静压下(CdTe)_2(ZnTe)_4-ZnTe多量子阱结构的多声子共振拉曼散射

用加静高压的方法改变光学能隙来实现共振条件。在以(CdTe)_2(ZnTe)_4短周期超晶格为阱层,(ZnTe)_(4)为垒层的多量子阱结构中观察到高达四阶的类 ZnTe 纵光学声子模的多声子共振拉曼散射。通过对拉曼位移随压力变化的分析,发现在与(CdTe)_2(ZnTe)_4短周期超晶格共振时测得的类ZnTe 纵光学声子模的频率比与 ZnTe 势垒层共振时测得的 ZnTe 纵光学声子模的频率低4cm~(-1)。并将它归结为在短周期超品格中纵光学声子模的限制效应。在与短周期超品格严格的2LO 声子出射共振条件下观察到了类 CdTe 的2LO 声子的共振拉曼峰。     

希格斯粒子之理论浅析

被誉为上帝粒子的希格斯玻色子于2012年7月4日在欧洲核子研究中心的大型强子对撞机(LHC)上被发现,这一发现震惊了世界。文章将从理论方面介绍希格斯玻色子,内容包括:(1)世界的基本组分和希格斯玻色子在其中扮演的角色;(2)希格斯玻色子的本质和希格斯机制;(3)希格斯玻色子在LHC上的产生、衰变和发现;(4)希格斯玻色子存在的和谐社会——超对称理论。     

希格斯粒子之理论浅析

被誉为上帝粒子的希格斯玻色子于2012年7月4日在欧洲核子研究中心的大型强子对撞机(LHC)上被发现,这一发现震惊了世界。文章将从理论方面介绍希格斯玻色子,内容包括：(1)世界的基本组分和希格斯玻色子在其中扮演的角色;(2)希格斯玻色子的本质和希格斯机制;(3)希格斯玻色子在LHC上的产生、衰变和发现;(4)希格斯玻色子存在的和谐社会——超对称理论。     

在T2HDM模型中中性希格斯粒子对B→X_s1 1-衰变过程的影响(英文)

在T2HDM模型中计算了中性希格斯粒子圈图对稀有衰变过程B→X_s1 1-的贡献.通过计算发现:(a)中性希格斯粒子对衰变过程B→X_s1 1-的修正能够增强其标准模型的预言,但增幅很小;(b)在中性希格斯玻色子的质量大于100GeV和tanβ<40的情况下,中性希格斯粒子对稀有衰变过程B→X_s1 1-的分支比的贡献可忽略.     

含色散介质的一维光子晶体微腔中简正耦合模的物理图像

对一维光子晶体中的色散介质采用洛伦兹振子模型,对线性层及色散δ层均采用传输矩阵的方法,研究了一维含色散介质的光子晶体微腔中的简正耦合模.通过改变洛伦兹振子和微腔之间的失谐频率,分析了简正耦合模频率的变化情况.在失谐频率比较大时,光与洛仑兹振子间的耦合作用较小,简正耦合模中的一个接近腔模频率,而另一个则接近洛仑兹振子的共振频率;在失谐频率比较小时,光与洛仑兹振子间的耦合作用较大,简正耦合模与未耦合的腔模频率和洛仑兹振子的共振频率之间的差别较为明显.最后通过引进该结构的复有效折射率,对含色散介质的系统,由于带隙中间的共振模被湮灭并分裂为左右两个耦合模,其复有效折射率虚部在原共振峰处跃变为一较大值,而在新生成的两个耦合模附近趋近于零,光与色散介质相互耦合而形成的腔极化激元的物理图像十分清晰.     

HERMES五夸克强子态Θ+实验探索

一个新的强子态的实验证据在2?7.6GeV正电子轰击氘靶产生的虚光子产物中被发现.HERMES通过分析衰变道K0sp→π+π–p,在K0sp不变质量谱上质量1528±2.6(stat.)±2.1(sys.)MeV处观察到共振峰.该共振峰可以被解释为理论预言的五夸克强子态Θ+(uudds).而K+p不变质量谱上未能观察到共振预示Θ+很可能是同位旋单态.     

