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大学物理实验误差理论课教学探索与改革 被引量:3
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作者 熊翠秀 《教育教学论坛》 2016年第24期141-142,共2页
针对大学物理实验中存在的一些问题,尝试从大学物理实验的误差理论教学开始进行改革与实践,提出从以下两个方面进行改革与尝试:大学物理实验误差理论课安排在首次实验项目之后;用实测实验数据的具体数据处理加深对概念和方法的掌握。这... 针对大学物理实验中存在的一些问题,尝试从大学物理实验的误差理论教学开始进行改革与实践,提出从以下两个方面进行改革与尝试:大学物理实验误差理论课安排在首次实验项目之后;用实测实验数据的具体数据处理加深对概念和方法的掌握。这些改革能有效促进大学物理实验的教学效果。 展开更多
关键词 大学物理实验误差理论 安排顺序 实测实验数据处理
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谈实验误差理论教学
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作者 莘乃钢 《河北建筑工程学院学报》 CAS 1996年第1期67-70,共4页
强化实验误差理论教学是提高实验教学质量的关键。必须改变集中讲授的做法。把误差理论的教学贯穿到每个实验及整个实验教学全过程中。文中介绍的“分散讲授,逐步深化”的教学方法是切实可行的。
关键词 实验误差理论 强化教学 改革教法
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电表读数与电表等级的关系 被引量:1
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作者 李世明 《物理教师》 1997年第5期33-33,共1页
在1996年第5期刊登了《浅谈物理仪器读数》一文,该文在电压表和电流表读数方法中举例说明了对于0~0.6A挡的电流表读数应读到千分位,0~15V的电压表应读到百分位,并以高考试题评分标准予以说明,本文将从电表等级、误差理论角度对此提出... 在1996年第5期刊登了《浅谈物理仪器读数》一文,该文在电压表和电流表读数方法中举例说明了对于0~0.6A挡的电流表读数应读到千分位,0~15V的电压表应读到百分位,并以高考试题评分标准予以说明,本文将从电表等级、误差理论角度对此提出一些不同看法,供大家参考.按照实验误差理论,实验测量的读数应按有效数字规则读数,即有效数字的最后一位一定要同误差所在的一位对齐,即测量误差出现在哪一位,读数时就应读到哪一位.这样,对电表读数时,首先要估计一下电表的测量误差,然后再确定读到哪一位.根据规定,电表的准确度等级分为0.1、0.2、0.5、1.0、1.5、2.5、5.0共七个等级.从电表的等级数可以确定电表的测量误差.电表的等级通常指明电表测量时的相对额定误差,如1.5级的电表,其相对额定误差为1.5%,则电表指针指示任一测量值时,所包含的最大测量误差为: 展开更多
关键词 电表等级 表读数 测量误差 有效数字位数 实验误差理论 电压表 千分位 评分标准 高考试题 实验测量
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Low energy SUSY confronted with new measurements of W-boson mass and muon g-2 被引量:2
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作者 Jin-Min Yang Yang Zhang 《Science Bulletin》 SCIE EI CAS CSCD 2022年第14期1430-1436,M0003,共8页
The new CDF II measurement of W-boson mass shows a 7σdeviation from the standard model(SM)prediction,while the recent FNAL measurement of the muon g-2 shows a 4.2σdeviation(combined with the BNL result)from the SM.B... The new CDF II measurement of W-boson mass shows a 7σdeviation from the standard model(SM)prediction,while the recent FNAL measurement of the muon g-2 shows a 4.2σdeviation(combined with the BNL result)from the SM.Both of them strongly indicate new physics beyond the SM.In this work,we study the implication of both measurements on low energy supersymmetry.With an extensive exploration of the parameter space of the minimal supersymmetric standard model(MSSM),we find that in the parameter space allowed by current experimental constraints from colliders and dark matter detections,the MSSM can simultaneously explain both measurements on the edge of 2σlevel,taking theoretical uncertainties into consideration.The favored parameter space,characterized by a compressed spectrum between bino,wino and stau,with the stop being around 1 TeV,may be covered in the near future LHC searches. 展开更多
关键词 W-boson mass SUPERSYMMETRY Muon g-2 Large Hadron Collider
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Study on the Effects of the Light CP-odd Higgs via the Leptonic Decays of Pseudoscalar Mesons
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作者 汤亮 柯红卫 李学潜 《Communications in Theoretical Physics》 SCIE CAS CSCD 2012年第11期732-738,共7页
To explain the anomALously large decay rate of ∑+→p+μ+μ-, it was proposed that a new mechanism where a light CP-odd pseudoscaJar boson of mAo = 214.3 MeV makes a crucial contribution. Later, some authors have s... To explain the anomALously large decay rate of ∑+→p+μ+μ-, it was proposed that a new mechanism where a light CP-odd pseudoscaJar boson of mAo = 214.3 MeV makes a crucial contribution. Later, some authors have studied the transition π0→e+e- and γ→γA10 in terms of the same mechanism and their result indicates that with the suggested mass one cannot fit the data. This discrepancy might be caused by experimental error of ∑+→p+μ+μ- because there were only a few events. Whether the mechanism is a reasonable one motivates us to investigate the transitions π0→e+e-;η(η′)→μ+μ-;ηc→μ+μ-;ηb→τ+τ- within the same framework. It is noted that for π0→ e+ e-, the standard model (SM) prediction is smaller than the data, whereas the experimental central value of η→μ+μ- is also above the SM prediction. It means that there should be extra contributions from other mechanisms and the contribution of A may be a possible one. Theoretically calculating the branching ratios of the concerned modes, we would cheek if we can obtain a univers mass for A10 which reconcile the theoretical predictions and data for all the modes. Unfortunately, we find that it is impossible conclude that the phenomenology does not favor such a to have such a mass with the same coupling|gt|. Therefore we light A10, even though a small window is still open. 展开更多
关键词 supersymmetric Higgs bosons supersymmetric models leptonic decays of pseudoscalar mesons
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