Patent Grant
11835461
This application claims priority to German patent application DE 10 2019 101 773.4, filed Jan. 24, 2019, the entire content of which is incorporated herein by reference.
The present disclosure relates to a microscopy system and to a method for operating a microscopy system. In particular, the microscopy system and the method serve for simultaneously observing fluorescent and non-fluorescent regions of an object admixed with a fluorescent dye, for example protoporphyrin IX (PpIX) or fluorescein.
Microscopy systems for simultaneously or sequentially observing fluorescent and non-fluorescent regions of an object are used for example in the field of tumour surgery. A fluorescent dye is added to a tumorous tissue and binds to the tumorous tissue. However, the fluorescent dye does not bind to non-tumorous tissues. After the fluorescent dye has been excited, the tumorous tissue can be localized by recording an image of the tissue by fluorescent light and identifying the fluorescent regions therein.
In order that the tumorous tissue can be removed from the healthy tissue surrounding the tumorous tissue, the tumorous tissue has to be identified and localized relative to its surroundings. It is therefore necessary also to capture the surroundings, that is to say non-fluorescent regions of the object.
In order to achieve this, in conventional microscopy systems for simultaneously observing fluorescent and non-fluorescent regions of an object, use if made of a white light source having a spectrally approximately homogenous intensity in the visible wavelength range, for example a xenon lamp. The setting of the wavelength-dependent intensity of illumination light that is fed to the object is usually set by way of one or more illumination filters. The light emanating from the object and including both fluorescent light and light reflected at non-fluorescent regions is usually filtered by an observation filter and fed to an observer.
Since the ratio between the intensity of the fluorescent light and the intensity of the light used for exciting the fluorescent dye is very small, the fluorescent light and light reflected at non-fluorescent regions of the object are perceived as having greatly different brightnesses, which makes it more difficult to localize the fluorescent regions and thus the tumorous tissue. Moreover, the intensity of the fluorescent light that emanates from low grade tumors, in comparison with the intensity of the fluorescent light that emanates from high grade tumors, is smaller by a factor of up to 20, which additionally hampers the localization.
Moreover, the color rendering of non-fluorescent regions is often not true color, but rather characterized by a dominant color, with the result that the non-fluorescent region is presented to the surgeon in an unnatural color, which hampers the orientation in the non-fluorescent region. This rendering that is not true color is in part also caused by the fact that better profiles of the wavelength-dependent transmittances of the filters are technically not realizable, for example are not realizable as interference filters.
It is an object of the present disclosure to provide a microscopy system, a method for operating a microscopy system, and a microscopy method which solves the problems mentioned above.
First Aspect
In accordance with a first aspect of the disclosure, a microscopy system for simultaneously observing fluorescent and non-fluorescent regions of an object includes a microscopy optical unit configured to image an object plane through an observation beam path onto an image plane, an observation filter arrangeable in the observation beam path, at least two (narrowband) light sources, and a controller configured to control one or a plurality of the at least two light sources individually, with the result that the ratio of the intensities of the light generated by the at least two light sources is variable.
An image detector can be arranged in the image plane of the microscopy optical unit in order thus to record an image of an object arranged in the object plane.
Of the at least two light sources, (at least) a first light source is configured to generate first light and to direct it onto the object region, wherein the first light is suitable for exciting a fluorescent dye present in the object. For this purpose, the first light includes light having wavelengths in the absorption range of the fluorescent dye. For PpIX, the first light can include wavelengths in the range of 380 nm to 420 nm.
Of the at least two light sources, (at least) a second light source is configured to generate second light and to direct it onto the object region, wherein the second light serves for visualizing non-fluorescent regions of the object. For this purpose, the second light includes light having wavelengths outside the absorption and emission ranges of the fluorescent dye.
One or a plurality of the light sources can be narrowband. Narrowband light sources generate light in accordance with a spectral intensity distribution, wherein the spectral intensity distribution has a maximum spectral emission intensity at a central wavelength and wherein the difference between an upper limiting wavelength, at which the spectral emission intensity is 1% of the maximum spectral emission intensity and which is larger than the central wavelength, and a lower limiting wavelength, at which the spectral emission intensity is 1% of the maximum spectral emission intensity and which is less than the central wavelength, is at most 150 nm, in particular at most 100 nm, more particularly at most 50 nm or at most 20 nm or at most 10 nm.
One or a plurality of the light sources can be controlled individually by the controller. That is to say that a light source can be controlled independently of the other light sources. The intensity of the light generated by the individually controllable light sources can thus be set individually. The ratio of the intensities of light generated by different light sources can thus be varied. By way of example, the controller is configured to vary the operating current and/or the operating voltage of the individually controllable light sources in order thereby to vary the intensity of the light generated by said light sources. The light sources are light emitting diodes, for example.
The (wavelength-dependent) transmittance of the observation filter is defined—as usual—as the ratio of the intensity of light of one wavelength that is transmitted by the observation filter to the intensity of light of the same wavelength that is directed onto the observation filter.
The transmittance of the observation filter is embodied such that it blocks (does not transmit) the light used for exciting the fluorescent dye, that it transmits to a predetermined degree the light used for visualizing non-fluorescent regions and that it transmits the fluorescent light in the best possible manner.
The following advantages are afforded by the individual settability of the light sources and thus of the spectral intensity components of the light directed onto the object and the suitable choice of the transmittance in the wavelength ranges used for visualizing non-fluorescent regions:
Firstly, the fluorescent regions and the non-fluorescent regions can be perceived as almost equally bright by virtue of the intensity of the light generated by the individual light sources being set accordingly. The first light source can be used to set the intensity of the fluorescent light emanating from the fluorescent regions (substantially independently of the second light source). The second light source can be used to set the intensity of the light reflected from the object at non-fluorescent regions (substantially independently of the first light source). The intensities of the light emanating from fluorescent and non-fluorescent regions can thus be coordinated with one another, with the result that both regions appear to be approximately equally bright.
Furthermore, all light sources can be operated in their emission-stable working ranges. The emission spectrum of light sources is generally not stable at very small operating currents and/or voltages. That is to say that the emission spectrum changes as the operating current changes. In order to avoid this, all light sources can be operated in their emission-stable working ranges, for example by all light sources being operated with at least 0.1% of their respective maximum power consumption. In order that the intensity of the light which is used for visualizing non-fluorescent regions and which is operated by a light source with at least 0.1% of its maximum power consumption is approximately equal to the intensity of the fluorescent light (i.e., fluorescent and non-fluorescent regions appear equally bright), the transmittance of the observation filter in the wavelength ranges used for visualizing non-fluorescent regions can be chosen to be correspondingly small. As a result, all light sources can be operated in their emission-stable working ranges.
Furthermore, an illumination filter is not required.
