基于CT扫描的煤中孔裂隙精细表征

为了深入探究煤层气赋存和运移的机理,需要对煤中孔裂隙进行定性分析和精细定量表征。为此,以沁水盆地南部五阳矿3号煤层的原煤为研究对象,应用X射线对原煤煤心进行360°全角度步进式扫描,借助CT分析构建出其三维数字化可视模型,在此基础上,采用DTM灰度阈值分割法求出孔裂隙的灰度阈值分割点,识别煤中孔裂隙,并与扫描电镜观测到的结果进行对比;采用Avizo软件建立孔裂隙系统的球棒模型,实现了对孔裂隙的定量表征,并与压汞实验结果进行对比。研究结果表明:(1)DTM灰度阈值分割法可以准确识别煤中孔裂隙,并且与扫描电镜图像中同一裂隙的形态和发育尺度基本一致;(2)利用CT扫描可以准确识别直径19.20 mm、高度10.59 mm样品中孔径大于12.40μm的孔裂隙,展现孔裂隙在三维空间的分布情况;(3)压汞实验结果与CT扫描结果仅在以非连通孔隙为主的20~40μm孔径段存在差异,而在40μm以上孔径段二者的孔裂隙体积变化趋势则一致,其中CT扫描的分析结果更为可靠。

风对某型爆炸式催泪弹烟雾扩散特性的影响分析

在研究风对爆炸式催泪弹烟雾扩散的影响时,首先运用FLUENT软件建立一个基础模型,其次分别分析风速和风向对某点烟雾质量浓度以及有效作用面积的影响,最后得出风速和风向对烟雾扩散的相关规律,对武警部队使用爆炸式催泪弹具有一定的借鉴意义.

新型背腔式对数周期缝隙天线阵列设计

介绍了一种新型背腔式对数周期缝隙天线单元,对其各参数特性进行了分析,并采用这种新型天线单元设计了9×7天线阵列。通过HFSS13进行天线阵列的设计。仿真结果表明,该天线阵列在1.5 GHz^6 GHz的工作带宽内,驻波比小于3,回波损耗小于-10 d B,天线阵列最大增益为29.6 d Bi,在整个工作带宽内,增益均大于20 d Bi。具有良好的定向辐射能力,可用于UWB雷达、探测等领域。

某型强光爆震弹强光辐射分析

区别于传统爆震弹,某型强光爆震弹采用双层结构,即开孔外壳覆盖内壳,内壳集聚能量爆炸破裂,光通过外壳喷口泄出作用于目标,外壳体不发生破裂。为了研究这种新型结构对闪光强度的影响,在探讨烟火剂爆炸或燃烧产生的强光辐射的物理参量的基础上,分析强光辐射对人员的杀伤机理。通过对强闪光与人眼关系的分析,选择与之对应的技战参数。并利用声光威力测试系统对喷孔处的强光辐射进行了分析研究。结果表明,该弹满足设定的技战指标。为该弹的药剂设计提供了必要的依据。

基于压汞法对中高阶煤孔隙特征的研究

为了研究中高阶煤孔隙特征,以晋城矿区成庄矿、潞安矿区五阳矿和漳村矿、焦作矿区方庄矿主采煤层煤样为研究对象,采用压汞法对其进行实验测定,研究结果表明:中高级煤以半封闭型孔为主,孔隙之间的连通性较差;中高阶煤样都是以微小孔为主,中孔、大孔所占比例较少,且随着变质程度的升高,微小孔所占比例也呈增加趋势;同为中高阶煤样,不同矿井之间、同一煤层不同分层之间,样品的孔隙特征差异不大,较为相近。

Amplitude analysis of the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)

Using e^(+)e^(−)annihilation data corresponding to an integrated luminosity of 2.93 fb^(−1)taken at the center-of-mass energy√s=3.773 GeV with the BESIII detector,a joint amplitude analysis is performed on the decays D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η).The fit fractions of individual components are obtained,and large interferences among the dominant components of the decays D^(0)→a_(1)(1260)π,D^(0)→π(1300)π,D^(0)→ρ(770)ρ(770),and D^(0)→2(ππ)_(S)are observed in both channels.With the obtained amplitude model,the CP-even fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are determined to be(75.2±1.1_(stat).±1.5_(syst.))%and(68.9±1.5_(stat).±2.4_(syst.))%,respectively.The branching fractions of D^(0)→π^(+)π^(−)π^(+)π^(−)and D^(0)→π^(+)π^(−)π^(0)π^(0)(non-η)are measured to be(0.688±0.010_(stat.)±0.010_(syst.))%and(0.951±0.025_(stat.)±0.021_(syst.))%,respectively.The amplitude analysis provides an important model for the binning strategy in measuring the strong phase parameters of D^(0)→4πwhen used to determine the CKM angleγ(ϕ_(3))via the B^(−)→DK^(−)decay.

