Abstract
Based on the generalized Huygens-Fresnel integral and the Hermite-Gaussian expansion of a Lorentz distribution, analytical expressions for the mutual coherence function, the effective beam size, and the spatial complex degree of coherence of a partially coherent Lorentz-Gauss beam through a paraxial and real ABCD optical system are derived, respectively. As a numerical example, the focusing of a partially coherent Lorentz-Gauss beam is considered. The normalized intensity distribution, the effective beam size, and the spatial complex degree of coherence for the focused partially coherent Lorentz-Gauss beam are numerically demonstrated in the focal plane. The influence of the spatial coherence length on the normalized intensity distribution, the effective beam size, and the spatial complex degree of coherence is mainly discussed.
©2010 Optical Society of America
1. Introduction
With the identical spatial extension, the angular spreading of a Lorentz-Gaussian distribution is higher than that of a Gaussian distribution [1]. Therefore, Lorentz-Gauss beams provide appropriate models to describe the radiation emitted by a single mode diode laser [2,3]. The Lorentz beam is a special case of Lorentz-Gauss beams. Within the framework of the paraxial and non-paraxial cases, the properties of Lorentz-Gauss beams have been extensively investigated [4–14]. However, the reported researches were mainly confined to the case of fully coherent Lorentz-Gauss beams. In the practical optical systems, laser beams are almost partially coherent [15], which denotes that fully coherent laser sources are the ideal cases. In the paraxial optics, an arbitrary optical system is described by an ABCD matrix, which is very simple and convenient to the practical applications. To properly design an optical system that includes a single mode diode laser, the analysis of propagation of a Lorentz-Gauss beam passing through an ABCD optical system is prerequisite. In the remainder of this paper, therefore, the propagation of a partially coherent Lorentz-Gauss beam through a paraxial and real ABCD optical system is investigated. Moreover, analytical expressions for the mutual coherence function, the effective beam size, and the spatial complex degree of coherence are derived by means of the mathematical techniques. A numerical example is also demonstrated.
2. Propagation of a partially coherent Lorentz-Gauss beam through a paraxial and real ABCD optical system
In the Cartesian coordinate system, the z-axis is taken to be the propagation axis. The mutual coherence function of a partially coherent Lorentz-Gauss beam in the source plane z=0 is characterized by
with E(x 01,y 01,0), E(x 02,y 02,0), and g(x 01, x 02;y 01, y 02) given by where p=1 or 2 (hereafter). w 0 x and w 0 y are the parameters related to the beam widths of the Lorentz part in the x- and y-directions, respectively. w 0 is the waist of the Gaussian part. is the complex degree of spatial coherence of beams generated by a Schell-model source. σx and σy are the spatial coherence length in the x- and y-directions, respectively. The time-dependent factor exp(-iωt) is omitted in the Eq. (1), and ω is the circular frequency. The Lorentz distribution can be expanded into the linear superposition of Hermite-Gaussian functions:where N is the number of the expansion. a 2 m and a 2 n are the weight coefficients and can be indexed in [16]. H 2 m(.) and H 2 n(.) are the 2mth- and 2nth-order Hermite polynomials, respectively. Therefore, Eq. (2) can be rewritten as follows:whereand j=x or y (hereafter). The propagation of a partially coherent Lorentz-Gauss beam through a paraxial ABCD optical system is described by the generalized Huygens-Fresnel diffraction integral:where is the wave number. λ is the wavelength. A, B, C, and D are matrix elements of the optical system between the source and the output planes. Moreover, there is no inherent aperture between the source and the output planes. Therefore, A, B, C, and D are all real-valued. Using the following mathematical formulae [17]: we can obtain the mutual coherence function of a partially coherent Lorentz-Gauss beam in the output plane aswith and given bywhere [m-l 1+l 3/2] gives the greatest integer less than or equal to (m-l 1+l 3/2), andThe effective beam size of the partially coherent Lorentz-Gauss beam in the x- and y-directions of the output plane is defined as [18]
Substituting Eq. (11) into Eq. (15), the analytical effective beam size of the partially coherent Lorentz-Gauss beam yieldswith Ω1 j and Ω2 j given by whereand Γ(.) is a Gamma function.The spatial complex degree of coherence of the partially coherent Lorentz-Gauss beam at two points (x 1, y 1, z) and (x 2, y 2, z) turns out to [19,20]
with and given byInserting Eq. (12) into Eq. (21), one can calculate the spatial complex degree of coherence.3. Numerical calculations and analyses