If at least two light sources and at least two separate passbands in the observation filter are used for visualizing non-fluorescent regions, a further advantage is afforded as a result: The color rendering of non-fluorescent regions can be set by the suitable choice of the intensities of the light generated by the light sources used for visualizing non-fluorescent regions and the transmittances of the passbands correspondingly provided for this purpose in the observation filter. In particular, the color rendering can be set to a true color rendering.
In the exemplary embodiments described below, the transmittance of the observation filter from λ1 to λ2 is less than W1, from λ3 to λ4 is larger than W2 and from λ5 to λ6 is larger than W3, wherein λ1, λ2, λ3, λ4, λ5, and λ6 are wavelengths for which 350 nm<λ1<λ2≤λ3<λ4≤λ5<λ6<750 nm holds true, and wherein W1, W2, and W3 are values for which 0<W1<W2<W3<1 holds true; and a first light source is configured to generate first light having wavelengths of between λ1 and λ2, and a second light source is configured to generate second light having wavelengths of between λ3 and λ4.
For the simultaneous observation of fluorescent and non-fluorescent regions of an object admixed with PpIX, the observation filter and the light sources can be configured as follows:
350 nm<λ1<400 nm; and/or 410 nm<λ2<440 nm; and/or
440 nm<λ3<460 nm; and/or 480 nm<λ4<620 nm; and/or
530 nm<λ5<620 nm; and/or 650 nm<λ6<750 nm; and/or
W1=0.1% or W1=0.01%; and/or
W2=1%; and/or
W3=90%.
For observing the non-fluorescent regions in the blue wavelength range, as is customary and desired in specific applications, the following settings furthermore hold true: 480 nm<λ4<520 nm, and/or wherein the transmittance of the observation filter from λ3 to λ4 is larger than 10% and less than 60%, and/or wherein the transmittance of the observation filter from λ2+Δ to λ3−Δ and from λ4+Δ to λ5−Δ is less than 0.1 times W1, wherein 3 nm≤Δ≤10 nm holds true, and/or wherein the intensity of the first light above λ3 is at most 1% of its maximum spectral intensity, and/or wherein the intensity of the second light below λ2 and above λ5 is at most 1% of its maximum spectral intensity.
In order to be able to set the color rendering of the non-fluorescent regions, in particular to a true color rendering, the microscopy system further includes a third light source configured to generate third light having wavelengths of between λ7 and λ8 and to direct it onto the object plane, wherein λ7, λ8 are wavelengths and λ2<λ7<λ8<λ5 holds true. A description is given below of some configurations used to achieve a true color rendering of the non-fluorescent regions by suitable operation of the light sources.
The transmittance of the observation filter from λ3 to λ6 is larger than W3. Typically, the intensity of the first light above λ3 is at most 1% of its maximum spectral intensity. Typically, the intensity of the second light below λ2 and above λ5 is at most 1% of its maximum spectral intensity. Typically, the intensity of the third light below λ2 and above λ5 is at most 1% of its maximum spectral intensity.
The transmittance of the observation filter from λ3 to λ4 is less than 5% and 600 nm<λ4<λ5<620 nm holds true. Typically, the intensity of the first light above λ3 is at most 1% of its maximum spectral intensity. Typically, the intensity of the second light below λ2 and above λ5 is at most 1% of its maximum spectral intensity. Typically, the intensity of the third light below λ2 and above λ5 is at most 1% of its maximum spectral intensity.
With further preference, the microscopy system according to the third exemplary embodiment further includes an illumination filter arrangeable between the light sources and the object plane, wherein the transmittance of the illumination filter from λ1 to λ3′ and from λ4′ to λ4 is larger than W3 and from λ3′+Δ to λ4′−Δ and from λ4+Δ is less than W1, wherein 3 nm≤Δ≤10 nm holds true, and wherein λ3′ and λ4′ are wavelengths and λ3<λ3′<λ4′<λ4 and 480 nm<λ3′<520 nm and 520 nm<λ4′<550 nm and λ4′−λ3′>20 nm hold true. Typically, the intensity of the first light above λ3 is at most 1% of its maximum spectral intensity. Typically, the intensity of the second light below λ2 and above λ4′ is at most 1% of its maximum spectral intensity. Typically, the intensity of the third light between λ4′ and λ4 is significantly high and below λ3′ and above λ5 is at most 1% of its maximum spectral intensity.
The transmittance of the observation filter from λ3 to λ4 is less than 5%; the transmittance of the observation filter from λ7 to λ8 is larger than W2 and less than 5%, and the transmittance of the observation filter from λ4+Δ to λ7−Δ is less than W1, wherein 3 nm<Δ<10 nm holds true, wherein λ7 and λ8 are wavelengths and wherein λ4<λ7<λ8<λ5 and 480 nm<λ4<520 nm and 520 nm<λ7<550 nm and λ7 −λ4>20 nm and λ5 −λ8<30 nm hold true. Typically, the intensity of the first light above λ3 is at most 1% of its maximum spectral intensity. Typically, the intensity of the second light below λ2 and above λ7 is at most 1% of its maximum spectral intensity. Typically, the intensity of the third light below λ4 and above λ5 is at most 1% of its maximum spectral intensity.
The transmittance of the observation filter from λ3 to λ4 is less than 5%, the transmittance of the observation filter from λ4+Δ to λ5 −Δ is less than W1, wherein 480 nm<λ4<520 nm and 530 nm<λ5<560 nm and λ5 −λ4>20 nm hold true. The microscopy system further includes an illumination filter arrangeable between the light sources and the object plane, wherein the transmittance of the illumination filter from λ1 to λ4 is larger than W3, wherein the transmittance of the illumination filter from λ4+Δ to λ5′−Δ is less than W1, wherein the transmittance of the illumination filter from λ5′ to λ6′ is larger than W2 and less than 5%, wherein the transmittance of the illumination filter from λ6′ to λ6 is less than W1, wherein 3 nm≤Δ≤10 nm holds true, wherein λ5′ and λ6′ are wavelengths and λ4<λ5′<λ6′<λ6 holds true, and wherein 530 nm<λ5′<570 nm and 600 nm<620 nm hold true. Typically, the intensity of the first light above λ3 is at most 1% of its maximum spectral intensity. Typically, the intensity of the second light below λ2 and above λ5 is at most 1% of its maximum spectral intensity. Typically, the intensity of the third light below λ4 and above λ5 is at most 1% of its maximum spectral intensity.
For the simultaneous observation of fluorescent and non-fluorescent regions of an object admixed with PpIX, the light sources configured as follows are suitable, in particular, for the embodiments described above: The first light source can be a light emitting diode having a spectral emission maximum in the range of 400 nm to 420 nm and a full width at half maximum in the range of 10 nm to 20 nm. The second light source can be a light emitting diode having a spectral emission maximum in the range of 440 nm to 470 nm and a full width at half maximum in the range of 20 nm to 50 nm. The third light source can be a light emitting diode having a spectral emission maximum in the range of 500 nm to 560 nm and a full width at half maximum in the range of 40 nm to 110 nm.
