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1-methyl-3,6-dioxo-cyclohexane-1,2-dicarboxylic acid dimethyl ester | 861316-25-8

中文名称
——
中文别名
——
英文名称
1-methyl-3,6-dioxo-cyclohexane-1,2-dicarboxylic acid dimethyl ester
英文别名
Opt.-inakt. 3,6-Dioxo-1-methyl-cyclohexan-dicarbonsaeure-(1,2)-dimethylester;1-Methyl-3,6-dioxo-cyclohexan-1,2-dicarbonsaeure-dimethylester
1-methyl-3,6-dioxo-cyclohexane-1,2-dicarboxylic acid dimethyl ester化学式
CAS
861316-25-8
化学式
C11H14O6
mdl
——
分子量
242.229
InChiKey
RITNGGMMHDCQNY-UHFFFAOYSA-N
BEILSTEIN
——
EINECS
——
  • 物化性质
  • 计算性质
  • ADMET
  • 安全信息
  • SDS
  • 制备方法与用途
  • 上下游信息
  • 反应信息
  • 文献信息
  • 表征谱图
  • 同类化合物
  • 相关功能分类
  • 相关结构分类

计算性质

  • 辛醇/水分配系数(LogP):
    -0.11
  • 重原子数:
    17.0
  • 可旋转键数:
    2.0
  • 环数:
    1.0
  • sp3杂化的碳原子比例:
    0.64
  • 拓扑面积:
    86.74
  • 氢给体数:
    0.0
  • 氢受体数:
    6.0

反应信息

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文献信息

  • Optimal control of one- and two-photon transitions with shaped femtosecond pulses and feedback
    作者:T. Hornung、R. Meier、D. Zeidler、K.-L. Kompa、D. Proch、M. Motzkus
    DOI:10.1007/s003400000346
    日期:2000.9
    This paper reports two pump-probe experiments in sodium where dynamically tailored ultrashort pulses from a Ti:Sapphire-pumped optical parametric amplifier were employed. The first study focuses on the one-photon Na(3s --> 3p) transition to derive sensitive criteria which judge the performance of a frequency-domain pulse shaper using a spatial light modulator. On the basis of the interpretation, follow-up experiments are suggested to test their cogency. The second experiment uses coherent quantum control by placing an appropriate phase distribution on the incident beam to enhance or cancel the transition probability in the nonresonant two-photon process Na(3s -->--> 5s). Ignorant of the "ideal" phase function, an evolutionary algorithm which uses a feedback derived from the experiment performs the optimization and produces the desired bright or dark pulses within a few minutes. Attention is given to the role of resonant 3s --> 3p transitions excited by the spectral wings of the pump pulse. Different parametrizations of the phase distribution have been examined. Two of these produced solutions which had not previously been predicted by theory still meet the objective of the experiment. The study represents the first successful application of a feedback-organized self-learning algorithm to the design of dark pulses.
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