摘要:
The invention relates to novel and improved photostable rhodamine dyes of the general structural formulae I or II and their uses as fluorescent markers, e.g. for immunostainings and spectroscopic and microscopic applications, in particular in conventional and stimulated emission depletion (STED) microscopy and fluorescence correlation spectroscopy. The partially deuterated analogues are useful as molecular mass distribution tags in mass spectroscopic applications. wherein R1=an unsubstituted or substituted alkyl group, including a cycloalkyl group, or heterocycloalkyl group; R2═H, an unsubstituted or substituted alkyl group, including a cycloalkyl group, or heterocycloalkyl group, or an unsubstituted or substituted aryl group or heteroaryl group, or any combination of such groups; X═CH2, C═O, C═NORa, C═NNRaNRb, CH(ORa), O, S, SO, SO2, or any other derivatives of these groups, with Ra and Rb independently being H or an organic residue, in particular an unsubstituted or substituted (cyclo) alkyl group or heterocycloalkyl group, an unsubstituted or substituted aryl group or heteroaryl group; Z=a negatively charged group with 1, 2, 3, 4 or 5 charges per anion.
摘要翻译:本发明涉及通用结构式I或II的新型和改进的光稳定罗丹明染料及其作为荧光标记物的用途。 用于免疫染色和光谱和微观应用,特别是在常规和受激发射耗尽(STED)显微镜和荧光相关光谱学中。 部分氘代类似物可用作质谱分析应用中的分子量分布标签。 其中R1 =未取代或取代的烷基,包括环烷基或杂环烷基; R 2 = H,未取代或取代的烷基,包括环烷基或杂环烷基,或未取代或取代的芳基或杂芳基,或这些基团的任何组合; X = CH 2,C = O,C = NOR a,C = NR N R a R b,CH(OR a),O,S,SO,SO 2或这些基团的任何其它衍生物,其中Ra和Rb独立地为H或有机残基 特别是未取代或取代的(环)烷基或杂环烷基,未取代或取代的芳基或杂芳基; Z =带负电荷的基团,每个阴离子具有1,2,3,4或5个电荷。
摘要:
The invention relates to novel and improved photostable rhodamine dyes of the general structural formulae I or II and their uses as fluorescent markers, e.g. for immunostainings and spectroscopic and microscopic applications, in particular in conventional and stimulated emission depletion (STED) microscopy and fluorescence correlation spectroscopy. The partially deuterated analogues are useful as molecular mass distribution tags in mass spectroscopic applications, wherein R1=an unsubstituted or substituted alkyl group, including a cycloalkyl group, or heterocycloalkyl group; R2=H, an unsubstituted or substituted alkyl group, including a cycloalkyl group, or heterocycloalkyl group, or an unsubstituted or substituted aryl group or heteroaryl group, or any combination of such groups; X=CH2, C═O, C═NORa, C═NNRaNRb, CH(ORa), O, S, SO, SO2, or any other derivatives of these groups, with Ra and Rb independently being H or an organic residue, in particular an unsubstituted or substituted (cyclo)alkyl group or heterocycloalkyl group, an unsubstituted or substituted aryl group or heteroaryl group; Z=a negatively charged group with 1, 2, 3, 4 or 5 charges per anion.
摘要翻译:本发明涉及通用结构式I或II的新型和改进的光稳定罗丹明染料及其作为荧光标记物的用途。 用于免疫染色和光谱和微观应用,特别是在常规和受激发射耗尽(STED)显微镜和荧光相关光谱学中。 部分氘代类似物可用作质谱应用中的分子量分布标签,其中R1 =未取代或取代的烷基,包括环烷基或杂环烷基; R 2 = H,未取代或取代的烷基,包括环烷基或杂环烷基,或未取代或取代的芳基或杂芳基,或这些基团的任何组合; X = CH2,C = O,C = NORa,C = NNRaNRb,CH(ORa),O,S,SO,SO2或这些基团的任何其他衍生物,其中Ra和Rb独立地为H或有机残基, 特别是未取代或取代的(环)烷基或杂环烷基,未取代或取代的芳基或杂芳基; Z =带负电荷的基团,每个阴离子具有1,2,3,4或5个电荷。
摘要:
A method of producing spatial fine structures comprises the steps of: selecting a luminophore from the group of luminophores displaying two different states, one of the two states being an active state in which luminescence light is obtainable from the luminophore, the other of the two states being an inactive state in which no luminescence light is obtainable from the luminophore, and the luminophore being reversibly, but essentially completely, transferable out the one state into the other state by means of an optical signal; adding the luminophore to a material; forming a spatial fine structure of the material; and fluorescence-microscopically examining whether the desired fine structure is present. The step of fluorescence-microscopically examining comprises the sub-steps of: outside measuring points of interest, transferring the luminophore into the other state with the optical signal, the luminophore being essentially completely transferred into the inactive state outside the measuring points, and measuring luminescence light only emitted by the luminophore in the active state, to even resolve lines of the fine structure at a distance of less than 100 nm.
