The General Hospital Corporation

Asml Netherlands B.v.

Evans, Conor Lee

De Boer, Johannes F.

De Groot, Mattijs

Johannes Fitzgerald De Boer

Guillermo J Tearney

Brett Eugene Bouma

Seok-Hyun Yun

Wang-Yuhl (William) Oh

Seok-Hyun (Andy) Yun

Arie Jeffrey Den Boef

Vasco Tomas Tenner

Koenraad Arndt Vermeer

Mattijs De Groot

Christos Messinis

Conor L Evans

Wang-Yuhl Oh

Boris Hyle Park

Abraham J Cense

Conor Lee Evans

Ki Hean Kim

Methods and apparatus are disclosed for determining a characteristic of a structure. In one arrangement, the structure is illuminated with first illumination radiation to generate first scattered radiation. A first interference pattern is formed by interference between a portion of the first scattered radiation reaching a sensor and first reference radiation. The structure is also illuminated with second illumination radiation from a different direction. A second interference pattern is formed using second reference radiation. The first and second interference patterns are used to determine the characteristic of the structure. Azimuthal angles of the first and second reference radiations onto the sensor are different.

Method of determining a characteristic of a structure, and metrology apparatus

An apparatus and source arrangement for filtering an electromagnetic radiation can be provided which may include at least one spectral separating arrangement configured to physically separate one or more components of the electromagnetic radiation based on a frequency of the electromagnetic radiation. The apparatus and source arrangement may also have at least one continuously rotating optical arrangement which is configured to receive at least one signal that is associated with the one or more components. Further, the apparatus and source arrangement can include at least one beam selecting arrangement configured to receive the signal.

Process and apparatus for a wavelength tuning source

Exemplary apparatus, arrangement and method can be provided for obtaining information associated with an anatomical structure or a sample using optical microscopy. For example, a light radiation can be separated into first light radiation(s) directed to an anatomical sample and second light radiation directed to a reference. A wavelength of the radiation can vary over time, and the wavelength can be shorter than approximately 1150 nm. An interference can be detected between third and fourth radiations associated with the first and second radiations and fourth radiation, respectively. At least one image corresponding to portion(s) of the sample can be generated using data associated with the interference. In addition, source(s) can be provided which can be configured to provide an electromagnetic radiation having a wavelength that varies over time. A period of a variation of the wavelength of the first electromagnetic radiation(s) can be shorter than 1 millisecond, and the wavelength can be shorter than approximately 1150 nm.

Process, arrangements and systems for providing frequency domain imaging of a sample

The human eye is constantly in motion. For many imaging applications in the eye, eye motion on the time scale of the image acquisition distorts the images. For imaging applications where the signal is very low, image distortion is so severe that imaging is impossible. According to an exemplary embodiment of the present disclosure, systems, methods and computer-accessible medium can be provided to determine eye motion in real time, and provide real time correction of the eye motion for secondary imaging methods to provide stable images and permit long integration times of single images to increase the signal to noise.

System, method and computer accessible medium for determining eye motion by imaging retina and providing feedback for acquisition of signals from the retina

Exemplary apparatus and method are provided. In particular, an electromagnetic radiation can be emitted with, e.g. a light source arrangement. For example, the light source arrangement can include a cavity and a filter, and a spectrum of the electromagnetic radiation can be controlled, e.g., with such cavity and filter, to have a mean frequency that changes (i) at an absolute rate that is greater than about 100 terahertz per millisecond, and (ii) over a range that is greater than about 10 terahertz. Additionally or alternatively, the light source arrangement can include a frequency shifting device which can shift the mean frequency of the electromagnetic radiation.

Method and apparatus for performing optical imaging using frequency-domain interferometry

Systems and methods according to exemplary embodiments of the present disclosure can be provided that can efficiently detect the amplitude and phase of a spectral modulation. Such exemplary scheme can be combined with self-interference fluorescence to facilitate a highly sensitive depth localization of self-interfering radiation generated within a sample. The exemplary system and method can facilitate a scan-free depth sensitivity within the focal depth range for microscopy, endoscopy and nanoscopy.

