Measurement of the transverse beam spin asymmetry in elastic electron-proton scattering and the inelastic contribution to the imaginary part of the two-photon exchange amplitude

We report on a measurement of the asymmetry in the scattering of transversely polarized electrons off unpolarized protons, A( perpendicular), at two Q2 values of 0.106 and 0.230 (GeV/c)(2) and a scattering angle of 30 degrees 相似文献   

多光子激发荧光与毛细管电泳联用的实验研究

将多光子激发荧光探测与毛细管电泳技术相结合,研制了多光子激发荧光-毛细管电泳联用装置。这种方法可以高效快速的分离检测复杂样品中多种不同的荧光分子。作者对5HT,FAD,NADH这三种重要的生物分子,不用染料标记,分别用双光子激发和三光子激发,进行了直接的分离、识别和检测。得到的检测限分别是5HT 1.0×10-6 mol·L-1,FAD 7.4×10-７ mol·L-1,NADH 9.8×10-７ mol· L-1。5HT的检测限比紫外吸收低2个数量级;FAD和NADH的检测限比紫外吸收低1个数量级。     

Observation of rubidium 5S1/2 --> 7S1/2 two-photon transitions with a diode laser

The 5S1/2 --> 7S1/2 two-photon transition of atomic rubidium, which is 100 times weaker than the 5S-5D transition, is observed with an extended-cavity diode laser and a vapor cell. Signals with a signal-to-noise ratio of 280 are obtained with a laser power of 10 mW, and the observed linewidth is 3 MHz. The laser wavelength is 760 nm and is locked on the transitions to a stability of 2 x 10(-11). For the first time to our knowledge, the isotope shift of this transition is measured to be 130(4) MHz in atomic frequency.     

Dendrimer molecules with record large two-photon absorption cross section

We report what is to our knowledge a record high value for an intrinsic two-photon absorption (TPA) cross section, sigma(2) = 11 x 10(-47)> cm>(4)> s photon(-1) molecule(-1), measured with femtosecond pulses in a new dendrimer molecule comprising 29 repeat units of 4, 4(?)-bis(diphenylamino)stilbene chromophore. We measure the dependence of TPA on excitation wavelength in three consecutive generations of the dendrimer and show that the maximum sigma(2) value increases faster than the total number of stilbene chromophores. This result indicates that it is possible to obtain even larger sigma(2) values in higher generations of this dendrimer family.     

Conversion of high-power 15-fs visible pulses to the mid infrared

We measure the efficiency of converting high-power 15-fs 0.8-mum pulses to the mid infrared in GaAs and GaSe as well as the pulse duration and the spectrum of the infrared radiation that is produced. Free-carrier production limits the conversion efficiency in GaAs to approximately 5x10(-7) , allowing us to produce 2.5-pJ, 30-fs pulses spanning the spectral range from 6 to 14 mum . In GaSe we obtain, in a moderately saturated regime, a conversion efficiency of 7.5x10(-5) , limited by two-photon absorption, allowing us to produce pulses of 100-fs duration containing 10 nJ of energy.     

Self-phase modulation in polydiacetylene single crystal measured at 720-1064nm

Detailed measurement of spectral broadening in a poly-[2, 4 hexadiyne-1, 6 diol-bis-(p -toluene sulfonate)] (PTS) single crystal owing to self-phase modulation was performed as a function of wavelength by use of a Ti:sapphire laser producing 200-fs pulses at 720-920 nm and a Nd:YAG laser producing 50-ps pulses at 1064 nm. The nonlinear refractive index (n(2)) of PTS at these wavelengths was determined from the measured phase shift. Group-velocity dispersion was estimated and found to have a negligible effect on the observed spectral broadening. The two-photon absorption coefficient (alpha(2)) over this wavelength range was determined from nonlinear transmission measurements. The largest magnitude of n(2) observed at 720 nm was 3.9x10(-5)cm (2)/MW . The results show that the magnitude of n(2) monotonically decreases as wavelength is increased away from resonance, and two-photon absorption does not make a significant contribution to n(2) at off-resonant wavelengths up to 1064 nm.     

