The technical field of the invention is the optical measurement of a cardiac frequency of an individual or of an animal.
Optical measurements are frequently implemented to determine physiological parameters of a living being, in particular blood-related parameters. Devices, called pulse oximeters, are commonly used to determine an oxygen saturation of the haemoglobin in the blood. These measurements are based on the absorption of light by the haemoglobin, the latter varying between oxyhaemoglobin and deoxyhaemoglobin. Commercial devices are widely used, these devices being based on a measurement of the light transmitted by a sufficiently thin member, in an infrared spectral band and in a red spectral band. The examined member may in particular be the end of a finger or the lobe of an ear. Measurements of the transmitted light, in each of the spectral bands, allow concentrations of oxyhaemoglobin and deoxyhaemoglobin in the blood to be estimated, from which the oxygen saturation of the blood is estimated. These measurements also allow a pulsatile blood flow to be detected and a cardiac frequency to be deduced therefrom. Most commercial oximeters also allow the cardiac frequency to be estimated from measurements carried out in one or other spectral band.
European patent EP2355693 for example describes a device including a first light source emitting at a red wavelength and a second light source emitting at an infrared wavelength. A photodetector is configured to detect light radiation emanating from a finger illuminated by one of the light sources. The infrared light source is in particular used to detect the presence of the finger against the device, subsequent to which the red light source is activated, so as to allow parameters such as cardiac frequency or pulse oximetry to be determined.
U.S. Pat. No. 9,042,971 describes a portable actigraphy device allowing a cardiac frequency to be determined optically via detection of light radiation backscattered by a finger under the effect of an illumination. This device allows measurements to be carried out in a back-scatter configuration, also called the reflectance configuration, the light sources being placed adjacent to the photodetector.
The inventors have observed that such devices may make errors when measuring cardiac frequency, in particular when they are worn by a moving person. The invention proposes to solve this problem, and hence allow more reliable measurements of cardiac frequency to be obtained.
A first subject of the invention is a method for estimating a cardiac frequency of a living being comprising the following steps:
By temporal coincidence, what is meant is simultaneously, i.e. in the same time window. This time window may be preset or adjustable.
By light beam or light radiation, what is meant is a flux of photons the spectral band of which is comprised in the visible domain, or in the near infrared domain, or in the near UV domain, for example between 200 nm and 1000 nm.
The cardiac frequency may be equal to the occurrence frequency.
The second spectral band is preferably different from the first spectral band.
According to an embodiment, step d) includes calculating a first derived function, derived from the first detection function, and a second derived function, derived from the second detection function, and identifying characteristic instants from each of the derived functions.
According to an embodiment, each derived function is obtained via a difference between the value of a corresponding detection function at two different instants.
The method may include one of the following features, individually or in combination:
The detected radiation may be backscattered radiation, in which case the light source and the photodetector are placed adjacent one with respect to the other. The detected radiation may also be transmitted radiation, in which case the bodily zone extends between the light source and the photodetector.
Preferably, the first spectral band and the second spectral band do not overlap, or if they do, only by a negligible amount.
Another subject of the invention is a device including:
The photodetector may be configured to detect radiation backscattered by the bodily zone under the effect of its illumination. Alternatively, the photodetector is configured to detect radiation transmitted by the illuminated bodily zone.
The light source may include:
Other advantages and features will become more clearly apparent from the following description of particular embodiments of the invention, which are given by way of nonlimiting example and shown in the appended figures, which are listed below.
The photons composing the incident light beam 12 penetrate into the sample and some thereof are backscattered in a direction parallel to the propagation axis, in a direction opposite to the latter. These backscattered photons form backscattered radiation 14. The backscattered radiation 14 may be detected by a photodetector 30 placed facing the surface 21 of the sample. The photodetector may be configured so as to detect backscattered radiation emanating from the sample at a distance d, called the back-scatter distance, which is generally non-zero, smaller than a few millimeters and typically smaller than 15 mm or 10 mm.
