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Optics Express

  • Editor: Michael Duncan
  • Vol. 13, Iss. 19 — Sep. 19, 2005
  • pp: 7458–7465
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Robustness of holographic optical traps against phase scaling errors

Sang-Hyuk Lee and David G. Grier  »View Author Affiliations


Optics Express, Vol. 13, Issue 19, pp. 7458-7465 (2005)
http://dx.doi.org/10.1364/OPEX.13.007458


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Abstract

Complex three-dimensional patterns of multifunctional optical traps can be encoded in phase-only computer-generated holograms and projected with the holographic optical trapping technique. The trap-forming holograms, in turn, are implemented as diffractive optical elements whose phase transfer functions generally do not faithfully reproduce the design. We demonstrate that phase encoding errors reduce the overall intensities of the projected traps but, remarkably, do not affect their positions, relative intensities or mode structure. We exploit this robust performance to implement dual-color holographic optical tweezers with a single hologram.

© 2005 Optical Society of America

Holographic optical traps use phase-only holograms to form large arrays of optical traps from a single input laser beam. By combining the beam-splitting and wavefront-shaping capabilities of computer generated holograms, holographic traps can be arranged in arbitrary three-dimensional configurations, with each trap having independently specified characteristics, including relative intensity and mode structure. The unsurpassed control over the microscopic world afforded by this technique has been widely adopted for fundamental research in soft-matter systems and for biomedical and industrial applications [1

1. D. G. Grier, “A revolution in optical manipulation,” Nature 424, 810–816 (2003). [CrossRef] [PubMed]

].

In principle, holographic trapping patterns can be projected with absolute fidelity to design and near-ideal efficiency. Practical diffractive optical elements (DOEs), however, seldom offer the requisite continuously varying phase profiles, and almost never provide precisely the phase pattern required for in a given design. This has been recognized as a central problem for holographic projection systems since the introduction of the kinoform [2

2. L. B. Lesem, P. M. Hirsch, and J. A. Jordan, “The kinoform: A new wavefront reconstruction device,” IBM J. Res. Develop. 13, 150–155 (1969). [CrossRef]

]. Imperfectly imprinting the designed phase pattern onto the input beams wavefronts degrades the projected intensity patterns. To quantify this, we adapt the classic expansion of the projected field into generalized conjugates of the designed field [3

3. J. W. Goodman and A. M. Silverstri, “Some effects of Fourier-domain phase quantization,” IBM J. Res. Dev. 14, 478 (1970). [CrossRef]

, 4

4. J. P. Riley and F. N. Birkett, “A reflection kinoform for use with a CO2 laser,” Optica Acta 24, 999–1009 (1977). [CrossRef]

]. This analysis demonstrates that the performance of optimized [5

5. M. Polin, K. Ladavac, S.-H. Lee, Y. Roichman, and D. G. Grier, “Optimized holographic optical traps,” Opt. Express 13, 5831–5845 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-15-5831. [CrossRef] [PubMed]

] holographic trapping systems is remarkably robust against phase defects, and further suggests useful extensions of the technique.

A standard holographic optical trapping system [6

6. E. R. Dufresne and D. G. Grier, “Optical tweezer arrays and optical substrates created with diffractive optical elements,” Rev. Sci. Instr. 69, 1974–1977 (1998). [CrossRef]

, 7

7. M. Reicherter, T. Haist, E. U. Wagemann, and H. J. Tiziani, “Optical particle trapping with computer-generated holograms written on a liquid-crystal display,” Opt. Lett. 24, 608–610 (1999). [CrossRef]

, 8

8. J. Liesener, M. Reicherter, T. Haist, and H. J. Tiziani, “Multi-functional optical tweezers using computer-generated holograms,” Opt. Comm. 185, 77–82 (2000). [CrossRef]

, 9

9. E. R. Dufresne, D. Altman, and D. G. Grier, “Brownian dynamics of a sphere in a slit pore,” Europhys. Lett. 53, 264–270 (2001). [CrossRef]

, 10

10. J. E. Curtis, B. A. Koss, and D. G. Grier, “Dynamic holographic optical tweezers,” Opt. Comm. 207, 169–175 (2002). [CrossRef]

] is powered by a collimated laser beam, which is relayed to the input pupil of a high-numerical-aperture lens such as a microscope objective lens. This lens focuses the beam to a diffraction-limited spot at a location determined by the beam’s angle of incidence and degree of collimation at the lens’ input pupil. Such a focused spot acts as a single-beam optical gradient force trap known as an optical tweezer [11

11. A. Ashkin, J. M. Dziedzic, J. E. Bjorkholm, and S. Chu, “Observation of a single-beam gradient force optical trap for dielectric particles,” Opt. Lett. 11, 288–290 (1986). [CrossRef] [PubMed]

] and is capable of capturing and holding mesoscopic objects in three dimensions.

