Carl Zeiss Microimaging Gmbh

Carl Zeiss Microscopy Gmbh

Carl Zeiss Jena Gmbh

Carl Zeiss Meditec Ag

Carl Zeiss Meditec Gmbh

Boston University

Carl Zeiss Ag

The Trustees of Boston College

Nanoscribe Gmbh

Michael Kempe

Ralf Wolleschensky

Gerhard Krampert

Matthew J Everett

Ingo Kleppe

Daniel Bublitz

Yue Qiu

Tobias Schmitt-Manderbach

Csaba Farkas

Michael Schwertner

Mario Gerlach

Dirk Muehlhoff

Martin Wiechmann

Olaf Kittelmann

Alexander Kalies

Mark Bischoff

Manfred Dick

Martin Hacker

Helmut Lippert

Ralf Netz

Matthias Wald

Michael Bergt

Peter Westphal

Alexandre R Tumlinson

Markus Sticker

Stefan Wilhelm

Utkarsh Sharma

Tobias Bühren

John T Fourkas

Tilman Schmoll

Benno Radt

Christopher Power

Peter Klopfleisch

Dirk Mühlhoff

Christian Dietrich

Diego Zimare

Alexander Sergienko

Malvin C Teich

Bahaa E A Saleh

Markus Strehle

Dick Manfred

Wolfgang Grau

Georg Von Freymann

Eva Simbürger

Mark C Booth

Diegeo Zimare

Tobias BÜHREN

Systems and methods for Broad Line Fundus Imaging (BLFI), an imaging approach that is a hybrid between confocal and widefield imaging systems, are presented. These systems and methods are focused on improving the quality and signal of broad line fundus images or imaging methods to create high contrast and high resolution fundus images. Embodiments related to improved pupil splitting, artifact removal, reflex minimization, adaptable field of view, instrument alignment and illumination details are considered.

Systems and methods for broad line fundus imaging

An ophthalmic lens has a changeable corrective effect, which automatically changes over a predetermined period of time. Further, the ophthalmic lens provides a gradually increasing undercorrection of the far point of the eye over the course of a day, which brings about a deceleration in the axial length growth of the eyeball. In addition, a method for automatically adapting a corrective effect, a pair of spectacles, and a use of an ophthalmic lens are disclosed.

Method for adapting a corrective effect of an ophthalmic lens, ophthalmic lens and use of an ophthalmic lens

A method for the optical detection of an illuminated specimen, wherein the illuminating light impinges in a spatially structured manner in at least one plane on the specimen and several images of the specimen are acquired by a detector in different positions of the structure on the specimen. An optical sectional image and/or an image with enhanced resolution is then calculated. The method includes generating a diffraction pattern in the direction of the specimen in or near the pupil of the objective lens or in a plane conjugate to the pupil. A phase plate with regions of varying phase delays is dedicated to the diffraction pattern in or near the pupil of the objective lens or in a plane conjugate to said pupil, and different phase angles of the illuminating light are set.

Method and configuration for the optical detection of an illuminated specimen

A method and a configuration for the depth-resolved optical detection of a specimen, in which a specimen or a part of the specimen is scanned by means of preferably linear illumination. The illumination of the specimen is periodically structured in the focus in at least one spatial direction. Light coming from the specimen is detected and images of the specimen are generated. At least one optical sectional image and/or one image with enhanced resolution is calculated through the specimen. Images are repeatedly acquired and sectional images are repeatedly blended while changing the orientation of the linear illumination relative to the specimen and/or spatial intervals between lines exposed to detection light from the illuminated specimen region are generated for the line-by-line non-descanned detection on an area detector or a camera and/or, during a scan, light is further deflected upstream of the detector through the line in the direction of the scan of the specimen.

Method and configuration for depth resolved optical detection of an illuminated specimen

A method for the three-dimensional imaging of a sample in which image information from different depth planes of the sample is stored in a spatially resolved manner, and the three-dimensional image of the sample is subsequently reconstructed from this stored image information is provided. A reference structure is applied to the illumination light, at least one fluorescing reference object is positioned next to or in the sample, images of the reference structure of the illumination light, of the reference object are recorded from at least one detection direction and evaluated. The light sheet is brought into an optimal position based on the results and image information of the reference object and of the sample from a plurality of detection directions is stored. Transformation operators are obtained on the basis of the stored image information and the reconstruction of the three-dimensional image of the is based on these transformation operators.

