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Dark transition states state detection

Fig. 19.3. Molecular transitions and states utilized to break the diffraction barrier. Each nanoscopy modality resorts to a specific pair of bright and dark states. Several concepts share the same states, but differ by the direction in which the molecule is driven optically (say A B or B A) oi hy whether the transition is performed in a targeted way or stochastically. The targeted read-out modality drives the transition with an optical intensity I and hence operates with probabilities of the molecule of being in A or B. This probability depends on the rates k of the transitions between the two states and hence also on the applied intensity I. The probability pA of the molecule to remain in A typically decreases as indicated in the panel, pa -C 1 means that the molecule is bound or switched to the state B. This switching from A to B or vice versa allows the confinement of A to subdiffraction-sized coordinates of extent Ar at a position rt where /(r) is zero. In the stochastic read-out mode, the probability that state A emerges in space is evenly distributed across the sample and kept so low that the molecules in state A are further apart from each other than the diffraction limit. An optically nonlinear aspect of the stochastic concept is the fact that the molecules undergo a switch to A from where they suddenly emit 1 detectable photons in a row... Fig. 19.3. Molecular transitions and states utilized to break the diffraction barrier. Each nanoscopy modality resorts to a specific pair of bright and dark states. Several concepts share the same states, but differ by the direction in which the molecule is driven optically (say A B or B A) oi hy whether the transition is performed in a targeted way or stochastically. The targeted read-out modality drives the transition with an optical intensity I and hence operates with probabilities of the molecule of being in A or B. This probability depends on the rates k of the transitions between the two states and hence also on the applied intensity I. The probability pA of the molecule to remain in A typically decreases as indicated in the panel, pa -C 1 means that the molecule is bound or switched to the state B. This switching from A to B or vice versa allows the confinement of A to subdiffraction-sized coordinates of extent Ar at a position rt where /(r) is zero. In the stochastic read-out mode, the probability that state A emerges in space is evenly distributed across the sample and kept so low that the molecules in state A are further apart from each other than the diffraction limit. An optically nonlinear aspect of the stochastic concept is the fact that the molecules undergo a switch to A from where they suddenly emit 1 detectable photons in a row...
The analysis of tetramethylammonium hydroxide (TMAH) solutions manufactured by SACHEM Inc. of Cleburne, Texas, includes the determination of trace elements. These elements cause less-than-optimum performance of integrated circuit boards manufactured by SACHEM s customers that use these solutions in their processes. Alkali and alkaline earth metals (e.g., Li, Na, K, Mg, Ca, and Ba) can reduce the oxide breakdown voltage of the devices. In addition, transition and heavy metal elements (e.g., Ti, Cr, Mn, Fe, Co, Ni, Cu, Zn, Ag, Au, and Pb) can produce higher dark current. Doping elements (e.g., B, Al, Si, P, As, and Sn) can alter the operating characteristics of the devices. In SACHEM s quality control laboratory, ICP coupled to mass spectrometry is used to simultaneously analyze multiple trace elements in one sample in just 1 to 4 min. This ICP-MS instrument is a state-of-the-art instrument that can provide high throughput and low detection Emits at the parts per thousand level. Trace elemental determination at the parts per thousand level must be performed in a clean room so that trace elemental contamination from airborne particles can be minimized. [Pg.292]


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