Three-dimensional image formation in fiber-optical second-harmonic-generation microscopy

doi:10.1364/OE.14.001175

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Three-dimensional image formation in fiber-optical second-harmonic-generation microscopy

Min Gu and Ling Fu »View Author Affiliations

Optics Express, Vol. 14, Issue 3, pp. 1175-1181 (2006)
http://dx.doi.org/10.1364/OE.14.001175

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– Abstract
1. Introduction
2. Three-dimensional coherent transfer function in fiber-optical SHG microscope
3. Results and discussion
4. Conclusions
– References and links

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Abstract

Three-dimensional (3-D) image formation in fiber-optical second-harmonic-generation microscopy is revealed to be purely coherent and therefore can be described by a 3-D coherent transfer function (CTF) that exhibits the same spatial frequency passband as that of fiber-optical reflection-mode non-fluorescence microscopy. When the numerical aperture of the fiber is much larger than the angle of convergence of the illumination on the fiber aperture, the performance of fiber-optical second-harmonic-generation microscopy behaves as confocal second-harmonic-generation microscopy. The dependence of axial resolution on fiber coupling parameters shows an improvement of approximately 7%, compared with that in fiber-optical two-photon fluorescence microscopy.

1. Introduction

Second-harmonic-generation (SHG) microscopy was proposed by Gannaway and Sheppard in 1970s [1

J. N. Gannaway and C. J. R. Sheppard, “Second-harmonic imaging in the optical scanning microscope,” Opt. Quantum Electron. 10, 435 (1978). [CrossRef]

] and has been recently extensively explored for biological studies [2–5

Y. Guo, P. P. Ho, H. Savage, D. Harris, P. Sacks, S. Schantz, F. Liu, N. Zhadin, and R. R. Alfano, “Optical harmonic generation from animal tissue by the use of picosecond and femtosecond laser pulses,” Opt. Lett. 22, 1323 (1997). [CrossRef]

]. Together with two-photon (2-p) excited fluorescence microscopy [6

W. Denk, J. H. Strickler, and W. W. Webb, “Two photon laser scanning fluorescence microscopy,” Science 248, 73 (1990). [CrossRef] [PubMed]

], SHG microscopy provides the cellular-level functionality and morphology information of a sample, an inherent sectioning ability for three-dimensional (3-D) imaging, and relatively deep optical penetration within biological tissue [2–6

]. In order to apply these new nonlinear optical imaging techniques into in vivo applications, fiber-optical components such as a fiber coupler have been adopted for miniaturization [7–11

D. Bird and M. Gu, “Compact two-photon fluorescence microscope based on a single-mode fiber coupler,” Opt. Lett. 27, 1031 (2002). [CrossRef]

]. Physically, 2-p excited fluorescence and SHG microscopy corresponds to incoherent and coherent imaging processes which can be understood by an optical transfer function and a coherent transfer function (CTF) [12

M. Gu, Principles of Three-Dimensional Imaging in Confocal Microscopes (World Scientific, Singapore, 1996). [CrossRef]

, 13

C. J. R. Sheppard and M. Gu, “The significance of 3D transfer functions in confocal scanning microscopy,” J. Micros. 165, 377 (1992). [CrossRef]

], respectively. Therefore, a 3-D optical transfer function has been derived to describe the imaging performance in fiber-optical 2-p fluorescence microscopy [14

M. Gu and D. Bird, “Three-dimensional optical-transfer-function analysis of fiber-optical two-photon fluorescence microscopy,” J. Opt. Soc. Am. A 20, 941 (2003). [CrossRef]

]. However, such a description is not applicable to fiber-optical SHG microscopy.

In the case of a non-fluorescent linear sample, fiber-optical scanning microscopy behaves fully coherently even for finite values of fiber spot size [15

M. Gu, C. J. R. Sheppard, and X. Gan, “Image formation in a fiber-optical confocal scanning microscope” J. Opt. Soc. Am. A 8, 1755 (1991). [CrossRef]

, 16

S. Kimura and T. Wilson, “Confocal scanning optical microscope using single-mode fiber for signal detection,” Appl. Opt. 30, 2143 (1991). [CrossRef] [PubMed]

] and therefore can be described by a 3-D CTF that can be expressed by an analytical expression [17

M. Gu, X. Gan, and C. J. R. Sheppard, “Three-dimensional coherent transfer functions in fiber-optical confocal scanning microscopes,” J. Opt. Soc. Am. A 8, 1019 (1991). [CrossRef]

]. The aim of this paper is to understand 3-D image formation in fiber-optical SHG microscopy using the concept of the 3-D CTF and to reveal the dependence of axial resolution on fiber coupling parameters.