Method for the microscopic three-dimensional reproduction of a sample

A luminescence microscopy method includes a sample being used, which comprises a certain substance, wherein the certain substance can be converted repeatedly from a first state, in which it can be excited into emitting luminescence radiation, into a second state, in which it cannot be excited into emitting luminescence radiation. The substance present in the sample can be brought into the first state by irradiating switch radiation. The certain substance can be excited into emitting luminescence radiation by irradiating excitation radiation. The sample emitting luminescence radiation can be displayed. A high-resolution selection of sample regions extending perpendicularly to a sample surface is carried out by irradiating either the switch radiation or the excitation radiation as structured illumination of the sample. A high-resolution selection of the sample surface is carried out by irradiating the switch radiation and/or the excitation radiation as TIRF illumination of the sample.

Luminescence microscopy

In structured illumination microscopy, the multiple recording of images with different phase positions of the structuring requires a high stability in the optical arrangement and sample throughout the entire measuring process. Also, the structuring must be projected into the sample in a highly homogeneous manner. The current invention optimizes recording of individual images in order to achieve the best possible resolution in the result image even in problematic samples. An optimization of this kind can be carried out in different ways, for example, by determining an optimal adjustment for at least one illumination parameter or recording parameter or by pulsed illumination such that an excitation from a triplet state of the fluorescent dye to a higher triplet state is reduced, or by illuminating the sample with depletion light for depopulating a triplet state of the fluorescent dye, which reduces bleaching.

Methods and apparatuses for structured illumination microscopy

Swept source designs that eliminate or significantly reduce artifacts in optical coherence tomography are presented. One embodiment of the present invention is a source design that frequency shifts the coherence revival interference signal to a frequency larger than the A/D detection bandwidth or the post-processing bandwidth. In another embodiment, the introduced frequency shift is large enough to introduce a Doppler shift of the modes of the laser, which causes a blurring of the comb function, and thus eliminates or reduces mode hopping. In another embodiment, adjusting the cavity optical path length prior to data acquisition depending on the given optical layout configuration to reduce or eliminate coherence revival artifacts is described.

Systems and methods for artifact suppression by frequency shifting or cavity length adjustment

A microscope device which has a diffraction-limited resolution volume, with multiple dye molecules that can be switched between different states, at least one of which is fluorescent. The fluorescence is focused using an objective lens and is imaged onto a spatially resolving detector. In at least one portion of the sample, the dye molecules have a distribution density that is greater than the inverse of the diffraction-limited resolution volume. One or more light sources are provided for emitting a switching radiation in order to switch a first subset of the dye molecules in the sample, and for emitting an excitation radiation in order to excite the first subset of dye molecules. A phase mask which generates a light distribution having an at least partially limited local minimum radiation on the detector plane is provided in the beam path, preferably in the detection beam path.

Apparatus, especially microscope, for the analysis of samples

The invention relates to a device for measuring an optical penetration that is triggered in a tissue underneath the tissue surface by means of therapeutic laser radiation which a laser-surgical device concentrates in a treatment focus located in said tissue. The inventive device is provided with a detection beam path comprising a lens system which couples radiation emanating from the tissue underneath the tissue surface into the detection beam path. A detector device generating a detection signal which indicates the spatial dimension and/or position of the optical penetration in the issue is arranged downstream of the detection beam path.

Device and method for measuring an optical break-through in a tissue

A microscope with means for adjusting the focal range, comprising a first objective lens for transmitting the object light of an illuminated object in the direction of a detector, with a second objective lens being disposed in the direction of the light upstream of the detector, which second objective lens is followed by a first mirror that can be adjusted in the direction of the optical axis, with at least one second mirror for transmitting light from the first objective lens in the direction of the second objective lens and from the second objective lens to the detector being disposed in the optical path, which second mirror is a fully reflective mirror, or a microscope with means for adjusting the focal range, comprising a first objective lens for transmitting the object light of an illuminated object in the direction of a detector, with a second objective lens being disposed in the direction of light upstream of the detector, which second objective lens is followed by a first mirror that can be adjusted in the direction of the optical axis, with a polarizing beam splitter for splitting the object light into two components that are oriented perpendicular to each other being disposed between the first and the second objective lens for light transmission.

Microscope having an adjustment device for the focus range

Growing community of inventors

Jena, Germany

Michael Kempe