共查询到20条相似文献,搜索用时 296 毫秒
1.
2.
利用高斯分布拟合HT-6M托卡马克Hα线型,得出了由反射进入等离子体中的氢原子、氢分子离解后产生的氢原子,以及电荷交换产生的氢原子辐射Hα谱线的份额,由Doppler频移和展宽分别得出它们的入射速度和离子温度.在简化模型下讨论了氢原子的输运行为,得出了氢原子的密度分布和体发射系数,以及入射速度大小对粒子约束时间的影响,并与实验数据进行比较.由中性氢原子能量分布得出发生在边界的分子过程是氢分子的离解激发和电离离解
关键词: 相似文献
3.
4.
简述了若干转动谱理论及其对超形变带的应用 ,并用 Bohr- Mottelson的 I(I+1 )展开公式分析了 A=1 90区超形变带的性质和指定了它们的能级自旋 ,用 Harris的ω2 展开公式 J(1) =2α+(4/3 )βω2 +(6 /5 )γω4分析了 A=1 5 0区 Tb和 Dy同位素 2 0条超形变带的性质 ,指定了它们的能级自旋 .对于首次发现的152 Dy(1 )超形变带 ,带首自旋指定为 2 6 h,与实验结果更加符合. The recent developments of rotational spectral theories and its application to superdeformed bands were briefly reviewed. The superdeformed bands in A ≈190 region were analyzed and the spins of energy level were determined by the least square fitting experimental transition energy with the formula of Bohr Mottelson’s I(I+1) expansions. The superdeformed bands in A ≈150 region were analyzed by using the kinematic moments of inertia formula J (1) =2α+(4/3)βω 2+(6/5)γω 4 in... 相似文献
5.
在超重核区(Z≥104)使用文献[7—9]给出的3组参数应用Viola-Seaborg公式计算了α衰变寿命,所得结果与实验值进行比较,发现其结果与实验值相差较大。为此,利用最小二乘法分别在重核区和超重核区重新对参数进行了拟合,得到的计算结果与实验值相比符合得较理想,尤其是由超重核得到的参数的结果非常理想。 相似文献
6.
7.
用傅立叶变换光谱仪和激光腔内吸收光谱仪记录了H2 SiCl2 分子 2 0 0 0~ 90 0 0和 12 0 0 0~ 12 90 0cm-1的红外吸收光谱 .依据局域模理论的非谐性耦合非谐振子 (ACAO)模型 ,分析并拟合了Si-H的对称伸缩振动和反对称伸缩振动 ,得到描述Si-H伸缩振动的Morse离解能De、Morse振子参数α和键振子势能耦合系数frr′.分析中忽略了SiCl2 “基座”对Si-H伸缩振动的影响 ,拟合结果与实验值符合的很好 ,拟合方差小于 1cm-1,表明这一近似是可取的 .分析拟合结果表明 ,Si-H振动时“基座”SiCl2 的有效质量为 75 . 相似文献
8.
通过构造一个转折点值α可变的三分段线性奇函数,研究一种新型混沌产生器.这种混沌产生器的主要特征是,随着转折点值α在0<α≤1范围内变化时,系统从倍周期分岔进 入混沌状态,可产生双层单螺旋、单层单螺旋、双层双螺旋和单层双螺旋四种不同类型的混沌吸引子,其中双层单螺旋和双层双螺旋为本电路实验中所发现的两类新型混沌吸引子.分析了这种混沌产 生器随α值在0<α≤1范围内变化时的分岔图、李雅普诺夫指数谱、最大李雅普诺夫指 数λ_max以及单层双螺旋和双层双螺旋的功率谱.在此基础上设计硬件电路,进行了计算机模拟和电路实
关键词:
混沌产生器
双层双螺旋
双层单螺旋
电路实验 相似文献
9.
10.
真空下气-固界面热适应系数的数值计算 总被引:2,自引:0,他引:2
根据热适应系数的理论研究成果,结合国外学者的部分实验数据,对气-固界面热适应系数的主要影响因素进行定性的讨论;同时在S.Song和M.M.Yovannovich的公式基础上,最小二乘法拟合国外学者低温下实验测量的热适应系数,采用C语言编程算出拟合公式中的参数,分析拟合公式α=aFM/(b+M)+2.4μ(1-F)/(1+μ)2,F=exp(c(T-T0)/T0)中的参数a,b,c的特性;数值计算迭代收敛和拟合公式的计算误差在±20%以内表明:数值拟合公式可用在工程上计算热适应系数,S.Song和M.M.Yovannovich的公式可数值拟合低温下不同气-固界面的热适应系数的计算公式。 相似文献
11.