High-sensitivity intracavity laser absorption spectroscopy with vertical-external-cavity surface-emitting semiconductor lasers

We report the demonstration of high-sensitivity intracavity laser absorption spectroscopy with multiple-quantum-well vertical-external-cavity surface-emitting semiconductor lasers (VECSEL's). A detection limit of 3x10(-10) cm (-1) has been achieved. The spectrotemporal dynamics of a VECSEL in the 1030-nm wavelength region has been studied. The laser was operating cw at room temperature, with a baseline signal-to-noise ratio as high as 400. The laser was optically pumped with a threshold as low as 80 mW and was broadly tunable over a spectral range of ~75 nm .     

New CP-violation and preferred-frame tests with polarized electrons

We used a torsion pendulum containing approximately 9 x 10(22) polarized electrons to search for CP-violating interactions between the pendulum's electrons and unpolarized matter in the laboratory's surroundings or the Sun, and to test for preferred-frame effects that would precess the electrons about a direction fixed in inertial space. We find, /g(P)(e)g(S)(N)//(Planck's constant x c) < 1.7 x 10(-36), and /g(A)(e)g(V)(N)//(Planck's constant x c) < 4.8 x 10(-56) for lambda > 1 AU. Our preferred-frame constraints, interpreted in the Kostelecky framework, set an upper limit on the parameter /b(e)/ 相似文献   

Shear viscosity of strongly coupled N = 4 supersymmetric Yang-Mills plasma

Using the anti-de Sitter/conformal field theory correspondence, we relate the shear viscosity eta of the finite-temperature N = 4 supersymmetric Yang-Mills theory in the large N, strong-coupling regime with the absorption cross section of low-energy gravitons by a near-extremal black three-brane. We show that in the limit of zero frequency this cross section coincides with the area of the horizon. From this result we find eta = pi / 8N(2)T3. We conjecture that for finite 't Hooft coupling g(2)(YM)N the shear viscosity is eta = f(g(2)(YM)N)N2T3, where f(x) is a monotonic function that decreases from O(x(-2)ln(-1)(1/x)) at small x to pi/8 when x-->infinity.     

Limits on variations in fundamental constants from 21-cm and ultraviolet Quasar absorption lines

Quasar absorption spectra at 21-cm and UV rest wavelengths are used to estimate the time variation of x [triple-bond] alpha(2)g(p)mu, where alpha is the fine structure constant, g(p) the proton g factor, and m(e)/m(p) [triple-bond] mu the electron/proton mass ratio. Over a redshift range 0.24 < or = zeta(abs) < or = 2.04, (Deltax/x)(weighted)(total) = (1.17 +/- 1.01) x 10(-5). A linear fit gives x/x = (-1.43 +/- 1.27) x 10(-15) yr(-1). Two previous results on varying alpha yield the strong limits Deltamu/mu = (2.31 +/- 1.03) x 10(-5) and Deltamu/mu=(1.29 +/- 1.01) x10(-5). Our sample, 8 x larger than any previous, provides the first direct estimate of the intrinsic 21-cm and UV velocity differences 6 km s(-1).     

三元杂多酸-甲基紫超分子化合物的合成及光谱研究

在水溶液条件下合成了一系列具有Keggin结构的PWxV12 -x MV(x =2 ,4 ,6 ,8,10 )超分子化合物 (PWxV12 -x为具有不同配比的磷钨矾三元杂多酸 ,MV为甲基紫 ) ,并对其紫外光谱 ,红外光谱和荧光光谱进行了研究。结果表明 ,杂多酸阴离子上的端氧与甲基紫阳离子上的N 间通过配合作用相互连结而形成超分子化合物。超分子化合物中仍保持有杂多阴离子的Keggin结构以及甲基紫的基本结构。且随着V的含量增加 ,杂多阴离子的氧化能力增强 ,阴离子PWxV12 -x和阳离子MV的相互作用增强 ,νas(M =Ot) ,νas(M Ob M )和νas(M Oc M )的FTIR吸收峰分别从 96 6 ,886和 80 4cm-1变化至 95 5 ,875和 786cm-1;紫外吸收峰也从 5 19nm移至 5 0 6nm ;用 5 30nm的光激发的荧光发射峰也从 6 92移至 6 4 4nm ,与PWxV12 -x和MV间配合作用的强弱呈现了很好的对应关系。     

