Transport of anti-sperm monoclonal IGA and IGC into murine male and female genital tracts from blood - Effect of sex hormones

Ab levels in the genital tract may be important in fertility and in preventing sexually transmitted diseases, In this study, I-125-labeled polymer or monomer mAb IgA (C4pIgA or C4mIgA) and IgC2b (C4IgC) to murine lactate dehydrogenase C4 and a polymer mAb IgA (npIgA) not cross-reacting with mouse sperm were intravenously injected into BALB/c mice, and the relative distribution of these Abs was determined. Polymer IgA was transported much more efficiently into the genital tract, trachea, and duodenum of both sexes than C4IgG and C4 mIgA (p < 0.01), The transport of polymer IgA (C4pIgA and npIgA) into the male genital tract greatly increased following orchiectomy (p < 0.01); this change was not affected by testosterone, suggesting that the unknown regulatory factor(s) from the testis may suppress polymer IgA transport, However, the transport of polymer IgA into female genital tissues was significantly decreased by ovariectomy (p < 0.01); this decline can be rectified by P-estradiol but not progesterone treatment, suggesting that estradiol may stimulate polymer IgA transport, Furthermore, the transport of C4IgG into tissues of the Fallopian tubes and the uterus was significantly decreased by treatment with progesterone (p < 0.01). Together, these findings indicate that serum polymer IgA can be transported selectively into the genital tracts of both sexes, that this transport is strongly under the control of gonads, and that transport of Ige into the Fallopian tubes and uterus is downregulated by progesterone.

抗 LDH－C4 IgA 和IgG 抗体在粘膜免疫系统的分布及其抗生育作用的研究

已有的研究表明，小鼠背部携带能分泌抗原特异的IgA 单克隆抗体的杂交细 胞瘤，可以保护小鼠抵抗微生物和病毒等多种病原体经粘膜途径感染机体。我们 利用背部携带能分泌抗精子特异抗原（LDH-C4）的IgA 和IgG 杂交细胞瘤、以 及抗DNP 的IgA 骨髓细胞瘤的小鼠为动物模型，采用定量ELISA 法研究了抗 LDH－C4 IgA 与抗DNP IgA 单克隆抗体在呼吸道、肠道及生殖道内转运和分布， 抗LDH-C4 IgG2b 在肠道内转运与分布，以及抗LDH-C4 IgA 和IgG 单克隆抗体 在体内抗生育作用。 研究结果表明，带瘤小鼠血液中含有较高水平抗原特异的 IgA 和IgG 单克 隆抗体。PA4 和MOPC IgA 单克隆抗体在呼吸道、肠道以及雌性生殖道分泌物 内有较高的分布水平。在肠道，PA4 和MOPC IgA 单克隆抗体的分布水平显著 高于IgG（p<0.01 和p<0.05）。在肠道和生殖道的不同部位，IgA 抗体的分布水 平不同。在肠道，结肠分泌物中的IgA 单克隆抗体显著高于其它肠道部位 （p<0.01）。在生殖道，IgA 单克隆抗体分布水平以子宫角分泌物中最高。雄性 的前列腺也有较高的IgA 抗体水平。在呼吸道、肠道以及雌性生殖道相应部位的 分泌物内，PA4 IgA 单克隆抗体的水平显著高于MOPC IgA 单克隆抗体的分布水 平（p<0.05）。PA4 和MOPC IgA 单克隆抗体在粘膜分泌物内的分布水平差异可 能与其IgA 聚合形式的不同有关。另外，除气管外，在两时间点间分泌物中的 IgA 抗体水平没有显著差异。 检测背部带瘤小鼠交配后的两细胞胚胎期，发现携带PA4 和G2b 杂交细瘤 的雌性小鼠的受精率与对照组并没有显著的差异，这表明抗LDH-C4 IgA 和IgG 单克隆抗体在体内不能明显抑制小鼠的精子和卵子的结合或受精过程。注射细 胞后的27 天，检测鼠着床胚胎时，发现带瘤两性小鼠均携带PA4 时或者只有 雌性携带PA4 杂交瘤时，以及雌雄两性小鼠均携带G2b 杂交瘤细胞时，交配后的怀孕率与能分泌抗DNP 抗体的MOPC 的骨髓瘤细胞瘤的相应组别相比，显 著降低（p<0.01）。但PA4 各组与G2b 各组之间无显著差异(p>0.05）。然而，雌 雄的小鼠均带瘤时，最高怀孕减少率未能达100%。这些结果提示，抗LDHC4 IgA 和IgG 单克隆抗体在小鼠体内不能有效地抑制小鼠的精子与卵子的结 合，但能显著地抑制小鼠受精后胚胎的发育。抗LDH-C4 的IgA 和IgG 单克隆 抗体单独存在时，在体内均具有抗生育作用，但不能完全抑制生育。