System and method for efficient detection of the phase and amplitude of a periodic modulation associated with self-interfering fluorescence

An apparatus and method are provided. In particular, a radiation can be provided which includes at least one first electro-magnetic radiation directed to a sample and at least one second electro-magnetic radiation directed to a reference, whereas a frequency of the radiation varies over time. An interference between at least one third radiation associated with the first radiation(s) and at least one fourth radiation associated with the second radiation(s) can be detected to generate an electrical first signal. A second signal associated with at least one phase of at least one frequency component of the electrical first signal can be obtained. Further, comparison data can be generated by comparing the second signal to at least one particular information.

In depth-resolved imaging of scattering media, incident light interacts with tissue in a complex way before the signal reaches the detector: Light interacts with media between the light source and a specific depth, then scatters at that depth and the backscattered light again interacts with media on its way to the detector. The resulting depth-resolved signal therefore likely does not directly represent a physical or optical property of the media at those depths. Exemplary systems, methods and computer-accessible medium can determine physical or optical properties based on such depth-resolved signals. For example, almost all the light can interact with the media, and that the energy of the incident light at a certain depth is likely therefore related to the integral of the scattered light from all deeper locations. Based on the detected signals, the properties of the media can be estimated in an iterative way.

Systems, methods and computer-readable medium for determining depth-resolved physical and/or optical properties of scattering media by analyzing measured data over a range of depths

An apparatus and method are provided. In particular, at least one first electro-magnetic radiation may be provided to a sample and at least one second electro-magnetic radiation can be provided to a non-reflective reference. A frequency of the first and/or second radiations varies over time. An interference is detected between at least one third radiation associated with the first radiation and at least one fourth radiation associated with the second radiation. Alternatively, the first electro-magnetic radiation and/or second electro-magnetic radiation have a spectrum which changes over time. The spectrum may contain multiple frequencies at a particular time. In addition, it is possible to detect the interference signal between the third radiation and the fourth radiation in a first polarization state. Further, it may be preferable to detect a further interference signal between the third and fourth radiations in a second polarization state which is different from the first polarization state. The first and/or second electro-magnetic radiations may have a spectrum whose mean frequency changes substantially continuously over time at a tuning speed that is greater than 100 Tera Hertz per millisecond.

A system and method for imaging of a sample, e.g., biological sample, are provided. In particular, at least one source electro-magnetic radiation forwarded to the sample and a reference may be generated. A plurality of detectors may be used, at least one of the detectors capable of detecting a signal associated with a combination of at least one first electro-magnetic radiation received from the sample and at least one second electro-magnetic radiation received from the reference. At least one particular detector may have a particular electrical integration time, and can receive at least a portion of the signal for a time duration which has a first portion with a first power level greater than a predetermined threshold and a second portion immediately preceding or following the first portion. The second portion may have a second power level that is less than the predetermined threshold, and extends for a time period which may be, e.g., approximately more than 10% of the particular electrical integration time.

System and method for optical coherence imaging

Exemplary apparatus and/or method can be provided using which, it is possible to provide information associated with at least one portion of a sample. For example, at least one electro-magnetic radiation received from the at least one portion of the sample can be separated into a plurality of first radiations, one of the first radiations having a phase delay that is different from a phase delay of another of the first radiations. In addition, at least one of the first radiations can be received and separated into second radiations according to wavelengths of the received at least one of the first radiations. Further, it is possible to detect the second radiations and generate information regarding a position of the at least one portion of the sample as a function of at least one characteristic of at least one interference of the first radiations. According to another exemplary embodiment, it is possible to provide system, method and computer accessible medium, in which data associated with first radiations can be obtained, and the information regarding a position of the at least one portion of the sample may be generated. Such information can be generated based on the data by separating second radiations associated with the portion(s) of the sample according to wavelengths of at least one of the second radiations. For example, one of the second radiations can have a phase delay that is different from a phase delay of another one of the second radiations, and the second radiations may be interfering.

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Amstelveen, Netherlands

Johannes Fitzgerald De Boer