Placing a wavefront-shaping hologram in a plane conjugate to the input pupil transforms the single optical tweezer into a pattern of holographic optical traps whose number, three-dimensional configuration, relative and absolute intensities, and mode structure all are encoded in the hologram. Deficiencies in the hologram’s implementation might reasonably be expected to degrade all of these characteristics. An analysis based on scalar diffraction theory shows otherwise.

E(r)=1λfΩu0(ρ)exp(iφ0(ρ))exp(iΦ(ρ))exp(ikρ22f2z)exp(ikrρf)d2ρ,
(1)

where we have suppressed overall phase factors and assumed zf. Here, u 0 (ρ) and φ 0 (ρ) are the real-valued amplitude and phase profiles, respectively, of the input beam at position ρ in the input pupil Ω, as shown in Fig. 1, and k = 2π/λ is the wavenumber of light of wavelength λ. A diffractive optical element (DOE) imposes the additional phase profile Φ(ρ), which ideally would correspond to the computer-generated hologram φ(ρ) encoding a desired pattern of traps. In practice, Φ(ρ) differs from the Φ(ρ), so that I(r) = |E(r)|2 differs from the planned trapping pattern in the plane of best focus.

Particularly when considering DOEs that encode three-dimensional trapping configurations, identifying the plane of best focus is the first step in assessing performance. If a simple beam-splitting DOE is illuminated with a collimated beam, we may take φ 0 (ρ) = 0, and the resulting pattern of traps comes to sharpest focus when the remaining ρ 2-dependent phase term in the integrand of Eq. (1) vanishes, which occurs in the plane z = 0. The optimized holographic trapping technique [5

5. M. Polin, K. Ladavac, S.-H. Lee, Y. Roichman, and D. G. Grier, “Optimized holographic optical traps,” Opt. Express 13, 5831–5845 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-15-5831. [CrossRef] [PubMed]

] instead uses a slightly converging beam with

φ0(ρ)=kρ22f2z0,
(2)

which shifts the plane of best focus to z = -z 0, for z 0f. Artifacts due to imperfect phase modulation need not focus in the same plane, as we will see, and the resulting axial displacement can minimize their influence. Off-axis displacements have long been used to improve ki-noforms’ reconstruction performance, and have proven useful for improving the mode quality of holographically projected optical traps [13

13. H. He, N. R. Heckenberg, and H. Rubinsztein-Dunlop, “Optical particle trapping with higher-order doughnut beams produced using high efficiency computer generated holograms,” J. Mod. Opt. 42, 217–223 (1995). [CrossRef]

]. Axial displacements [14

14. N. R. Heckenberg, R. McDuff, C. P. Smith, H. Rubinsztein-Dunlop, and M. J. Wegener, “Laser beams with phase singularities,” Opt. Quantum Elect. 24, S951–S962 (1992). [CrossRef]

, 15

15. A. Jesacher, S. Furhpater, S. Bernet, and M. Ritsch-Marte, “Size selective trapping with optical ”cogwheel” tweezers,” Opt. Express 12, 4129–4135 (2004). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-17-4129. [CrossRef] [PubMed]

, 5

5. M. Polin, K. Ladavac, S.-H. Lee, Y. Roichman, and D. G. Grier, “Optimized holographic optical traps,” Opt. Express 13, 5831–5845 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-15-5831. [CrossRef] [PubMed]

] offer additional benefits for holographic trapping.

Our implementation of optimized holographic optical trapping is described in detail in Ref. [5

5. M. Polin, K. Ladavac, S.-H. Lee, Y. Roichman, and D. G. Grier, “Optimized holographic optical traps,” Opt. Express 13, 5831–5845 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-15-5831. [CrossRef] [PubMed]

], and is built around a 100 × NA 1.4 Plan Apo oil immersion objective lens mounted in a Nikon TE-2000U inverted optical microscope. Laser light at a wavelength of 532 nm provided by a Coherent Verdi laser, is imprinted with computer-generated holograms by a Hamamatsu X8267-16 spatial light modulator (SLM) which acts as a DOE with a 768 × 768 array of phase pixels. The focused optical traps are imaged by placing a mirror in the objective lens’ focal plane and capturing the reflected light with an NEC TI-324AII charge-coupled device (CCD) camera.

Most DOEs, including our SLM, can impose only a limited range of phase delays, which ideally corresponds to one wavelength of light, so that φ(ρ) mod 2π = φ(ρ). Introducing the DOE’s phase transfer function, f(x), such that Φ(ρ) = f(φ(ρ)), and noting that exp() is a periodic function of φ with period 2π, we may expand the DOE’s contribution to the field’s phase factor in a Fourier series [3

3. J. W. Goodman and A. M. Silverstri, “Some effects of Fourier-domain phase quantization,” IBM J. Res. Dev. 14, 478 (1970). [CrossRef]

, 4

4. J. P. Riley and F. N. Birkett, “A reflection kinoform for use with a CO2 laser,” Optica Acta 24, 999–1009 (1977). [CrossRef]

