Abstract: The invention relates to a method for determining positions of mutually spaced molecules (M) in a sample (20), having the steps of generating (101) a plurality of light distributions, each light distribution having a local intensity minimum (110, 310) and adjacent regions (120, 320) of increasing intensity, comprising an excitation light distribution (100) and a deactivation light distribution (300); illuminating (102) the sample (20) with the excitation light distribution (100) and the deactivation light distribution (300); detecting (103) photons emitted by the molecule (M) for different positions of the excitation light distribution (100); and deriving (104) the position of the molecule (M) on the basis of the photons detected for the different positions of the excitation light distribution (100), wherein the local minimum (110) of the excitation light distribution (100) is arranged at a plurality of scanning positions (201) one after the other within a scanning region (200), and the light intensity of the

Abstract: In high spatial resolution imaging, a structure in a specimen is marked with a substance which, in a first electronic state, is excited by light of one wavelength to emit fluorescent light, which is also converted from its first into a second electronic state by that light, and which returns from its second into its first electronic state. The specimen is imaged onto a sensor at a spatial resolution not resolving an average spacing between neighboring molecules of the substance, and exposed to the light at such an intensity that the molecules in the first state are alternately excited to emit fluorescent light and converted into their second state, and that at least 10% of the molecules presently in their first state lie at a distance from their closest neighboring molecules in their first state which is greater than the spatial resolution of the imaging onto the sensor.

Abstract: For imaging of a structure, the structure is marked with a substance which can be converted by a switching signal from a first into a second state, and which provides an optical measurement signal in one of its states, only. The switching signal is applied such that at least 10% of the molecules of the substance being in the measurement signal providing state are at a distance from their closest neighbors, which is greater than the spatial resolution limit of imaging the specimen onto a sensor array, which in turn is greater than an average distance between the molecules of the substance. From an intensity distribution of the measurement signal recorded with the sensor array, the position is only determined for those molecules of the substance which are at a distance from their closest neighboring molecules in the measurement signal providing state, which is greater than the spatial resolution limit.

Abstract: For imaging of a structure, the structure is marked with a substance which can be converted by a switching signal from a first into a second state, and which provides an optical measurement signal in one of its states, only. The switching signal is applied such that at least 10% of the molecules of the substance being in the measurement signal providing state are at a distance from their closest neighbors, which is greater than the spatial resolution limit of imaging the specimen onto a sensor array, which in turn is greater than an average distance between the molecules of the substance. From an intensity distribution of the measurement signal recorded with the sensor array, the position is only determined for those molecules of the substance which are at a distance from their closest neighboring molecules in the measurement signal providing state, which is greater than the spatial resolution limit.

Abstract: In high spatial resolution imaging, a structure in a specimen is marked with a substance which, in a first electronic state, is excited by light of one wavelength to emit fluorescent light, which is also converted from its first into a second electronic state by that light, and which returns from its second into its first electronic state. The specimen is imaged onto a sensor at a spatial resolution not resolving an average spacing between neighboring molecules of the substance, and exposed to the light at such an intensity that the molecules in the first state are alternately excited to emit fluorescent light and converted into their second state, and that at least 10% of the molecules presently in their first state lie at a distance from their closest neighboring molecules in their first state which is greater than the spatial resolution of the imaging onto the sensor.

Abstract: For the high spatial resolution imaging of a structure of interest in a specimen, a substance is selected from a group of substances which have a fluorescent first state and a nonfluorescent second state; which can be converted fractionally from their first state into their second state by light which excites them into fluorescence, and which return from their second state into their first state; the specimen's structure of interest is imaged onto a sensor array, a spatial resolution limit of the imaging being greater (i.e.

Abstract: A method of determining a measurement value on the basis of a plurality of single molecule events of marker molecules in a sample comprises the steps of selecting the marker molecules from a group of marker molecules which are transferable between a measurable state in which a measurement signal necessary for determining the at least one measurement value is obtainable from the marker molecules and a non-measurable state, of providing the marker molecules in the sample at such an absolute concentration that the at least one measurement value is not determinable, if all marker molecules are in their measurable state, and adjusting a measurement concentration of the marker molecules in the measurable state by means of applying the physical signal to the sample at such an intensity that the at least one measurement value is determinable within a defined measurement area of the sample.

Abstract: For the high spatial resolution imaging of a structure of interest in a specimen, a substance is selected from a group of substances which have a fluorescent first state and a nonfluorescent second state; which can be converted fractionally from their first state into their second state by light which excites them into fluorescence, and which return from their second state into their first state; the specimen's structure of interest is imaged onto a sensor array, a spatial resolution limit of the imaging being greater (i.e.