For the simultaneous observation of fluorescent and non-fluorescent regions of an object admixed with fluorescein, the microscopy system furthermore includes a third light source configured to generate third light having wavelengths of between λ5′ and λ6′ and to direct it onto the object plane, an illumination filter arrangeable between the light sources and the object plane, wherein the transmittance of the illumination filter from λ1 to λ4 is larger than W3, wherein the transmittance of the illumination filter from λ5′ to λ6′ is larger than W2 and less than 5%, wherein λ5′, λ6′ are wavelengths and λ5<λ5′<λ6′ holds true, and wherein the transmittance of the observation filter from λ3 to λ4 is less than 5%.
Typically, the transmittance of the illumination filter from λ4+Δ to λ5′−Δ is less than W1, wherein 3 nm<Δ<10 nm holds true. Typically, the transmittance of the illumination filter from λ6′ to 750 nm is less than W1. Typically, the transmittance of the observation filter from λ4+Δ to λ5−Δ is less than W1, wherein 3 nm<Δ<10 nm holds true.
The observation filter and the light sources can be configured as follows for the simultaneous observation of fluorescent and non-fluorescent regions of an object admixed with fluorescein:
350 nm<λ1<460 nm; and/or 460 nm<λ2<480 nm; and/or
470 nm<λ3<490 nm; and/or 490 nm<λ4<510 nm; and/or
520 nm<λ5<550 nm; and/or 680 nm<λ6<750 nm; and/or
620 nm<λ5′<650 nm; and/or 680 nm<λ6′<750 nm; and/or
W1=0.1% or W1=0.01%; and/or
W2=0.5%; and/or
W3=90%.
Typically, the intensity of the first light above λ5 is at most 1% of its maximum spectral intensity. Typically, the intensity of the second light below λ3 and above λ5′ is at most 1% of its maximum spectral intensity. Typically, the intensity of the third light below λ4 is at most 1% of its maximum spectral intensity.
For the simultaneous observation of fluorescent and non-fluorescent regions of an object admixed with fluorescein, the light sources configured as follows are suitable, in particular, for the exemplary embodiments described above: The first light source can be a light emitting diode having a spectral emission maximum in the range of 440 nm to 470 nm and a full width at half maximum in the range of 10 nm to 20 nm. The second light source can be a light emitting diode having a spectral emission maximum in the range of 500 nm to 560 nm and a full width at half maximum in the range of 40 nm to 110 nm. The third light source can be a light emitting diode having a spectral emission maximum in the range of 600 nm to 640 nm and a full width at half maximum in the range of 10 nm to 20 nm.
Typically, wavelength-dependent transmittances of the illumination filter and of the observation filter are coordinated with one another such that between 350 nm and 750 nm no wavelength exists at which both the absolute value of the wavelength-dependent gradient of the transmittance of the illumination filter and the absolute value of the wavelength-dependent gradient of the transmittance of the observation filter are larger than 2%/nm. This prevents a large change in the transmittance of the illumination filter and of the observation filter at a wavelength. Production dictated tolerances with regard to the transmittance of the illumination filter and of the observation filter therefore do not significantly affect the trueness of color and the brightness of different spectral ranges which are achieved with the illumination filters and observation filters.
Second Aspect
A second aspect of the present disclosure relates to a method for operating a microscopy system, in particular one of the microscopy systems described herein.
The method includes: generating illumination light and directing the generated illumination light onto an object; generating an observation beam path, which images the object into an image plane, wherein an observation filter is arranged in the observation beam path. The illumination light is generated such that
|{right arrow over (W)}−{right arrow over (f)}|≤0.2 (1)
holds true, wherein {right arrow over (W)} represents a color locus of a white point in the CIE standard chromaticity diagram of the CIE 1931 standard colorimetric system, and {right arrow over (f)} represents a color locus having coordinates xf and yf in the CIE standard chromaticity diagram of the CIE 1931 standard colorimetric system.
The distance |⋅| between a color locus {right arrow over (A)} having coordinates xA and yA in the CIE standard chromaticity diagram of the CIE 1931 standard colorimetric system and a color locus {right arrow over (B)} having coordinates xB and yB and in the CIE standard chromaticity diagram of the CIE 1931 standard colorimetric system is defined as:
The coordinates xf and yf of the color locus {right arrow over (f)} are defined by
wherein X , Y and Z represent tristimulus values of the CIE 1931 standard colorimetric system which are defined by
X=k∫I(λ)·T(λ)·
Y=k∫I(λ)·T(λ)·
Z=k∫I(λ)·T(λ)·
wherein I(λ) represents the intensity of the illumination light, T(λ) represents the transmittance 41, 61, 81, 101, 121, 141, 161 of the observation filter 23, {right arrow over (x)}(λ), {right arrow over (y)}(λ), and {right arrow over (z)}(λ) represent the spectral value functions of the TRG909926 CIE 1931 standard colorimetric system, and k is a constant.
The white point can be for example the white point D50 having the coordinates x=0.3457 and y=0.3585 in the CIE standard chromaticity diagram of the CIE 1931 standard colorimetric system. Alternatively, the white point can be for example the white point D65 having the coordinates x=0.3127 and y=0.329 in the CIE standard chromaticity diagram of the CIE 1931 standard colorimetric system. As a further alternative, the white point can correspond to a color valence whose color locus is at a distance of at most 0.2, in particular at most 0.1 or at most 0.05, from the color locus of the white point D50 in the CIE 1976 u′v′ chromaticity diagram.
The distance |⋅| between a color locus {right arrow over (A)} having coordinates u′A and v′A in the CIE 1976 u′v′ chromaticity diagram and a color locus {right arrow over (B)} having coordinates u′B and v′B in the CIE 1976 u′v′ chromaticity diagram is defined as:
Typically, the illumination light is generated such that |{right arrow over (W)}−{right arrow over (f)}|≤0.15 or |{right arrow over (W)}−{right arrow over (f)}|≤0.1 holds true. The integrals over the wavelength λ are integrated from 380 nm to 780 nm.
Equation 1 describes a condition for a maximum color valence distance in the CIE 1931 standard chromaticity diagram. In this case, {right arrow over (f)} represents a color locus in the CIE standard chromativcity diagram of the CIE 1931 standard colorimetric system that is obtained if illumination light of the intensity I(λ) impinges on a white object and the light emanating from the white object is filtered by an observation filter having the transmittance T(λ). The required small distance from the white point in the CIE 1931 standard chromaticity diagram means that the white object can be observed as approximately white. When applied to general objects, this means that the object can be observed as approximately true color. This facilitates the orientation in the operating area for a surgeon.
The illumination light is generated for example by a plurality of light sources that generate light in different wavelength ranges. Generating the illumination light can include: setting, in particular varying, an energy fed to at least one of the plurality of light sources for generating the illumination light.