]

exp(iΦ(ρ))=n=anexp(inφ(ρ))
(3)
Fig. 1. Schematic diagram of the geometry of an optimized holographic trapping system. Light in the input pupil Ω is focused by a strongly converging lens of focal length f to form an optical trap at r, which is shown trapping a particle.

with coefficients

an=12π02πexp(if(x))exp(inx)dx.
(4)

We accordingly define the generalized n-th order conjugate fields,

En(r)=1λfΩu0(ρ)exp(iφ0(ρ))exp(inφ(ρ))exp(ikρ22f2z)exp(ikrρf)d2ρ.
(5)

The projected field is then

E(r)=n=anEn(r).
(6)

For example, if a DOE created for one wavelength of light, λ, is illuminated with another, λ′, then Φ(ρ) = γφ(ρ) with γ = λ/λ′ ≠ 1 and

an=exp(iπ(nγ))sin(π(nγ))π(nγ).
(7)

Comparable results may be obtained for more general phase transfer functions, including those featuring discrete phase levels. The most stringent test, imperfect binary phase holograms with

f(x)={0xaba<x2π,
(8)

are described in this way with coefficients

an=2inπexp(ina2)exp(ib2)sin(na2)sin(b2).
(9)

These terms also fall off with order as 1/ |n|. Best performance, in this case, is obtained with a = b = π.

Equation (6) reveals that the projected image

I(r)=m,n=anam*En(r)Em*(r)
(10)

includes a proportion |a 1|2 of the intended intensity profile, I 1(r) = |E 1(r)|2, even if the DOE imperfectly implements the requisite hologram. This first-order image is a faithful, undistorted realization of the designed pattern whose accuracy is limited only by errors in calculating φ(ρ) and physical imperfections in the optical train. The other terms in Eq. (10) represent artifacts introduced by the DOE’s phase transfer function f(x).

Fig. 2. Experimentally realized generalized conjugate images, I 0(r) and I -1(r), to a planar arrangements of optical traps, I 1(r).

The term |a 0|2 |E 0(r)|2 in Eq. (10

10. J. E. Curtis, B. A. Koss, and D. G. Grier, “Dynamic holographic optical tweezers,” Opt. Comm. 207, 169–175 (2002). [CrossRef]

) describes the undiffracted portion of the input beam, which typically comes to a focus in the center of the plane z = -z 0. Because it receives a fixed proportion of the light, the resulting “central spot” can be brighter than any of the intended traps in I 1(r).

In conventional holographic optical traps whose DOE is illuminated with collimated light, the entire hierarchy of conjugate fields is focused into the same plane. The central spot, the ghosts, and the undesirable superpositions thus maximally affect the trapping pattern.

The optimized holographic trapping system eliminates most of these defects. Here, the input beam’s curvature is offset by a compensating Fresnel lens function,

φz(ρ,z1)=kρ2z12f2,
(11)

added to the trap-forming hologram and implemented by the DOE [5

5. M. Polin, K. Ladavac, S.-H. Lee, Y. Roichman, and D. G. Grier, “Optimized holographic optical traps,” Opt. Express 13, 5831–5845 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-15-5831. [CrossRef] [PubMed]

]. This shifts the trapping pattern a distance z 1 back along the optical axis toward the focal plane. Because φz (ρ, z 1) also is affected by the DOE’s phase transfer function, it contributes to the hierarchy of conjugate fields in Eq. (5). Noting also that z (ρ, z 1) = φz (ρ,nz 1) shows that the n-th order generalized conjugate field En (r) comes to best focus in the plane z ≈ -z 0 + nz 1. Both the central spot and the ghost images therefore are projected away from the intended trapping pattern, and spurious superpositions are strongly suppressed. Artifacts due to practical limitations of the DOE’s phase transfer function therefore should have a minimal influence on the number, configuration, or relative intensity of traps in an optimized holographic trapping system. This is consistent with the observed performance of such systems [5

5. M. Polin, K. Ladavac, S.-H. Lee, Y. Roichman, and D. G. Grier, “Optimized holographic optical traps,” Opt. Express 13, 5831–5845 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-15-5831. [CrossRef] [PubMed]

]. The principal ramification of a non-ideal f(x) is a reduction in the overall intensity |a 1|2 of the projected trapping pattern.

Adding φz (ρ,z 1) increases the complexity of the projected hologram, which can challenge the capabilities of DOE technologies with limited spatial bandwidths. Systematic metrics for assessing hologram complexity relative to DOE capabilities have yet to be developed. Consequently, the practical limitations of the optimized holographic trapping technique cannot yet be assessed a priori. Nevertheless, complex three-dimensional optimized trapping patterns consisting of hundreds of independent traps have been created with a 768 × 768 array of phase pixels [16

16. Y. Roichman and D. G. Grier, “Holographic assembly of quasicrystalline photonic heterostructures,” Opt. Express 13, 5434–5439 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-14-5434. [CrossRef] [PubMed]

].