2. Three-dimensional coherent transfer function in fiber-optical SHG microscope

In order to investigate the effect of optical fibers on illumination and collection separately, let us consider the schematic diagram of a fiber-optical SHG microscope as shown in Fig. 1. Two optical single-mode fibers F₁ and F₂ are used to deliver illumination at wavelength 2λ ₀ and collect SHG signal at wavelength λ ₀, respectively. When the illumination optical fiber F₁ and the collection optical fiber F₂ are identical, the performance of the system is equivalent to that using a fiber coupler [10

L. Fu, X. Gan, and M. Gu, “Use of single-mode fiber coupler for second-harmonic-generation microscopy,” Opt. Lett. 30, 385 (2005). [CrossRef] [PubMed]

]. As SHG is a coherent process, the analysis of image formation in fiber-optical SHG microscopy is similar to that in fiber-optical non-fluorescence microscopy described elsewhere [17

M. Gu, X. Gan, and C. J. R. Sheppard, “Three-dimensional coherent transfer functions in fiber-optical confocal scanning microscopes,” J. Opt. Soc. Am. A 8, 1019 (1991). [CrossRef]

]. Considering that the electrical field of the SHG emission from a sample is proportional to the square of the field of the illumination field on the sample, the image intensity from a scan point r _s = (x_s , y_s , z_s ) in the fiber-optical SHG microscope can be expressed, if the optical axis is assumed along the zdirection, as

Fig. 1. Schematic diagram of the fiber-optical SHG scanning microscope.

I (r_{s}) = ∣ \int_{- \infty}^{\infty} U_{2}^{*} (x_{2}, y_{2}) δ (z_{2}) {[\int_{- \infty}^{\infty} U_{1} (x_{0}, y_{0}) δ (z_{0}) \exp [ik (z_{0} - z_{1})] h_{1} (r_{0} + M_{1} r_{1}) d r_{0}]}^{2}

ε (r_{s} - r_{1}) \exp [ik (\pm z_{1} - z_{2})] h_{2} (r_{1} + M_{2} r_{2}) d r_{2} d r_{1} ∣^{2},

(1)

where the letters r _i (i=0,1,2) represent vectors with components x_i , y_i , z_i . The functions U ₁ (x, y) and U ₂ (x, y) are the amplitude mode profile on the output end of fiber F₁ and on the input end of fiber F₂, respectively. * denotes the conjugate operation and the parameters M ₁ and M ₂ are diagonal matrices of the magnification factors of the illumination and collection lenses, respectively. The term in the first square brackets results from the quadratic dependence of SHG. h ₁( r )and h ₂( r ) are the 3-D amplitude point spread functions (PSFs) for the objective in illumination and collection paths, respectively [17

M. Gu, X. Gan, and C. J. R. Sheppard, “Three-dimensional coherent transfer functions in fiber-optical confocal scanning microscopes,” J. Opt. Soc. Am. A 8, 1019 (1991). [CrossRef]

]. ε( r ) is the object function representing the SHG strength of the object. Using the 3-D convolution relation, one can simplify Eq. (1) as

I (r_{s}) = {∣ h_{eff} (r_{s}) \otimes_{3} ε (r_{s}) ∣}^{2},

(2)

where ⊗₃ denotes the 3-D convolution operation. h_eff is the 3-D effective PSF for fiber-optical SHG microscopy and given by

h_{eff} (r) = {[U_{1} (M_{1} x, M_{1} y) \otimes_{2} h_{1} (M_{1} r)]}^{2} [U_{2}^{*} (M_{1} x, M_{1} y) \otimes_{2} h_{2} (r)] .

(3)

Here ⊗₂ denotes the 2-D convolution operation.