抗LDH-C4的IgA单克隆抗体在生殖道局部的分布

为了弄清生殖道内抗体，特别是IgA抗体的准确来源和它的调控因子，同时也为了弄清生殖的局部免疫与典型的粘腊免疫之间的关系，以同位素标记的针对精子特有抗原乳酸脱氢酶C4(LDH-C4)的多聚IgA单抗及其单体，与小鼠精子发生反应的IgA单抗，以及LDH-C4特异的IgG抗体，尾静脉注射给雌雄Balb/c小鼠，4小时后测定小鼠的生殖道及其分汾物，肠道、呼吸道及其分泌物，各相关淋巴组织以及其它器官内这些抗体的分布。还研究了特异抗原刺激、性激素等对这些抗体分布状况的影响。

Stiction and Anti-Stiction in Mems and Nems

Stiction in microelectromechanical systems (MEMS) has been a major failure mode ever since the advent of surface micromachining in the 80s of the last century due to large surface-area-to-volume ratio. Even now when solutions to this problem are emerging, such as self-assembled monolayer (SAM) and other measures, stiction remains one of the most catastrophic failure modes in MEMS. A review is presented in this paper on stiction and anti-stiction in MEMS and nanoelectromechanical systems (NEMS). First, some new experimental observations of stiction in radio frequency (RF) MEMS switch and micromachined accelerometers are presented. Second, some criteria for stiction of microstructures in MEMS and NEMS due to surface forces (such as capillary, electrostatic, van der Waals, Casimir forces, etc.) are reviewed. The influence of surface roughness and environmental conditions (relative humidity and temperature) on stiction are also discussed. As hydrophobic films, the self-assembled monolayers (SAMs) turn out able to prevent release-related stiction effectively. The anti-stiction of SAMs in MEMS is reviewed in the last part.

Stress intensity factors calculation in anti-plane fracture problem by orthogonal integral extraction method based on femol

For an anti-plane problem, the differential operator is self-adjoint and the corresponding eigenfunctions belong to the Hilbert space. The orthogonal property between eigenfunctions (or between the derivatives of eigenfunctions) of anti-plane problem is exploited. We developed for the first time two sets of radius-independent orthogonal integrals for extraction of stress intensity factors (SIFs), so any order SIF can be extracted based on a certain known solution of displacement (an analytic result or a numerical result). Many numerical examples based on the finite element method of lines (FEMOL) show that the present method is very powerful and efficient.

Unloading characteristics of anti-plane shear crack in softening materials

The local characteristics of the anti-plane shear stress and strain field are determined for a material where the stress increases linearly with strain up to a limit and then softens nonlinearly. Two unloading models are considered such that the unloading path always returns to the origin while the other assumes the unloading modulus to be that of the initial shear modulus. As the applied shear increases, an unloading zone is found to prevail between a zone in which the material softens and another zone in which the material is linear-elastic even though the crack does not propagate. The divisions of these zones are displayed graphically.

