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1.
We have performed a dynamical calculation of the bound state problem of D~0(D)~(*0) by considering the pion and sigma meson exchange potential.Our preliminary analysis disfavors the molecular interpretation of X(3872) if we use the experimental D~* Dπ coupling constant g=0.59 and a reasonable cutoff around 1 GeV,which is the typical hadronic scale.In contrast,there probably exists a loosely bound S-wave B (-B)~* molecular state.Such a molecular state would be rather stable since its dominant decay mode is the radiative decay through B~*→Bγ.  相似文献   

2.
Inspired by the newly observed state X~*(3860), we analyze the strong decay behaviors of some charmoniumlike states, X~*(3860), X(3872), X(3915), X(3930) and X(3940), with the ~3P_0 model. We carry out our work based on the hypothesis that all of these states are charmonium systems. Our analysis indicates that, as a 0~(++) charmonium state, X~*(3860) can reproduce the experimental data. As for X(3872), it can tentatively be interpreted as the mixture0 of a cc system and a D~*D~0 molecular state. If we consider X(3940) as a 3~1 S_0 state, its total width in the present work is much lower than the experimental result. Thus, the 3~1 S_0 charmonium state seems not to be a good candidate for X(3940). Furthermore, our analysis implies that it is reasonable to assign X(3915) and X(3930) to be the same state, 2~(++). However, combining our analysis with that in Refs.[14, 71], we speculate that X(3915)/X(3930) might also be the mixture of a cc system and a molecular state.  相似文献   

3.
We have studied Z~+ (4430)as a D~* D_1 molecule from the quark model,state mixing effect is considered by solving the coupled channel Schr(o)dinger equation numerically.More precise measurements of Z~+ (4430)mass and width,partial wave analysis are helpful to understand its structure.If it lies below the D~* D_1 threshold,molecule interpretation with J~P=1~- is favored,and JP =0~- can not be ruled out.Otherwise Z~+ (4430)may be a virtual state with J~P=2~-.The analogous heavy flavor mesons Z~+_(bb) and Z~(++)_(bc) are considered as well,and the masses predicted in our model are in agreement with the predictions from the potential model and QCD sum rule.  相似文献   

4.
张晓燕  王景峰 《发光学报》2005,26(3):299-303
势阱中的类氢杂质的能级问题一直为学术界所长期关注。讨论了异质界面上中性施主D0和负施主离子D-的能量随垂直于界面的磁场的变化情况,同时将磁场和势阱结合起来考虑其对类氢杂质的影响。研究发现随磁场的增大,其对D0基态能的影响越来越大,对其束缚能的影响逐渐变小,而对D-中心,磁场的作用使得D-由非束缚态转变为束缚态。计算中分别选取了两种不同的波函数,分析了这两种波函数的适用范围,利用变分的方法得到此结构中D0中心的基态能量和束缚能与D-中心角动量L=-1自旋三重态的本征能量和束缚能随磁场的变化关系,找到了此三重态由非束缚态转变到束缚态对应磁场的阈值。  相似文献   

5.
The D* D_1(2420) and DD '*(2600) interactions are studied in a one-boson-exchange model. Isovector bound state solutions with spin parity J~P= 1~+are found from the D* D_1(2420) interaction, which may be related to the observed charged charmonium-like state Z(4430). There is no bound state solution found from the DD '*(2600)interaction.  相似文献   

6.
We report our recent work on a hadronic molecule state of the K(K)N system with I=1/2 and J~P=1/2~+. We assume that the A(1405) resonance and the scalar mesons, f_0(980), a_0(980), are reproduced as quasi-bound states of (K)N and K(K), respectively. Performing non-relativistic three-body calculations with a variational method for this system, we find a quasibound state of the K(K)N system around 1910 MeV below the three-body breakup threshold. This state corresponds to a new baryon resonance of N~* with J~P = 1/2~+. We find also that this resonance has the cluster structure of the two-body bound states keeping their properties as in the isolated two-particle systems. We also briefly discuss another hadronic molecular state composed by two (K) and one (N), which corresponds to a Ξ~* resonance.  相似文献   

7.
We study the branching ratios of D+→D0e+ν,DS+→D0e+ν,BS0→B+e-ν,DS+→D+e-e+ and BS0→B0e-e+ rare semileptonic decay processes,which are induced by decays of light quarks,the heavy quarks remain unchanged.The branching ratios of these decay processes are estimated in the heavy quark limit and with SU(3) flavor symmetry.We find that the decay rates are very tiny in the framework of the Standard Model.We also estimate the sensitivities of the measurements of these rare decays at the future experiments,such as BES-Ⅲ,super-B and LHC-b.Observations of these decays may shed some light on new physics beyond the standard model.  相似文献   