It is necessary to point out that Eqs. (1) and (2) represent a superposition of the light amplitude from a sample and therefore implies that like fiber-optical non-fluorescence microscopy [15–17

M. Gu, C. J. R. Sheppard, and X. Gan, “Image formation in a fiber-optical confocal scanning microscope” J. Opt. Soc. Am. A 8, 1755 (1991). [CrossRef]

] fiber-optical SHG microscopy is purely coherent. This feature is of particular importance when one performs SHG interferometric microscopy/tomography [18

S. Yazdanfar, L. H. Laiho, and P. T. C. So, “Interferometric second harmonic generation microscopy,” Opt. Express 12, 2739 (2004). [CrossRef] [PubMed]

]. Therefore, fiber-optical SHG microscopy can be analyzed in terms of the 3-D CTF that is given by the 3-D Fourier transform of the effective PSF [12

M. Gu, Principles of Three-Dimensional Imaging in Confocal Microscopes (World Scientific, Singapore, 1996). [CrossRef]

, 17

M. Gu, X. Gan, and C. J. R. Sheppard, “Three-dimensional coherent transfer functions in fiber-optical confocal scanning microscopes,” J. Opt. Soc. Am. A 8, 1019 (1991). [CrossRef]

]. The 3-D CTF, c( m ), for fiber-optical SHG microscope can thus be described by

c (m) = c_{1} (m) \otimes_{3} c_{2} (m),

(4)

where

c_{1} (m) = F_{3} {{[U_{1} (M_{1} x, M_{1} y) \otimes_{2} h_{1} (M_{1} r)]}^{2}},

(5)

and

c_{2} (m) = F_{3} {U_{2}^{*} (M_{1} x, M_{1} y) \otimes_{2} h_{2} (r)} .

(6)

Here F ₃ is the 3-D Fourier transform with respect to r _s and m represents the spatial frequency vector with two transverse components m and n, and one axial component s. For a system using a circular lens, c ₁( m ) is the 3-D CTF for a fiber-optical reflection-mode non-fluorescence microscope with wavelength 2λ ₀ [17

M. Gu, X. Gan, and C. J. R. Sheppard, “Three-dimensional coherent transfer functions in fiber-optical confocal scanning microscopes,” J. Opt. Soc. Am. A 8, 1019 (1991). [CrossRef]

] and can be analytically expressed as:

c_{1} (l, s) = \exp (- 2 A_{1} s) {\begin{matrix} 1, \frac{l^{2}}{2} \leq s \leq \frac{1}{2} - l (1 - l), \\ (\frac{2}{π}) \sin^{- 1} {\frac{(1 - 2 s)}{[2 l {(2 s - l^{2})}^{\frac{1}{2}}]}, \frac{1}{2} - l (1 - l) \leq s \leq \frac{1}{2}} \\ 0, otherwise . \end{matrix}

(7)

Similarly, Eq. (6) represents the 3-D CTF for a single circular lens with wavelength λ ₀ and weighted by the Fourier transform of the fiber mode profile U ^* ₂(x, y), given by

c_{2} (l, s) = \exp (\frac{- A_{2} l^{2}}{2}) δ (\frac{s - l^{2}}{2}) .

(8)

In Eqs. (7) and (8), A_j = [2πaa_j /(λ_jd_j )]² (j = 1, 2) is the normalized fiber spot size for illumination and collection fibers. d_j is the distance between the fiber ends and the objective. The variables

l (l = \sqrt{m^{2} + n^{2}})

and s denote the radial and axial spatial frequencies normalized by sinα/λ ₀ and 4 sin²(α/2)/λ ₀, respectively, where sinα or is the numerical aperture of the objective of radius a. Here we have assumed that both illumination and collection fibers are single-mode fibers of mode spot radii a ₁ and a ₂. It has been shown that A_j is proportional to the square of the ratio of the numerical aperture of the objective in the illumination and collection paths to the numerical aperture of the fibers F₁ and F₂ [12

M. Gu, Principles of Three-Dimensional Imaging in Confocal Microscopes (World Scientific, Singapore, 1996). [CrossRef]

According to Eq. (4), the 3-D CTF can be numerically evaluated, if the delta function in Eq. (8) is taken into account, by

c (l, s) = \iint_{σ} \exp [\frac{- A_{2} (m^{2} + n^{2})}{2}] c_{1} (\sqrt{{(m - l)}^{2} + n^{2}}, s - \frac{m^{2} + n^{2}}{2}) dmdn,

(9)

where σ represents the area overlapped by m ² + n ² = 1 and (m-l)² + n ² = 1 . Finally, 3-D CTF for fiber-optical SHG microscopy can be explicitly written as

c (l, s) = \int_{0}^{\sqrt{1 - {(\frac{l}{2})}^{2}}} [\int_{l - \sqrt{1 - n^{2}}}^{\sqrt{1 - n^{2}}} \exp [\frac{- A_{2} (m^{2} + n^{2})}{2}] c_{1} (\sqrt{{(m - l)}^{2} + n^{2}}, s - \frac{m^{2} + n^{2}}{2}) dm] dn .