In this example, the light source 10 includes two elementary light sources 101 and 102. The first elementary light source 101 is a light-emitting diode emitting in a first spectral band Δλ1 centred on a first wavelength λ1 equal to 660 nm. It is a light-emitting diode sold by the manufacturer Kingbright under the reference APT1608SURCK. The second elementary light source 102 is a light-emitting diode emitting in a second spectral band Δλ2 centred on a second wavelength λ2 equal to 940 nm. It is a light-emitting diode sold by the manufacturer Kingbright under the reference APT1608F3C. Thus, the first spectral band Δλ1 preferably extends between 600 and 700 nm, this covering the red visible spectral band, whereas the second spectral band Δλ2 preferably extends between 700 and 1000 nm, and more preferably between 810 nm-1000 nm, this corresponding to a spectral band in the near infrared. Preferably, the first spectral band Δλ1 and the second spectral band Δλ2 are different and do not overlap. By do not overlap, what is meant is that most of the emission spectrum, and preferably 80% or even more than 90% of the emitted intensity, is not located in the same spectral range.
A microcontroller 15 commands the sequential activation of the elementary light sources 101 and 102. Thus, the sample is successively illuminated by a first incident light beam 121, in the first spectral band Δλ1, and by a second incident light beam 122, in the second spectral band Δλ2.
A photodetector 30 detects first backscattered radiation 141, in the first spectral band Δλ1, under the effect of the illumination by the first incident light beam 121, and second backscattered radiation 142, in the second spectral band Δλ2 under the effect of the illumination by the second incident light beam 122. In the example shown, the photodetector is a photodiode sold by VISHAY under the reference BPW345, the spectral band of detection of which allows the first and second backscattered radiation to be detected. The back-scatter distance d is, in this example, 7 mm.
A processor 32 is configured to establish a detection function, corresponding to a variation as a function of time of the intensity of radiation detected by the photodetector, in each of the spectral bands. It may be connected to a memory 33 configured to store instructions allowing a method described in this description to be implemented. It may also be connected to a display unit 34.
According to another embodiment, which is shown in
Such an estimation is generally calculated in a single spectral band, whether it be a red spectral band or an infrared spectral band. However, this type of estimation lacks robustness. More particularly, movements of the illuminated bodily zone, exposure to parasitic light sources or simple electronic noise may corrupt the estimation of cardiac frequency.
The inventors have defined a method allowing the detection of false characteristic instants to be avoided. This method, which combines the detection of signals backscattered or transmitted in two spectral bands, will be described below with reference to
Step 100: arranging the device 1 in such a way that the light source 10 is configured to illuminate a sample, i.e. a bodily zone 20 of a living being, and that the photodetector is configured to detect radiation backscattered or transmitted by the bodily zone consecutively to this illumination.
Step 110: illuminating the sample 20 in the first spectral band Δλ1 (substep 1101) and in the second spectral band Δλ2 (substep 1102). Depending on the photodetector used, this illumination may be simultaneous or successive. In this example, a single non-spectrally resolved photodetector is used. The sample is illuminated successively by each elementary source 101 and 102, the duration of each illumination being 1.66 ms. The successive activation of each elementary light source, which successive activation is designated by the term “illuminating sequence”, is controlled by the microcontroller 15. Alternatively, the light sources may be continuously activated, the backscattered (or transmitted) radiation being detected by two different photodetectors, each being configured to detect the radiation in the first spectral band Δλ1 or the second spectral band Δλ2, respectively. According to another variant, the photodetector may be spectrally resolved, thereby also allowing the bodily zone 20 to be illuminated simultaneously in the two spectral bands. Preferably, but optionally, after the activation of the second light source, no light source is activated for 1.66 ms (substep 1103). The signal SB detected by the photodetector 30 is thus representative of a dark current of the latter.
