共查询到18条相似文献,搜索用时 933 毫秒
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本文用数值解方法从Eliashberg方程计算出超导临界温度Tc,并考察Tc对有效声子谱的依赖关系。在这个研究中,a2F(ω)被取为双δ函数谱,并允许其中的谱参数可以在很宽范围内改变。作者发现在λ<∧区域(即在Tc级数解的收敛圆外),Tc除了依赖λ和矩比外,还依赖Tc级数解的收敛半径倒数Λ;它们之间的关系是有规律的。在这些结果的启示下,本文在μ*=0情形,用弥合数值解的方法得到一个适用于λ<Λ区域的Tc近似公式。接着,本文作者对吉光达和吴杭生的一篇文章进行了研究,指出:该文提出的超导体分类建议及其工作的主要结论是对的。但其中对决定A型超导体临界温度主要参量问题进行的分析,只适用于这样一些A型超导体,它们的收敛半径倒数Λ或者比λ0小,或者虽比λ0大、但λ又小于λ0,其中λ0是个依赖谱形状的参量,它的定义在正文中给出。对另一些A型超导体(λ0<λ<Λ),决定Tc的主要参量不再是λ,而是δ=1/∧0.5(ω1/2/ωlog)5.5λ1.55。
关键词: 相似文献
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本文指出,对于实际的归一化有效声子谱函数g(ω),一般来说,zph≡F(-ωph-2是函数z=F(y)≡∫0(ωph)(ω2y)/(ω2y+1)g(ω)dω的反函数的分支点。因此,在估算超导Tc级数的收敛半径时,应当予以考虑。
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We present an experimental investigation of a
filamentation-assisted fourth-order nonlinear optical process in KTP
crystals pumped by intense 1.53~eV (807~nm) femtosecond laser
pulses. Femtosecond light pulses at 2.58~eV (480~nm) are generated
by the fourth-order nonlinear polarization (P4(ω 2 ) =
χ 4(ω 2 ,ω ,ω ,ω ,- ω 1
)E3(ω )E* (ω 1 ), where E(ω ) corresponds to
the pump frequency and E(ω 1 ) to the supercontinuum
generated through filamentation). If the system is seeded by a laser
beam at ω 1 or ω 2 and there are spatial and
temporal overlaps with the pump beam, E(ω 1 ) and E(ω
2 ) are simultaneously amplified. When the intensity of the seed
laser beam exceeds a certain intensity threshold, the contribution
of P4(ω ) = χ 4(ω ,ω 1 ,ω 2 ,-ω, - ω )E(ω 1 )E(ω 2 )(E* (ω))2 becomes non-negligible, and the amplification weakens. The
conversion efficiency from the pump to the signal at 2.58~eV
(480~nm) attains to 0.1%. 相似文献
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用一架30厘米×30厘米×10厘米磁场为6200高斯的云室,在海拔3185米的云南落雪高山实验室拍摄了30000对照片,获得105个V0,而可以进行分类的有43个。其中有26个θ10,16个Λ0和一个θ20。本文对θ10,Λ0和一个θ20进行了研究,其结果如下:1)Q值,Q(Λ0)=(36.2±2.5)Mev,Q(θ10)=(233±11)Mev;2)平均寿命,τ(Λ0)=(3.19-0.92+2.42)×10-10秒,τ(θ10)=(1.14-0.27+0.49)×10-10秒;3)动量分布与以前的工作没有显著差别;4)N(Λ0)/N(θ10)=0.51±0.22(权衡数);5)Λ0和θ10在质心系的衰变角分布没有明显的不对称性;6)一个θ20在静止坐标系寿命为~10-9秒,衰变类型可能为θ20→π-+π++π0或者θ20→π±+μ?+ν。 相似文献
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本文在Ed=0.1—2.5MeV能量范围内,研究了Be9(d,p0)Be10(0),Be9(d,p1)Be10(3.368MeV),Be9(d,t0)Be8(0),Be9(d,α0)Li7(0)及Be9(d,α1)Li7(0.478MeV)诸反应。在Ed=0.150,0.220,0.401,0.706,1.005,1.301,1.484,1.750,2.000,2.250和2.500MeV共十一个能量上分别测量了这五群出射粒子在θL=10—155°区间的角分布。在θL=135°,Ed=0.1—2.5MeV,在θL=95°,Ed=0.1—2.2MeV,和在θL=112.5°,Ed=0.5—2.5MeV测量了Be9(d,p0)Be10的激发函数。在θL=135°和112.5°,Ed=1.2MeV,用较厚靶(100—300μg/cm2)测量了Be9(d,p0)Be10(0)反应的截面绝对值,结果为σ(p0)(θL=135°)=1.60mb/sr,σ(p0)(θL=112.5°)=1.55mb/sr。这样就得到了在此能区内,这五群出射粒子的截面情况。对所得结果进行了一些讨论。 相似文献