8.
分别采用B3LYP/6-31G(d)和CIS/6-31G(d)方法对咪唑[4, 5-f] 1, 10-邻菲罗啉(ip)及其8种2-取代芳基衍生物的基态(S0)和单重激发态(S1)的几何构型进行了全优化, 并采用含时的度泛函理论(TD-DFT)计算了上述化合物的电子吸收和电子发射光谱. 分析了取代基对咪唑[4, 5-f] 1, 10-邻菲罗啉的电子结构、前线分子轨道、电离势Ip、电子亲和势EA及电子光谱的影响. 计算结果表明, 取代基使8种取代衍生物前线分子轨道(LUMO-HOMO)能隙降低,导致其最大吸收和发射波长均发生了红移. 化合物1~8的跃迁类型均为分子内电荷转移(ICT)跃迁,且1~4和5~8的电子转移方向刚好相反. 溶剂对其电子光谱也有影响, 振子强度增大, 最大发射波长红移. 另外, 8种取代衍生物的电离势降低, 电子亲和势增大, 化合物1~4易于空穴的注入, 5~8易于电子的注入.  相似文献   

9.
分别采用B3LYP/6-31G(d)和CIS/6-31G(d)方法对咪唑[4, 5-f] 1, 10-邻菲罗啉(ip)及其8种2-取代芳基衍生物的基态(S0)和单重激发态(S1)的几何构型进行了全优化, 并采用含时的度泛函理论(TD-DFT)计算了上述化合物的电子吸收和电子发射光谱. 分析了取代基对咪唑[4, 5-f] 1, 10-邻菲罗啉的电子结构、前线分子轨道、电离势Ip、电子亲和势EA及电子光谱的影响. 计算结果表明, 取代基使8种取代衍生物前线分子轨道(LUMO-HOMO)能隙降低,导致其最大吸收和发射波长均发生了红移. 化合物1~8的跃迁类型均为分子内电荷转移(ICT)跃迁,且1~4和5~8的电子转移方向刚好相反. 溶剂对其电子光谱也有影响, 振子强度增大, 最大发射波长红移. 另外, 8种取代衍生物的电离势降低, 电子亲和势增大, 化合物1~4易于空穴的注入, 5~8易于电子的注入.  相似文献   

10.
应用偏振红外、拉曼光谱研究了一种反铁电液晶化合物在78℃时,SCA 相中的烷基链、刚性核部分的构象、分子排布。用二维相关技术对所得到的偏振红外、拉曼光谱进行分析,把与手性碳相连的甲基的反对称及对称伸缩振动谱带同烷基链中的甲基伸缩振动谱带区分开,并发现在反铁电相中同时存在s-cis和s-trans两种构象。  相似文献   

11.
The exclusive Born cross sections of the production of D~0, D~+ and D_s~+ smesons in e~+e~- annihilation at 13 energy points between 3.970 and 4.260 Ge V are obtained by applying corrections for initial state radiation and vacuum polarization to the observed cross sections measured by the CLEO-c experiment. Both the statistical and the systematic uncertainties for the obtained Born cross sections are estimated.  相似文献   

12.
Very recently the LHCb collaboration reported their observation of the first two fully open-flavor tetraquark states,the X0(2900) of JP=0+ and the X1(2900) of JP=1-.We study their possible interpretations using the method of QCD sum rules,paying special attention to an interesting feature of this experiment that the higher resonance X1(2900) has a width significantly larger than the lower one X0(2900).Our res...  相似文献   

13.
合成并表征了以2-苯基吡啶为第一配体,水杨酸及其衍生物为第二配体,以铱为内核的新型配合物(ppy)2Ir(LX)(ppy=2-苯基吡啶,LX=水杨酸Sal、4甲基水杨酸MSal、4-三氟甲基水杨酸FSal)。对其分子结构、光物理性能及热稳定性进行了测试和分析。结果表明, 室温下在二氯甲烷溶液中(ppy)2Ir(LX)(LX= Sal, MSal, FSal)的吸收峰分别在270, 370, 450及484 nm附近,其中前2个吸收峰应归属于第一配体2-苯基吡啶的1π—π*跃迁和水杨酸配体到2-苯基吡啶的电荷转移跃迁,在450及484 nm附近的吸收峰,应该归属于金属到配体的电荷转移(1MLCT和3MLCT)跃迁和配体3π—π*跃迁的混合;其PL发射峰最大波长分别为520,522,510 nm;(ppy)2Ir(Sal)和(ppy)2Ir(MSal)的发射主要来源于三重态3MLCT的辐射跃迁,而(ppy)2Ir(FSal)的发射主要来源于水杨酸到2-苯基吡啶的电荷转移态的辐射跃迁,也有单重态1MLCT和三重态3MLCT的辐射跃迁的贡献。其量子效率分别为0.37,0.33,0.29,热分解温度为306~328 ℃。(ppy)2Ir(LX)是一组热稳定性较好的高效有机磷光材料,可用于有机电致发光器件中。  相似文献   