The method can be carried out by the microscopy systems described herein.
Third Aspect
A third aspect of the present disclosure relates to a microscopy method in which fluorescent regions and non-fluorescent regions can be perceived as approximately equally bright.
For this purpose, the microscopy method includes: generating illumination light and directing the generated illumination light onto an object, generating an observation beam path, which images the object into an image plane, wherein an observation filter is arranged in the observation beam path, wherein a first value, which represents a mean value of the transmittance of the observation filter over a first wavelength range, is less than a second value, which represents a mean value of the transmittance of the observation filter over a second wavelength range, wherein the second value is less than a third value, which represents a mean value of the transmittance of the observation filter over a third wavelength range, wherein a fourth value, which represents a mean value of the intensity of the illumination light over the first wavelength range is larger than a fifth value, which represents a mean value of the intensity of the illumination light over the second wavelength range, wherein the fifth value is larger than a sixth value, which represents a mean value of the intensity of the illumination light over the third wavelength range, wherein the first, second, and third wavelength ranges do not overlap one another and are in each case between 350 nm and 1000 nm.
The first wavelength range corresponds to that wavelength range in which a fluorescent dye present in the object has a significant absorption. In order to be able to excite the fluorescent dye efficiently, the illumination light in the first wavelength range has a high intensity characterized by the fourth value. In order that light in the first wavelength range that is reflected at the object does not swamp the fluorescent light generated substantially exclusively in the third wavelength range, the observation filter has in the first wavelength range a low transmittance characterized by the first value.
In order that the fluorescent light can be observed efficiently, the observation filter has in the third wavelength range a high transmittance characterized by the third value. In order that the fluorescent light is not swamped by illumination light in the third wavelength range that is reflected at the object, the illumination light in the third wavelength range has a low intensity characterized by the sixth value.
The second wavelength range serves for visualizing non-fluorescent regions of the object. For this purpose, the illumination light has a medium intensity in the second wavelength range, said intensity being characterized by the fifth value, and the observation filter has in the second wavelength range an average transmittance characterized by the second value.
The light in the first and second wavelength ranges that is transmitted by the observation filter brings about the visualization of non-fluorescent regions of the object and thus predominantly contributes to the brightness of the non-fluorescent regions in the image plane. The light in the third wavelength range that is transmitted by the observation filter brings about the visualization of fluorescent regions of the object and thus predominantly contributes to the brightness of the fluorescent regions in the image plane. The indicated relation of the first to sixth values with respect to one another has the effect that the non-fluorescent regions and the fluorescent regions of the object appear approximately equally bright. Moreover, they are coordinated with one another such that moreover an approximately true color observation of non-fluorescent regions is made possible.
The first wavelength range can contain wavelengths at which an absorption rate—normalized to their maximum value—of the fluorescent dye present in the object is at least 5%, in particular at least 10%, more particularly at least 50%. Accordingly, the first wavelength range contains those wavelengths at which the fluorescent dye can be excited efficiently.
The third wavelength range can contain wavelengths at which an emission rate—normalized to their maximum value—of the fluorescent dye present in the object is at least 5%, in particular at least 10%, more particularly at least 50%. Accordingly, the third wavelength range contains those wavelengths at which the fluorescent dye can be excited efficiently.
The second wavelength range can contain exclusively wavelengths at which an absorption rate—normalized to their maximum value—of the fluorescent dye present in the object is at most 20%, in particular at most 10%, more particularly at most 5%, and at which an emission rate—normalized to their maximum value—of the fluorescent dye present in the object is at most 20%, in particular at most 10%, more particularly at most 5%. Accordingly, the second wavelength range contains substantially only those wavelengths which lie outside the wavelength ranges in which the fluorescent dye can be excited efficiently and generates fluorescent light.
With the use of the fluorescent dye protoporphyrin IX, the first wavelength range typically includes the wavelength 405 nm and/or wavelengths of 390 nm to 420 nm, the second wavelength range typically includes wavelengths of 450 nm to 600 nm and the third wavelength range typically includes wavelengths of 620 nm to 720 nm.
With the use of the fluorescent dye fluorescein, the first wavelength range typically includes wavelengths of 480 nm to 500 nm, the second wavelength range typically includes wavelengths of 620 nm to 750 nm and the third wavelength range typically includes wavelengths of 550 nm to 600 nm.
Typically, a ratio of the first value to the second value is at most 1/100, in particular at most 1/1000. Typically, a ratio of the second value to the third value is at most 0.9, in particular at most 0.8, more particularly at most 0.5. Typically, a ratio of the fourth value to the fifth value is at least 2, in particular at least 5. Typically, a ratio of the fourth value to the sixth value is at least 1000, in particular at least 10000. Both an approximately equal brightness and an approximately true color rendering are achieved as a result.
The illumination light can be generated using a plurality of (narrowband) light sources, for example using the light sources described with regard to other aspects. At least one of the light sources generates light having wavelengths in the first wavelength range; at least one of the light sources generates light having wavelengths in the second wavelength range. At least one of the light sources can be individually controllable in order thereby to be able to vary the ratio between the intensity of the light having wavelengths in the first wavelength range and the intensity of the light having wavelengths in the second wavelength range.
Typically, the light sources generate substantially no light having wavelengths in the third wavelength range. This prevents the light generated by the light sources from corrupting the fluorescent light in the third wavelength range.
An alternative microscopy method includes generating illumination light and directing the generated illumination light onto an object, generating an observation beam path, which images the object into an image plane, wherein the illumination light is generated such that a ratio of a first characteristic value to a second characteristic value has a value in the range of 20/1 to 1/20, wherein the first characteristic value is a value of a characteristic variable for the intensity of light of the observation beam path at first locations in the image plane, at which first locations color valences of the light of the observation beam path lie within a first color valence range of a color space, wherein the second characteristic value is a value of the characteristic variable for the intensity of the light of the observation beam path at second locations in the image plane, at which second locations color valences of the light of the observation beam path lie within a second color valence range of the color space.
Typically, the illumination light is generated such that the ratio of the first characteristic value to the second characteristic value has a value in the range of 10/1 to 1/10 or 5/1 to 1/5 or 3/1 to 1/3.
A projected image of the object is generated in the image plane through the observation beam path. If a fluorescent dye present in the object is excited by the illumination light, the projected image generally includes fluorescent regions (first locations) and non-fluorescent regions (second locations). Strongly fluorescent regions (first locations) have in the projected image the color valences typical of the fluorescent dye, which lie within the first color valence range. Weakly fluorescent and non-fluorescent regions (second locations) have in the projected image other color valences, which lie within the second color valence range. Accordingly, the first and second color valence ranges are non-overlapping ranges of the same color space.
