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excited state

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excited state 【物理學】受激態。

【物理學】受激態。 “excited“ 中文翻譯：   adj. 1.激昂的，激動的，興奮的。 2.【物理學】激 ...“state“ 中文翻譯：   n. 1.〔常作 S-〕國，國家；〔通例作 S-〕(美國 ...“state, excited“ 中文翻譯：   受激狀態“doubly excited state“ 中文翻譯：   雙重激發態“excited electronic state“ 中文翻譯：   電子激發態; 激發電子態“excited single state“ 中文翻譯：   激發單一態; 受激單線態“excited singlet state“ 中文翻譯：   受激單能態“excited state chemistry“ 中文翻譯：   激發態化學“excited state lifetime“ 中文翻譯：   激發狀態壽命“excited state of nuclei“ 中文翻譯：   核激發態“excited state quencher“ 中文翻譯：   激發態抑制劑“excited state spectroscopey“ 中文翻譯：   激發態光激學“excited state spectroscopy“ 中文翻譯：   激勵態光譜學“excited state well“ 中文翻譯：   激發態阱“excited triplet state“ 中文翻譯：   激發三重態“first excited state“ 中文翻譯：   第一激發態“ground-excited state transition“ 中文翻譯：   基態-激發態躍遷“half life of excited state“ 中文翻譯：   激發態的半衰期“lifetime of excited state“ 中文翻譯：   激發態壽命“low excited state“ 中文翻譯：   低激發態“manifold of excited state“ 中文翻譯：   受激態簇“physical chemistry of excited state“ 中文翻譯：   激發態物理化學“triplet excited state“ 中文翻譯：   三重激態“be excited“ 中文翻譯：   情緒激動“excited“ 中文翻譯：   adj. 1.激昂的，激動的，興奮的。 2.【物理學】激發的，勵磁的。 adv. -ly 激昂，興奮。

excitement

We calculated the states “ binding energy in finite and infinite quantum well with different width of well such as 10 a , 20 a 30 a 50 a 70 a 100 a . we obtained the well width that some low - lying excited states appeared in strong field and in fixed well width the value of magnetic field when these states began appear 我什計算了在階寬為10a 、 20a 、 30a 、 50a 、 70a 、 100a的有限深和無限深量于階中的廠中心的束縛態，得到一些二維廠中心所沒有的低激發態在強磁場下出現時的階寬，以及一些態在某一階寬下出現的臨界磁場值。

We used density functional theory ( b3lyp ) , which is becke ' s three parameter hybrid function using the lee , yang and parr ( lyp ) correlation function . the basis sets we used is 6 - 31g * . the excited state energies and electric dipole transition moments are calculated by time - dependent dft 分子的幾何結構在雜化的密度泛函理論( dft ) b3lyp水平上優化，其中電子的交換能采用becke的三參數交換函數，而電子的相關能采用lee , yang ，和parr的相關能函數，選用的基矢是6 - 31g *

A typical model is the atomic barium in which the state 6s 1s0 corresponds to the ground state and the states 6s6p 1p1 and 6s6p 3p1 correspond to the excited states of strong and weak transition , respectively . the decay rates of the excited states are 47khz and 19mhz , respectively , and the ratio of them is 400 原子ba是一個典型的系統(其中能級6s ~ 1s _ 0為基態， 6s6p ~ 1p _ 1和6s6p ~ 3p _ 1分別是上述強躍遷和弱躍遷的激發能級，兩個躍遷的自發衰減速率分別為47khz和19mhz ，兩者之比為400 ) 。

Using different combinations of the nucleon density distributions of the ground state of 6he and the second excited state of 6li with and without the halo , we have calculated the microscopic optical potentials of the input and output channels , and , with these potentials , calculated the angular distribution of the “ h ( he , li ) n reaction populating the second excited states of 6li by using a dwba code 我們用假定的~ 6he基態和~ 6li第二激發態有暈和無暈的各種核子密度分布的組合分別計算了入射道和出射道的微觀光學勢并將其輸入通用的dwba核反應程序計算了~ 1h ( ~ 6he , ~ 6li ) n反應布居~ 6li第二激發態的角分布。

We obtained the system energy and binding energy of ground and some low - lying excited states by solving the equation hnm - e = 0 . different from the variational method ' s result closely depending on the form of the trial wave function , our result has high accuracy as long as the matrix we used is big enough 與變分法的結果對選取的變分波函數依賴性很大不同，從理論上來沁j北師他人學礬卜畢業論義陳紅葉說，只要我們的矩陣展開的足夠大，我們的結果就能保證足夠高的計算精度。

This study introduces the energy consistent method ( ecm ) , the ecm potential function , and the new formulae of vibrational force constants which are proposed by weiguo sun and hao feng [ 45 , 46 ] recently . the ecm is applied to study the diatomic potential functions for some electronic ground states and excited states of gif , ch , bh , xeo , laf , 7lid , na7li , narb and krb molecules . the ecm potentials are compared with the experimental based rkr ( rydberg - klein - rees ) potentials , ipa ( inverted - perturbation - approach ) potentials , analytical morse potentials , and hms ( huxley - murrell - sorbie ) potentials 本文詳細地介紹了孫衛國和馮灝運用二階微擾理論所導出的高階振動力常數的求解公式、能量自洽法( energyconsistentmethod - ecm ) 、 ecm勢能函數的定義以及用能量自洽法計算穩定雙原子分子體系勢能函數的具體步驟，并將ecm方法推廣應用于cif 、 ch 、 bh 、 xeo 、 laf 、 ~ 7lid 、 na ~ 7li 、 narb和krb等九種異核雙原子分子的十二個電子基態和激發態的勢能函數。

