The present invention claims priority under 35 U.S.C. § 119 to Japanese Patent Application No. 2018-074710 filed Apr. 9, 2018, the contents of which are hereby incorporated herein by reference in their entirety.
The present invention relates to a light emission/reception system and an optical biometer including such a system.
In general, the jaundice, in particular, the severe neonatal jaundice is likely to result in death. Even if one can escape from death, the jaundice may progress to the kernicterus that leaves sever aftereffects, such as cerebral palsy. Hence, the early detection of the jaundice is significantly important. In order to precisely determine the severity of the jaundice, the bilirubin levels in the sera collected from newborn infants should be measured. The blood collection from all the newborn infants, however, is difficult and is often superfluous.
A typical icteric indicator measures the intensity of the yellowish color of the bilirubin in the subcutaneous tissue of a newborn infant from the difference in optical density between the wavelength region of blue light having a central wavelength of 450 nm and the wavelength region of green light having a central wavelength of 550 nm. The tip of a probe is put into tight contact with the forehead or breast of a newborn infant to radiate light from a light source through an optical lighting fiber. The light travels through the skin and the subcutaneous tissue and then generate backscattered light. The two colors of above-mentioned wavelengths of the backscattered light are detected by a sensor. The yellowish color intensity is calculated in the ratio of the intensity of the blue light to that of the green light. The severity of the jaundice is determined from the calculated value.
The precision of the measured transdermal bilirubin level depends on the effective lengths of the optical paths in the light emission/reception systems. Thus, the systems having different effective optical paths may exhibit different results even in the case of the measurement of the transdermal bilirubin level of a single newborn infant. Hence, a means is required that reduces the unevenness of the light brightness at the light inlets of the systems to keep the center of gravity of light brightness constant.
Japanese Unexamined Patent Application Publication No. 2011-163953 discloses a light emission/reception system including a light outlet, where the unevenness of the brightness of the light from the light source is high in the circumference of the light outlet. The center of gravity of light brightness can be thereby kept stable.
Unfortunately, the invention disclosed in Japanese Unexamined Patent Application Publication No. 2011-163953 is focused only on the optical path in the light emission system and not on the optical path in the light reception system. In a typical traditional icteric indicator, the end face of the probe tilts by a specific angle from the surface of a living body of interest and is not in uniform contact with the surface, resulting in a reduction in the precision of measurement.
In detail, the following three factors adversely affects the precision of the measurement. 1. VARIATIONS IN THE OPTICAL PATH AND THE LENGTH THEREOF (i.e., shift from a predetermined optical path)
An intended design condition is that a probe P vertically stands on and is in close contact with a surface BS of the living body under a uniform pressure as illustrated in
As illustrated in
As illustrated in
2. INTERFERENCE WITH EXTERNAL LIGHT DUE TO IMPERFECT CONTACT OF THE PROBE WITH THE SURFACE OF THE LIVING BODY
External light passes through the partial surface with which the end face of the probe P is not in contact. Typical traditional icteric indicators cancel the effects of the external light (and the fluctuation of the ambient light) through the subtracting operation of dark counts indicating the times where no light is radiated between the cycles of the light radiation. Since the acquisition of the dark counts inevitably shifts from the acquisition of the light radiation counts, components that cannot be completely cancelled affect the observed results.
Even in the case of a slight tilt of the probe P as illustrated in
Traditional icteric indicators may include a switch operable in cooperation with pressing of the probe P onto the surface BS. This switch can restrict the subcutaneous blood flow to reduce the optical effects of, for example, hemoglobins in the blood (the spring force of the switch optimizes the ischemic levels). Unfortunately, the tilting probe P causes the contact area to decrease and the pressure to increase even under a constant load. The uneven pressure fluctuates the ischemic levels.
The factors described above are summarized in Table 1.
An object of the present invention is to provide a light emission/reception system and an optical biometer using such a system that can detect the uniformity of the contact of the end face of a probe with a surface of a living body and thereby improve the precision or reproducibility and accuracy of measurement affected by the uneven contact.