Fluorescent regions of the object (first locations) can be distinguished from non-fluorescent regions (second locations) in the image plane on the basis of the color valences typical of the fluorescent dye. In order that both fluorescent and non-fluorescent regions can be distinguished by an observer or a controller, it is advantageous if the fluorescent and the non-fluorescent regions appear approximately equally bright, that is to say have an intensity of approximately equal magnitude or a luminous flux of approximately equal magnitude in the image plane. Luminous flux denotes that proportion of a radiation power which is visible to the human eye, weighted with the luminous efficiency curve of the human eye.
This is achieved in the microscopy method by virtue of the illumination light being generated such that the ratio of the first characteristic value to the second characteristic value has a value in the range of 20/1 to 1/20. The first characteristic value represents for example the mean value of the intensity of the light in the observation beam path in the image plane at the first locations, that is to say those locations in the image plane at which the light in the observation beam path has the color valences typical of the fluorescent dye. In this example, the second characteristic value represents the mean value of the intensity of the light in the observation beam path in the image plane at the second locations, that is to say those locations in the image plane at which the light in the observation beam path does not have the color valences typical of the fluorescent dye.
The first characteristic value and the second characteristic value respectively represent a value of a characteristic variable of the same type. By way of example, if the first characteristic value represents a maximum value, then the second characteristic value likewise represents a maximum value. Alternatively, if the first characteristic value represents a mean value, for example, then the second characteristic value likewise represents a mean value.
The first characteristic value can represent a maximum value or a mean value of the intensity (or of the luminous flux) of the light of the observation beam path at the first locations. The second characteristic value can represent a maximum value or a mean value of the intensity (or of the luminous flux) of the light of the observation beam path at the second locations.
The microscopy method can furthermore include determining the first locations in the image plane, at which first locations the color valences of the light of the observation beam path lie within the first color valence range of the color space, determining the second locations in the image plane, at which second locations the color valences of the light of the observation beam path lie within the second color valence range of the color space, wherein the illumination light is generated depending on the intensity of the light of the observation beam path at the first locations determined and depending on the intensity of the light of the observation beam path at the second locations determined. As a result, the first and second locations in the image plane are identified and the illumination light is generated depending on the intensity at these locations.
The microscopy method can further include determining the intensity of the light in the observation beam path at the first and second locations for determining the luminous flux of the light in the observation beam path at the first and second locations. By way of example, an image detector is arranged in the image plane, and is configured to record a color image of the projected image, based on which firstly the first and second locations can be identified and secondly the intensity of the light in the observation beam path at the first and second locations can be determined.
The microscopy method can furthermore include recording an image of the object in the image plane, wherein the image includes a plurality of image points, comparing color valences at the image points of the image with the first color valence range and/or with the second color valence range, determining first image points from the plurality of image points based on a result of the comparison, wherein the first image points correspond to the first locations in the image plane and wherein color valences at the first image points lie within the first color valence range of the color space, and determining second image points from the plurality of image points on the basis of a result of the comparison, wherein the second image points correspond to the second locations in the image plane and wherein color valences at the second image points lie within the second color valence range of the color space.
The microscopy method can further includes determining the first characteristic value on the basis of the determined intensity of the light of the observation beam path at the first locations determined, and determining the second characteristic value on the basis of the determined intensity of the light of the observation beam path at the second locations determined, wherein the illumination light is generated depending on the first characteristic value determined and depending on the second characteristic value determined. Accordingly, the first and second characteristic values are determined, for example calculated, specifically based on the determined or measured intensity values at the first and second locations that were identified previously on the basis of a recorded image and on the basis of their color valences, in particular by comparison with the first and second color valence ranges. The first and second characteristic values thus obtained are then used for generating the illumination light.
The illumination light is generated for example by a plurality of light sources which generate light in different wavelength ranges. Generating the illumination light can include setting, in particular varying, an energy fed to at least one of the plurality of light sources for generating the illumination light, depending on the first and second characteristic values.
In particular, provision can be made for the illumination light to be generated independently of the intensity of light of the observation beam path at third locations in the image plane, wherein color valences of the light of the observation beam path at the third locations lie outside the first and second color valence ranges. That is to say that exclusively the intensity of the light in the observation beam path at the first and second locations is used for generating the illumination light. The intensity of the light in the observation beam path at other locations in the image plane is not used for generating the illumination light.
The first color valence range and the second color valence range can be chosen such that a smallest color difference between the first color valence range and the second color valence range in the CIE 1976 u′v′ chromaticity diagram is at least 0.01, in particular at least 0.1. Furthermore, the first color valence range can be chosen such that it is limited to color valences which have a color difference of at most 0.1, in particular at most 0.03 or at most 0.01, with respect to reference color valences in the CIE 1976 u′v′ chromaticity diagram, wherein the reference color valences correspond to light in a reference wavelength range containing exclusively wavelengths at which an emission rate—normalized to their maximum value—of a fluorescent dye present in the object is at least 5%, in particular at least 10%, more particularly at least 50%. The reference color valence is for example a color valence which corresponds to the emission spectrum of a fluorescent dye in the object. Accordingly, only such color valences which are separated from said reference color valence by not more than the maximum difference indicated belong to the first color valence range.
If the fluorescent dye is PpIX, it is typical for the first color valence range to include a color valence which corresponds to light having a wavelength of 635 nm. Furthermore, it is typical for the first color valence range to be limited to color valences which have a color difference of at most 0.1, in particular at most 0.03 or at most 0.01 with respect to a reference color valence corresponding to light having a wavelength of 635 nm in the CIE 1976 u′v′ chromaticity diagram.
If the fluorescent dye is fluorescein, it is typical for the first color valence range to comprise a color valence which corresponds to light having a wavelength of 530 nm. Furthermore, it is typical for the first color valence range to be limited to color valences which have a color difference of at most 0.1, in particular at most 0.03 or at most 0.01 with respect to a reference color valence corresponding to light having a wavelength of 530 nm in the CIE 1976 u′v′ chromaticity diagram.
Features of the first, second, and third aspects can be combined with one another.
The observation filters and illumination filters described herein can be embodied for example as interference filters. Interference filters include a plurality of layers of materials having different optical properties, for example different refractive indices. Each layer can have a different thickness. The number of layers can be between a few and several hundred, depending on the requirements made of the filter. The transmittances described herein can be realized by the specific choice of the thickness and the optical property of each layer.
Aids for determining the thicknesses and optical properties of the layers of a filter depending on a predefined wavelength-dependent transmittance are known. Such layer sequences can be designed using simulation programs that use as input data the optical properties (refractive index and absorption depending on the wavelength, dispersion) of the materials to be used and also the desired transmission and/or reflection spectrum. The simulation program outputs the simulated transmission and/or reflection spectrum and also the layer sequence and/or the thickness of the layers and the optical properties and/or materials used. The calculation can be carried out in an iteration method. In this way, even filters with complicated requirements, e.g. multiband filters, can be designed and produced.
