首页 | 本学科首页   官方微博 | 高级检索  
相似文献
 共查询到19条相似文献,搜索用时 156 毫秒
1.
彩色电视荧光级氧化钇中稀土杂质的ICP—AES测定   总被引:1,自引:0,他引:1  
本文采用国产WP-2L型平面光栅摄谱仪配置国产GP3.5D型ICP光源进行了彩色电视荧光级氧化钇中14个稀土杂质元素分析方法的研究。样品溶液以不去溶方式引入ICP。当样品溶液中Y2O3的浓度为20mg/ml时,测定了限分别为铕,镱和镥0.00020%,镧,铈,钕,钆,镝,钬,铒和铥0.00050%,镨,钐和铽0.0010%。相对标准偏差为3.2-9.8%。  相似文献   

2.
采用5-Br-PADAP-OP显色体系测定铜,考查了测定条件。以正三辛胺萃取分离干扰高子,考查了萃取分离条中。人工合成样品回收率100.8%,铝合金标样测定误差<-2.2%,人发分析结果的相对标准偏差<4.0%。  相似文献   

3.
在pH5~6的缓冲溶液中,铜与对二甲氨基苄基罗丹宁反应生成红色络合物。本文应用β-修正双波长光度法测定铜,可消除过量显色剂PDR产生的影响,明显的提高了测定的灵敏度。实验结果表明:RSD<2.9%,加标回收率87.7%~112.0%,最低检测限0.55μg/mL。本法适合于金属材料、环境水体中痕量铜的测定。  相似文献   

4.
分光光度法测定生药中微量元素锌   总被引:3,自引:0,他引:3  
采用湿法消解样品,用0.1%PAN「1-2(-吡啶偶氮)2-萘酚」-20%OP(聚乙二醇辛基苯基醚)显色分光光度法测定10种生药中微量元素锌。  相似文献   

5.
本文提出了用ICP-AES法测定马口铁中的痕量铅。试样用NaOH-H2O2溶解镀层。测得四种样品的含铅量在0.14~0.38μg/cm2范围内。方法的回收率为96.1%~103.2%。方法的精密度(RSD)为2.6%~3.8%。本法简便迅速,测量结果的准确度、精密度满足分析要求。  相似文献   

6.
本文采用国产WP-2L型平面光栅摄谱仪配置国产GP3.5D型ICP光源进行了彩色电视荧光级氧化钇中14个稀土杂质元素分析方法的研究。样品溶液以不去溶方式引入ICP。当样品溶液中Y2O3的浓度为20mg/ml时,测定下限分别为铕、镱和0.00020%,镧、铈、钛、钆、镝、钬、铒和铥0.00050%,镨、钐和铽0.0010%。相对标准偏差为3.2~9.8%。  相似文献   

7.
采用多波长K系数法可同时测定克感敏片中非那西丁,氨基比林和咖啡因的含量,结果准确,方法快速。其平均回收率和相对标准偏差分别为99.91%,0.41%,100.1%,0.29%;100.1%,0.56%。  相似文献   

8.
为研制百焦耳级KrF激光放大器,发展MOPA系统,我们用自探测法在百焦耳级电子束泵浦KrF激光装置上进行了激光放大器的增益与吸收的测量。泵浦率约为0.67MW/cm ̄2,激光介质为89.6%Ar:10%Kr:0.4%F_2的混合气体,总气压0.25MPa,实验测得激光放大器的小信号增益系数g_0=6.6%cm ̄(-1)、非饱和吸收系数α_n=0.93%cm ̄(-1)、饱和光强I_s=2.5MW/cm ̄2。  相似文献   

9.
为研制百焦耳级KrF激光放大器,发展MOPA系统,我们用自探测法在百焦耳级电子束泵浦KrF激光装置上进行了激光放大器的增益与吸收的测量。泵浦率约为0.67MW/cm ̄2,激光介质为89.6%Ar:10%Kr:0.4%F_2的混合气体,总气压0.25MPa,实验测得激光放大器的小信号增益系数g_0=6.6%cm ̄(-1)、非饱和吸收系数α_n=0.93%cm ̄(-1)、饱和光强I_s=2.5MW/cm ̄2。  相似文献   

