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1.
教育考试考生诚信系统是一个能在一定时间、一定区域内完整体现考生参加教育考试的诚信情况、失信惩处情况,并经诚信评级形成信用报告的系统。教育考试考生诚信系统的构建应遵循有效性、尊重考生的知情权与监督权、坚持动态化管理、坚持公开与保密相结合等原则,可包括系统维护模块、考生诚信档案模块、诚信信息查询模块、考生信用评级模块、考生信用报告模块五个子系统。这一系统的有效运行应以诚信宣传教育为基础、以诚信管理制度建设作保障、以信用服务为工具,旨在增强考生履信愿望,提高考生的诚信智慧和履信力,最终引导考生由诚信他律转向诚信自律。  相似文献   

2.
为加强对考生遵守考试纪律的教育,减少违纪舞弊现象的发生,教育部要求考生在普通高等学校招生全国统一考试前阅读“诚信考试承诺书”并签字认可。2004年7月,教育部颁布了《国家教育考试违规处理办法》。其中第三十条规定“教育考试机构应当建立考生诚信档案,记录、保留在国家教育考试中作弊考生的相关信息”。教育考试机构应当接受社会有关方面对考生诚信档案的查询,并及时向招生机构提供相关信息。“承诺书”的主要内容包括:考生须知晓和遵守的有关考试规定、纪律要求,考生愿意在考试中自觉遵守,如有违反将接受处理。  相似文献   

3.
6月7日《人民日报》报道,今年高考实施部、省两级国家教育考试诚信档案网络管理。凡是在国家教育考试中严重违规的考生,将被记入国家教育考试诚信档案数据库,供高等学校、招生单位甚至将来的用人部门查询。  相似文献   

4.
肖华 《云南教育》2007,(6X):38-38
6月7日《人民日报》报道,今年高考实施部、省两级国家教育考试诚信档案网络管理。凡是在国家教育考试中严重违规的考生,将被记人国家教育考试诚信档案数据库,供高等学校、招生单位甚至将来的用人部门查询。  相似文献   

5.
为解决近年来在考试中出现的身份验证问题,利用指纹终身唯一的特性,结合IC卡技术,采用带有考生指纹信息的IC卡准考证,建立基于指纹特征匹配的IC卡考试身份验证管理系统,考场现场进行指纹考试身份验证,可以保证报名者与考生身份完全一致.  相似文献   

6.
考试作弊行为对社会、对考生本人的负面影响是惨痛的,同时也影响教育事业的健康发展,培养考生的考试诚信是杜绝考生作弊的重要途径。考生的考试诚信形成是各个主体之间重复博弈的结果,只有通过为考生考试诚信形成的重复博弈提供良好的外在环境,并通过多种形式教育,才能形成考生考试诚信的良好环境。  相似文献   

7.
《教育科学论坛》2005,(6):79-79
考生电子档案是高等学校录取新生的主要依据。2005年高考考生的电子档案中将在考生报名信息(含身份证号、思想政治品德考核鉴定或评语等)、体检信息、志愿信息、成绩信启、基础上,增加考生参加国家教育考试的诚信记录,主要内容为考试违规的简要事实及处理结果。  相似文献   

8.
人脸识别技术在智能考生身份验证系统的应用与研究   总被引:2,自引:0,他引:2  
余强 《宜春学院学报》2011,33(4):64-65,87
现行考试的考生身份验证,都是靠人工肉眼识别方式,存在着错判、露判和其他人为因素等问题,严重影响了考试的公开性。借助人脸识别技术和视频技术,智能化的验证考生身份的真实性,可从源头上避免替考和假证等现象,大大提高考生身份验证的安全性和有效性。  相似文献   

9.
事件:教育部从今年起首次将考试诚信记录记入考生电子档案,并与高校录取挂钩;凡携带规定以外的物品进入考场或者未放在指定位置,都有可能影响录取。对有违规记录的考生,将在考生特征标志信息项中,统一用字母“W”予以标示。(《中国教育报》)评论:诚信教育与现实的最佳结合考生电子档案是高等学校录取新生的主要依据,考生的诚信记录被载入档案,明白无误地传递了一个信息:有作弊等失信行为的考生,很可能因此而失去被高校录取的资格。作为一个更广泛的导向,诚信记录进入考生电子档案,也告诉我们:诚信记录成为个人在社会上的“通行证”,已不仅…  相似文献   

10.
招生考试是国家选拔与培养人才的主要手段,对于考生来说更是人生的重要转折点,因此,一定要保证其公平公正。有少数考生存有侥幸心理,试图以舞弊行为通过考试,给教育考试的安全带来极大挑战,也给考务工作人员带来很大压力。因此,我们需要将更便捷高效的现代化技术应用到考生身份验证工作中,以杜绝替考现象的发生。  相似文献   

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13.
Let Γd2nbe the set of trees with a given diameter d having a perfect matching,where 2n is the number of vertex.For a tree T in Γd2n,let Pd+1be a diameter of T and q = d m,where m is the number of the edges of perfect matching inPd+1.It can be found that the trees with minimal energy in Γd2nfor four cases q = d 2,d 3,d 4,[d2],and two remarks aregiven about the trees with minimal energy in Γd2nfor2d 33q d 5 and [d2] + 1 q2d 33 1.  相似文献   