The Mitogenic and Anti-Apoptotic Activity of Tumor Conditioned Medium on Endothelium

This study was designed to observe the effect of tumor conditioned medium (TCM) on the proliferation and apoptosis of human umbilical vein endothelial cells (HUVECs). HUVECs were exposed to TCM from breast carcinoma cell line MDA-MB-231, then we measured their proliferation, apoptosis and cell cycle distribution by MTT and flow cytometery (FCM). Following the stimulation of TCM, HUVECs showed higher pro-mitogenic and anti-apoptotic ability than did the negative control group (ECGF-free medium with 20% FBS), but a similar ability to the positive control group (medium with ECGF and 20% FBS). From these results, we can conclude that breast carcinoma cell line MDA-MB-231 could secret soluble pro-angiogenic factors that induce HUVEC angiogenic switching, including cell cycle progression, proliferation and growth. The role and character of these factors remain to be further studied.

Imaging properties of coherent anti-Stokes Raman scattering microscope

The coherent anti-Stokes Raman scattering (CARS) microscope with the combination of confocal and CARS techniques is a remarkable alternative for imaging chemical or biological specimens that neither fluoresce nor tolerate labelling. CARS is a nonlinear optical process, the imaging properties of CARS microscopy will be very different from the conventional confocal microscope. In this paper, the intensity distribution and the polarization property of the optical field near the focus was calculated. By using the Green function, the precise analytic solution to the wave equation of a Hertzian dipole source was obtained. We found that the intensity distributions vary considerably with the different experimental configurations and the different specimen shapes. So the conventional description of microscope (e.g. the point spread function) will fail to describe the imaging properties of the CARS microscope.

The intensity distributions of collected signals in coherent anti-Stokes Raman scattering microscopy

Coherent anti-Stokes Raman scattering (CARS) microscopy with the combining of confocal and CARS techniques is a remarkable alternative for imaging chemical or biological specimens that neither fluoresce nor tolerate labeling. The CARS is a nonlinear optical process, the imaging properties of CARS microscopy will be very different from the conventional confocal microscopy. In this paper, we calculated the propagation of CARS signals by using the wave equation in medium and the slowly varying envelope approximation (SVEA), and find that the intensity angular distributions vary considerably with the different experimental configurations and the different specimen shapes. So the conventional description of microscopy (e.g.. the point spread function) will fail to descript the imaging properties of CARS microscopy. (c) 2004 Elsevier B.V. All rights reserved.

Encoded cell grating array in anti-counterfeit technology

The dot matrix hologram (DMH) has been widely used in anti-counterfeiting label. With the same technology and cell array configuration, we can encode to the incidence beam. These codes can be some image matrix grating with different grating gap and different grating orientation. When the multi-level phase diffractive grating is etched, the incidence beam on the cell appears as an encoding image. When the encoded grating and DMH are used in the same label synchronously, the technology of multi-encoded grating array enhances the anti-counterfeit ability.

Influence of vacuum organic contaminations on laser-induced damage of 1064 nm anti-reflective coatings

We investigate the influence of vacuum organic contaminations on laser-induced damage threshold (LIDT) of optical coatings. Anti-reflective (AR) coatings at 1064 nm made by Ta2O5/SiO2 are deposited by the ion beam sputtering method. The LIDTs of AR coatings are measured in vacuum and in atmosphere, respectively. It is exhibited that contaminations in vacuum are easily to be absorbed onto optical surface because of lower pressure, and they become origins of damage, resulting in the decrease of LIDT from 24.5 J/cm(2) in air to 15.7 J/cm(2) in vacuum. The LIDT of coatings in vacuum has is slightly changed compared with the value in atmosphere after the organic contaminations are wiped off. These results indicate that organic contaminations are the main reason of the LIDT decrease in vacuum. Additionally, damage morphologies have distinct changes from vacuum to atmosphere because of the differences between the residual stress and thermal decomposability of filmy materials.