Forward-backward asymmetries of lepton pairs in events with a large-transverse-momentum jet at hadron colliders

We discuss forward-backward charge asymmetries for lepton-pair production in association with a large-transverse-momentum jet at hadron colliders. The lepton charge asymmetry relative to the jet direction A(j)(FB) gives a new determination of the effective weak mixing angle sin((2)theta(lept)(eff)(M(2)(Z)) with a statistical precision after cuts of approximately 10(-3) (8x10(-3)) at LHC (Tevatron). This is to be compared with the current uncertainty at LEP and SLD from the asymmetries alone, 2x10(-4). The identification of b jets also allows for the measurement of the bottom-quark-Z asymmetry A(b)(FB) at hadron colliders, the resulting statistical precision for sin((2)theta(lept)(eff)(M(2)(Z)) being approximately 9x10(-4) (2x10(-2) at Tevatron), also lower than the reported precision at e(+)e(-) colliders, 3x10(-4).     

Rovibrational Intensities of the (00(0)3) <-- (10(0)0) Dyad Absorption Bands of (12)C(16)O(2)

Absolute line intensities of (12)C(16)O(2) are experimentally measured for the first time for the (00(0)3)(I) <-- (10(0)0)(II) band at 5687.17 cm(-1) and the (00(0)3)(I) <-- (10(0)0)(I) band at 5584.39 cm(-1). The spectra were obtained using a Bomem DA8 Fourier transform spectrometer and a 25-m base-path White cell at NASA-Ames Research Center. The rotationless bandstrengths at a temperature of 296 K and the Herman-Wallis parameters are S(0)(vib) = 6.68(30) x 10(-25) cm(-1)/(molecule/cm(2)); A(1) = 1.4(9) x 10(-4), and A(2) = -1.1(5) x 10(-5) for the (00(0)3)(I) <-- (10(0)0)(II) band and S(0)(vib) = 6.07(22) x 10(-25) cm(-1)/(molecule/cm(2)); A(1) = 5.2(1.5) x 10(-4) and A(2) = -4.0(7) x 10(-5) for the (00(0)3)(I) <-- (10(0)0)(I) band.     

邻-吡啶苯并噻二唑衍生物的合成与双光子荧光传感性能

以吡啶苯并噻二唑基元为荧光传感"接受体(齿)",将其与咔唑"核"键合获得单齿和双齿两个化合物:2,8-(2-吡啶苯并噻二唑)-N-乙基氮杂笏(CPTZ1)和2,8-双(2-吡啶苯并噻二唑)-N-乙基氮杂芴(CPTZ2),并通过红外光谱、核磁共振谱、质谱表征.通过稳态/瞬态单光子荧光测试和飞秒钛宝石激光器泵浦探测,探讨了CPTZ1和CPTZ2化合物对质子[H+]的敏感性.Stern-Volmer方程给出CPTZ1的单、双光子荧光的猝灭常数分别为:k1PSV=0.04 L·mol-1,k2PSV=0.20 L·moL-1;而CPTZ2的猝灭常数则分别为k1PSV=0.10 L·moL-1,k2PSV(CPTZ2)=0.22 L·moL-1.研究结果表明,双光子荧光(TPF)检测表现出对质子更高的敏感性,其灵敏度是相应的单光子荧光(OPF)的2～5倍.     

