驰豫的英文

• relaxation

• "驰"英文翻译    speed; gallop
• "豫"英文翻译    pleased
• "驰豫谱" 英文翻译 :    relaxation spectrum
• "热驰豫" 英文翻译 :    thermal relaxation
• "驰豫长度" 英文翻译 :    relaxation length
• "驰豫过程" 英文翻译 :    relaxation process
• "驰豫时间" 英文翻译 :    relaxation lifetime; relaxation time
• "驰豫试验" 英文翻译 :    relaxation test
• "电介质驰豫" 英文翻译 :    dielectric relaxation
• "结构驰豫" 英文翻译 :    structural; stuctural
• "介电驰豫" 英文翻译 :    dielectric relaxation
• "应力驰豫" 英文翻译 :    relaxation of stress
• "岩块驰豫时间" 英文翻译 :    block relaxation time
• "自旋晶格驰豫" 英文翻译 :    spin lattice relaxation
• "纵向驰豫时间" 英文翻译 :    spin lattice relaxation time
• "自旋晶格驰豫时间" 英文翻译 :    spin lattice relaxation time
• "驰压安全壳" 英文翻译 :    pressure suppression containment
• "驰星周" 英文翻译 :    hase seishu; seishu hase
• "驰信息技术有限公司" 英文翻译 :    infoprint solutions company
• "驰心旁骛" 英文翻译 :    one's mind kept wandering off (onto ...).; in an absent-minded sort of way
• "驰下来" 英文翻译 :    abfahren

• Dynamic analysis of polar microregions in therelaxor ferr oelectrics
  驰豫铁电体中极化微区动力学分析
• It is explained by cross relaxation of the ( 2h11 / 2 , 4s3 / 2 ) states
  这主要是由于交叉驰豫作用的结果。
• Longitudinal relaxation time
  驰豫时间
• This special type of material may possess optical constants that are different from those at the fully relaxed material
  这种特别的材料类型可能会拥有与完全驰豫材料不同光学常数。
• It ' s generally believed that the qgp , if formed in the relativistic heavy ion collisions , be in a thermal non - equilibrium state during initial stage and then evaluates into equilibrium state
  通常认为在相对论重离子碰撞中生成的qgp首先是处于非平衡态，它要经过一个由非平衡态向平衡态演化的驰豫过程。
• All the heat treated samples have a damping peak over the range of 150 and 260 ( called tp peak ) . by analyzing , the peak is a dislocation peak and it can be explained with g - l theory
  分析表明，此峰为位错峰，因为该峰从峰的位置，频率驰豫特性，以及阻尼性能测量的应变振幅相关性，都与g一l理论符合的很好。
• It is found that the current amplification coefficient strongly depends on the spin polarization of the electrons injected from the emitter to the base , the spin relaxation time and the width of the base
  自旋晶体管中的电流放大系数主要取决于注入基区的自旋极化电子的极化程度，基区中自旋的驰豫时间及基区的宽度。
• The bulk electronic properties of gaas have been described both by the second - neighbour tight - binding formalism for ( 112 ) , ( 113 ) ( 114 ) surface and nearest neighbour tight - binding sp3s * for ( 2 5 11 ) surface
  再构后，不考虑表面原子的驰豫变化， gaas ( 2511 )表面表面态的变化主要表现在o . gev ~ 1 . oev的一些表面态完全消失。
• When the coupling rabi frequency c satisfies the condition of c > 1 / 2 3 , the transient process is a relaxation oscillation behavior . as the coupling rabi frequency c decreases , the transient oscillation behavior slows up
  当_ c _ 3 / 2时，这个瞬态过程为一驰豫振荡过程，在不同大小的耦合光rabi频率_ c条件下， _ c取值越小，瞬态过程振荡越慢。
• But for the furnace cooling samples , all samples have another damping peak about at 3 00 ( called tp2 peak ) . the peak is not of relaxation model , the peak temperature does not vary with frequencies
  除炉冷试样外，其余各热处理态试样均在300左右，有一内耗峰几2峰，此内耗峰无驰豫特性。频率变化，内耗峰的位置不变，对同一热处理态试样内耗峰位置不变。