摘要:
A method of microscopically examining a spatial fine structure comprises the steps of selecting a luminophore from the group of luminophores which have two physical states, the two states differing from each other with regard to the luminescence properties displayed by the luminophore, and which are reversibly, but essentially completely transferable out of one into the other state of their two states by means of an optical signal; overlaying a surface of the spatial fine structure with the luminophore; and determining the profile of the surface overlaid with the luminophore. The step of determining the profile of the surface comprises the sub-steps of transferring the luminophore by means of the optical signal out of the one into the other of its two states outside a presently observed measurement point, measuring luminescence light emitted by the luminophore, and repeating the sub-steps of transferring and measuring for further measurement points distributed over the surface.
摘要:
A method of producing spatial fine structures comprises the steps of: selecting a luminophore from the group of luminophores displaying two different states, one of the two states being an active state in which luminescence light is obtainable from the luminophore, the other of the two states being an inactive state in which no luminescence light is obtainable from the luminophore, and the luminophore being reversibly, but essentially completely, transferable out the one state into the other state by means of an optical signal; adding the luminophore to a material; forming a spatial fine structure of the material; and fluorescence-microscopically examining whether the desired fine structure is present. The step of fluorescence-microscopically examining comprises the sub-steps of: outside measuring points of interest, transferring the luminophore into the other state with the optical signal, the luminophore being essentially completely transferred into the inactive state outside the measuring points, and measuring luminescence light only emitted by the luminophore in the active state, to even resolve lines of the fine structure at a distance of less than 100 nm.
摘要:
In an optical assembly having a light source which provides two optically different light components with essentially planar wavefronts on an optical axis, wherein the light components differ at least in their wavelength; in the case of an objective lens which projects the two optically different light components into a projection space; and in the case of an optical component which is arranged on the optical axis and has an plane through which the wavefronts of the two light components pass and in which at least two different areas of the optical component with different dispersion behaviors n(λ) abut against one another in the lateral direction with respect to the optical axis; the optical component causes phase shifts of the wavefronts of the two light components, wherein the phase shift of the wavefronts of the one light component differs by at least one quarter of the wavelength of that light component between the two different areas, and wherein the phase shift of the wavefronts of the other light component does not differ between the two different areas, such that an intensity distribution of the one light component in the projection space by interference with itself differs from an intensity distribution of the other light component in the projection space.
摘要:
An optical coherence tomography (OCT) system including an interferometer provides illuminating light along a first optical path to a sample and an optical delay line and collects light from the sample along a second optical path remitted at several scattering angles to a detector. In one embodiment, illuminating light is directed along a number of incident light paths through a focusing lens to a sample. The light paths and focusing lens are related to the sample and to both the incident light source and the detector. In another embodiment, a focusing system directs light to a location in the sample. A transmission grating or acousto-optic modulator directs light from the sample at an angle representative of the wavelength of the incident light on the transmission grating or acousto-optic modulator.
摘要:
A method of correcting optical coherence tomography (OCT) image data obtained from a layered media sample includes identifying at least one interface from the obtained OCT data and correcting the OCT data for distortion at the at least one interface. The OCT image data can be corrected for extrinsic distortions, such as those caused by scan geometry, as well as, intrinsic distortions, such as those caused by refraction at each interface.
摘要:
A phase-referenced Doppler optical coherence tomography (OCT) system includes a low-coherence optical radiation source and a reference source co-propagated to a sample arm and a reference arm. The low-coherence and reference optical radiation reflected from the reference and arms is detected by a pair of detectors, yielding OCT and reference interferometric data output signals. The reference interferometric data output signal can be used to correct the OCT interferometric to yield velocity-indicating images that are free from defects due to sample motion and/or interferometer jitter.