The final characteristic of holographically projected traps that we will consider is their mode structure. Conventional optical tweezers typically are formed from collimated TEM00 modes with planar wavefronts. More exotic traps such as optical vortices [13

13. H. He, N. R. Heckenberg, and H. Rubinsztein-Dunlop, “Optical particle trapping with higher-order doughnut beams produced using high efficiency computer generated holograms,” J. Mod. Opt. 42, 217–223 (1995). [CrossRef]

, 17

17. N. B. Simpson, L. Allen, and M. J. Padgett, “Optical tweezers and optical spanners with Laguerre-Gaussian modes,” J. Mod. Opt. 43, 2485–2491 (1996). [CrossRef]

, 18

18. K. T. Gahagan and G. A. Swartzlander, “Optical vortex trapping of particles,” Opt. Lett. 21, 827–829 (1996). [CrossRef] [PubMed]

] and Bessel beams [19

19. A. Vasara, J. Turunen, and A. T. Friberg, “Realization of general nondiffracting beams with computer-generated holograms,” J. Opt. Soc. Am. A 6, 1748–1754 (1989). [CrossRef] [PubMed]

, 20

20. J. Arlt, V. Garces-Chavez, W. Sibbett, and K. Dholakia, “Optical micromanipulation using a Bessel light beam,” Opt. Comm. 197, 239–245 (2001). [CrossRef]

] derive their interesting and useful properties from the detailed structure of their wavefronts. The structure necessary to create such traps can be imposed on a TEM00 beam by a mode-forming hologram. Indeed, the beam-splitting and mode-forming operations can be combined in a single computer-generated hologram to create arrays of multifunctional optical traps [8

8. J. Liesener, M. Reicherter, T. Haist, and H. J. Tiziani, “Multi-functional optical tweezers using computer-generated holograms,” Opt. Comm. 185, 77–82 (2000). [CrossRef]

, 10

10. J. E. Curtis, B. A. Koss, and D. G. Grier, “Dynamic holographic optical tweezers,” Opt. Comm. 207, 169–175 (2002). [CrossRef]

, 5

5. M. Polin, K. Ladavac, S.-H. Lee, Y. Roichman, and D. G. Grier, “Optimized holographic optical traps,” Opt. Express 13, 5831–5845 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-15-5831. [CrossRef] [PubMed]

]. Here again, the phase transfer function, f(x), of the DOE can affect the fidelity with which a particular mode is projected, and thus can influence the associated trap’s functionality.

As a practical example, we consider optical vortices, torque-exerting traps created by focusing helical light beams. Helical modes are characterized by an overall phase factor exp(iℓθ), where θ is the azimuthal angle about the optical axis. The integer winding number ℓ sets the pitch of the helix, and is often referred to as the topological charge [21

21. L. Allen, M. W. Beijersbergen, R. J. C. Spreeuw, and J. P. Woerdman, “Orbital angular-momentum of light and the transformation of Laguerre-Gaussian laser modes,” Phys. Rev. A 45, 8185–8189 (1992). [CrossRef] [PubMed]

]. The helical topology suppresses the intensity along the axis of such a beam, not because the amplitude vanishes but rather because of destructive interference due to the coincidence of all phases there. An optical vortex, therefore, focuses to a dark spot surrounded by a bright ring of light. In optical vortices created by imposing a helical phase profile on a Gaussian beam, the ring’s radius scales linearly with topological charge [22

22. J. E. Curtis and D. G. Grier, “Structure of optical vortices,” Phys. Rev. Lett. 90, 133901 (2003). [CrossRef] [PubMed]

, 23

23. J. E. Curtis and D. G. Grier, “Modulated optical vortices,” Opt. Lett. 28, 872–874 (2003). [CrossRef] [PubMed]

, 24

24. S. Sundbeck, I. Gruzberg, and D. G. Grier, “Structure and scaling of helical modes of light,” Opt. Lett. 30, 477–479 (2005). [CrossRef] [PubMed]

].

Now we consider what happens to an optical vortex designed to have winding number ℓ when projected by a non-ideal DOE. Because the Fourier coefficients in Eq. (6) fall off with index, we approximate the field in the focal plane by the principal terms

E(r)a1E1(r)+a0E0(r)+a1E1(r).
(12)

Taking E 1(r) = u (r) exp(iℓθ) for an optical vortex centered within a standard holographic optical trapping system, the conjugate field is

E1(r)=E1*(r)=(1)u(r)exp(iℓθ).
(13)

The resulting intensity distribution,

I(r)=A0(r)+A1cos(ℓθ+θ1)+A2(r)cos(2ℓθ+θ2),
(14)

is characterized by azimuthal intensity modulations with both ℓ-fold and 2ℓ-fold symmetry. Taking an = |an | exp(n ), and defining a 2 = |a 1|2 + |a -1|2 and b 2 = 2|a 1||a -1| these terms’ relative amplitudes are A 0(r) = |a 0|2 u02(r) + a 2 u2(r), A 1(r) = 2|a 0| [a 2 + (- 1) b 2 cos(2β 0 - β 1 - β -1)] u 0(r)u (r), and A 2(r) = b 2 u2(r). Their relative phases are given by

tanθ1=a1sin(β1β0)+(1)a1sin(β0β1)a1sin(β1β0)+(1)a1sin(β0β1).
(15)

and θ 2 = ℓπ + β 1 - β -1

Fig. 3. (a) Interference between an on-axis optical vortex and its first-order conjugate creates 2ℓ-fold modulation of the principal ring’s intensity. Here an ℓ = 30 optical vortex is projected on axis in a standard holographic optical trapping geometry. The bright central spot marks the position of the optical axis in the field of view. The ℓ-fold radial striations result from the finite spatial resolution of the DOE. (b) Displacing the vortex away from the optical axis lifts the superposition of conjugate fields and eliminates the circumferential modulation.