(10)

It should be pointed out that 3-D CTF for fiber-optical SHG microscopy has a spatial frequency passband of l ²/4 <(s + s0)< 1 with axial and transverse cutoffs 1 and 2, respectively. Here s0 = 1/[2sin²(α/2)] is a constant axial spatial-frequency shift resulting from the reflection imaging geometry [12

M. Gu, Principles of Three-Dimensional Imaging in Confocal Microscopes (World Scientific, Singapore, 1996). [CrossRef]

]. This feature is the same as fiber-optical reflection-mode non-fluorescence microscopy [17

M. Gu, X. Gan, and C. J. R. Sheppard, “Three-dimensional coherent transfer functions in fiber-optical confocal scanning microscopes,” J. Opt. Soc. Am. A 8, 1019 (1991). [CrossRef]

3. Results and discussion

When A_j → 0, which corresponds to the case when the numerical aperture of the fiber is much larger than that of the objective in illumination and collection paths, the 3-D CTF describes confocal SHG microscopy of a point source and a point detector. If either A ₁ or A ₂ becomes infinity, c(l, s) becomes Eq. (8) or Eq. (7). No image is formed because c(l, s) is zero. For a SHG microscope based on a fiber coupler [10

L. Fu, X. Gan, and M. Gu, “Use of single-mode fiber coupler for second-harmonic-generation microscopy,” Opt. Lett. 30, 385 (2005). [CrossRef] [PubMed]

], we have 4A ₁ = A ₂ and the corresponding 3-D CTFs for A ₁ = 0, 1, 5 are shown in Figs. 2(a)–(c). Figure 2(a) represents the 3-D CTF for confocal SHG microscopy with a point source and a point detection. For a finite value of A ₁, the strength of the 3-D CTF is reduced in particular along the axial direction, as shown in Figs. 2(b) and (c). Figure 2(d) also denotes the 3-D CTF when a point source is used (A ₁ = 0) and a fiber is used for collection. In this case, the collection function of the objective becomes weak. Ultimately, when A ₂ → ∞, c ₂(l,s) approaches a delta function at l = 0 and thus the 3-D CTF for SHG microscopy is given by Eq. (7).

Fig. 2. 3-D CTF for fiber-optical SHG microscopy. (a) A ₁ = 0, A ₂=4A ₁. (b) A ₁ = 1, A ₂=4A ₁.

It is important to investigate the axial cross section, c(l = 0, s) of the 3-D CTF further as it gives the axial imaging performance. The solid curves in Fig. 3 represent the normalized axial cross section of the 3-D CTF for SHG microscopy using a fiber coupler (4A ₁ = A ₂), while the dashed line depicts the condition for A ₁ = 0 and A ₂ → ∞. For 4A ₁ = A ₂ = 0, the CTF increases linearly up to s = 1/3, which is contributed by the constant region in Eq. (7). After the maximum value at s = 1/3, the CTF decreases and finally cuts off at s = 1. When 4A ₁ = A ₂ and A ₁ ≠ 0, the strength of the CTF for s <1/3 is enhanced while that for s >1/3 is reduced. When eventually 4A ₁ = A ₂ → ∞, the CTF approaches a delta function at s = 0, which means that there is no axial imaging ability.

Fig. 3. Axial cross section of the 3-D CTF for fiber-optical SHG microscopy using a fiber coupler (A ₂=4A ₁) for different values of the normalized optical spot size parameter A ₁. The dashed curve represents the case for A ₁ = 0 and A ₂→∞.