To achieve at least one of the abovementioned objects, according to a first aspect of the present invention, a light emission and reception system for optical biometric measurement includes:
a light radiator that radiates source light to a living body; and
a light receiver that receives return light scattered from the living body,
wherein
the light radiator and the light receiver are disposed at an end face of the system which is to be put into contact with a surface of the living body during the optical biometric measurement,
the system measures biometric data of the living body based on intensity of the light detected by the light receiver, and
(i) the light receiver comprises segments which respectively detect an intensity of the return light and which are at different angular ranges around a center axis of the light radiator, and/or (ii) the light radiator comprises segments which respectively radiate the source light and which are at different angular ranges around a center axis of the light receiver.
According to a second aspect of the present invention, an optical biometer includes:
the light emission and reception system; and
a control/arithmetic processor that controls radiation of the source light through the light radiator and calculates an observed result from the return light detected in the light receiver,
wherein
if the light receiver comprises one segment and the light radiator comprises multiple segments, the control/arithmetic processor controls time-divisional radiation of the source light from the segments of the light radiator and detection of the sequential return lights in the segment of the light receiver to obtain light intensities for the segments of the light radiator, and
if a difference among the light intensities detected for the segments of the light radiator falls within a predetermined threshold, the control/arithmetic processor calculates the observed result.
According to a third aspect of the present invention, an optical biometer includes:
the light emission and reception system; and
a control/arithmetic processor that controls radiation of the source light through the light radiator and calculates an observed result from a return light detected in the light receiver,
wherein
if the light receiver comprises one segment and the light radiator comprises multiple segments, the control/arithmetic processor controls time-divisional radiation of the source light from the segments of the light radiator and detection of the sequential return lights in the segment of the light receiver to obtain light intensities for the segments of the light radiator, and
the control/arithmetic processor controls preliminary radiation of the source light and, if a difference among the light intensities detected for the segments of the light radiator during the preliminary radiation falls within a predetermined threshold, the control/arithmetic processor controls true radiation of the source light and calculates the observed result from true light intensities detected in the light receiver.
According to a fourth aspect of the present invention, an optical biometer includes:
the light emission and reception system; and
a control/arithmetic processor that controls radiation of the source light through the light radiator and calculates an observed result from a return light detected in the light receiver,
wherein
if the light receiver comprises one segment and the light radiator comprises multiple segments, the control/arithmetic processor controls time-divisional radiation of the source light from the segments of the light radiator and detection of the sequential return lights in the segment of the light receiver to obtain light intensities for the segments of the light radiator, and
the control/arithmetic processor controls the light radiator not to radiate and, if a difference among light intensities detected for the segments of the light radiator during no radiation falls within the predetermined threshold, the control/arithmetic processor controls true radiation of the source light and calculates the observed result from the true light intensities detected in the light receiver.
According to a fifth aspect of the present invention, an optical biometer includes:
the light emission and reception system; and
a control/arithmetic processor that controls radiation of the source light through the light radiator and calculates an observed result from a return light detected in the light receiver,
wherein
if the light receiver comprises one segment and the light radiator comprises multiple segments, the control/arithmetic processor controls time-divisional radiation of the source light from the segments of the light radiator and detection of the sequential return lights in the segment of the light receiver to obtain light intensities for the segments of the light radiator, and
if a difference among the light intensities detected for the segments of the light radiator exceeds a predetermined threshold, the control/arithmetic processor calculates the observed result from the light intensities detected for some of the segments of the light radiator.
According to a sixth aspect of the present invention, an optical biometer includes:
the light emission and reception system; and
a control/arithmetic processor that controls radiation of the source light through the light radiator and calculates an observed result from a return light detected in the light receiver,
wherein
if the light receiver comprises one segment and the light radiator comprises multiple segments, the control/arithmetic processor controls time-divisional radiation of the source light from the segments of the light radiator and detection of the sequential return lights in the segment of the light receiver to obtain light intensities for the segments of the light radiator, and
the control/arithmetic processor (i) controls predetermined cycles of sequential radiation of the source light for each of the segments of the light radiator, (ii) calculates a difference among the light intensities for the segments for each cycle of radiation, and (iii) calculates the observed result from relatively even light intensities detected in the light receiver.
