enter the linear light-collective areas  10   1  and  10   2 , they move from obliquely above to below in the drawing: they pass through the gap between the left  10   1  and the right linear light-collective area  10   2  as if focused or concentrated on that gap.  
         [0055]     As shown in  FIG. 4 ( c ), the angles of cylindrical lenses CL 1  and CL 2  are adjusted with their refracting powers acting in the same direction such that the left and right light-collective areas  10   1  and  10   2  at the same position in the direction of a flow within a flow passage  5  are formed parallel at a spacing in an obliquely lower right direction. Then, microscopic particles  11  flowing at angles with the linear light-collective areas  10   1  and  10   2  under the radiation pressure of laser light go into the linear light-collective areas  10   1  and  10   2 , and once they enter the linear light-collective areas  10   1  and  10   2 , they move from obliquely above to below of the drawing. The microscopic particles  11  gathering together at the lower ends of the respective linear light-collective areas  10   1  and  10   2  are saturated, leaving the respective lower ends while separated into two.  
         [0056]     As shown in  FIG. 4 ( d ), the angles of cylindrical lenses CL 1  and CL 2  are separately adjusted such that at the same position in the direction of a flow within a flow passage  5 , the left linear light-collective area  10   1  lies in an obliquely lower left direction and the right linear light-collective area  10   2  lies in an obliquely lower right direction, as shown in  FIG. 3 ( c ), and the areas  10   1  and  10   2  are positioned by the adjustment of the positions and angles of mirrors M 1  and M 2  in the respective optical paths with the upper right end of the left  10   1  in contact with the upper left end of the right linear light-collective area  10   2 . Then, microscopic particles  11  flowing at angles with the linear light-collective areas  10   1  and  10   2  under the radiation pressure of light laser go into the respective linear light-collective areas  10   1  and  10   2 , and once they enter the linear light-collective areas  10   1  and  10   2 , they move from obliquely above to below of the drawing, whereupon the microscopic particles  11  gathering together at the lower ends of the linear light-collective areas  10   1  and  10   2  are saturated, leaving the respective lower ends while separated into two.  
         [0057]     As described above, by the adjustment of the angles and relative positions of two linear light-collective areas  10   1  and  10   2  formed within the flow passage  5  with respect to the direction of the flow, for instance, it is possible to pick up, collect, concentrate, separate, deflect, deliver, mix, and sort out suspending microscopic particles, cells, DNAs or the like flowing within the flow passage  5 . Fast rotation of the cylindrical lenses CL 1  and CL 2  is capable of stirring, mixing or otherwise processing them, too. Of course, the provision of three or more linear light-collective areas  10  formed by simultaneous collection of light makes more complicated manipulations possible.  
         [0058]     In the arrangement of the embodiment of  FIG. 1 , cylindrical mirrors may just as well be used in place of the cylindrical lenses CL 1  and CL 2 ; instead of the mirrors M 1  and M 2 , other optical elements such as prisms may just as well be employed; and in lieu of the beam splitters BS 1  and BS 2 , other light splitting means or optical combinations such as half-silvered mirrors may just as well be used.  
         [0059]     While the optical substance manipulator of the invention has been described with reference to some embodiments, it is contemplated that the invention is in no sense limited to them, and so many modifications could be possible. For instance, it is understood that the number of linear light-collective areas to be formed within the flow passage is not always limited to two; three or more such areas may just as well be used.