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Glucose concentration measuring method and apparatus with short coherence source and heterodyne interferometer    

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United States Patent5835215   
Link to this pagehttp://www.wikipatents.com/5835215.html
Inventor(s)Toida; Masahiro (Kanagawa-ken, JP); Miyagawa; Ichirou (Kanagawa-ken, JP)
AbstractA low coherence light beam is irradiated to the eyeball. A backward scattered light beam, which is reflected from each depth position in the eyeball, and a reference light beam, which is reflected from a mirror capable of moving, are caused to interfere with each other. A first backward scattered light beam, which comes from the interface between the cornea and the anterior aqueous chamber, and a second backward scattered light beam, which comes from the interface between the anterior aqueous chamber and the crystalline lens, are thus separated accurately from each other. An optical absorbance of the anterior aqueous chamber (the aqueous humor) is calculated from the intensities of the two backward scattered light beams. Each of a plurality of low coherence light beams having different wavelengths is irradiated to the eyeball, and the aforesaid operation is repeated. The concentration of glucose in the aqueous humor is measured by utilizing near-infrared spectroscopy. The measurement is thus achieved non-invasively and accurately.
   














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Inventor     Toida; Masahiro (Kanagawa-ken, JP); Miyagawa; Ichirou (Kanagawa-ken, JP)
Owner/Assignee     Fuji Photo Film Co., Ltd. (Kanagawa-ken, JP)
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Publication Date     November 10, 1998
Application Number     08/857,205
PAIR File History     Application Data   Transaction History
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Litigation
Filing Date     May 15, 1997
US Classification     356/484 600/319
Int'l Classification     G01B 009/02
Examiner     Turner; Samuel A .
Assistant Examiner    
Attorney/Law Firm     Sughrue, Mion, Zinn, Macpeak & Seas, PLLC
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Priority Data     May 16, 1996[JP]8-121790
USPTO Field of Search     356/345 356/357 356/361 356/349 250/227.27 351/211 600/316 600/318 600/319
Patent Tags     glucose concentration measuring short coherence source heterodyne interferometer
   
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What is claimed is:

1. A glucose concentration measuring method, comprising the steps of:

i) splitting a low coherence light beam, which has been radiated out of a predetermined light source, into a signal light beam and a reference light beam, each of which travels along one of two different optical paths,

ii) modulating at least either one of said signal light beam and said reference light beam such that a slight difference in frequency may occur between them,

iii) irradiating said signal light beam to the eyeball lying at a predetermined position,

iv) causing a first backward scattered light beam of said signal light beam having been irradiated to the eyeball, said first backward scattered light beam coming from an interface between the cornea and the anterior aqueous chamber of the eyeball, and said reference light beam to interfere with each other by adjusting an optical path length of said reference light beam, a first interference light beam being thereby obtained,

v) measuring an intensity of said first interference light beam,

vi) calculating an intensity of said first backward scattered light beam from the intensity of said first interference light beam,

vii) causing a second backward scattered light beam of said signal light beam having been irradiated to the eyeball, said second backward scattered light beam coming from an interface between the anterior aqueous chamber and the crystalline lens of the eyeball, and said reference light beam to interfere with each other by adjusting the optical path length of said reference light beam, a second interference light beam being thereby obtained,

viii) measuring an intensity of said second interference light beam,

ix) calculating an intensity of said second backward scattered light beam from the intensity of said second interference light beam,

x) obtaining light absorption characteristics of constituents of the aqueous humor, which fills the anterior aqueous chamber, from the intensity of said first backward scattered light beam and the intensity of said second backward scattered light beam,

xi) obtaining light absorption characteristics of the constituents of the aqueous humor with respect to each of a plurality of other low coherence light beams, which are of wavelength bands different from the wavelength band of said low coherence light beam, in the same manner, and

xii) calculating a concentration of glucose in the constituents of the aqueous humor from the light absorption characteristics, which have been obtained with respect to the plurality of said low coherence light beams.

2. A method as defined in claim 1 wherein each of said low coherence light beams is selected as a portion of light, which is of an emission wavelength band wider than the wavelength band of each low coherence light beam.

3. A method as defined in claim 1 wherein each of said low coherence light beams is radiated out of one of a plurality of different light sources.

