青蒿的遗传转化及青蒿素生物合成的调控

利用发根农杆菌(Agrobacterium rhizogenes)1601，1000，1500，15834，A4，均成功地转化了中药青蒿(Artemisia annua L.)并且建立了pRi1601，pRi15834，pRiA4诱导的发根培养。pRi1601，pRi15834的发根诱导率比其它质粒高。太老或太幼的叶片不利子发根的诱导;发根主要从叶脉的伤口处萌发;带顶芽或带侧芽的叶片容易诱导根，但不一定是发根。光照有利于发根的诱导和发根的生长。以每个发根的“绝对生长速率”(Gtowth Ratio，GR)和绝对“侧根”数量(Number of Side Roots，NSR），通过大量的发根系的筛选，建立了8个发根系，1601-L-1, 1601-L-2, 1601-L-3, 1601-L-4, 15834-L-1, 1601-P-I, 16 01-P-2，15834-L-2。Southern分子检测表明，160l-1-1，1801-L-2, 1601-L-3，1601-L-4，1601-P-1，1601-P-2均为转化子。8个建立的发根系之间无论生长或者QHS的合成存在明显的差异。比较光／暗(16/8hrs)，25℃条件下培养的16 01-L-1，1601-L-2，1601-L-3，1601-L-4，1601-P-l，和1601-P-2，其中16 01-L-3的生长最快，160l-L-1的生长最慢;但是，1601-L-1的QHS的含量最高（可达1. 048%），1601-1-3的QHS的含量最低。160Z-L-3，15834 -L-1和2583:1-L-2的生长速率相差不大。用盛有l000mLMS液体培养基的3000mL的锥形瓶扩大培养1601-L -3，15834-L-1和15834-L-2，转速为ll0rlpm，培养过程中发根容易形成发根球（Hairy Root Balis，HRB），HRB的形成严重影响发根的生长和QHs的合成，HpLC分析表明扩大培养发根中QHS的含量比较低。 改变MS基本培养基中的无机离子的浓度，研究不同无机离子对发根生长和QHS的合成的影响。 l、KN03为18.79×10-3M时有利于1601- L-1生长，为14. 84×10-3M时有利于QHS的合成。NH-4N0-3浓度在10.93-12. 49×10—3M范围内有利于1601-L-1生长，在0-20.62×10-3M范围内对QHS的合成影响不大，大于20. 62×lO-3M不利QHS的合成。培养基中NH-4+／N0-3-比值为0. 37-0. 4-0.52:1时有利于发根的生长，比值为0.52 - 0.58:1时有利于QHS的合成。 2、H-2P0-4-浓度为2.498×10-3M时有利于发根的生长在0-2. 498×l0-3M范围内，随着浓度的提高，促进发根的生长。培养基中的H2P4 -的浓度在0-1.249×lO-3M的范围内，随着浓度的提高，促进QHS的合成，为1.249×10-3M时QHS的含量最高。 3、培养基中最适16 01-L-1生长的Ca-2+浓度为0.198- 0.766×10-3M，大于或小于该浓度范围，显著地抑制发根的生长。但是，在0-3.695×10-3M范围内，随着培养基中Ca-2+浓度提高，促进QHS的合成，最适Ca-2+浓度为3.695×l0-3M。 4、培养基中不加Mg-2+时，完全抑制发根生长，在0. 142×10-3M-7.506×l0-3M浓度范围内，对发根生长影响没有明显的差别。但是，HPLC和UV分析发根中QHS含量，培养基中不加Mg-2+时，发根中QHS含量最高。 5、培养基中的Fe-2+浓度在0. 25 -1．0×10-3M范围内，同时有利于16 01- L-1的生长和QHS的形成。 6、培养基中最适合予16 01- L-3生长的KI浓度为2.5ppm，大于或小予该浓度均显著地抑制发根的生长，培养基中加入KI明显地降低发根中的QHS的含量。 