According to a seventh aspect of the present invention, an optical biometer includes:
the light emission and reception system; and
a control/arithmetic processor that controls radiation of the source light through the light radiator and calculates an observed result from a return light detected in the light receiver,
wherein
if the light receiver comprises one segment and the light radiator comprises multiple segments, the control/arithmetic processor controls time-divisional radiation of the source light from the segments of the light radiator and detection of the sequential return lights in the segment of the light receiver to obtain light intensities for the segments of the light radiator, and
in order to calculate the observed result from the light intensities for the segments of the light radiator, the control/arithmetic processor adds an offset according to the difference among the light intensities for the segments.
The advantages and features provided by one or more embodiments of the invention will become more fully understood from the detailed description given hereinbelow and the appended drawings which are given by way of illustration only, and thus are not intended as a definition of the limits of the present invention.
FIG. 19B1 is a plan view of a configuration of a light outlet of an exemplary backward optical fiber bundle according to an embodiment of the invention.
FIG. 19B2 is a side view of the configuration of the light outlet of the exemplary backward optical fiber bundle according to the embodiment of the invention.
FIG. 19C1 is a plan view of a configuration of a light outlet of an exemplary backward optical fiber bundle according to another embodiment of the invention.
FIG. 19C2 is a side view of the configuration of the light outlet of the exemplary backward optical fiber bundle according to the embodiment of the invention.
FIG. 19D1 is a plan view of a configuration of a light outlet of an exemplary backward optical fiber bundle according to another embodiment of the invention.
FIG. 19D2 is a side view of the configuration of the light outlet of the exemplary backward optical fiber bundle according to the embodiment of the invention.
FIG. 20B1 is a plan view of a configuration of a light inlet of a forward optical fiber bundle according to the embodiment of the invention.
FIG. 20B2 is a side view of the configuration of the light inlet of the forward optical fiber bundle according to the embodiment of the invention.
FIG. 21B1 is a plan view of a light outlet of a backward optical fiber bundle according to the embodiment of the invention.
FIG. 21B2 is a side view of the light outlet of the backward optical fiber bundle according to the embodiment of the invention.
FIG. 21C1 is a plan view of a configuration of a light inlet of the forward optical fiber bundle according to the embodiment of the invention.
FIG. 21C2 is a side view of the configuration of the light inlet of the forward optical fiber bundle according to the embodiment of the invention.
The embodiments of a light emission/reception system and an optical biometer according to the present invention will now be described in reference to the accompanying drawings. However, the scope of the invention is not limited to the disclosed embodiments. The same components are denoted by the same reference numerals without redundant description throughout the embodiments.
Overview of Optical Biometer
The forward optical fiber bundle 2 and the backward optical fiber bundles 3A and 3B are light guides composed of optical fibers, each having end faces which the light enters or exits. The forward optical fiber bundle 2 and the backward optical fiber bundles 3A and 3B are optically isolated from each other such that the source light from the forward optical fiber bundle 2 inevitably goes through the living body 9 and return to the backward optical fiber bundles 3A and 3B. One of the combination of backward optical fiber bundle 3A, the diffuser plate 4A, and the photodetector 5A and the combination of the backward optical fiber bundle 3B, the diffuser plate 4B, and the photodetector 5B may be omitted to build up a single-path light receiving system.
The xenon tube 1 is a long straight light source. Thus, the light inlet 2p of the forward optical fiber bundle 2 has a horizontally rectangular profile to receive source light from the xenon tube 1.
The light outlet 2q of the forward optical fiber bundle 2 and the light inlets 3pA and 3pB of the backward optical fiber bundles 3A and 3B reside at the end face AS of the probe of the icteric indicator 20. The end face AS of the probe is urged onto the living body 9, for example, onto the forehead or breast of a newborn infant, and the xenon tube 1 radiates white source light for measurement. The white source light beams LW from the xenon tube 1 enter the light inlet 2p and travel through the forward optical fiber bundle 2. The white source light beams are then guided to the light outlet 2q and radiated in a circular flux toward the living body 9.