The disclosure will now be described with reference to the drawings wherein:
The microscopy system 1 includes an illumination device 3. The illumination device 3 comprises a plurality of light sources 5, an illumination optical unit 7 and an illumination filter 9, which can optionally be arranged in an observation beam path 10 formed by the illumination optical unit 7. This is illustrated by a double headed arrow in
The microscopy system 1 includes a controller 12 configured to control the plurality of light sources 5 individually, i.e., independently of one another. By way of example, the light sources are two or more light emitting diodes. Each of the light emitting diodes can be controlled individually by the controller 12. By way of example, the controller 12 controls the operating current and/or the operating voltage fed and/or respectively applied to a light emitting diode in order to generate light. The intensity of the light generated by the light sources 5 can be set individually as a result.
By the observation beam path 10, the illumination device 3 directs illumination light onto the object region 11, in which an object 13 can be arranged, which can be admixed with a fluorescent dye. The fluorescent dye fed to the object 13 accumulates greatly in some regions of the object 13 (fluorescent regions). These regions contain tumor cells, for example, to which the fluorescent dye binds. The fluorescent dye does not accumulate or accumulates only slightly in other regions of the object 13 (non-fluorescent regions). These regions contain no tumor cells, for example.
The microscopy system 1 further includes a microscopy optical unit 14, which in the present example includes an objective 15 and further lenses 16 and 17. The microscopy optical unit 14 is configured to image the object region 11, in particular an object plane 18, onto an image plane 19. In the present example, a detection area of a light detector 20 of the microscopy system 1 is arranged in the image plane 19. The light detector 20 can be an image sensor for example. The light detector 20 outputs a signal representing the intensity of the light impinging on the detection area of the light detector 20. The light detector 20 is connected to the controller 12 and the controller 12 receives from the light detector 20 the signal 21 output by the latter. The controller can process and display the image generated by the light detector 20. Instead of or in addition to the light detector 20, an eyepiece can be provided, which, in conjunction with the microscopy optical unit 14, is suitable for imaging the object plane 18 onto the retina of an eye.
An observation filter 23 can be arranged in the observation beam path 22 provided by the microscopy optical unit 14, said observation beam path imaging the object plane 18 onto the image plane 19. Furthermore, an actuator (not shown) can be provided, which can introduce the observation filter 23 into the observation beam path 22 and can withdraw the observation filter 23 from the observation beam path 22. This is illustrated by a double headed arrow in
Depending on the configuration of the plurality of light sources 5, of the illumination filter 9 and of the observation filter 23, fluorescent and non-fluorescent regions of the object 13 can be observed simultaneously. Various exemplary embodiments for the fluorescent dyes protoporphyrin IX (PpIX) and fluorescein are described below.
The fluorescent dye PpIX has an absorption spectrum PpIX which between 350 nm and 430 nm has a normalized absorption intensity of more than 0.2. The normalized absorption intensity is normalized to the maximum absorption intensity, i.e., the normalized absorption spectrum only has values of between 0 and 1. The fluorescent dye PpIX can therefore be excited efficiently in the range of 350 nm to 430 nm. The fluorescent dye PpIX has the maximum of the absorption at approximately 405 nm. The fluorescent dye PpIX emits fluorescent light in a spectral range from approximately 600 nm to 750 nm, with a main maximum of the emission intensity lying at 635 nm and a secondary maximum lying at approximately 705 nm.
The fluorescent dye fluorescein has a normalized absorption intensity of more than 0.2 between approximately 450 nm and 530 nm. Therefore, the fluorescent dye fluorescein can be excited well in this range. The absorption spectrum of fluorescein has a maximum at approximately 495 nm. The fluorescent dye fluorescein emits emission light in the range from approximately 490 nm to 650 nm. The maximum of the emission spectrum lies at approximately 520 nm.
Example with Respect to the First Embodiment
The first light source generates an illumination light spectrum 31 having a spectral emission maximum in the range of 400 nm to 410 nm and a full width at half maximum in the range of 10 nm to 20 nm. Below approximately 370 nm and above approximately 450 nm, the intensity of the first light generated by the first light source is at most 1% of its maximum spectral intensity. The first light source is a light-emitting diode, for example.
The second light source generates an illumination light spectrum 32 having a spectral emission maximum in the range of 440 nm to 470 nm and a full width at half maximum in the range of 20 nm to 50 nm. Below approximately 440 nm and above approximately 500 nm, the intensity of the second light generated by the second light source is at most 1% of its maximum spectral intensity. The second light source is a light-emitting diode, for example.
The first and second light sources are operated such that the maximum spectral intensity of the first light source is at most 20 times and at least 3 times the magnitude of the maximum spectral intensity of the second light source.
Accordingly, the observation filter 23 suppresses the first light reflected at the object 13, said first light having a high intensity substantially only between λ1 and λ2. Furthermore, the second light reflected at the object 13, said second light having a high intensity substantially only between λ3 and λ4, is transmitted by the observation filter 23, with the result that non-fluorescent regions of the object 13 can be observed as bluish. Furthermore, the fluorescent light emanating from the object 13, said fluorescent light having a high intensity substantially only between λ5 and λ6 is transmitted by the observation filter 23, with the result that fluorescent regions of the object 13 can be observed as reddish color valences.
Two major advantages are afforded by the individual settability of the intensities of the first and second light (cf.
Examples with Respect to the Second to Sixth Exemplary Embodiments
The first and second light sources correspond to those of the example with respect to the first exemplary embodiment. That is to say that the illumination light spectrum 31 of the first light source of the first exemplary embodiment as illustrated in
The third light source generates an illumination light spectrum 53 having a spectral emission maximum in the range of 500 nm to 560 nm and a fullwidth at half maximum in the range of 40 nm to 110 nm. Below approximately 470 nm and above approximately 630 nm, the intensity of the third light generated by the third light source is at most 1% of its maximum spectral intensity. The third light source is a light-emitting diode, for example.
The first and third light sources are operated such that the maximum spectral intensity of the first light source is at most 20 times and at least 3 times the magnitude of the maximum spectral intensity of the third light source.
Example with Respect to the Second Exemplary Embodiment
Accordingly, the observation filter 23 suppresses the first light reflected at the object 13, said first light having a high intensity substantially only between λ1 and λ2. Furthermore, the second and third light reflected at the object 13, said second and third light having a high intensity substantially only between λ3 and λ4 is transmitted by the observation filter 23, with the result that non-fluorescent regions of the object 13 can be observed as approximately true color. Furthermore, the fluorescent light emanating from the object 13, said fluorescent light having a high intensity substantially only between λ5 and λ6 is transmitted by the observation filter 23, with the result that fluorescent regions of the object 13 can be observed as reddish color valences.
Three major advantages are afforded by the individual settability of the intensities of the first, second and third light (cf.