7、H2BO3对l601-L-l生长影响不大，HPLC分析QHS的含量，培养基中的H3BO3浓度为100ppm和400ppm，QHS的含量分别为1.69mg/g和1.80mg/g(DW)。 8、Cu-2+对1601-L-3的生长影响显著，最适合1601-L-3生长的Cu-2+浓度为1.00ppm，在0 -1.00ppm的浓度范围内，随着培养基中的Cu+浓度的提高，发根的生物量不断增加。培养基中QHS合成的最适Cu2+浓度为0.05ppm，大于或小于该浓度均显著地抑制发根中QHS的合成。 比较光培养和暗培养对发根生长的影响，结果表明光照明显地促进1601-L-l的生长，暗培养明显不利于发根的生长。最适合于发根生长的温度为25℃，大于35℃显著地抑制发根的生长，影响发根的根尖细胞的正常分裂。 改变培养基中的蔗糖浓度和在发根培养的不同时期给培养基中添加蔗糖，试验结果表明蔗糖作为碳源对1601-L-3和1601-L-1的生长具有显著的影响。 (1)培养基中缺少蔗糖显著地抑制发根的生长。 (2)发根培养的前5天时间内，蔗糖浓度为30- 60glL昀培养基最有利于发根的生长，50glL的培养基中的发根生长最快，培养基中的蔗糖浓度大于60g/L小于30g／L时，发根的生物量增加较少。 (3)发根培养至第15天时，蔗糖浓度为60g/L的培养基最有利予发根的生物量的增加。发根培养至30天时，蔗糖浓度为60-90g/L的培养基，发根的生物量的增加相差不大，但是为蔗糖浓度为30-40g/L的培养基中的发根生物量一倍。 (4)发根培养过程中，分别于第5和15天给蔗糖浓度为30g/L的培养基中添加一次或二次蔗糖，使培养基中的蔗糖终浓度相当于60g/L或90g/L，培养至30天时，添加蔗糖的培养基中的发根的干重生物量相当于不添加蔗糖培养基中的发根生物量一倍，相当于初始蔗糖浓度为60g/L和90g/L培养基中发根的生物量。 (5)随着培养基中蔗糖浓度的提高，发根干重/鲜重比显著增加。培养基中的蔗糖的消耗量与发根生物量的增加呈正相关，蔗糖消耗越多，发根生物量的增加越大。 比较pH值对发根生长和QHS合成的影响表明，灭菌前pH值在5.O-6.5范围内的培养基适合予1601-L-1的生长，小于5.O不利于发根的生长，pH5.8有利于1601-1-1生长和QHS的生物合成。发根收获时培养基中的pH值一般为4.5-5.2. pH7.O抑制发根的生长，pHl0.O对发根具有强烈的致死作用。发根在培养过程中，对培养基中的pH值具有显著的调节作用，发根能在很短的时间内(24- 48hrs)使pl:l值为5.8、6.4、7.0培养基降低到pH4. 5-5.2，pH为5.8的培养基有利于QHS合成。 比较不同基本培养基对发根生长和QHS合成的影响，试验结果表明N6、DCR、Litvay培养基有利于1601-L-1的生长，WS、White、B5培养基不利于发根的生长。DCR培养基中的QHS含量最高。 根据三水平试验选用三水平正交表来安排试验的原则，选用三水平正交表L7(3-)，研究多因子效应对发根生长和QHS合成的影响，试验结果表明，Mg2+，Fe2+，Mn-2+，NH4NO3，KN03 ,KI,Ca-2+为发根生长的主要因子，NH4N03，KNOs，Mg2+，Ca2+，肌醇为QHS合成的主要因子。 通过TLC分析发根中QHS和其它化学成分，同时比较发根和无菌苗及野生植株的化学成分，发根和无菌苗均能合成包括QHS在内的野生青蒿叶片中的大部分非挥发性的化台 物。 研究青蒿植株在发育过程中QHS的含量的变化以及发根、无菌苗和野生青蒿中QHS的合成，HP分析结果表明，l、不同的单株青蒿之间的QHS量相差很大。2、同一植株幼 叶的QHS含量比老叶的QHS含量高。3、不同单株青蒿之间达到最高QHS含量的时间不一样，开花期或开花之前。4、无菌苗（带根）或者不带根丛生芽均能合成QHS，但是带根的无菌蕾的QHS量比丛生芽中的QIS的含量高。5、不同发根农杆菌转化的发根系1601-L-1和15834-L-1都能合成ＱＨＳ。