Determination of the number ofψ(3686)events taken at BESⅢ

The number ofψ(3686)events collected by the BESⅢdetector during the 2021 run period is determined to be(2259.3±11.1)×10~6 by counting inclusiveψ(3686)hadronic events.The uncertainty is systematic and the statistical uncertainty is negligible.Meanwhile,the numbers ofψ(3686)events collected during the 2009 and 2012run periods are updated to be(107.7±0.6)×10~6 and(345.4±2.6)×10~6,respectively.Both numbers are consistent with the previous measurements within one standard deviation.The total number ofψ(3686)events in the three data samples is(2712.4±14.3)×10~6.

Observation of e^(+)e^(-)→pppñπ-+c.c.

Using data taken at 29 center-of-mass energies between 4.16 and 4.70 GeV with the BESⅢdetector at the Beijing Electron Positron Collider corresponding to a total integrated luminosity of approximately 18.8 fb^(-1),the process e^(+)e^(-)→pppñπ+c.c.is observed for the first time with a statistical significance of 11.5σ.The average Born cross sections in the energy ranges of(4.160,4.380)GeV,(4.400,4.600)GeV and(4.610,4.700)GeV are measured to be(21.5±5.7±1.2)fb,(46.3±10.6±2.5)fb and(59.0±9.4±3.2)fb,respectively,where the first uncertainties are statistical and the second are systematic.The line shapes of the pñ and ppπ^(-)invariant mass spectra are consistent with phase space distributions,indicating that no hexaquark or di-baryon state is observed.

Search for hidden-charm tetraquark with strangeness in e^(+)e^(−)→K^(+)D_(s)^(∗−) D^(∗0 )+ c.c.

We report a search for a heavier partner of the recently observed Z_(cs)(3985)^(-) state,denoted as Z_(cs)^('-),in the process e^(+)e^(−)→K^(+)D_(s)^(∗−) D^(∗0 )+ c.c.,based on e^(*)e^(-)collision data collected at the center-of-mass energies of √s=4.661,4.682 and 4.699 GeV with the BESIII detector.The Z_(cs)^('-) is of interest as it is expected to be a candidate for a hidden-charm and open-strange tetraquark.A partial-reconstruction technique is used to isolate K^(+)recoil-mass spectra,which are probed for a potential contribution from Z_(cs)^('-)→D_(s)^(∗−) D^(∗0 )+ c.c.We find an excess of Z_(cs)^('-)→D_(s)^(*-)-D^(*0)(c.c.)candidates with a significance of 2.1o,after considering systematic uncertainties,at a mass of(4123.5±0.7_(sat)±4.7_(syst.))MeV/c^(2).As the data set is limited in size,the upper limits are evaluated at the 90%confidence level on the product of the Born cross sections(σ^(Borm))and the branching fraction(B)of Z_(cs)^('-)→D_(s)^(*-)-D^(*0),under different assumptions of the Z_(cs)^('-) mass from 4.120 to 4.140 MeV and of the width from 10 to 50 MeV at the three center-of-mass energies.The upper limits of σ^(Born).B are found to be at the level of O(1)pb at each energy.Larger data samples are needed to confirm the Z_(cs)^('-) state and clarify its nature in the coming years.

Search for the weak decayψ(3686)→■+c.c.

Using(448.1±2.9)×10^(6)ψ(3686)for the weak baryonic decayψ(3686)→Λc+∑-+c.c..The analysis procedure is optimized using a blinded method.No significant signal is observed,and the upper limit on the branching fraction(B)ofψ(3686)→Λc+∑-+c.c.is set as 1.4×10^(-5)at the 90%confidence level.

Observations of the Cabibbo-Suppressed decays Λ_(c)^(+)→nπ+π^(0),nπ^(+)π^(-)π^(+) and the Cabibbo-Favored decay Λ_(c)^(+)→nK^(-)π^(+)π^(+)