14.
Abstract

Consciousness is a natural and integral part of human beings that is at the core of our physical, emotional, mental, and spiritual functions throughout our lives. However, we tend to be too occupied with or distracted by the details of our daily existence to be fully aware of our own consciousness. More often than not, we are engaged in the surface consciousness in the materialistic world or emotional realm, which interferes us to get connected with our deeper consciousness and capacity. This paper will unpack the layers of human consciousness (or lack of consciousness) from philosophical perspective to examine the relations between our understanding of consciousness and its impact on our holistic wellbeing and growth (Singh, 2016 Singh, L. P. (2016). Science, spirituality, and ontological mysticism: the philosophical enquiry and reflection. Delhi, India: Concept Publishing Co. [Google Scholar]; Suzuki, 1999 Suzuki, S. (1999). Zen Mind. New York: Weatherhill. [Google Scholar]; Thompson, 2015 Thompson, E. (2015). Waking, dreaming, being. New York: Columbia University Press. [Google Scholar]). What is consciousness? How do human beings choose our consciousness? What is the relation between micro and macro consciousness? How do we expand, develop, and apply our consciousness for the maximum wellbeing and growth through education? The paper intends to go beyond the compartmentalized analysis of consciousness (e.g. biological, psychological, neurological etc.) by engaging a holistic metaphysical viewpoint as well as relational and dialectic approaches (Ames & Hall, 2003 Ames, T. R. & Hall, L. D. (2003). Daodejing: making this life significant. New York: Ballantine. [Google Scholar]) Hegel, 1807, 1977 Hegel, G. W. F. (1807, 1977). The Phenomenology of spirit. (A. V. Miller Trans.). Oxford: Clarendon Press. [Google Scholar]; Laozi, 1999 Laozi. (1999). Daodejing (道德经). Shanxi, China: Shanxi Classics Press. [Google Scholar]). It aims to connect theory, learning, and living together with nature and universe beyond the limitation of time and space.  相似文献   

15.
Consider the positive d-dimensional lattice d (d≥2) with partial ordering ≤, let {XK; K ∈ d } be i.i.d. random vari- ables taking values in a real separable Hilbert space (H, ||·||) with mean zero and covariance operator ∑, and set partial sums SN =∑K≤NXK, K , N ∈ d . Under some moment conditions, we obtain the precise asymptotics of a kind of weighted infinite series for partial sums SN as ε 0 by using the truncation and approximation methods. The results are related to the convergence rates of the law of the logarithm in Hilbert space, and they also extend the results of (Gut and Spǎtaru, 2003).  相似文献   

16.
Chemically processed Nb-doped SrTiO3 films and properties   总被引:1,自引:0,他引:1  
Homogeneous, crack-free SrNbxTi1−x O3 thin films on (110) silicon substrates were successfully fabricated by sol-gel processing. The optimum route and conditions were systematically investigated. Sr(OAc)2 glacial acctic acid solution, after being refluxed and reacted with tartrate, formed Sr(OAc)2(C4H6O6)2; Ti(OBu)4 formed Ti(OAc)4−x (AcAc)x after having the ligand partially exchanged with AcAc, while Nb(OC2H5)5 formed (OAc)2Nb(AcAc) (C4H6O6) by exchanging of ligand in glacial acetic acid with (CH3CO)2O. All the metal species after undergoing partial hydrolysis and polymerization with hydroxyl or oxygen, formed SrNbxTi1−x O13 cluster sol. Methyl cellulose (MCL) caused SrNbxTi1−x O3 sol to have polymeric structure and easily form films. SrNbxTi1−x O3 films with perovskite were subsequently formed after being annealed at 650∼750 °C for 60 min in 25% N2+75% H2 (volume ratio) atmosphere. Resistivity of the SrNb0.1Ti0.9O3 films at room temperature was 64 μω·cm, a particular T 2 temperature dependence of the resistivity, from 25 K up to room temperature, was observed. Project (No. 2002CB613305) supported by the National Basic Research Program (973) of China  相似文献   

17.
LetH n be the set of real algebraic polynomials of degreen, whose zeros all lie in the interval [−1,1]. The well known Turán type inequalities tell us that forf(x)∈H n , it holds ‖f′‖≥Cnf‖. This note deals with the weighted Turán type inequalities with the weights having inner singularities underL p norm for 0<p≤∞. Our results essentially extend the result of Wang and Zhou (2002), and the method used in this paper is simpler and more direct than that of Wang and Zhou (2002). The results and methods have their own values in approximation theory and computation.  相似文献   

18.
In this paper, we consider some polynomial (α,β)-metrics, and discuss the sufficient and necessary conditions for a Finsler metric in the form F=α a1β a2β2/α a4β4/α3 to be projectively flat, where ai (i=1,2,4) are constants with a1≠0, α is a Riemannian metric and β is a 1-form. By analyzing the geodesic coefficients and the divisibility of certain polynomials, we obtain that there are only five projectively flat cases for metrics of this type. This gives a classification for such kind of Finsler metrics.  相似文献   

19.
In this work, we study the Asanov Finsler metric F=α(β2/α2 gβ/α 1)1/2exp{(G/2)arctan[β/(hα) G/2]}, where α=(αijyiyj)1/2 is a Riemannian metric and β=biyj is a 1-form, g∈(-2,2), h=(1-g2/4)1/2, G=g/h. We give the necessary and sufficient condition for Asanov metric to be locally projectively flat, i.e., α is projectively flat and β is parallel with respect to α. Moreover, we proved that the Douglas tensor of Asanov Finsler metric vanishes if and only if β is parallel with respect to α.  相似文献   

20.
INTRODUCTION Throughout this paper, we shall work with a filtered complete probability space (?,F,(Ft),P) sat-isfying the usual conditions. Let B=(Bt)t≥0 be a stan-dard Brownian motion with B0=0. Denote by ú the set of all non-negative real numbers. Recall that a diffusion process X starting at x≥0 is called the square of a Bessel process of dimension δ>0 if d X t = δd t 2 | X t |d Bt , X 0= x, (1) Clearly, this equation has a unique non-negative strong solution X, i.e., …  相似文献   

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