In principle, the central spot’s amplitude profile, u 0(r), is sharply peaked around the optical axis and so should not overlap substantially with the optical vortex’s ring-like profile, u (r). The amplitude A 1(r) of the ℓ-fold intensity corrugation resulting from their interference therefore should be negligible for ℓ ≫ 1. Even so, holographically projected optical vortices such as the example in Fig. 3(a) often are surrounded by ℓ radial spokes extending to very large radii. These outer spokes are projected from the hologram’s central region [25

25. C.-S. Guo, X. Liu, J.-L. He, and H.-T. Wang, “Optimal annulus structures of optical vortices,” Opt. Express 12, 4625–4634 (2004). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-19-4625. [CrossRef] [PubMed]

], whose features typically are too fine to be reproduced faithfully by a pixellated DOE [22

22. J. E. Curtis and D. G. Grier, “Structure of optical vortices,” Phys. Rev. Lett. 90, 133901 (2003). [CrossRef] [PubMed]

]. The undersampled phase pattern near the optical axis acts as a diffuser and scatters light to larger radii where it contributes to the visible spokes. Both these and the optical vortex’s higher-order diffraction rings can be eliminated by excising the central region of the mode-forming phase mask [25

25. C.-S. Guo, X. Liu, J.-L. He, and H.-T. Wang, “Optimal annulus structures of optical vortices,” Opt. Express 12, 4625–4634 (2004). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-19-4625. [CrossRef] [PubMed]

, 26

26. K. Ladavac and D. G. Grier, “Colloidal hydrodynamic coupling in concentric optical vortices,” Europhys. Lett. 70, 548–554 (2005). [CrossRef]

].

Whereas the ℓ-fold features are due in large part to the DOE’s pixellated structure, the 2ℓ-fold corrugation results from interference between the principal and conjugate fields. This corrugation, which also can be seen in Fig. 3(a), has been described before and significantly affects the dynamics of objects trapped on the circumference of an optical vortex [22

22. J. E. Curtis and D. G. Grier, “Structure of optical vortices,” Phys. Rev. Lett. 90, 133901 (2003). [CrossRef] [PubMed]

]. It can be minimized by displacing the principal vortex away from the center of the field of view [13

13. H. He, N. R. Heckenberg, and H. Rubinsztein-Dunlop, “Optical particle trapping with higher-order doughnut beams produced using high efficiency computer generated holograms,” J. Mod. Opt. 42, 217–223 (1995). [CrossRef]

, 25

25. C.-S. Guo, X. Liu, J.-L. He, and H.-T. Wang, “Optimal annulus structures of optical vortices,” Opt. Express 12, 4625–4634 (2004). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-19-4625. [CrossRef] [PubMed]

]. Ideally, this eliminates modulation of the optical vortex’s circumferential intensity profile altogether, as shown in Fig. 3(b). Because optical vortices cover a larger area than conventional optical tweezers, however, some interference with neighboring and ghost traps can occur in more complex configurations [27

27. K. Ladavac and D. G. Grier, “Microoptomechanical pump assembled and driven by holographic optical vortex arrays,” Opt. Express 12, 1144–1149 (2004). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-6-1144. [CrossRef] [PubMed]

]. Optimizing the phase transfer function to minimize these interactions thus is more important in creating multifunctional optical traps than in projecting arrays of conventional optical tweezers.

Fig. 4. Simultaneous projection of red (685 nm) and green (532 nm) holographic optical trapping patterns with a single computer-generated DOE.

The ability to project multifunctional optical traps in multiple wavelengths should facilitate simultaneous manipulation and photochemical transformation of light-sensitive systems. This would be useful for non-invasive intracellular surgery and for assembling and photochemically bonding three-dimensional heterostructures [16

16. Y. Roichman and D. G. Grier, “Holographic assembly of quasicrystalline photonic heterostructures,” Opt. Express 13, 5434–5439 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-14-5434. [CrossRef] [PubMed]

]. Multicolor arrays also will be useful for sorting objects by their absorptivity or index of refraction, for example in holographically implemented optical fractionation [33

33. K. Ladavac, K. Kasza, and D. G. Grier, “Sorting by periodic potential energy landscapes: Optical fractionation,” Phys. Rev. E 70, 010901(R) (2004). [CrossRef]

]. Combining these functions on a single DOE would simplify the implementation by projecting all wavelengths along a single path.