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从1955年到1957年用多板云室进行了两次V0粒子实验,共得V0约550个。按α-∈方法分类为Λ0的67个,为θ0的44个。其中产生于Pb板的Λ058个、θ038个;产生于Al板的Λ09个、θ06个。对这些V0粒子进行分析,得到下列结果。1.Λ0,θ0衰变时质量中心系中衰变角均匀分布。产生面与衰变面的关联角均匀分布。无自旋>1/2的迹象。2.对Pb核中出来的Λ0衰变看不出因宇称不守恒引起的不对称角分布。Al中产生的Λ0有不对称的倾向。3.由动量分布和产生角分布看,在产生重介子与超子对时超子多向后去。4.得平均寿命τ(Λ0)=(3.39-0.440.63)×10-10秒,τ(θ0)=(0.86-0.160.26)×10-10秒。5.N(Λ0)/N(θ0)~1.4 6.估计整个奇异粒子产生截面可合0.8mb/核子。对Pb,Al都合。7.按V0佔次粒子总数比例看,Pb原子核对产生V0来讲比Al原子核有效。 相似文献
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Ira W. Herbst 《Communications in Mathematical Physics》1979,64(3):279-298
The resolvent of the operatorH 0(ε, θ)=?Δe -20+εx 1 e θ is not analytic in θ for θ in a neighborhood of a real point, if the electric field ε is non-zero. (One manifestation of this singular behavior is that for 0<|Im θ|<π/3,H 0(ε, θ) has no spectrum in the finite plane.) Nevertheless it is shown that the techniques of dilation analyticity still can be used to discuss the long-lived states (resonances) of a system described by a Hamiltonian of the formH=?Δ+εx 1+V(x). 相似文献
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By using the Fourier expansion method, we have developed an approach to calculate the effective dielectric index of a two-dimensional photonic crystal. The approach is very general: it can take into account various Bravais lattice structure as well as arbitrary spatial variation of the dielectric index. It has been found that near a nondegenerate frequency ωn(Γ) at Γ point, the transverse magnetic (TM) mode is ordinary, as it is independent of the propagation direction, whereas in general the transverse electric (TE) mode depends on the propagation direction, it is extraordinary. Therefore, a two-dimensional photonic crystal can always be described by an effective dielectric index for TM mode near the nondegenerate frequency ωn(Γ). However, the TE mode is much more complicated unless the lattice structure is highly symmetric. Moreover, a two-dimensional square photonic crystal has been identified as an effective birefringent crystal having two negative refractive indexes from the perspective of Snell's law. 相似文献
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电子俘获是激光尾波场加速电子的主要机理,增大电子的初速度可以使更多的电子被尾波场俘获.提出三角脉冲激发尾波加速电子的方案,三角脉冲平缓上升沿激发受激Raman散射,用以初步加速电子,三角脉冲陡峭下降沿激发尾波场,将更多的电子加速到接近光速.2D3V粒子模拟结果证实了这一点.同时表明:脉冲长度为几个等离子体波长的超强激光在稀薄等离子体中传播时,还激发侧向Raman散射.在侧向受激Raman散射中,静电波增长最快的波矢模式为kp=(2ωp/ω0
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有质动力
电子俘获
前向受激Raman散射
侧向受激Raman散射 相似文献
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D.G. Hummer 《Journal of Quantitative Spectroscopy & Radiative Transfer》1984,31(3):283-284
The moments Mn(r) ≡ 1/2 ∝2π0 dθ sinn θ I(r,θ) of the intensity I(r, θ) in free space surrounding a spherical object emitting radiation with an arbitrary directional dependence are shown to be exactly proportional to r-(n+1), n = 0, 1,…. 相似文献