Example with Respect to the Third Exemplary Embodiment
Accordingly, the observation filter 23 suppresses the first light reflected at the object 13, said first light having a high intensity substantially only between λ1 and λ2. Furthermore, the second and third light reflected at the object 13, said second and third light having a high intensity substantially only between λ3 and λ4 is transmitted by the observation filter 23, with the result that non-fluorescent regions of the object 13 can be observed as approximately true color. Furthermore, the fluorescent light emanating from the object 13, said fluorescent light having a high intensity substantially only between λ5 and λ6 is transmitted by the observation filter 23, with the result that fluorescent regions of the object 13 can be observed as reddish color valences.
The advantages of the example of the second exemplary embodiment can be afforded by the individual settability of the intensities of the first, second and third light (cf.
Example with respect to the fourth exemplary embodiment
From 360 nm to λ3′=500 nm the transmittance 102 of the illumination filter 9 is approximately 95%. From approximately λ3′ to approximately λ4′=560 nm the transmittance 102 of the illumination filter 9 is approximately 0.005%. From λ4′ to approximately λ4 the transmittance 102 of the illumination filter 9 is approximately 95%. From approximately λ4 to λ6 the transmittance 102 of the illumination filter 9 is approximately 0.005%. Furthermore, it holds true that W1=0.01%, W2=1%, and W3=80%.
The illumination filter and the observation filter together have substantially the same effect as the observation filter of the example with respect to the fifth exemplary embodiment. The observation filter suppresses the first light reflected at the object 13, said first light having a high intensity substantially only between λ1 and λ2 and passing through the illumination filter substantially without being damped. Furthermore, the second light reflected at the object 13 is restricted by the illumination filter and the observation filter to wavelengths lying substantially only between λ3 and λ3′. Furthermore, the third light reflected at the object 13 is restricted by the illumination filter and the observation filter to wavelengths lying substantially only between λ4′ and λ4. Light in the wavelength range from λ3′ to λ4′ is effectively suppressed by the illumination filter and the observation filter. Non-fluorescent regions of the object 13 can therefore be observed as approximately true color. Furthermore, the fluorescent light emanating from the object 13 and having a high intensity substantially only between λ5 and λ6 is transmitted by the observation filter 23, with the result that fluorescent regions of the object 13 can be observed with reddish color valences.
Three major advantages are afforded by the individual settability of the intensity 52 of the second light and the intensity 53 of the third light (cf.
The dashed line depicted in
Example with Respect to the Fifth Exemplary Embodiment
Accordingly, the observation filter 23 suppresses the first light reflected at the object 13, said first light having a high intensity substantially only between λ1 and λ2. Furthermore, the fluorescent light emanating from the object 13, said second light having a high intensity substantially only between λ3 and λ4, is transmitted by the observation filter 23. Furthermore, the third light reflected at the object 13 is transmitted efficiently by the observation filter 23 substantially only between λ7 and λ8. Non-fluorescent regions of the object 13 can therefore be observed as approximately true color. Furthermore, the fluorescent light emanating from the object 13, said fluorescent light having a high intensity substantially only between λ5 and λ6 is transmitted by the observation filter 23, with the result that fluorescent regions of the object 13 can be observed as reddish color valences.
The advantages of the example with respect to the third exemplary embodiment can be afforded by the individual settability of the intensities of the first, second, and third light (cf.
The dashed line depicted in
Example with Respect to the Sixth Exemplary Embodiment
From λ1=350 nm to λ2=430 nm the transmittance 141 of the observation filter 23 is approximately 0.005%. From λ3=435 nm to λ4=500 nm the transmittance 141 of the observation filter 23 is approximately 2%. From approximately λ4 to λ5=560 nm the transmittance 141 of the observation filter 23 is approximately 0.005%. From λ5 to λ6=750 nm the transmittance 141 of the observation filter 23 is approximately 95%. Furthermore, it holds true that: W1=0.01%; W2=1%; and W3=80%.
From 360 nm to approximately λ4 the transmittance 142 of the illumination filter 9 is approximately 95%. From approximately λ4 to approximately λ5′=565 nm the transmittance 142 of the illumination filter 9 is approximately 0.005%. From λ5′ to approximately λ6′=620 nm the transmittance 142 of the illumination filter 9 is approximately 2%. From approximately λ6′ to λ6 the transmittance 142 of the illumination filter 9 is approximately 0.005%.
The illumination filter and the observation filter of the example with respect to the sixth exemplary embodiment together have substantially the same effect as the illumination filter and the observation filter of the example with respect to the fifth exemplary embodiment. The observation filter 23 suppresses the first light reflected at the object 13, said first light having a high intensity substantially only between λ1 and λ2 and passing through the illumination filter 9 substantially without being damped. Furthermore, the second light reflected at the object 13 is restricted by the illumination filter and the observation filter to wavelengths lying substantially only between λ3 and λ4. Furthermore, the third light reflected at the object 13 is restricted by the illumination filter and the observation filter to wavelengths lying substantially only between λ5′ and λ6′. Light in the wavelength range from approximately λ4 to λ5 is effectively suppressed by the illumination filter and the observation filter. Non-fluorescent regions of the object 13 can therefore be observed as approximately true color. Furthermore, the fluorescent light emanating from the object 13 and having a high intensity substantially only between λ6′ and λ6 is transmitted by the observation filter 23, with the result that fluorescent regions of the object 13 can be observed with reddish color valences.
Example with Respect to the Seventh Exemplary Embodiment
The first light source serves substantially exclusively for exciting the fluorescent dye fluorescein, i.e. for visualizing fluorescent regions of the object. The second and third light sources serve substantially exclusively for visualizing non-fluorescent regions of the object.
The first light source generates an illumination light spectrum 151 having a spectral emission maximum in the range of 440 nm to 470 nm and a full width at half maximum in the range of 20 nm to 50 nm. Below approximately 430 nm and above approximately 500 nm, the intensity of the first light generated by the first light source is at most 1% of its maximum spectral intensity. The first light source is a light-emitting diode, for example.
The second light source generates an illumination light spectrum 152 having a spectral emission maximum in the range of 500 nm to 560 nm and a full width at half maximum in the range of 40 nm to 110 nm. Below approximately 430 nm and above approximately 650 nm, the intensity of the second light generated by the second light source is at most 1% of its maximum spectral intensity. The second light source is a light-emitting diode, for example.
The third light source generates an illumination light spectrum 153 having a spectral emission maximum in the range of 610 nm to 640 nm and a full width at half maximum in the range of 10 nm to 20 nm. The third light source is a light-emitting diode, for example.