Step 120: detecting radiation backscattered (or transmitted) by the sample following the illumination in each spectral band. The photodetector generates a first detection signal S1 depending on the intensity of the radiation backscattered (or transmitted) 141 under the effect of the illumination of the sample in the first spectral band Δλ1 (substep 1201) and a second detection signal S2 dependent on the intensity of the radiation backscattered (or transmitted) 142 under the effect of the illumination of the sample in the second spectral band Δλ2 (substep 1202). In this example, the first detection signal S1 and the second detection signal S2 are detected during the illumination by the first elementary source and during the illumination by the second elementary source, respectively. When no light source is activated, the photodetector acquires a background-noise signal or dark-current signal SB (substep 1203). This dark current may be subtracted from the detection signals S1 and S2.
Thus, as shown in
Step 130: establishing a first detection function S1(t) and a second detection function S2(t) representing the variation as a function of time of the first detection signal S1 and of the second detection signal S2, respectively. Each of these functions is obtained by sampling over time the first signal S1 and the second signal S2, respectively, the sampling frequency for example being 200 Hz, this corresponding to an acquisition of a first signal S1 and of a second signal S2 every 5 ms. The establishment of each detection function may comprise a preprocessing step in which the signal is smoothed, allowing a high-frequency component of the detected signal to be removed. This preprocessing may take the form of application of a low-pass filter or of a moving average. In this example, a moving average is calculated for a time interval of 25 ms, i.e. 5 samples.
Step 140: determining a first derived function S′1(t) and a second derived function S′2(t). Each derived function is obtained via a difference of a detection function at two different times t and t+St. The time difference St is preferably smaller than 500 ms, or even than 100 ms. In this example, t and t+St are successive instants, i.e. instants spaced apart by the sampling period, i.e. 5 ms. The derived function may be obtained by normalizing the difference described above by the time difference, this corresponding to the conventional definition of a rate of variation.
In other words,
The second derived function S′2(t) is obtained identically to the first derived function S′1(t), from the second detection function S2(t).
Step 150: identifying characteristic instants. By characteristic instant, what is meant is an instant at which the detection function or its derived function reaches a particular value, crosses a threshold or reaches a local extremum, for example a local minimum or local maximum. In this example, as described with reference to
Step 160: determining cardiac frequency hr. From the characteristic instants ti selected in step 150, an occurrence frequency f of the successive characteristic instants is established, this frequency corresponding to the cardiac frequency hr. For example, the occurrence frequency is obtained by averaging the occurrence frequency of a number N of successive characteristic instants ti. The frequency fi attributed to a characteristic instant ti may then be established depending on the average time difference between N successive instants preceding the characteristic instant, such that:
The cardiac frequency hri at the instant ti is equal to fi. The units may then be changed to obtain a cardiac frequency in min−1.
The invention will possibly be implemented in devices to be worn by individuals and operating in a transmission or back-scatter mode. The back-scatter configuration is particularly suitable for integration into a compact watch-type device, a portable device for monitoring actigraphy or a dermal patch. In order to improve the reliability of the estimation, the device will preferably maintain contact with the skin of the person, or be kept a fixed distance from the latter, by means of a strap or another rigid or elastic mount structure.
The invention will possibly be used to monitor living beings, such as new-borns, elderly people, athletes or people at risk. The use of the red and infrared spectral bands are suitable for integration into pulsed oximetry devices based on the same spectral bands, so as to determine other physiological parameters, such as blood saturation, according to known methods.
Number | Date | Country | Kind |
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16 51656 | Feb 2016 | FR | national |
Number | Name | Date | Kind |
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20090105565 | Xu | Apr 2009 | A1 |
20130072771 | Gu et al. | Mar 2013 | A1 |
20150196257 | Yousefi et al. | Jul 2015 | A1 |
Entry |
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French Preliminary Search Report issued Nov. 28, 2016 (with Written Opinion) in French Application 16 51656 filed on Feb. 29, 2016 (with English Translation of Categories of Cited Documents). |
Number | Date | Country | |
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20170248469 A1 | Aug 2017 | US |