In summary, we have shown that an optimized holographic optical trapping system’s performance is remarkably insensitive to details of the DOE’s phase transfer function. This accounts for the success of early implementations [6

6. E. R. Dufresne and D. G. Grier, “Optical tweezer arrays and optical substrates created with diffractive optical elements,” Rev. Sci. Instr. 69, 1974–1977 (1998). [CrossRef]

, 9

9. E. R. Dufresne, D. Altman, and D. G. Grier, “Brownian dynamics of a sphere in a slit pore,” Europhys. Lett. 53, 264–270 (2001). [CrossRef]

] whose DOEs were not accurately tuned to the wavelength of input light. It also suggests new applications, such as multicolor trapping, and opportunities for simplified implementation of dynamic holographic optical trapping systems.

This work was supported by NSF Grants Number DMR-0451589 and DBI-0233971. S.L. acknowledges support from the Kessler Family Foundation.

References and links

1.

D. G. Grier, “A revolution in optical manipulation,” Nature 424, 810–816 (2003). [CrossRef] [PubMed]

2.

L. B. Lesem, P. M. Hirsch, and J. A. Jordan, “The kinoform: A new wavefront reconstruction device,” IBM J. Res. Develop. 13, 150–155 (1969). [CrossRef]

3.

J. W. Goodman and A. M. Silverstri, “Some effects of Fourier-domain phase quantization,” IBM J. Res. Dev. 14, 478 (1970). [CrossRef]

4.

J. P. Riley and F. N. Birkett, “A reflection kinoform for use with a CO2 laser,” Optica Acta 24, 999–1009 (1977). [CrossRef]

5.

M. Polin, K. Ladavac, S.-H. Lee, Y. Roichman, and D. G. Grier, “Optimized holographic optical traps,” Opt. Express 13, 5831–5845 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-15-5831. [CrossRef] [PubMed]

6.

E. R. Dufresne and D. G. Grier, “Optical tweezer arrays and optical substrates created with diffractive optical elements,” Rev. Sci. Instr. 69, 1974–1977 (1998). [CrossRef]

7.

M. Reicherter, T. Haist, E. U. Wagemann, and H. J. Tiziani, “Optical particle trapping with computer-generated holograms written on a liquid-crystal display,” Opt. Lett. 24, 608–610 (1999). [CrossRef]

8.

J. Liesener, M. Reicherter, T. Haist, and H. J. Tiziani, “Multi-functional optical tweezers using computer-generated holograms,” Opt. Comm. 185, 77–82 (2000). [CrossRef]

9.

E. R. Dufresne, D. Altman, and D. G. Grier, “Brownian dynamics of a sphere in a slit pore,” Europhys. Lett. 53, 264–270 (2001). [CrossRef]

10.

J. E. Curtis, B. A. Koss, and D. G. Grier, “Dynamic holographic optical tweezers,” Opt. Comm. 207, 169–175 (2002). [CrossRef]

11.

A. Ashkin, J. M. Dziedzic, J. E. Bjorkholm, and S. Chu, “Observation of a single-beam gradient force optical trap for dielectric particles,” Opt. Lett. 11, 288–290 (1986). [CrossRef] [PubMed]

12.

J. W. Goodman, Introduction to Fourier Optics, 2nd ed. (McGraw-Hill, New York, 1996).

13.

H. He, N. R. Heckenberg, and H. Rubinsztein-Dunlop, “Optical particle trapping with higher-order doughnut beams produced using high efficiency computer generated holograms,” J. Mod. Opt. 42, 217–223 (1995). [CrossRef]

14.

N. R. Heckenberg, R. McDuff, C. P. Smith, H. Rubinsztein-Dunlop, and M. J. Wegener, “Laser beams with phase singularities,” Opt. Quantum Elect. 24, S951–S962 (1992). [CrossRef]

15.

A. Jesacher, S. Furhpater, S. Bernet, and M. Ritsch-Marte, “Size selective trapping with optical ”cogwheel” tweezers,” Opt. Express 12, 4129–4135 (2004). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-17-4129. [CrossRef] [PubMed]

16.

Y. Roichman and D. G. Grier, “Holographic assembly of quasicrystalline photonic heterostructures,” Opt. Express 13, 5434–5439 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-14-5434. [CrossRef] [PubMed]

17.

N. B. Simpson, L. Allen, and M. J. Padgett, “Optical tweezers and optical spanners with Laguerre-Gaussian modes,” J. Mod. Opt. 43, 2485–2491 (1996). [CrossRef]

18.

K. T. Gahagan and G. A. Swartzlander, “Optical vortex trapping of particles,” Opt. Lett. 21, 827–829 (1996). [CrossRef] [PubMed]

19.

A. Vasara, J. Turunen, and A. T. Friberg, “Realization of general nondiffracting beams with computer-generated holograms,” J. Opt. Soc. Am. A 6, 1748–1754 (1989). [CrossRef] [PubMed]

20.