Now, we consider the focusing of the partially coherent Lorentz-Gauss beam. A thin lens with the focal length f is placed in front of the single mode diode laser, so that the partially coherent Lorentz-Gauss beam is transformed into a converging beam. In the case of diode-fiber coupling, a fiber end is placed in the focal region. The matrix elements of this optical arrangement are A=0, B=f, C=−1/f, and D=1. The normalized light intensity, the effective beam size, and the spatial complex degree of coherence for the partially coherent Lorentz-Gauss beam in the focal plane are calculated by using the formulae derived above. As the x- and y-directions are separable, only the x-direction is considered in the following calculations. Moreover, we mainly concentrate on the effect of the spatial coherence length. Figure 1 represents the normalized intensity distribution in the focal plane. The parameters used are chosen as follow: λ=0.8μm, f=1m and w 0 x=1mm. w 0=2mm in Fig. 1(a) and w 0=∞ in Fig. 1(b). The normalized intensity distribution of the partially coherent Lorentz-Gauss beam spreads with decreasing the spatial coherence length σx. The effective beam size of partially coherent Lorentz-Gauss beams in the focal plane versus the coherence length σx is depicted in Fig. 2 . The inset shows the detail change of Wxz within the range of 0.2mm≤σx≤1mm. With increasing the spatial coherence length σx, the effective beam size first quickly decreases and then tends to a minimum value. The better coherence the partially coherent Lorentz-Gauss beam has, the smaller effective beam size it has. If the spatial coherence length σx keeps invariant, the partially coherent Lorentz-Gauss beam with smaller w 0 and w 0 x has the larger effective beam size. Figure 3 shows the spatial complex degree of coherence in the focal plane. w 0=2mm and w 0 x=1mm. σx=1mm, 2mm, and mm in Figs. 3(a)–3(c), respectively. With given two given points (x 1, f) and (x 2, f), their spatial complex degree of coherence increases with increasing the spatial coherence length σx. To quantitatively evaluate the influence of the spatial coherence length on the spatial complex degree of coherence, we calculate the spatial complex degree of coherence at two points (0.1mm, f)and (0.4mm, f) by altering the spatial coherence length σx, which is shown in Fig. 4 . With increasing the spatial coherence length σx, the spatial complex degree of coherence first quickly increases and then tends to the saturated value 1. With a given σx, the partially coherent Lorentz-Gauss beam with the smaller w 0 and w 0 x has the larger spatial complex degree of coherence.
It should be pointed out that the presented formulae are valid for the case of the three beam parameters being far larger than the wavelength. In the paraxial case, the beam propagation fa-ctor of a partially coherent Lorentz-Gauss beam has been presented as Eq. (22) in [21]. By expanding the complementary error function, the beam propagation factor of a partially coherent Lorentz-Gauss beam can be verified to be larger than that of a corresponding partially coherent Gaussian beam. Therefore, the angular spreading of a partially coherent Lorentz-Gauss beam still preserves high within the paraxial propagation. When the three beam parameters are of the order of the wavelength, an efficaciously non-paraxial method is to be sought to treat the propagation of partially coherent Lorentz-Gauss beams.
4. Conclusions
Based on the generalized Huygens-Fresnel integral and the expansion of Lorentz distribution, the analytical propagation equation of a partially coherent Lorentz-Gauss beam through a paraxial and real ABCD optical system is derived. Moreover, the analytical formulae for the effective beam size and the spatial complex degree of coherence are also presented. As a numerical example, the normalized light intensity, the effective beam size, and the spatial complex degree of coherence for the partially coherent Lorentz-Gauss beam focused by a thin lens are calculated in the focal plane. The effect of the spatial coherence length is mainly discussed. With increasing the spatial coherence length, the partially coherent Lorentz-Gauss beam has the smaller effective beam size and the higher spatial complex degree of coherence. As apertures usually exist in the practical optical system, the propagation of a partially coherent Lorentz-Gauss beam through a paraxial and complex ABCD optical system also deserves to be investigated. This research is useful to the optical designs that are involved in the single mode diode laser.
Acknowledgements
This research was supported by National Natural Science Foundation of China under Grant No. 10974179 and Zhejiang Provincial Natural Science Foundation of China under Grant No. Y1090073.
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