在T2HDM模型中中性希格斯粒子对B→Xsl+l－衰变过程的影响

在T2HDM模型中计算了中性希格斯粒子圈图对稀有衰变过程B→X_sl⁺l^－的贡献. 通过计算发现: (a)中性希格斯粒子对衰变过程B→X_sl⁺l^－的修正能够增强其标准模型的预言, 但增幅很小; (b)在中性希格斯玻色子的质量大于100GeV和tanβ<40的情况下, 中性希格斯粒子对稀有衰变过程B→X_sl⁺l^－的分支比的贡献可忽略.     

二维光栅角度信号响应函数研究

本文在平行相干光照明条件下,推导出了二维光栅剪切成像系统的角度信号响应函数,并描绘出了角度响应函数二维曲面.虽然光栅剪切成像系统常用的分束光栅有四种,分析光栅有三种,分析光栅和分束光栅之间还存在多种不同组合,但是产生的角度信号响应函数曲面却只有三种,即峰型位移曲面、谷型位移曲面和峰谷对称型位移曲面.其中峰型位移曲面和谷型位移曲面之间具有数值互补关系,由此还可以把峰型位移曲面和谷型位移曲面归纳为一种,最终只需要考虑两种位移曲面.这个理论结果无疑显著简化了人们对二维光栅剪切成像的认识,将对今后讨论定量提取二维角度信号的工作奠定基础.     

粒子模拟中阳极栅网模型的实现

在3维Yee网格和蛙跳模型上建立了一种合理的描述阳极栅网中电子散射过程的物理模型,在经典碰撞理论基础上推导了散射角和动量公式,并运用蒙特卡罗法模拟了高斯分布电子束在径向虚阴极情景下的阳极栅网散射过程。模拟结果出现了明显的虚阴极现象,平均功率0.60 GW,虚阴极效率4.5%,微波主频4.7 GHz,主模是TM01模。这些参数与文献模拟的数据基本符合,证明了虚阴极中阳极栅网数值模拟实现的正确性。     

注入原子相干性对双模MAZER的影响

首先简单介绍超冷原子注入的微脉塞(MAZER)的基本理论和研究进展,然后具体介绍我们目前关于超冷V型三能级原子注入的双模微脉塞(双模MAZER)的研究工作.我们研究了原子相干性对这种双模MAZER系统中原子的发射几率和原子通过腔的透射几率的影响.结果表明,原子的发射几率随腔长变化的曲线中存在共振峰和非共振平台;当两个模的耦合强度之比一定时,不同注入原子相干性对应的发射几率共振峰呈现出相当大的区别.在原子透射几率随原子动量的变化曲线中也存在共振峰和非共振平台.腔长对原子的速度具有选择性,当腔长给定时,通过适当选择原子的相干参量,可调节原子通过腔的透射几率,从而可对原子的速度进行选择.     

Evolution of edge states and critical phenomena in the Rashba superconductor with magnetization

We study Andreev bound states (ABS) and the resulting charge transport of a Rashba superconductor (RSC) where two-dimensional semiconductor (2DSM) heterostructures are sandwiched by spin-singlet s-wave superconductor and ferromagnet insulator. ABS becomes a chiral Majorana edge mode in the topological phase (TP). We clarify two types of quantum criticality about the topological change of ABS near a quantum critical point (QCP), whether or not ABS exists at QCP. In the former type, ABS has an energy gap and does not cross at zero energy in the nontopological phase. These complex properties can be detected by tunneling conductance between normal metal-RSC junctions.     

