摘要:
In a method of detecting changes in direction of a collimated coherent light beam, the light beam is split into partial light beams which are superimposed on a camera to form an interference pattern displaying light intensity minima and maxima alternatingly following to one another in a transverse direction oriented transversely to an average propagation direction of the partial beams. The light beam is focused into at least one focus located in front of the camera. Pictures of the interference pattern including a plurality of the light intensity maxima are registered with the camera. An average shift of the plurality of light intensity maxima with regard to the camera in the at least one transverse direction is determined from the pictures. A change in angular orientation of the collimated coherent light beam in the at least one transvers direction is deduced from the average shift.
摘要:
In a STED fluorescence light microscope pulses of excitation light (3) are applied to a sample, which excite fluorescent entities contained in the sample for fluorescence, and which are focused on at least one focal area. Further, de-excitation light (12) is applied to the sample, which de-excites the excited fluorescent entities and which comprises an intensity zero point in the at least one focal area, as a continuous wave. Fluorescence light emitted by the excited fluorescent entities in the sample is registered after each pulse of the excitation light (3) and overlapping with applying the de-excitation light (13) with high temporal resolution between consecutive pulses of the excitation light (3).
摘要:
In a method of detecting changes in direction of a collimated coherent light beam, the light beam is split into partial light beams which are superimposed on a camera to form an interference pattern displaying light intensity minima and maxima alternatingly following to one another in a transverse direction oriented transversely to an average propagation direction of the partial beams. The light beam is focused into at least one focus located in front of the camera. Pictures of the interference pattern including a plurality of the light intensity maxima are registered with the camera. An average shift of the plurality of light intensity maxima with regard to the camera in the at least one transverse direction is determined from the pictures. A change in angular orientation of the collimated coherent light beam in the at least one transvers direction is deduced from the average shift.
摘要:
For forming and shifting a light intensity distribution in a focal area of an objective lens, portions of coherent input light are one by one directed into non-identical two-dimensional pupil areas of a pupil of the objective lens. Each of the portions of coherent input light is collimated in the pupil. The pupil areas include a pair of two pupil areas which are axially symmetrically arranged on opposite sides of an optical axis of the objective lens. At least one of the two discrete portions of coherent input light that are directed into the pair of pupil areas is separately modulated with regard to its phase by means of an electro optical modulator such as to form the light intensity distribution in the focal area with a local intensity minimum delimited by intensity maxima and to shift the local intensity minimum laterally with regard to the optical axis.
摘要:
Upstream a microscope objective lens, a polarization direction of a light beam is tilted with a first electro-optical deflector between a first polarization direction with which the light beam is deflected by a first polarization beam splitter by a first angle and a second polarization direction with which it is deflected by a second angle. With a second electro-optical deflector, the polarization direction of the light beam is tilted between a third polarization direction with which the light beam is deflected by a second polarization beam splitter by a third angle and a fourth polarization direction with which it is deflected by a fourth angle. By rotating the polarization direction of the light beam by means of the first and second electro-optical deflectors in a coordinated way the light beam is tilted about a fixed point in a pupil of the objective lens.
摘要:
For forming and shifting a light intensity distribution in a focal area of an objective lens, portions of coherent input light are one by one directed into non-identical two-dimensional pupil areas of a pupil of the objective lens. Each of the portions of coherent input light is collimated in the pupil. The pupil areas include a pair of two pupil areas which are axially symmetrically arranged on opposite sides of an optical axis of the objective lens. At least one of the two discrete portions of coherent input light that are directed into the pair of pupil areas is separately modulated with regard to its phase by means of an electro optical modulator such as to form the light intensity distribution in the focal area with a local intensity minimum delimited by intensity maxima and to shift the local intensity minimum laterally with regard to the optical axis.
摘要:
Upstream a microscope objective lens, a polarization direction of a light beam is tilted with a first electro-optical deflector between a first polarization direction with which the light beam is deflected by a first polarization beam splitter by a first angle and a second polarization direction with which it is deflected by a second angle. With a second electro-optical deflector, the polarization direction of the light beam is tilted between a third polarization direction with which the light beam is deflected by a second polarization beam splitter by a third angle and a fourth polarization direction with which it is deflected by a fourth angle. By rotating the polarization direction of the light beam by means of the first and second electro-optical deflectors in a coordinated way the light beam is tilted about a fixed point in a pupil of the objective lens.
摘要:
In a STED fluorescence light microscope pulses of excitation light (3) are applied to a sample, which excite fluorescent entities contained in the sample for fluorescence, and which are focused on at least one focal area. Further, de-excitation light (12) is applied to the sample, which de-excites the excited fluorescent entities and which comprises an intensity zero point in the at least one focal area, as a continuous wave. Fluorescence light emitted by the excited fluorescent entities in the sample is registered after each pulse of the excitation light (3) and overlapping with applying the de-excitation light (13) with high temporal resolution between consecutive pulses of the excitation light (3).
摘要:
In a method for imaging a structure (33) marked with a fluorescent dye in a sample, the sample is repeatedly scanned in a scanning range (28) with a light intensity distribution localised around a focal point (29) of a focused fluorescence excitation light beam. The light intensity distribution further comprises a focused fluorescence inhibiting light beam (7) whose wave fronts are modulated so that a fluorescence inhibiting light intensity distribution comprises a minimum at the focal point (29) of the fluorescence excitation light beam (4). The scanning conditions are coordinated in such a way that the fluorescence light is emitted out of the scanning range (28) as individually detectable photons. When these photons are detected, the location (32) of the focal point (28) at the respective point in time is allocated to them. An image of the structure (33) is composed of the locations (32) to which the detected photons have been allocated during several repetitions of scanning the scanning range (28).