We study the CP-averaged branching fractions and the CP-violating asymmetries in the pure annihilation decays ofB _s~0→a_0~+a _0~-andB _d~0→K_0~(*+)K_0~(*-),where a_0[K_0~*]denotes the scalar a_0(980) and a_0(1450)[K_0~*(800)(ork)and K_0~*(1430)],with the perturbative QCD factorization approach under the assumption of two-quark structure for the a_0and K_0~*states.The numerical results show that the branching ratios of theB _d~0→K_0~(*+)K_0~(*-)decays are in the order of 10~(-6),while the decay rates of theB_s~0→a_0~+a _0~-modes are in the order of 10~(-5).In light of the measured modes with the same quark components in the pseudoscalar sector,namely,B _d~0→K~+K~-and B_s~0→p p~(+-),the predictions for the considered decay modes in this work are expected to be measured at the Large Hadron Collider beauty and/or Belle-Ⅱ experiments in the (near) future.Meanwhile,it is of great interest to find that the twist-3 distribution amplitudes φ~S and φ~T with inclusion of the Gegenbauer polynomials for the scalar a_0(1450) and K_0~*(1430)states in scenario2 contribute slightly to the branching ratios while significantly to the CP violations in the B_d~0→K_0~*(14 30)~+K_0*(14 30)~-and B_s~0→a_0(1450)~+a_0(1450)~-decays,which indicates that,compared to the asymptotic φ~Sand φ~T,these Gegenbauer polynomials could change the strong phases evidently in these pure annihilation decay channels.These predictions await for the future confirmation experimentally,which could further provide useful information to help explore the inner structure of the scalars and shed light on the annihilation decay mechanism. 相似文献
12.
Measurement of the heavy neutral MSSM Higgs bosons H and A production in the process γγ → A/H → b
at the Photon Linear Collider [1,2] has been considered in two independent analyses for the parameter range corresponding
to the so-called ‘LHC wedge’. Significantly different conclusions were obtained; signal-to-background ratio 36 vs. 2. Here
assumptions and results of these two analyses are compared. We have found that differences in the final results are mainly
due to different assumptions on γγ-luminosity spectra, jet definitions and selection cuts.
相似文献
13.
Level structure and electromagnetic transitions in ~(98)Mo have been investigated on the basis of the proton-neutron interacting boson model(IBM-2) by considering the energy difference between neutron boson ε_ν and proton boson ε_π. The results are compared with the recent experimental data and it is observed that they are in good agreement. In particular, the strongest M1 transition from 2_5~+ state to 2_2~+ can be well reproduced, from which one can determine the 2_5~+ as an mixed-symmetry(MS) state. We have calculated the electric monopole strength ρ~2(E0,0_2~+→0_1~+), and our result agrees with the experimental one. The calculation indicates that shape coexistence and MS states are simultaneously well described using IBM-2. 相似文献
14.
The mixedness of the N-qubit quantum states with exchange symmetry has been studied, and the results show that the linear entropy of the single qubit reduced density matrix (RDM), which can describe the mixedness, is completely determined by the expectation values 〈Sz〉 and 〈S±〉 for both the pure and the mixed states. The mixedness of the pure states can be used to describe the bipartite entanglement, as an example we have calculated the mixedness of the Dicke state and the spin squeezed Kitagawa-Ueda state. For the mixed states, we determine the mixedness properties of both the ground states and the thermal states in mean-field clusters of spin-1/2 particles interacting via the anisotropy Heisenberg XXZ interaction, and found for the ferromagnetic case (J 〈 0), the mixedness will approximate to the pairwise entanglement when the anisotropic parameter △ 〉 △c. 相似文献
15.
Chun Liu 《The European Physical Journal C - Particles and Fields》2008,53(3):413-419
From the large- QCD point of view, baryonia, tetraquark states, hybrids, and glueballs are studied. The existence of these states is argued
for. They are constructed from baryons. In large- QCD, a baryonium is always identical to a glueball with valence gluons. The ground state glueball has a mass of about 2450 MeV. is identified as the lowest glueball. The lowest four-quark nonet should be , , and . Combining with the heavy quark effective theory, spectra of heavy baryonia and heavy tetraquark states are predicted. corrections are discussed.