J. Arlt, V. Garces-Chavez, W. Sibbett, and K. Dholakia, “Optical micromanipulation using a Bessel light beam,” Opt. Comm. 197, 239–245 (2001). [CrossRef]

21.

L. Allen, M. W. Beijersbergen, R. J. C. Spreeuw, and J. P. Woerdman, “Orbital angular-momentum of light and the transformation of Laguerre-Gaussian laser modes,” Phys. Rev. A 45, 8185–8189 (1992). [CrossRef] [PubMed]

22.

J. E. Curtis and D. G. Grier, “Structure of optical vortices,” Phys. Rev. Lett. 90, 133901 (2003). [CrossRef] [PubMed]

23.

J. E. Curtis and D. G. Grier, “Modulated optical vortices,” Opt. Lett. 28, 872–874 (2003). [CrossRef] [PubMed]

24.

S. Sundbeck, I. Gruzberg, and D. G. Grier, “Structure and scaling of helical modes of light,” Opt. Lett. 30, 477–479 (2005). [CrossRef] [PubMed]

25.

C.-S. Guo, X. Liu, J.-L. He, and H.-T. Wang, “Optimal annulus structures of optical vortices,” Opt. Express 12, 4625–4634 (2004). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-19-4625. [CrossRef] [PubMed]

26.

K. Ladavac and D. G. Grier, “Colloidal hydrodynamic coupling in concentric optical vortices,” Europhys. Lett. 70, 548–554 (2005). [CrossRef]

27.

K. Ladavac and D. G. Grier, “Microoptomechanical pump assembled and driven by holographic optical vortex arrays,” Opt. Express 12, 1144–1149 (2004). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-6-1144. [CrossRef] [PubMed]

28.

J. Bengtsson, “Kinoforms designed to produce different fan-out patterns for two wavelengths,” Appl. Opt. 37, 2011–2020 (1998). [CrossRef]

29.

U. Levy, E. Marom, and D. Mendlovic, “Simultaneous multicolor image formation with a single diffractive optical element,” Opt. Lett. 26, 1149–1151 (2001). [CrossRef]

30.

L. L. Doskolovich, N. L. Kazanskiy, V. A. Soifer, P. Perlo, and P. Repetto, “Design of DOEs for wavelength division and focusing,” J. Mod. Opt. 52, 917–926 (2005). [CrossRef]

31.

J. Leach and M. J. Padgett, “Observation of chromatic effects near a white-light vortex,” New J. Phys. 5, 154 (2003). [CrossRef]

32.

P. Fischer, C. T. A. Brown, J. E. Morris, C. López-Mariscal, E. M. Wright, W. Sibbett, and K. Dholakia, “White light propagation invariant beams,” Opt. Express 13, 6657–6666 (2005). http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-17-6657. [CrossRef] [PubMed]

33.

K. Ladavac, K. Kasza, and D. G. Grier, “Sorting by periodic potential energy landscapes: Optical fractionation,” Phys. Rev. E 70, 010901(R) (2004). [CrossRef]

OCIS Codes
(090.1760) Holography : Computer holography
(120.4610) Instrumentation, measurement, and metrology : Optical fabrication
(140.7010) Lasers and laser optics : Laser trapping

ToC Category:
Research Papers

History
Original Manuscript: August 16, 2005
Revised Manuscript: September 6, 2005
Published: September 19, 2005

Citation
Sang-Hyuk Lee and David Grier, "Robustness of holographic optical traps against phase scaling errors," Opt. Express 13, 7458-7465 (2005)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-13-19-7458