To characterize axial resolution, one usually considers imaging of a perfect SHG reflector scanning through the focus of the objective. This axial response is a measure of axial resolution or the optical sectioning property [10

L. Fu, X. Gan, and M. Gu, “Use of single-mode fiber coupler for second-harmonic-generation microscopy,” Opt. Lett. 30, 385 (2005). [CrossRef] [PubMed]

, 11

L. Fu, X. Gan, and M. Gu, “Nonlinear optical microscopy based on double-clad photonic crystal fibers,” Opt. Expess 13, 5528 (2005). [CrossRef]

] and can be calculated using the modulus squared of the Fourier transform of the axial cross section of the 3-D CTF at l = 0 [12

M. Gu, Principles of Three-Dimensional Imaging in Confocal Microscopes (World Scientific, Singapore, 1996). [CrossRef]

, 17

M. Gu, X. Gan, and C. J. R. Sheppard, “Three-dimensional coherent transfer functions in fiber-optical confocal scanning microscopes,” J. Opt. Soc. Am. A 8, 1019 (1991). [CrossRef]

]. After mathematical manipulations, such an axial response can be expressed as

I (u) = {∣ \int_{0}^{1} {\int \frac{\exp {- l^{2} [(A_{1} - \frac{iu}{2}) + \frac{(A_{2} - iu)}{2}]}}{A_{1} - \frac{iu}{2}} {1 - \exp [- ρ_{0}^{2} (A_{1} - \frac{iu}{2})]} d θ} ldl ∣}^{2},

(11)

where

ρ_{0} = - l \cos θ + \sqrt{1 - l^{2} \sin^{2} θ}

and u = (8π/λ ₀)z sin²(α/2).

Fig. 4. Half width at half maximum of the axial response, Δu_1/2, as a function of the normalized fiber spot size parameter when A ₂=4A ₁ (bottom axis) and when A ₁ = 0 (up axis). The squares are experimental results for A ₁ =2.0, 4.2, 6.4, 7.3, 8.4, respectively. Inset: Normalized axial response of a perfect SHG reflector in fiber-optical SHG microscopy using a fiber coupler (A ₂=4A ₁) for different values of the normalized optical spot size parameter A ₁. The dashed curve represents the case for A ₁ = 0 and A ₂→∞.

The normalized SHG axial response and the half width at half maximum (HWHM, Δu _1/2) as a function of the normalized fiber spot size parameters A_j are shown in Fig. 4. It shows that the SHG axial resolution approaches 5.57 for A ₁ = 0 and A ₂ → ∞. In this case, Eq. (11) reduces to I(u) = [sin(u/4)/(u/4)]² and is depicted as a dashed curve in the inset of Fig. 4, which confirms that SHG microscopy exhibits an inherent optical section property without necessarily using finite-sized detection. This feature also implies that SHG microscopy has an improvement of axial resolution by 35% compared with 2-p fluorescence microscopy without any pinhole [19

M. Gu and C. J. R. Sheppard, “Comparison of three-dimensional imaging properties between two-photon and single-photon fluorescence microscopy,” J. Micros. 177, 128 (1995). [CrossRef]

In the case of SHG microscopy using a fiber coupler [10

L. Fu, X. Gan, and M. Gu, “Use of single-mode fiber coupler for second-harmonic-generation microscopy,” Opt. Lett. 30, 385 (2005). [CrossRef] [PubMed]

], the HWHM is approximately 4.72 for 4A ₁ = A ₂= 0. The HWHM as a function of A ₁ exhibits a linear dependence when A ₁ >5. Under the experimental conditions [10

L. Fu, X. Gan, and M. Gu, “Use of single-mode fiber coupler for second-harmonic-generation microscopy,” Opt. Lett. 30, 385 (2005). [CrossRef] [PubMed]

] of A ₁ = 2.0, 4.2, 6.4, 7.3, 8.4, the measured values of Δu _1/2 are shown as square spots in Fig. 4. Δu _1/2 is derived from the axial response of the fiber-optic SHG microscope to a thin layer of AF-50 dye. Parameter A ₁ is varied by using various values of numerical apertures of the objective to couple the SHG signal into the single-mode fiber coupler. It is shown that experimental results further confirm the dependence of the axial resolution on the normalized fiber spot size parameters. The deviations between the theory and the experimental data might be due to the presence of spherical aberration and the finite thickness of the SHG layer. Compared with the HWHM in fiber-optical 2-p fluorescence microscopy [14

M. Gu and D. Bird, “Three-dimensional optical-transfer-function analysis of fiber-optical two-photon fluorescence microscopy,” J. Opt. Soc. Am. A 20, 941 (2003). [CrossRef]

], the axial resolution in fiber-optical SHG microscopy is increased approximately by 7%.