Spin–orbit effects and superconductivity in oxide materials

In a variety of materials superconductivity is associated with the existence of a quantum critical point (QCP). In the case of the hole doped cuprates there is evidence which suggests that the important quantum degrees of freedom near the superconducting critical point are localized charge and spin density fluctuations. We argue that if these degrees of freedom are strongly coupled by spin–orbit interactions, a new type of quantum criticality arises with monopole-like quasi-particles as the important quantum degrees of freedom. In layered material this type of quantum criticality can be modeled using a 2-dimensional non-linear Schrodinger equation with an SU(N) gauge field. We exhibit a pairing wave function for quasi-particles that has topological order and anisotropic properties. The superconducting transition would in some respects resemble a KT transition.     

Quantum critical scaling in graphene

We show that the emergent relativistic symmetry of electrons in graphene near its quantum critical point (QCP) implies a crucial importance of the Coulomb interaction. We derive scaling laws, valid near the QCP, that dictate the nontrivial magnetic and charge response of interacting graphene. Our analysis yields numerous predictions for how the Coulomb interaction will be manifested in experimental observables such as the diamagnetic response and electronic compressibility.     

Pairing collective modes in superfluid nuclei: a semiclassical approach

Collective pairing excitations in superfluid nuclei are studied by using the semiclassical time-dependent Hartree-Fock-Bogoliubov equations of motion in a linear approximation. It is found that the strength function associated with the semiclassical anomalous density response function has a resonance structure with a sharp peak around double energy gap that displays the monopole pairing collective mode.     

Benchmark study of the SF-MI phase transition of the Bose–Hubbard model with density-induced tunneling

The Bose–Hubbard model (BHM) is a standard model which describes the quantum behavior of ultracold bosons in optical lattice. When tuning the model parameters, a quantum phase transition from superfluid (SF) phase to Mott insulating (MI) phase emerges. However, an extra tunneling process – the density-induced tunneling – is usually ignored in the standard BHM. Using process-chain method, we give a thorough study of the phase diagram of the BHM with density-induced tunneling in different particle density regions and spatial dimensions. We find the density-induced tunneling process can affect the SF-MI phase boundary dramatically, by suppressing the MI region and tune the tip of the phase boundary to lower chemical potential. Our unbiased numerical study gives benchmark results of the phase diagram of the BHM with density-induced tunneling.     

Higgs portal inflation

The Higgs sector of the Standard Model offers a unique opportunity to probe the hidden sector. The Higgs squared operator is the only dimension two operator which is Lorentz and gauge invariant. It can therefore couple both to scalar curvature and the hidden sector at the dim-4 level. We consider the possibility that a combination of the Higgs and a singlet from the hidden sector plays the role of inflaton, due to their large couplings to gravity. This implies that the quartic couplings satisfy certain constraints which leads to distinct low energy phenomenology, including Higgs signals at the LHC. We also address the unitarity issues and show that our analysis survives the unitarization procedure.     

Quaternion Gravi-Electromagnetism

Defining the generalized charge, potential, current and generalized fields as complex quantities where real and imaginary parts represent gravitation and electromagnetism respectively, corresponding field equation, equation of motion and other quantum equations are derived in manifestly covariant manner. It has been shown that the field equations are invariant under Lorentz as well as duality transformations. It has been shown that the quaternionic formulation presented here remains invariant under quaternion transformations.     

The boson transformation and the vortex solutions

The boson transformation, which allows the construction of spontaneously broken solutions with space and/or time-dependent vacuum directly from the translationally invariant ones, is examined in the context of the Higgs mechanism. Both the Lorentz and the radiation gauge are treated in detail. The classical vortex solution is derived by fully quantum field theoretical considerations. The general form of the vortex solution is presented, and various special cases of interest are examined in detail.     

Superfluid transitions in bosonic atom-molecule mixtures near a Feshbach resonance

We study bosonic atoms near a Feshbach resonance and predict that, in addition to standard normal and atomic superfluid phases, this system generically exhibits a distinct phase of matter: a molecular superfluid, where molecules are superfluid while atoms are not. We explore zero- and finite-temperature properties of the molecular superfluid (a bosonic, strong-coupling analog of a BCS superconductor), and study quantum and classical phase transitions between the normal, molecular superfluid, and atomic superfluid states.