As illustrated in
The dual-wavelength photodetectors 5A and 5B each have green and blue filters on the light reception face to detect the intensities of the blue band having a central wavelength at 450 nm and the green band having a central wavelength at 550 nm in the transmitted light beams. The intensity of the yellowish color is measured from the intensity of the blue light relative to the intensity of the green light or the ratio of the intensity of the blue light to that of the green light. For example, a low intensity of the blue light relative to the intensity of the green light signifies a high intensity of yellowish color, and determines that the severity of the jaundice is high. In other words, the intensity of the yellowish color of the bilirubin present in the subcutaneous tissue 9c of the living body 9 corresponds to a difference in the optical density between the wavelength regions of the two spectral colors of blue and green. A light receiving system of a dual-path type as in the present embodiment can calculate the difference in the observed results obtained from the two light paths regardless of the color and thickness of the epidermis 9a. The severity of the jaundice can accordingly be more precisely measured.
Embodiments of Light Emission/Reception System
Based on the overview of the biometer described above, embodiments of a light emission/reception system will now be described that includes, for example, a light receiver having multiple segments.
As illustrated in
The light receiver segments p1, p2, and p3 are in different angular ranges around the center axis of the light outlet 2q which is the light exit. As illustrated in
As illustrated in
Instead of the dual-wavelength photodetectors 5A and 5B, photodetectors PD 1, PD 2, PD 3 are respectively disposed in the light outlet segments q1, q2, and q3 as illustrated in
The light detecting component according to the present embodiment consists of photosensors (for example, photodiodes) corresponding to the segments, such as the photodetectors PD 1, PD 2, and PD 3.
As illustrated in
In the embodiment illustrated in
Four filters (two green filters and two blue filters) are disposed for each segment. In other words, the photodetectors PD 1, PD 2, or PD 3 each are provided with four filters. The photodetectors PD 1, PD 2, and PD 3 are thus provided with twelve photodetectors in total.
In case that no green filter G and no blue filter B are disposed in the light outlets as illustrated in
The light outlet segments q1, q2, and q3 in
As illustrated in
As illustrated in
The backward optical fiber bundle 3B may diverge into the light outlet segments q1, q2, and q3 as illustrated in
As illustrated in
The illumination light emitters LT1, LT2, and LT3 can serve as light sources for preliminary light emission. For this purpose, the wavelengths of the light beams from the illumination light emitters LT1, LT2, and LT3 are equal to the wavelengths of the scattered return light beams for ready assessment of the effects of the wavelengths on the measurement.
The illumination light emitters LT1, LT2, and LT3 can serve as lamps for work in the darkness, in particular, for visual inspection of the target surface of the living body onto which the end face AS is urged.
In
The light reception system may include any of one optical path (in
The light reception system may include four or more segments (in
As illustrated in
One or more photodetectors may be disposed for each segment in the light reception system.
As illustrated in
In
The forward optical fiber bundle 2 and the backward optical fiber bundles 3A and 3B may be replaced with light guides, light pipes, or combination thereof having the same functions.
As illustrated in
The control/arithmetic processor 21 performs the control and calculation according to any of the following schemes.
First Measurement Scheme
In accordance with a first measurement scheme, the control/arithmetic processor 21 calculates an observed result from the light intensities with proviso that the difference among the light intensities detected in the segments falls within a predetermined threshold.
The control/arithmetic processor 21 instructs the light radiator to radiate the source light toward the living body and the light receiver segments p1, p2, and p3 to receive the scattered return light from the living body. If the difference among the light intensities falls within a predetermined threshold, the observed results are calculated from the light intensity and presented on the display 22. Since multiple light intensities are detected, operations, for example, averaging procedures, may be employed. The light intensity detected in any one of the segments may be selected for calculation of an observed result. The difference falling within the predetermined threshold indicates that the tilt of the probe P relative to the surface or the contact of the end face AS with the surface is kept at a predetermined level, resulting in calculation of a correct value.
In this scheme, the control/arithmetic processor 21 instructs the light radiator to reradiate the source light if the difference among the light intensities does not fall within the predetermined threshold. The light radiator repeats the radiation of the source light until the difference falls within the predetermined threshold.
The light intensities from which the difference is calculated may be ones detected by the light receiver segments p1, p2, and p3 or parameters reflecting the intensity. This holds in other measurement schemes.