4. Conclusions

In conclusion, the 3-D CTF has been reported to analyze the three-dimensional image formation in fiber-optical SHG microscopy. Its spatial frequency passband is identical to that for fiber-optical reflection-model non-fluorescence microscopy though the strength of the 3-D CTF is reduced due to the finite-sized fiber aperture. For a system based on a fiber coupler and a given illumination wavelength, the axial resolution in SHG microscopy is increased approximately by 7%, compared with 2-p fluorescence microscopy.

Acknowledgments

The authors thank the Australian Research Council for its support.

References and links

1.	J. N. Gannaway and C. J. R. Sheppard, “Second-harmonic imaging in the optical scanning microscope,” Opt. Quantum Electron. 10, 435 (1978). [CrossRef]
2.	Y. Guo, P. P. Ho, H. Savage, D. Harris, P. Sacks, S. Schantz, F. Liu, N. Zhadin, and R. R. Alfano, “Optical harmonic generation from animal tissue by the use of picosecond and femtosecond laser pulses,” Opt. Lett. 22, 1323 (1997). [CrossRef]
3.	P. J. Campagnola and L. M. Loew, “Second harmonic imaging microscopy for visualizing biomolecular arrays in cells, tissues and organisms,” Nat. Biotech. 21, 1356 (2003). [CrossRef]
4.	W. R. Zipfel, R. M. Williams, and W. W. Webb, “Nonlinear magic: multiphoton microscopy in the biosciences,” Nat. Biotech. 21, 1369 (2003). [CrossRef]
5.	R. Gauderon, P. B. Lukins, and C. J. R. Sheppard, “Three-dimensional second-harmonic generation imaging with femtosecond laser pulses,” Opt. Lett. 23, 1209 (1998). [CrossRef]
6.	W. Denk, J. H. Strickler, and W. W. Webb, “Two photon laser scanning fluorescence microscopy,” Science 248, 73 (1990). [CrossRef] [PubMed]
7.	D. Bird and M. Gu, “Compact two-photon fluorescence microscope based on a single-mode fiber coupler,” Opt. Lett. 27, 1031 (2002). [CrossRef]
8.	D. Bird and M. Gu, “Two-photon fluorescence endoscopy with a micro-optic scanning head,” Opt. Lett. 28, 1552 (2003). [CrossRef] [PubMed]
9.	D. Bird and M. Gu, “Fiber-optic two-photon scanning fluorescence microscopy,” J. Micros. 208, 35 (2002). [CrossRef]
10.	L. Fu, X. Gan, and M. Gu, “Use of single-mode fiber coupler for second-harmonic-generation microscopy,” Opt. Lett. 30, 385 (2005). [CrossRef] [PubMed]
11.	L. Fu, X. Gan, and M. Gu, “Nonlinear optical microscopy based on double-clad photonic crystal fibers,” Opt. Expess 13, 5528 (2005). [CrossRef]
12.	M. Gu, Principles of Three-Dimensional Imaging in Confocal Microscopes (World Scientific, Singapore, 1996). [CrossRef]
13.	C. J. R. Sheppard and M. Gu, “The significance of 3D transfer functions in confocal scanning microscopy,” J. Micros. 165, 377 (1992). [CrossRef]
14.	M. Gu and D. Bird, “Three-dimensional optical-transfer-function analysis of fiber-optical two-photon fluorescence microscopy,” J. Opt. Soc. Am. A 20, 941 (2003). [CrossRef]
15.	M. Gu, C. J. R. Sheppard, and X. Gan, “Image formation in a fiber-optical confocal scanning microscope” J. Opt. Soc. Am. A 8, 1755 (1991). [CrossRef]
16.	S. Kimura and T. Wilson, “Confocal scanning optical microscope using single-mode fiber for signal detection,” Appl. Opt. 30, 2143 (1991). [CrossRef] [PubMed]
17.	M. Gu, X. Gan, and C. J. R. Sheppard, “Three-dimensional coherent transfer functions in fiber-optical confocal scanning microscopes,” J. Opt. Soc. Am. A 8, 1019 (1991). [CrossRef]
18.	S. Yazdanfar, L. H. Laiho, and P. T. C. So, “Interferometric second harmonic generation microscopy,” Opt. Express 12, 2739 (2004). [CrossRef] [PubMed]
19.	M. Gu and C. J. R. Sheppard, “Comparison of three-dimensional imaging properties between two-photon and single-photon fluorescence microscopy,” J. Micros. 177, 128 (1995). [CrossRef]