Using electron-positron annihilation data samples corresponding to an integrated luminosity of 4.5 fb-1,collected by the BESⅢdetector in the energy region between 4599.53 MeV and 4698.82 MeV,we report the first observations of the Cabibbo-suppressed decaysΛ_(c)^(+)→nπ^(+)π^(0),Λ_(c)^(+)→nπ^(+)π^(-)π^(+),and the Cabibbo-favored decayΛ_(c)^(+)→nK^(-)π^(+)π^(+)with statistical significances of 7.9σ,7.8σ,and>10σ,respectively.The branching fractions of these decays are measured to be B(Λ_(c)^(+)→nπ^(+)π^(0))=(0.64±0.09±0.02)%,B(Λ_(c)^(+)→nπ^(+)π^(-)π^(+))=(0.45±0.07±0.03)%,and B(Λ_(c)^(+)→nK^(-)π^(+)π^(+))=(1.90±0.08±0.09)%,where the first uncertainties are statistical and the second are systematic.We find that the branching fraction of the decayΛ_(c)^(+)→nπ^(+)π^(0)is about one order of magnitude higher than that ofΛ_(c)^(+)→nπ^(+).

声频定向攻击点声源面阵列指向性仿真研究

为实现强噪声的高指向性传播，基于声频定向系统研究点声源面阵列的指向性函数，利用MATLAB对点声源面阵列指向性进行仿真，研究不同阵元间距、阵元数目对超声波指向性影响。由仿真得出，当点声源间距等于或接近超声波波长时，点声源面阵列指向性最好；增加面阵列点声源个数可提高指向性，并使旁瓣的幅值减小。

一江春水

多情自古空遗恨，伤罢离人又一分。错挽心头明月夜，滔滔春水若忧君。

春色方兴

春色方兴绿柳丛，嫩藤丝缕醉江风。漫寻诗意词难赋，离索天涯句便工。

游净月潭

携友从心去，浪涛卷雁边。寻诗来净月，信步往青莲。

Measurement of integrated luminosities at BESⅢ for data samples at center-of-mass energies between 4.0 and 4.6 GeV

The integrated luminosities of data samples collected in the BESⅢ experiment in 2016-2017 at centerof-mass energies between 4.19 and 4.28 GeV are measured with a precision better than 1% by analyzing large-angle Bhabha scattering events.The integrated luminosities of old datasets collected in 2010-2014 are updated by considering corrections related to detector performance,offsetting the effect of newly discovered readout errors in the electromagnetic calorimeter,which can haphazardly occur.

Number of J/ψ events at BESIII

Using inclusive decays of J/ψ aprecise determination of the number of J/ψ events collected with the BESIII detector was performed.For the two data sets taken in 2009 and 2012,the numbers of J/ψ events were recalculated to be(224.0±1.3)×10^(6) and(1088.5±4.4)×10^(6),respectively;these numbers are in good agreement with the previous measurements. For the J/ψ sample taken in 2017-2019,the number of events was determined to be(8774.0±39.4)×10^(6).The total number of J/ψ events collected with the BESIII detector was determined to be(10087±44)×10^(6),where the uncertainty is dominated by systematic effects,and the statistical uncertainty is negligible.

Luminosities and energies of e^(+)e^(−) collision data taken between √s=4.61 GeV and 4.95 GeV at BESⅢ

From December 2019 to June 2021,the BESⅢ experiment collected approximately 5.85 fb^(−1) of data at center-of-mass energies between 4.61 and 4.95 GeV.This is the highest collision energy BEPCⅡ has reached to date.The accumulated e^(+)e^(−) annihilation data samples are useful for studying charmonium(-like)states and charmed-hadron decays.By adopting a novel method of analyzing the production of A_(c)^(+)A_(c)^(-) pairs in e^(+)e^(−) annihilation,the center-of-mass energies are measured with a precision of 0.6 MeV.Integrated luminosities are measured with a precision of better than 1% by analyzing the events of large-angle Bhabha scattering.These measurements provide important inputs to analyses based on these data samples.

Observation of the Y(4230)and a new structure in e^(+)e^(-)→K^(+)K^(-)J/Ψ

The cross sections of e^(+)e^(-)→K^(+)K^(-)J/Ψat center-of-mass energies from 4.127 to 4.600 GeV are measured based on 15.6 fb-1data collected with the BESⅢ detector operating at the BEPCⅡ storage ring.Two resonant structures are observed in the line shape of the cross sections.The mass and width of the first structure are measured to be(4225.3±2.3±21.5)MeV and(72.9±6.1±30.8)MeV,respectively.They are consistent with those of the established Y(4230).The second structure is observed for the first time with a statistical significance greater than 8σ,denoted as Y(4500).Its mass and width are determined to be(4484.7±13.3±24.1)MeV and(111.1±30.1±15.2)MeV,respectively.The first presented uncertainties are statistical and the second ones are systematic.The product of the electronic partial width with the decay branching fractionΓ(Y(4230)→e^(+)e^(−))B(Y(4230)→K^(+)K^(−)J/Ψ)is reported.