10.
ICP-AES法测定铝锂合金中Li、Mg、Fe、Cu、Si、Zr的研究   总被引:1,自引:0,他引:1  
李莉  潘傥  徐普德 《光谱实验室》1999,16(4):434-438
本文研究了采用ICP-AES技术同时测定铝锂合金中Li、Mg、Fe、Cu、Si、Zr等六元素的分析方法,优化了工作条件,经对合成样品和实际样品测量,对Li(1%-4%)、Mg(0.5%-6%)、Fe(0.05%-2.5%)、Cu(0.5%-5%)、Si(0.05%-0.5%)、Zr(0.05%-0.5%),方法的相对标准偏差均小于5%,回收率为93%-105%。方法对照结果亦表明,本方法简便、快速、准确  相似文献   

11.
The goals of this study were to evaluate 31P MR spectroscopic imaging (MRSI) for clinical studies and to survey potentially significant spatial variations of 31P metabolite signals in normal and pathological human brains. In normal brains, chemical shifts and metabolite ratios corrected for saturation were similar to previous studies using single-volume localization techniques (n = 10; pH = 7.01 +/- 0.02; PCr/Pi = 2.0 +/- 0.4; PCr/ATP = 1.4 +/- 0.2; ATP/Pi = 1.6 +/- 0.2; PCr/PDE = 0.52 +/- 0.06; PCr/PME = 1.3 +/- 0.2; [Mg2+]free = 0.26 +/- 0.02 mM.) In 17 pathological case studies, ratios of 31P metabolite signals between the pathological regions and normal-appearing (usually homologous contralateral) regions were obtained. First, in subacute and chronic infarctions (n = 9) decreased Pi (65 +/- 12%), PCr (38 +/- 6%), ATP (55 +/- 6%), PDE (47 +/- 9%), and total 31P metabolite signals (50 +/- 8%) were observed. Second, regions of decreased total 31P metabolite signals were observed in normal pressure hydrocephalus (NPH, n = 2), glioblastoma (n = 2), temporal lobe epilepsy (n = 2), and transient ischemic attacks (TIAs, n = 2). Third, alkalosis was detected in the NPH periventricular tissue, glioblastoma, epilepsy ipsilateral ictal foci, and chronic infarction regions; acidosis was detected in subacute infarction regions. Fourth, in TIAs with no MRI-detected infarction, regions consistent with transient neurological deficits were detected with decreased Pi, ATP, and total 31P metabolite signals. These results demonstrate an advantage of 31P MRSI over single-volume 31P MRS techniques in that metabolite information is derived simultaneously from multiple regions of brain, including those outside the primary pathological region of interest. These preliminary findings also suggest that abnormal metabolite distributions may be detected in regions that appear normal on MR images.  相似文献   

12.
Forbidden transitions from levels with 3P and 1D cores in excited configurations of Cl-like Mn IX and Fe X have been isolated using interference filters. The fluorescence decay lifetimes of ions orbiting in a Kingdon ion trap were measured. New relativistic configuration interaction calculations of relevant level lifetimes, to aid the analysis, based on B-spline basis sets, are also presented. Line identifications and experimental lifetimes are Mn IX ((4)D(7/2)-(4)F(9/2)):363(-3/+7) nm; tau(Mn IX3p(4)(3P)3d (4)F(9/2)) = 210+/-42 ms; tau(Fe X,3p(4)(3P)3d (4)F(9/2)) = 85.7+/-9.2 ms; tau(Fe X,3p(4)(3P)3d (4)F(7/2)) = 93+/-30 ms; and tau(Fe X, 3p(4)(1D)3d (2)G(9/2)) = 17.8+/-3.1 ms.  相似文献   