Second Measurement Scheme
In accordance with a second measurement scheme, the control/arithmetic processor 21 controls preliminary radiation of source light. When the difference among the light intensities detected in the segments after the preliminary radiation falls within the predetermined threshold, the control/arithmetic processor 21 controls true radiation of the source light and calculates the observed results from the light intensities detected at the light receiver segments p1, p2, and p3.
The illumination light emitters LT1, LT2, and LT3 or the xenon tube 1, a light source for measurement, can serve as a light source for the preliminary emission of the source light. The preliminary radiation of the source light from the xenon tube 1 is performed under a radiating condition different from that for the true radiation, for example, the radiation of the source light with reduced intensity. The preliminary emission of the source light from the illumination light emitters LT1, LT2, and LT3 (LEDs) or the preliminary radiation of the source light with reduced intensity by the xenon tube 1 can reduce the power consumption before the true radiation.
The illumination light emitters LT1, LT2, and LT3 serving as light sources for preliminary emission of the source light may be operated in response to the start switch or a dedicated switch driving the illumination light emitters LT1, LT2, and LT3. The dedicated switch allows the illumination light emitters LT1, LT2, and LT3 to emit light at different cycles or for different periods and serve as luminaires for work in the darkness.
In accordance with a third measurement scheme, the control/arithmetic processor 21 uses incident external or environmental light for a light source instead of the preliminary light radiation to obtain a dark count value at a non-radiation time. The control/arithmetic processor 21 instructs the xenon tube 1 to control true radiation of the source light in response to the difference in intensity of the return light detected in the segments falling within a predetermined threshold. The control/arithmetic processor 21 then calculates the observed results from the intensity of the return light detected by the light receiver segments p1, p2, and p3 after the true radiation.
The unevenness over the positions of the incident external light can determine the tilt of the probe P or the uneven contact of the end face AS with the surface BS.
In the case that no external light is available or the end face AS is in close contact with, for example, a soft skin despite the tilting probe P, the external beams cannot be detected. In such a case, the second measurement scheme is employed to instruct the illumination light emitters LT1, LT2, and LT3 or the light source (xenon tube 1) to emit light. These light emitters mounted to the icteric indicator can precisely determine the tilt of the probe P or the uneven contact of the end face AS.
First Supplementary Function
The control/arithmetic processor 21 may have a supplementary function that instructs the display 22 to present that the difference in intensity of the return light detected in the segments exceeds a predetermined threshold.
The display may be a flat panel display or a dedicated LED display. The flat panel display capable of presenting characters and illustrations may present textual data, such as “The measurement probe is tilting relative to the living body” and “Keep the measurement probe vertical to the measured face”. Alternatively, the flat panel display may present graphic data indicating such messages.
The display 22 may include an audio output device (speaker) to inform a user of the tilt of the probe P through a voice or beep.
This alerting or informing function may be executed simultaneously with tentative display of the observed results even in the case that the difference exceeds the threshold. The observed results in the case that the difference exceeds the threshold can be displayed with an alerting indicator. The observed results in the case that the difference falls within the threshold can be displayed with an indicator of the normal state. Either or both of such displaying modes can be selected.
In the case that the difference exceeds the threshold, only an alert may be issued without display of the observed results.
The control/arithmetic processor 21 may have a supplementary function that instructs the display 22 to present the tilting direction of the probe P relative to the surface of the living body or the direction for correction of the tilt.
To execute this supplementary function, the icteric indicator 20 in
The audio outputting device or speaker of the display 22 may inform the user of the tilting direction of the probe P relative to the surface or the direction for correction of the tilting.
The first and second supplementary functions can be combined with the first and second measurement schemes to guide the user to quickly obtain observed results. The first and second supplementary functions can also be combined with the following measurement schemes to improve the precision of the measurement.
Fourth Measurement Scheme
If the difference in intensity of the return light in the segments exceeds a predetermined threshold, the control/arithmetic processor 21 may calculate an observed result from the intensity of return light detected in only some of the segments according to a fourth measurement scheme.