Measurement of the 1s-2s energy interval in muonium

The 1s-2s interval has been measured in the muonium (&mgr;(+)e(-)) atom by Doppler-free two-photon pulsed laser spectroscopy. The frequency separation of the states was determined to be 2 455 528 941.0(9.8) MHz, in good agreement with quantum electrodynamics. The result may be interpreted as a measurement of the muon-electron charge ratio as -1-1.1(2.1)x10(-9). We expect significantly higher accuracy at future high flux muon sources and from cw laser technology.     

CO2的腔增强吸收与高灵敏吸收光谱研究

腔增强吸收光谱(CEAS)是在衰荡吸收光谱的基础上发展起来的一种新型的直接吸收光谱技术.文章报道了用中心输出波长为1.573μm的窄线宽连续可调谐半导体激光器(DFB封装)作光源,用两块高反射率平凹透镜(在1.573μm附近,凹面反射率R～99.4%,曲率半径r～1 m)组成对称共焦腔作吸收池的腔增强吸收光谱系统.采用扫描腔长的方法改变谐振腔的模式,当激光器的输出频率与谐振腔的某一腔模之间满足共振匹配关系时,激光被耦合到谐振腔内,用探测器接收透过谐振腔的光信号,同时用波长计精确测量激光器的输出波长.在33.5 cm长的吸收池内测量了吸收强度为1.816×10-23cm-1·(molecule·cm-2)-1的二氧化碳分子的弱吸收谱线,探测灵敏度达到了6.78×10-7 cm-1.实验结果表明,腔增强吸收光谱具有灵敏度高,装置简单,易于操作等优点.     

新型尾式卟啉-吡啶季铵盐对铜(Ⅱ)显色反应研究

研究了三种新型不同链长尾式卟啉 -吡啶季铵盐与Cu2 的显色反应条件 ,其络合物最大吸收波长分别为 4 13nm(Ⅰ ) ,(Ⅱ ) ;4 14nm(Ⅲ )。在相同条件下 ,试剂最大吸收波长分别为 4 4 3 5nm(Ⅰ ) ;4 4 4nm(Ⅱ ) ;4 4 6nm(Ⅲ )。对比度大约 30nm。试剂与铜络合比均为 1∶1,表观摩尔吸光系数为 (Ⅰ ) 3 4× 10 5,(Ⅱ )2 9× 10 5;(Ⅲ ) 2 5× 10 5L·mol-1·cm-1,铜含量分别在 (Ⅰ ) 0～ 0 5 μg·( 10mL) -1;(Ⅱ ) 0～ 0 6 μg·( 10mL) -1;(Ⅲ ) 0～ 1 0 μg·( 10mL) -1内符合比尔定律 ,可用于痕量铜的测定。     

碘、碘离子和碘三离子的紫外吸收光谱

研究了碘I₂、碘离子I- 和碘三离子I-₃ 水溶液的紫外吸收光谱,测定了三种型体的摩尔吸光系数。I₂水溶液在203 nm呈现一吸收峰,摩尔吸光系数为1.96×104 L·mol-1·cm-1;I- 水溶液在193和226 nm呈现双吸收峰,摩尔吸光系数分别为1.42×104和1.34×104 L·mol-1·cm-1;当I₂水溶液与KI溶液混合时,在288和350 nm出现两个吸收峰,表明I-₃的形成。利用饱和法测得I-₃在288和350 nm处的摩尔吸光系数分别为3.52×104和2.32×104 L·mol-1·cm-1。     

Strong two-photon absorption at telecommunications wavelengths in nickel bis(dithiolene) complexes

The two-photon absorption spectrum of a nickel bis(dithiolene) complex with extended conjugation and pi-donor substitution is measured by using Z-scan and pump-probe techniques with femtosecond pulses over the spectral range from 1.20 to 1.58 microm, which includes much of the telecommunications range. The peak two-photon cross section of over 5000 GM (1 GM = 10(-50) cm4 s photon(-1) molecule(-1)) occurs at approximately 1.24 microm, with significant two-photon absorption (>440 GM) throughout the spectral range examined.