From λ1=420 nm to λ2=480 nm the transmittance 161 of the observation filter 23 is approximately 0.005%. From λ3=490 nm to λ4=500 nm the transmittance 161 of the observation filter 23 is approximately 2%. From approximately λ4 to approximately λ5=540 nm the transmittance 161 of the observation filter 23 is approximately 0.005%. From λ5 to λ6=700 nm the transmittance 161 of the observation filter 23 is approximately 95%. From approximately λ6 to 750 nm the transmittance 161 of the observation filter 23 is approximately 0.005%. Furthermore, it holds true that W1=0.01%, W2=0.5%, and W3=80%.
From 350 nm to approximately λ1 the transmittance 162 of the illumination filter 9 is approximately 0.005%. From λ1 to approximately λ4 the transmittance 162 of the illumination filter 9 is approximately 95%. From approximately λ4 to approximately λ5′=630 nm the transmittance 162 of the illumination filter 9 is approximately 0.005%. From approximately λ5′ to λ6′=690 nm the transmittance 162 of the illumination filter 9 is approximately 0.08%. From approximately λ6′ to 750 nm the transmittance 162 of the illumination filter 9 is approximately 0.005%.
Accordingly, the observation filter 23 suppresses the first light reflected at the object 13, said first light having a high intensity substantially only between λ1 and λ2. Furthermore, the second light is suppressed by the illumination filter 9 above λ4. The proportion of the second light between λ3 and λ4 is reflected at the object 13 and transmitted by the observation filter 23 and thus contributes to the visualization of the non-fluorescent regions. Furthermore, the third light is suppressed by the illumination filter 9 below λ5′. The proportion of the third light between λ5′ and λ6′ is reflected at the object 13 and transmitted by the observation filter 23 and thus contributes to the visualization of the non-fluorescent regions. Furthermore, the fluorescent light emanating from the object 13 and having a high intensity substantially only between λ5 and λ5′ is transmitted by the observation filter 23, with the result that fluorescent regions of the object 13 can be observed with yellowish color valences.
Three major advantages are afforded by the individual settability of the intensities of the first, second, and third light (cf.
Third Aspect
One example of a microscopy method in accordance with the third aspect is described with reference to
A first value W1 represents a mean value of the transmittance 186 of the observation filter 23 over a first wavelength range WLB1. A second value W2 represents a mean value of the transmittance 186 of the observation filter 23 over a second wavelength range WLB2. A third value W3 represents a mean value of the transmittance 186 of the observation filter 23 over a third wavelength range WLB3. The first value W1 is less than the second value W2. The second value W2 is less than the third value W3.
A fourth value W4 represents a mean value of the intensity 187 of the illumination light over the first wavelength range WLB1. A fifth value W5 represents a mean value of the intensity 187 of the illumination light over the second wavelength range WLB2. A sixth value W6 represents a mean value of the intensity 187 of the illumination light over the third wavelength range WLB3. The fourth value W4 is larger than the fifth value W5. The fifth value W5 is larger than the sixth value W6.
The first, second, and third wavelength ranges do not overlap one another and lie in each case between 350 nm and 1000 nm. In the example shown, the first wavelength range WLB1 extends from approximately 370 nm to 430 nm, the second wavelength range WLB2 extends from approximately 470 nm to 580 nm, and the third wavelength range WLB3 extends from approximately 600 nm to 750 nm.
What is achieved with the values for the ratios between the first to sixth values as indicated with regard to the third aspect is that non-fluorescent regions of the object can be observed by light in the first wavelength range WLB1 and in the second wavelength range WLB2, while fluorescent light can be observed by light in the third wavelength range WLB3. Moreover, what is achieved on the basis of the indicated ratios between the first to sixth values is that non-fluorescent regions and fluorescent regions can be perceived as approximately equally bright. What is furthermore achieved is that the non-fluorescent regions can be perceived as approximately true color.
In the example shown, the first wavelength range WLB1 extends from approximately 440 nm to 500 nm, the second wavelength range WLB2 extends from approximately 640 nm to 750 nm and the third wavelength range WLB3 extends from approximately 520 nm to 620 nm.
One example of an alternative microscopy method in accordance with the third aspect is described with reference to
In accordance with the alternative microscopy method, the illumination light is generated such that a ratio of a first characteristic value to a second characteristic value has a value within a predetermined delimited value range. The first characteristic value represents a value of a characteristic variable for the intensity (or the brightness or the luminous flux or the like) of the light in the observation beam path 22 at the first locations 201. The second characteristic value represents the same characteristic variable in relation to the light in the observation beam path 22 at the second locations 202.
By way of example, the first characteristic value represents a mean value of the intensity of the light in the observation beam path 22 at the first locations 201, and the second characteristic value represents the mean value of the intensity of the light in the observation beam path 22 at the second locations 202. If the illumination light is generated such that the ratio of the first characteristic value to the second characteristic value lies in the value range of 20/1 to 1/20 or a narrower value range, the first locations 201, that is to say the fluorescent regions of the object 13, and the second locations 202, that is to say the non-fluorescent regions of the object 13, can be perceived as approximately equally bright.
One example of the microscopy method is explained below with reference to
In step S1, an image of the object 13 in the image plane 19 is recorded by the color image detector 20. The image is an image of the projected image of the object 13 generated through the observation beam path 22 in the image plane 19.
In step S2, following step Si, first image points 207 are determined from the image points 206. The first image points 207 correspond to the first locations 201. The image 205 has at the first image points 207 color valences which lie within the first color valence range 211. The first image points 207 are determined for example by comparing the color valences at the image points 206 of the image 205 with the predetermined first color valence range 211.
In step S3, following step S1, second image points 208 are determined from the image points 206. The second image points 208 correspond to the second locations 202. The image 205 has at the second image points 208 color valences which lie within the second color valence range 212. The second image points 208 are determined for example by comparing the color valences at the image points 206 of the image 205 with the predetermined second color valence range 212.
In step S4, following step S2, the first characteristic value is determined on the basis of the intensity of the image 205 at the first image points 207. By way of example, the mean value or the maximum value of the intensity at the first image points 207 is determined.
In step S5, following step S3, the second characteristic value is determined on the basis of the intensity of the image 205 at the second image points 208. By way of example, the mean value or the maximum value of the intensity at the second image points 208 is determined.
In step S6, which follows when steps S4 and S5 are concluded, the illumination light is set depending on the first and second characteristic values or depending on the intensity of the light in the observation beam path 22 in the image plane 19 at the first and second locations 201, 202 or depending on the intensity at the first and second image points 207 and 208. That is to say that the wavelength-dependent intensity distribution of the illumination light is changed. In this case, the illumination light is generated such that the above-described ratio between the first and second characteristic values has a value within the predetermined value range.
The method can be carried out repeatedly, which is illustrated by an arrow from step S6 to step S1 in
It is understood that the foregoing description is that of the exemplary embodiments of the disclosure and that various changes and modifications may be made thereto without departing from the spirit and scope of the disclosure as defined in the appended claims.
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| 20200240918 A1 | Jul 2020 | US |