Anisotropic thermopiezoelectric solids with an elliptic inclusion or a hole under uniform heat flow

The two-dimensional problem of a thermopiezoelectric material containing an elliptic inclusion or a hole subjected to a remote uniform heat flow is studied. Based on the extended Lekhnitskii formulation for thermopiezoelectricity, conformal mapping and Laurent series expansion, the explicit and closed-form solutions are obtained both inside and outside the inclusion (or hole). For a hole problem, the exact electric boundary conditions on the hole surface are used. The results show that the electroelastic fields inside the inclusion or the electric field inside the hole are linear functions of the coordinates. When the elliptic hole degenerates into a slit crack, the electroelastic fields and the intensity factors are obtained. The effect of the heat how direction and the dielectric constant of air inside the crack on the thermal electroelastic fields are discussed. Comparison is made with two special cases of which the closed solutions exist and it is shown that our results are valid.

Fracture statistics of brittle materials: Weibull or normal distribution

The fit of fracture strength data of brittle materials (Si3N4, SiC, and ZnO) to the Weibull and normal distributions is compared in terms of the Akaike information criterion. For Si3N4, the Weibull distribution fits the data better than the normal distribution, but for ZnO the result is just the opposite. In the case of SiC, the difference is not large enough to make a clear distinction between the two distributions. There is not sufficient evidence to show that the Weibull distribution is always preferred to other distributions, and the uncritical use of the Weibull distribution for strength data is questioned.

A Finite Element Analysis of a Crack Penetrating or Deflecting into an Interface in a Thin Laminate

The crack tip driving force of a crack growing from a pre-crack that is perpendicular to and terminating at an interface between two materials is investigated using a linear fracture mechanics theory. The analysis is performed both for a crack penetrating the interface, growing straight ahead, and for a crack deflecting into the interface. The results from finite element calculations are compared with asymptotic solutions for infinitesimally small crack extensions. The solution is found to be accurate even for fairly large amounts of crack growth. Further, by comparing the crack tip driving force of the deflected crack with that of the penetrating crack, it is shown how to control the path of the crack by choosing the adhesion of the interface relative to the material toughness.

The effects of capillary force in micro or nano-indentation

Models describing wet adhesion between indenters and substrates joined by liquid bridges are investigated. The influences of indenter shapes and various parameters of structures on capillary force are focused. In the former, we consider several shapes, such as conical, spherical and truncated conical indenter with a spherical end. In the latter, the effects of the contact angle, the environmental humidity, the gap between the indenter and the substrate, etc. are included. Different dependences of the capillary force on the indenter shapes and the geometric parameters are observed. Most interesting finding is that applying the present results to micro- and nano-indentation experiments shows the size effect in indentation hardness not produced but underestimated by the effects of capillary force.(4 refs)

Lasing without or with inversion in an open four-level system with a phase-fluctuation driving field

The effect of exit rate and the ratio of atomic injection rate on gain behaviour has been investigated, and the effects of phase fluctuation on absorption, dispersion and population difference in an open four-level system have been analysed by using numerical simulation from the steady linear, analytical solution. The variation of the linewidth, Rabi frequency of the driving field, the exit rate or the ratio of atomic injection rate can change the lasing properties in the open system. The presence of finite linewidth due to driving-field phase fluctuation prevents the open four-level atomic system from obtaining a high refractive index along with zero absorption.

Hit-or-miss representation of a pattern spectrum and its optical implementation

We demonstrate that a pattern spectrum can be decomposed into the union of hit-or-miss transforms with respect to a series of structure-element pairs. Moreover we use a Boolean-logic function to express the pattern spectrum and show that the Boolean-logic representation of a pattern spectrum is composed of hit-or-miss min terms. The optical implementation of a pattern spectrum is based on an incoherent optical correlator with a feedback operation. (C) 1996 Optical Society of America

Superresolution, extended focal depth or focal shift with electrically controllable radial birefringent filter

In this paper an electrically controllable radial birefringent pupil filter is proposed. It consists of two polarizers and an improved electrically controllable optical azimuth rotator which has two lambda/4 retarders, one electro-optical crystal and one radial birefringent crystal. The evolution and distribution of polarization states of this pupil filter are discussed. The most interesting and useful advantage of such a structure is that the characteristic of transverse superresolution and axial extended focal depth or focal shift can be obtained merely by controlling the applied voltage on the electro-optical crystal. The radial birefringent crystal azimuth angle cooperating with different electrical inductive phase differences will determine the transverse and axial intensity distribution. It is shown that for particular ranges of electrical inductive phase difference it is possible to obtain transverse superresolution along with extended focal depth or with a focal shift.

Cooperative downconversion in Yb3+-RE3+ (RE = Tm or Pr) codoped lanthanum borogermanate glasses

We report on cooperative downconversion in Yb3+-RE3+ (RE = Tm or Pr) codoped lanthanum borogermanate glasses (LBG), which are capable of splitting a visible photon absorbed by Tm3+ or Pr3+ ions into two near-infrared photons. The results indicate that Pr3+-Yb3+ is a more efficient ion couple than Tm3+-Yb3+ in terms of cooperative downconversion. We have obtained a highest quantum yield of 165% and 138% for Pr3+-Yb3+ and Tm3+-Yb3+ codoped LBG glasses under 468 nm excitation, respectively. However, ultraviolet light excitation to the charge transfer band of Yb3+ does not result in quantum splitting as rapid relaxation from the charge transfer band to 4f(13) levels of Yb3+ dominates. (C) 2008 Optical Society of America