PACS 12.39.Mk; 14.20.-c; 12.38.Lg 相似文献
16.
In this article, we assume that there exist the pseudoscalar $D\bar{D}_{s0}^*(2317)$ and $D^*\bar{D}_{s1}^*(2460)$ molecular states $Z_{1,2}$ and construct the color singlet-singlet molecule-type interpolating currents to study their masses with the QCD sum rules. In calculations, we consider the contributions of the vacuum condensates up to dimension-10 and use the formula $\mu=\sqrt{M_{X/Y/Z}^{2}-(2{\mathbb{M}}_{c})^{2}}$ to determine the energy scales of the QCD spectral densities. The numerical results, $M_{Z_1}=4.61_{-0.08}^{+0.11}\,\text{GeV}$ and $M_{Z_2}=4.60_{-0.06}^{+0.07}\,\text{GeV}$, which lie above the $D\bar{D}_{s0}^*(2317)$ and $D^*\bar{D}_{s1}^*(2460)$ thresholds respectively, indicate that the $D\bar{D}_{s0}^*(2317)$ and $D^*\bar{D}_{s1}^*(2460)$ are difficult to form bound state molecular states, the $Z_{1,2}$ are probably resonance states. 相似文献
17.
Todd A. Oliynyk 《Communications in Mathematical Physics》2009,288(3):847-886
We prove the existence of a large class of dynamical solutions to the Einstein-Euler equations that have a first post-Newtonian
expansion. The results here are based on the elliptic-hyperbolic formulation of the Einstein-Euler equations used in [15],
which contains a singular parameter , where v
T
is a characteristic velocity associated with the fluid and c is the speed of light. As in [15], energy estimates on weighted Sobolev spaces are used to analyze the behavior of solutions
to the Einstein-Euler equations in the limit , and to demonstrate the validity of the first post-Newtonian expansion as an approximation. 相似文献
18.
本文采用多组态相互作用及Davidson修正方法和全电子基组计算了SH~-阴离子的X~1∑~+,a~3∏和A~1∏态的势能曲线、电偶极矩和跃迁偶极矩.计算的光谱常数与实验值及已有的理论值符合得很好.在计算中考虑了自旋-轨道耦合效应.计算得到a~3∏_1(v'=0)?X~1∑_(0+)~+(v"=0)和A~1∏_1(v'=0)?X~1Σ_(0+)~+(v"=0)跃迁具有高对角分布的弗兰克-康登因子,分别为0.9990和0.9999;计算得到a~3∏_1和A~1∏_1态的自发辐射寿命分别为1.472和0.188 ms.A~1∏_1?X~1∑_(0+)~+跃迁存在中间态a~3∏_(0+)和a~3∏_1,但中间态对激光冷却SH~-阴离子的影响可以忽略.分别利用a~3∏_1(v'=0)? X~1∑_(0+)~+(v"=0)和A~1∏_1(v'=0)? X~1∑_(0+)~+(v"=0)跃迁构建了准闭合的能级系统,冷却所需的激光波长分别为492.27和478.57 nm.最后预测了激光冷却SH~-阴离子能达到的多普勒温度和反冲温度.这些结果为进一步实验提供了理论参数. 相似文献
19.
20.
《The European Physical Journal C - Particles and Fields》2008,54(3):345-364
A determination of the single W spin density matrix (SDM) elements in the reaction e+e-→W+W-→lνqq̄(l=e/μ) is reported at centre-of-mass energies between 189 and 209 GeV. The data sample used corresponds to an integrated
luminosity of 520 pb-1 taken by DELPHI between 1998 and 2000.
The single W SDM elements, ρττ’
W± (τ,τ’=± 1 or 0), are determined as a function of the W- production angle with respect to the e- beam direction and are obtained from measurements of the W decay products by the application of suitable projection operators,
Λττ’, which assume the V-A coupling of the W-boson to fermions.
The measured SDM elements are used to obtain the fraction of longitudinally polarised Ws, with the result: at a mean energy of 198 GeV. The SDM elements are also used to determine the triple gauge couplings Δg1
Z,Δκγ,λγ and g4
Z, and . For the CP-violating couplings the results of single parameter fits are:
The errors are a combination of statistical and systematic errors. All results are consistent with the Standard Model. 相似文献