OCIS Codes
(110.2350) Imaging systems : Fiber optics imaging
(110.2990) Imaging systems : Image formation theory
(180.6900) Microscopy : Three-dimensional microscopy

ToC Category:
Microscopy

History
Original Manuscript: October 28, 2005
Revised Manuscript: January 23, 2006
Manuscript Accepted: January 23, 2006
Published: February 6, 2006

Virtual Issues
Vol. 1, Iss. 3 Virtual Journal for Biomedical Optics

Citation
Min Gu and Ling Fu, "Three-dimensional image formation in fiber-optical second-harmonic-generation microscopy," Opt. Express 14, 1175-1181 (2006)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-14-3-1175

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References

J. N. Gannaway and C. J. R. Sheppard, "Second-harmonic imaging in the optical scanning microscope," Opt. Quantum Electron. 10, 435 (1978). [CrossRef]
Y. Guo, P. P. Ho, H. Savage, D. Harris, P. Sacks, S. Schantz, F. Liu, N. Zhadin, and R. R. Alfano, "Optical harmonic generation from animal tissue by the use of picosecond and femtosecond laser pulses," Opt. Lett. 22, 1323 (1997). [CrossRef]
P. J. Campagnola and L. M. Loew, "Second harmonic imaging microscopy for visualizing biomolecular arrays in cells, tissues and organisms," Nat. Biotech. 21, 1356 (2003). [CrossRef]
W. R. Zipfel, R. M. Williams, and W. W. Webb, "Nonlinear magic: multiphoton microscopy in the biosciences," Nat. Biotech. 21, 1369 (2003). [CrossRef]
R. Gauderon, P. B. Lukins, and C. J. R. Sheppard, "Three-dimensional second-harmonic generation imaging with femtosecond laser pulses," Opt. Lett. 23,1209 (1998). [CrossRef]
W. Denk, J. H. Strickler, and W. W. Webb, "Two photon laser scanning fluorescence microscopy," Science 248, 73 (1990). [CrossRef] [PubMed]
D. Bird and M. Gu, "Compact two-photon fluorescence microscope based on a single-mode fiber coupler," Opt. Lett. 27, 1031 (2002). [CrossRef]
D. Bird and M. Gu, "Two-photon fluorescence endoscopy with a micro-optic scanning head," Opt. Lett. 28, 1552 (2003). [CrossRef] [PubMed]
D. Bird and M. Gu, "Fiber-optic two-photon scanning fluorescence microscopy," J. Micros. 208,35 (2002). [CrossRef]
L. Fu, X. Gan, and M. Gu, "Use of single-mode fiber coupler for second-harmonic-generation microscopy," Opt. Lett. 30, 385 (2005). [CrossRef] [PubMed]
L. Fu, X. Gan, and M. Gu, "Nonlinear optical microscopy based on double-clad photonic crystal fibers," Opt. Expess 13, 5528 (2005).Q1 [CrossRef]
M. Gu, Principles of Three-Dimensional Imaging in Confocal Microscopes (World Scientific, Singapore, 1996). [CrossRef]
C. J. R. Sheppard and M. Gu, "The significance of 3D transfer functions in confocal scanning microscopy," J. Micros. 165,377 (1992). [CrossRef]
M. Gu and D. Bird, "Three-dimensional optical-transfer-function analysis of fiber-optical two-photon fluorescence microscopy," J. Opt. Soc. Am. A 20,941 (2003). [CrossRef]
M. Gu, C. J. R. Sheppard, and X. Gan, "Image formation in a fiber-optical confocal scanning microscope" J. Opt. Soc. Am. A 8, 1755 (1991). [CrossRef]
S. Kimura and T. Wilson, "Confocal scanning optical microscope using single-mode fiber for signal detection," Appl. Opt. 30, 2143 (1991). [CrossRef] [PubMed]
M. Gu, X. Gan, and C. J. R. Sheppard, "Three-dimensional coherent transfer functions in fiber-optical confocal scanning microscopes," J. Opt. Soc. Am. A 8, 1019 (1991). [CrossRef]
S. Yazdanfar, L. H. Laiho, and P. T. C. So, "Interferometric second harmonic generation microscopy," Opt. Express 12, 2739 (2004). [CrossRef] [PubMed]
M. Gu and C. J. R. Sheppard, "Comparison of three-dimensional imaging properties between two-photon and single-photon fluorescence microscopy," J. Micros. 177,128 (1995). [CrossRef]

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