For example, the control/arithmetic processor 21 calculates the observed result only from the intensity detected in specific light receiver segments where received return light has a high intensity. The receiver segments where the received return light has a high intensity are in close contact with the surface and thus receive more return light scattered from the surface. Despite the probe P tilting relative to the surface or the end face AS being in imperfect contact with the end face AS, the control/arithmetic processor 21 calculates the observed results from the intensity of the return light detected in the light receiver segments at the end face AS that are in close contact with the surface among the light receiver segments p1, p2, and p3. Precision of the measurement is thereby improved.
Alternatively, the control/arithmetic processor 21 calculates an observed result only from the intensity of return light at a relatively similar level in the specific segments. The light intensity at a relatively similar level indicates that the segments on the end face AS are in substantially even contact with the surface. The light intensity shifted from the others or the light intensity detected in the segment at the end face AS in uneven contact with the surface is excluded. Then, the observed result is calculated only from the light intensity detected in the segments at the end face AS in even contact with the surface. The precision of the observed result is thereby improved.
In this scheme, the control/arithmetic processor 21 may instruct the display 22 to represent the low level of reliability of the observed result due to the difference in the return light exceeding the predetermined threshold between the segments. For example, the difference exceeding a first threshold is represented by “Measurement Reliability Level: Medium” and the difference exceeding a second threshold larger than the first threshold is represented by “Measurement Reliability Level: Low”.
The user may redetermine the intensity of the return light as required. The first and second supplementary functions can correct the orientation of the icteric indicator 20 to obtain an observed result corresponding to “Measurement Reliability Level: High”.
Fifth Measurement Scheme
In accordance with a fifth measurement scheme, the control/arithmetic processor 21 instructs predetermined cycles of sequential radiation of the source light. The control/arithmetic processor 21 calculates a difference in intensity of return light detected in the segments for each radiation. The control/arithmetic processor 21 calculates an observed result from the relatively even intensity of the return light detected in the light receiver segments.
Unlike the first and second measurement schemes, the fifth measurement scheme does not involve calculation of the difference for each radiation. A set of sequential light beams is radiated at a predetermined time rate, followed by the calculation of the difference for each radiation. The difference calculated from the relatively even light intensities detected in the light receiver segments can achieve a high precision of the measurement.
In this scheme, the user corrects the orientation of the icteric indicator 20 with reference to the indication on the display 22 as described in the first and second supplementary functions to achieve a higher precision of measurement.
This scheme can use a light source suitable for sequential emission of light beams, for example, an LED or a laser emitter.
In accordance with a sixth measurement scheme, the control/arithmetic processor 21 calculates a difference among light intensities detected in a plurality of segments and performs the correction of the detected value or corrects the effect of the tilt of the probe and the uneven contact of the end face with the surface to calculate a more accurate observed result. The effect of the tilting probe and the contact of the end face with the surface is preliminarily examined, in other words, the correlation of an offset with the difference above is determined. Arithmetic expressions including the correlation can be implemented in the icteric indicator 20 for offsetting of the difference.
Miscellaneous
Further description will be provided below.
Variation (a): In
The angular ranges in the light inlet at the end face AS of the backward optical fiber bundle 3B may be maintained in the outlet or converted into distribution on a specific coordinate. Alternatively, the angular ranges in the light inlet may be converted at random in each of the segments.
As illustrated in
In FIG. 19C1 and FIG. 19C2, the light inlet 3pB has a cross-section similar to that in
In FIG. 19D1 and FIG. 19D2, the light inlet 3pB has different angular ranges from that around the central axis of the light outlet 2q at the end face AS in
Separately from the design of the optical fiber bundle, the number of photodetectors can be determined and the number of segments at central angles can thereby be appropriately adjusted. In particular, a two-dimensional image sensor can acquire the continuously differing light intensities as continuous distributions, unlike other sensors acquiring the light intensities as integrated values of light beams detected in the respective areas. The uneven contact of the end face AS with the surface of the living body depending on the angles of the probe P can be more locally detected.
Variation (b): The above-mentioned configurations each include a light radiation/reception system having multiple detection channels disposed at angles around the axis of the light radiator. The segments cover different angular areas for detection of light intensity on the end face AS of the probe P. The target areas for detection on the end face AS are different among the detection channels.