13.
We use the non-relativistic constituent quark model and the bag model to study the stability of the dilambda H = (uuddss) and pentaquark states . While they are stable in the limit of exact SU(3)F flavour symmetry between u, d, and s quarks, the H and the P become unbound when a realistic breaking of SU(3)F is introduced.  相似文献   

14.
It is proved that the definitions of the norm given by Berggren and Romo are identical. Regularization in ref. 1) with any convergence factor of the form leads to the same result. The existence of the norm is also established for the proton. The norm for neutrons is analytically given.  相似文献   

15.
We show that the generalized holonomy groups of ungauged supergravity theories with 8 real supercharges must be contained in , where is the generalized structure group. Here n=4ν is the number of preserved supersymmetries, so the allowed values are limited to n=0,4,8. In particular, solutions of ungauged supergravities in four, five and six dimensions are examined and found to explicitly follow this pattern. We also argue that the G-structure has to be a subgroup of this generalized holonomy group, which may provide a possible classification for supergravity vacua with respect to the number of supercharges.  相似文献   

16.
系统研究了核磁共振碳谱与化学位移和规律 ,以及分子拓扑指数在定量 [结 ]构 [波 ]谱关系 (QSSR)中的应用 .本文基于矢量路径长度矢量 p =(P1,P2 ,P3 ,… ,Pm)与分子中原子相互作用 ,提出了一种新型分子距边矢量并发现它与烷烃13 CNMR化学位移和有良好线性相关性 ,回归方程及其统计参数为 :CSS =bν +p3 =Σmj=0 bjνj+b10 p3 =b0 ν +b1ν1+b2 ν2 +b3 ν3 +b4 ν4 +b5ν5+b6ν6+b7ν7+b8ν8+b9ν9ν +b10 P3 =- 13.6 0 11+2 2 .2 133ν1+2 8.412 1ν2 +2 5 .9416ν3 +2 6 .6 70 9ν4 +14.4976ν5+5 .72 40ν6- 5 .3830ν7- 3.2 15 2ν8- 15 .0 2 13ν9- 2 5 .70 99ν10 +12 .2 786P3 (n =6 3,R =0 .9970 ,EV =99 .6 8% ,RMS =3.734 8,F =2 418.2 ;交互校验CV为 :R =0 .9893,EV =98.83% ,RMS =7.12 6 1,F =6 6 4.0 46 ) ;结果良好 .  相似文献   

17.
The recoil proton polarization has been measured in the p(e-->,e'p-->)pi(0) reaction in parallel kinematics around W = 1232 MeV, Q2 = 0.121 (GeV/c)2, and epsilon = 0.718 using the polarized cw electron beam of the Mainz Microtron. All three proton polarization components, Px/P(e) = (-11.4+/-1.3+/-1.4)%, P(y) = (-43.1+/-1.3+/-2.2)%, and P(z)/P(e) = (56.2+/-1.5+/-2.6)%, could be measured simultaneously. The Coulomb quadrupole to magnetic dipole ratio, CMR = (-6.4+/-0.7(stat)+/-0.8(syst))%, was determined from Px in the framework of the Mainz Unitary Isobar Model. The consistency among the reduced polarizations and the extraction of the ratio of longitudinal-to-transverse response is discussed.  相似文献   

18.
Very light photinos, if they exist, should be produced in a SN explosion. Using the data from SN 1987A we set limits on the masses of selectrons (and squarks), the SUSY particles involved in the production (and diffusion) of photinos in the stellar medium. The bounds obtained are , where .  相似文献   

19.
The branching ratios are evaluated of the ψ (3770) and (4S) decays into ππ, , ωπ0, ωη, ωη ′, π, η, η′, , . They arise due to the transition through the real intermediate states and , respectively. It is shown that some branching ratios exceed the three-gluon one by an order of magnitude. The rates of the decays , and are evaluated also. τ-C and B factories coul be good tools for studying all decays mentioned.  相似文献   

设为首页 | 免责声明 | 关于勤云 | 加入收藏

Copyright©北京勤云科技发展有限公司  京ICP备09084417号