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References

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  2. L. B. Lesem, P. M. Hirsch, and J. A. Jordan, �??The kinoform: A new wavefront reconstruction device,�?? IBM J. Res. Develop. 13, 150�??155 (1969). [CrossRef]
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  8. J. Liesener, M. Reicherter, T. Haist, and H. J. Tiziani, �??Multi-functional optical tweezers using computer-generated holograms,�?? Opt. Comm. 185, 77�??82 (2000). [CrossRef]
  9. E. R. Dufresne, D. Altman, and D. G. Grier, �??Brownian dynamics of a sphere in a slit pore,�?? Europhys. Lett. 53, 264�??270 (2001). [CrossRef]
  10. J. E. Curtis, B. A. Koss, and D. G. Grier, �??Dynamic holographic optical tweezers,�?? Opt. Comm. 207, 169�??175 (2002). [CrossRef]
  11. A. Ashkin, J. M. Dziedzic, J. E. Bjorkholm, and S. Chu, �??Observation of a single-beam gradient force optical trap for dielectric particles,�?? Opt. Lett. 11, 288�??290 (1986). [CrossRef] [PubMed]
  12. J. W. Goodman, Introduction to Fourier Optics, 2nd ed. (McGraw-Hill, New York, 1996).
  13. H. He, N. R. Heckenberg, and H. Rubinsztein-Dunlop, �??Optical particle trapping with higher-order doughnut beams produced using high efficiency computer generated holograms,�?? J. Mod. Opt. 42, 217�??223 (1995). [CrossRef]
  14. N. R. Heckenberg, R. McDuff, C. P. Smith, H. Rubinsztein-Dunlop, and M. J.Wegener, �??Laser beams with phase singularities,�?? Opt. Quantum Elect. 24, S951�??S962 (1992). [CrossRef]
  15. A. Jesacher, S. Furhpater, S. Bernet, and M. Ritsch-Marte, �??Size selective trapping with optical �??cogwheel�?? tweezers,�?? Opt. Express 12, 4129�??4135 (2004). <a href= "http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-17-4129">http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-17-4129</a>. [CrossRef] [PubMed]
  16. Y. Roichman and D. G. Grier, �??Holographic assembly of quasicrystalline photonic heterostructures,�?? Opt. Express 13, 5434�??5439 (2005) <a href=. "http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-14-5434">http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-14-5434</a>. [CrossRef] [PubMed]
  17. N. B. Simpson, L. Allen, and M. J. Padgett, �??Optical tweezers and optical spanners with Laguerre-Gaussian modes,�?? J. Mod. Opt. 43, 2485�??2491 (1996). [CrossRef]
  18. K. T. Gahagan and G. A. Swartzlander, �??Optical vortex trapping of particles,�?? Opt. Lett. 21, 827�??829 (1996). [CrossRef] [PubMed]
  19. A. Vasara, J. Turunen, and A. T. Friberg, �??Realization of general nondiffracting beams with computer-generated holograms,�?? J. Opt. Soc. Am. A 6, 1748�??1754 (1989). [CrossRef] [PubMed]
  20. J. Arlt, V. Garces-Chavez, W. Sibbett, and K. Dholakia, �??Optical micromanipulation using a Bessel light beam,�?? Opt. Comm. 197, 239�??245 (2001). [CrossRef]
  21. L. Allen, M. W. Beijersbergen, R. J. C. Spreeuw, and J. P. Woerdman, �??Orbital angular-momentum of light and the transformation of Laguerre-Gaussian laser modes,�?? Phys. Rev. A 45, 8185�??8189 (1992). [CrossRef] [PubMed]
  22. J. E. Curtis and D. G. Grier, �??Structure of optical vortices,�?? Phys. Rev. Lett. 90, 133901 (2003). [CrossRef] [PubMed]
  23. J. E. Curtis and D. G. Grier, �??Modulated optical vortices,�?? Opt. Lett. 28, 872�??874 (2003). [CrossRef] [PubMed]
  24. S. Sundbeck, I. Gruzberg, and D. G. Grier, �??Structure and scaling of helical modes of light,�?? Opt. Lett. 30, 477�??479 (2005). [CrossRef] [PubMed]
  25. C.-S. Guo, X. Liu, J.-L. He, and H.-T. Wang, �??Optimal annulus structures of optical vortices,�?? Opt. Express 12, 4625�??4634 (2004) <a href=. "http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-19-4625">http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-19-4625</a>. [CrossRef] [PubMed]
  26. K. Ladavac and D. G. Grier, �??Colloidal hydrodynamic coupling in concentric optical vortices,�?? Europhys. Lett. 70, 548�??554 (2005). [CrossRef]
  27. K. Ladavac and D. G. Grier, �??Microoptomechanical pump assembled and driven by holographic optical vortex arrays,�?? Opt. Express 12, 1144�??1149 (2004) <a href "http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-6-1144">http://www.opticsexpress.org/abstract.cfm?URI=OPEX-12-6-1144</a>. [CrossRef] [PubMed]
  28. J. Bengtsson, �??Kinoforms designed to produce different fan-out patterns for two wavelengths,�?? Appl. Opt. 37, 2011�??2020 (1998). [CrossRef]
  29. U. Levy, E. Marom, and D. Mendlovic, �??Simultaneous multicolor image formation with a single diffractive optical element,�?? Opt. Lett. 26, 1149�??1151 (2001). [CrossRef]
  30. L. L. Doskolovich, N. L. Kazanskiy, V. A. Soifer, P. Perlo, and P. Repetto, �??Design of DOEs for wavelength division and focusing,�?? J. Mod. Opt. 52, 917�??926 (2005). [CrossRef]
  31. J. Leach and M. J. Padgett, �??Observation of chromatic effects near a white-light vortex,�?? New J. Phys. 5, 154 (2003). [CrossRef]
  32. P. Fischer, C. T. A. Brown, J. E. Morris, C. López-Mariscal, E. M. Wright, W. Sibbett, and K. Dholakia, �??White light propagation invariant beams,�?? Opt. Express 13, 6657�??6666 (2005) <a href=. "http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-17-6657">http://www.opticsexpress.org/abstract.cfm?URI=OPEX-13-17-6657</a>. [CrossRef] [PubMed]
  33. K. Ladavac, K. Kasza, and D. G. Grier, �??Sorting by periodic potential energy landscapes: Optical fractionation,�?? Phys. Rev. E 70, 010901(R) (2004). [CrossRef]

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