The light outlet may be divided into multiple segments around the circumference on the end face AS of the probe P, instead of the light inlet. In
In the case that light inlet 3pA has one segment and the light outlet has multiple segments, the control/arithmetic processor 21 controls the time-divisional radiation of light beams through the light radiator segments 2q1, 2q2, and 2q3. The scattered return light beams enter the light inlet 3pA, and then the light intensity from different segments are detected. This configuration also allows the independent detection of light intensity in the separate channels at different angular areas on the end face AS of the probe P.
This measurement scheme may involve preliminary time-divisional radiation of light beams from the light radiator segments 2q1, 2q2, and 2q3 and simultaneous true radiation of light beams from the light radiators 2q1, 2q2, and 2q3, resulting in detection of the scattered return light. Alternatively, an observed result may be computed from the intensity of time-divisionally radiated source light.
Instead of the light inlet divided in two or more segments, the light outlet may be divided in multiple segments. In both the cases, light emitting elements may be provided in the light inlet segments.
Multiple light receiver segments may require the same number of photodetectors, resulting in increases in manufacturing costs and/or dimensions of the product. In order to provide a sufficient light intensity, multiple light sources, for example, LED light sources disposed adjacent to the light radiator segments may be utilized for other purposes.
Variation (c): As illustrated in
This measurement scheme may involve simultaneous radiation of source light from the light radiator segments and subsequent detection of the scattered return light in the light receiver segments. Alternatively, the measurement scheme may involve the time-divisional radiation of light as described in Variation (b). Preliminary light may be time-divisionally radiated and the true light may be simultaneously radiated.
Compared to the embodiment in which only the light outlet is divided in multiple segments in
Other Solutions
Other solutions will now be described for a reduction in or the detection of the tilt of the probe P or the unevenness of the contact of the end face AS with the surface BS. The solutions that will be described below do not use an optical measurement system.
Solution (1): The solution for a reduction in the tilt of the probe P and the unevenness of the contact of the end face AS with the surface BS will now be described.
The probe P in
As illustrated in
As illustrated in
As illustrated in
A large, elongated, or heavy icteric indicator is likely to tilt. In such a case, the main body of the icteric indicator and the probe may be separated. A relatively small lightweight optical probe unlikely to tilt relative to a living body can achieve the close contact of the end face AS with the living body, resulting in an enhanced precision of measurement. As illustrated in
As in
An optical fiber cable 60 consists of, for example, fibers and an outer tube composed of flexible materials.
For use of the wireless communication link 61, an electric circuit is disposed on the end piece 59 to convert the intensity of received scattered return light into an electric signal and wirelessly transmit the signal to the main body 58.
For use of the electric cable 62, an electric circuit is disposed on the end piece 59 to convert the intensity of received scattered return light into an electric signal and transmit the signal to the main body 58 through the electric cable 62.
Solution (2): The solution for detection of tilt of the probe P and the unevenness of the contact of the end face AS with the surface BS will now be described. In response to the detection of the tilting or unevenness, remeasurement, alert or notice or correction of the measurement may be performed. The precision or reproducibility and accuracy of the observed results can be thereby improved.
Additional sensors different from those of the measurement system of the probe P are disposed to directly or indirectly detect the tilt of the probe P or the unevenness of the contact of the end face AS with the surface BS. As illustrated in
As illustrated in
As illustrated in
As illustrated in
The wavelengths of the light beams to be emitted by the light emitting devices 66a may be equal to the wavelength of the light beam to be detected from the probe P.
The detailed configurations or operations of the components of the light radiation/reception system and the optical biometer according to the embodiments can be appropriately varied without departing from the scope and spirit of the present invention.
Although embodiments of the present invention have been described and illustrated in detail, the disclosed embodiments are made for purposes of illustration and example only and not limitation. The scope of the present invention should be interpreted by terms of the appended claims.
The entire disclosure of Japanese Patent Application No. 2018-074710, filed on 9 Apr. 2018, is incorporated herein by reference in its entirety.
Number | Date | Country | Kind |
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2018-074710 | Apr 2018 | JP | national |