14.
运用密度泛函理论(DFT)方法,研究了异构体C60O[6,6]与C60O[5,6]之间的重排反应机理。结果显示: 它们之间的反应路径是经过一个过渡态没有中间体的一步反应。C60O[6,6] 转化成C60O[5,6]的反应能垒是42.7 kcal*mol-1,在反方向,C60O[5,6]转化成C60O[6,6]的反应能垒是47.3 kcal*mol-1,同时,扫描出氧原子在富勒烯C60(Ih)表面的势能面(PEC),以详细显示异构体C60O[6,6]与C60O[5,6]之间的重排反应机理。  相似文献   

15.
Using the data accumulated in 2002-2004 with the D0 detector in proton-antiproton collisions at the Fermilab Tevatron collider with a center-of-mass energy of 1.96 TeV, the branching fractions of the decays B --> D0(1)(2420)mu+ vmuX and B --> D2(*0)(2460)mu+ vmuX and their ratio have been measured: B(b --> B) x B(B --> D0(1)mu+ vmuX) x B(D0(*0) --> D*- pi+) = [0.087 +/- 0.007(stat) +/- 0.014(syst)]%; B(b --> B) x B(B --> D2(*0) mu+ vmuX) x B(D2(*0) --> D*- pi+) = [0.035 +/- 0.007(stat) +/- 0.008(syst)]% and [B(B --> D2(*0)mu+ vmuX) x B(D2(*0) --> D*- pi+)]/[B(B --> D0(1)mu+ vmuX) x B(D0(1) --> D*- pi+)] = 0.39 +/- 0.09(stat) +/- 0.12 (syst), where the charge conjugated states are always implied.  相似文献   

16.
运用密度泛函理论(DFT)方法,研究了异构体C60O[6,6]与C60O[5,6]之间的重排反应机理。结果显示: 它们之间的反应路径是经过一个过渡态没有中间体的一步反应。C60O[6,6] 转化成C60O[5,6]的反应能垒是42.7 kcal*mol-1,在反方向,C60O[5,6]转化成C60O[6,6]的反应能垒是47.3 kcal*mol-1,同时,扫描出氧原子在富勒烯C60(Ih)表面的势能面(PEC),以详细显示异构体C60O[6,6]与C60O[5,6]之间的重排反应机理。  相似文献   

17.
Two special dynamical transitions of universal character have recently been observed in macromolecules (lysozyme, myoglobin, bacteriorhodopsin, DNA and RNA) at T* ~100-150 K and T(D) ~180-220 K. The underlying mechanisms governing these transitions have been the subject of debate. In the present work, a survey is reported on the temperature dependence of structural, vibrational and thermodynamical properties of a nearly anhydrous amino acid (orthorhombic polymorph of the amino acid l-cysteine at a hydration level of 3.5%). The temperature dependence of x-ray powder diffraction patterns, Raman spectra and specific heat revealed these two transitions at T* = 70 K and T(D) = 230 K for this sample. The data were analyzed considering amino acid-amino acid, amino acid-water, water-water phonon-phonon interactions and molecular rotor activation. Our results indicated that the two referred temperatures define the triggering of very simple and particular events that govern all the interactions of the biomolecular: activation of CH(2) rigid rotors (T < T* ), phonon-phonon interactions between specific amino acid and water dimer vibrational modes (T* < T < T(D)), and water rotational barriers surpassing (T > T(D)).  相似文献   

18.
金毅  李世渊  谢去病 《中国物理 C》2003,27(10):852-856
研究了e+e-湮没中"初始"轻夸克和胶子劈裂产生的组合为介子(包括D-, D-s, 0)或*介子(包括D*-, D*-s, *0)的过程.发现尤其在s=MZ处,其产额相对较大,当限制或*的能量大于20GeV时,它和c夸克碎裂产物的不变质量谱在稍大于2M附近有一个峰,这是该过程区别于其它或*介子产生过程的显著特征.此过程产生的矢量介子基本上是纵向极化的,与实验上观测到的*介子的纵向极化一致.  相似文献   

19.
We report a study of the processes e+e- -->J/psiD*D[over](*). In J/psiD*D[over]* we observe a significant enhancement in the D*D[over]* invariant mass spectrum, which we interpret as a new charmoniumlike state and denote X(4160). The X(4160) parameters are M=(4156(-20)+25+/-15) MeV/c2 and Gamma=(139(-61)+111+/-21) MeV. We also report a new measurement of the X(3940) mass and width: M=(3942(-6)+7+/-6) MeV/c2 and Gamma=(37(-15)+26+/-8) MeV. The analysis is based on a 693 fb(-1) data sample recorded near the Upsilon(4S) resonance by the Belle detector at the KEKB asymmetric-energy collider.  相似文献   

20.
We present an improved calculation of the strong coupling constants g_(D~*Dp) and g_(B~*Bp) in light-cone sum rules, including one-loop QCD corrections of leading power with meson distribution amplitudes. We further compute subleading-power corrections from two-particle and three-particle higher-twist contributions at leading order up to twist-4 accuracy. The next-to-leading order corrections to the leading power contribution numerically offset the subleading-power corrections to a certain extent, and our numerical results are consistent with those of previous studies on sum rules. A comparison between our results and existing model-dependent estimations is also made.  相似文献   

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