Meanwhile , the ancs are 1 . 16 + 0 . 10 fin - 1 / 2 , 1 . 34 + 0 . 12 fm - 1 / 2 and 0 . 94 + 0 . 08 fm - 1 / 2 ; rms radii are 3 . 16 + 0 . 32 fm , 4 . 01 + 0 . 61 fin and 5 . 64 + 0 . 90 fin ; and the probabilities of valence neutrons outside the potentials are 19 . 9 % , 53 . 6 % and 66 . 8 % for the ground state , the second and third excited states of 12b , respectively 2 。結果證實13c的第一激發態為單中子暈核態，首次從實驗上證實在b穩定線上存在激發的暈核態。同時得到12b基態、第二和第三激發態anc系數分別為1

Those investigations have improved one ' s understanding of the structure , formation conditions , reaction mechanisms , and excitation modes of halo nuclei . inl990 ' s it was predicted that besides the ground state of the light nuclei near the drip line , the high isospin excited states may also have halo structure 除滴線附近輕核的基態外，九十年代有人預言穩定核的高同位旋激發態也可能具有暈結構， ~ ( 13 ) c第一激發態和~ 6li第二激發態被列為首選的研究對象。

With analogizing the evolution process of atomic transition from excited states to ground state , we proposed a novel non - linear optimization algorithm for geophysical inverse problem , called as simulated atomic transition algorithm ( sata ) 在此基礎上，模擬了物理學中原子從激發態向基態躍遷的物理過程，建立了一種與原子躍遷過程相對應的非線性隨機躍遷數學模型和模型解躍遷搜索準則，導出了適用于一般地球物理資料的模擬原子躍遷的非線性反演算法。

In the course of scattering with the same energy , the excited probabilities of lower exciting states are far off bigger than ones of higher exciting states . all in all , the adapted ms potential has advantages of concision form , less adjustable parameters , convenient for applicant 當體系能量一定時，不管是微分散射截面還是分波散射截面，彈性散射的幾率大，對總的散射截面貢獻最大；非彈性散射的幾率小，對總的散射截面的貢獻也小。

Because of the difficulty to calculate the wave function and transitive matrix element in high excited state , chaotic character of wave function is known a little . now many pay attention to the scar of wave function ; ( 3 ) the time evolutionary character of nonstationary state eigenfuction 由于計算高激發態波函數以及躍遷矩陣元的困難，人們對經典混沌給波函數帶來的特征的研究工作還很少，目前研究最多的是關于波函數的疤痕。

It was suggested that the concomitant of the independence in ground states and the interactions in excited states were ascribed to the synergetic enhancement and complementary effects uniform in the same composite photoreceptors 兩種材料在復合體系中既相互獨立從而發揮各自的功能，又在激發態下發生相互作用從而產生敏化作用，是復合體系光導性能互補效應和協同增強效應的本質因素。

It is thought that the exciplex ' s emission is eliminated completely by modulating the transient excited state of exciplex thought varying the ratio of two molecules and by action from the excited state level of rare - earth ions 對于稀土配合物，可以通過控制混合層中的分子比率調制激基復合物的瞬間激發態能級位置，使其與稀土離子的激發態能級匹配，將激基復合物完全消除。

The neutron halo structure of the first excited state of i3c and the neutron - proton halo structure of the second excited state of 6li , which is the isobaric analog state of the ground state of 6he , were considered the most probable candidates to search for 前者的中子暈結構已為實驗所證實，后者是中子暈核~ 6he (基態)的同位旋相似態，其中子-質子暈結構至今尚未被實驗證實。

The stronger orientation of potential is , the weaker repulsive potential is , and the bigger probability of non - elastic scattering is . the dcs in exciting states is smaller when small angles , and will be bigger when big angles 非彈性散射截面與勢能的方向性和排斥勢的強度密切相關，勢能的方向性越強，排斥勢越弱，產生非彈性散射的幾率就越大。

According to the result , we found whether the atom outside of the field is manipulated in the excited state or in the ground state , the probabilistic distribution of the atom inside the field does n ' t change 當糾纏態原子中只有一個原子在場內運動時，各能級均分裂成兩層；而當兩原子均處于場內時，原激發態和基態有著不同的能級分裂。

Short excited state lifetime and low activation energy for reactions in the excited states leave little room for manipulating the diastereomeric transition state when the photochemical reactions occur in solution 最新的研究表明，采用含手性空間或經手性修飾的微環境可以使光化學反應的立體選擇性大大提高。

This is attributed to the stabilization of the excited state of intermediate of luminol by the interaction with the positively charged pee modified layer 荷正電的聚乙烯亞胺修飾分子與魯米諾激發態3 -氨基鄰苯二甲酸陰離子間靜電相互作用而導致的激發態穩定性增加;對魯米諾分子的電化學發光的增強起著關鍵作用。

Using the expressions of the probabilities of finding atom b in excited state or ground state , the average values of the momenta and the kinetic energies of the entangled atoms system are easily obtained 第三章則根據求出的系統的量子態，進而得出原子處于高能態和低能態的幾率及原子的平均動量。