4. A glucose concentration measuring method, comprising the steps of:

with respect to concentrations of glucose in the constituents of the aqueous humor, which concentrations have been measured with a method as defined in claim 1, invasively measuring the corresponding concentrations of glucose in the blood, correlation between the concentrations of glucose in the constituents of the aqueous humor and the concentrations of glucose in the blood being thereby determined previously, and

thereafter non-invasively determining a concentration of glucose in the blood from a concentration of glucose in the constituents of the aqueous humor, which concentration is newly measured with a method as defined in claim 1, and said correlation.

5. A glucose concentration measuring apparatus, comprising:

i) a light source device for radiating out a plurality of low coherence light beams, which are of different emission wavelength bands,

ii) an optical path splitting means for splitting each of the low coherence light beams, which has been radiated out of said light source device, into a signal light beam irradiated to the eyeball and a reference light beam, each of which travels along one of two different optical paths,

iii) a modulation means, which is located in at least either one of the two different optical paths and modulates at least either one of said signal light beam and said reference light beam such that a slight difference in frequency may occur between them,

iv) an optical path length adjusting means for adjusting the length of the optical path, along which said reference light beam travels,

v) a wavefront matching means for:

matching a wave front of a first backward scattered light beam of said signal light beam having been irradiated to the eyeball, said first backward scattered light beam coming from an interface between the cornea and the anterior aqueous chamber of the eyeball, and a wave front of said reference light beam with each other, and

matching a wave front of a second backward scattered light beam of said signal light beam having been irradiated to the eyeball, said second backward scattered light beam coming from an interface between the anterior aqueous chamber and the crystalline lens of the eyeball, and a wave front of said reference light beam with each other,

vi) a photodetector for photoelectrically detecting an intensity of a first interference light beam, which is obtained from the matching of the wave front of said first backward scattered light beam and the wave front of said reference light beam with each other, and an intensity of a second interference light beam, which is obtained from the matching of the wave front of said second backward scattered light beam and the wave front of said reference light beam with each other,

vii) a heterodyne operation means for calculating an intensity of said first backward scattered light beam from the intensity of said first interference light beam, and calculating an intensity of said second backward scattered light beam from the intensity of said second interference light beam,

viii) a light absorption characteristics analyzing means for obtaining light absorption characteristics of constituents of the aqueous humor, which fills the anterior aqueous chamber, from the intensity of said first backward scattered light beam and the intensity of said second backward scattered light beam, and

ix) a glucose concentration calculating means for calculating a concentration of glucose in the constituents of the aqueous humor from the light absorption characteristics, which have been obtained with respect to the plurality of said low coherence light beams.

6. An apparatus as defined in claim 5 wherein said light source device comprises a single light source for radiating out low coherence light, which is of an emission wavelength band wider than the wavelength band of each of said low coherence light beams, and a wavelength selecting means for selecting each of said low coherence light beams with respect to the wavelength from said low coherence light, which is of the wide emission wavelength band.

7. An apparatus as defined in claim 5 wherein said light source device comprises a plurality of light sources, each of which radiates out one of said low coherence light beams.

8. A glucose concentration measuring apparatus, comprising a table representing correlation between concentrations of glucose in the constituents of the aqueous humor, which concentrations have been measured with an apparatus as defined in claim 5, and concentrations of glucose in the blood, which have been measured previously,

wherein a concentration of glucose in the blood is non-invasively determined from a concentration of glucose in the constituents of the aqueous humor, which concentration is newly measured with an apparatus as defined in claim 5, and said table.
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BACKGROUND OF THE INVENTION

1. Field of the Invention

This invention relates to a method and apparatus for measuring a concentration of glucose in a living body. This invention particularly relates to a method and apparatus for measuring non-invasively the concentration of glucose in the aqueous humor in the anterior aqueous chamber of the eyeball, and a method and apparatus for measuring non-invasively the concentration of glucose in the blood in accordance with the concentration of glucose in the aqueous humor.

2. Description of the Prior Art

The mean level of glucose in the blood varies for different persons and is an important index for determining whether drugs are to be or are not to be administered to diabetic patients.

The concentration of glucose in the blood has the characteristics such that it fluctuates markedly within a very short time in accordance with food intake, physical activity, a complication by another disease, or the like. Urgent dosage is often required due to a sharp increase in concentration of blood glucose.

Therefore, as for patients having such a disease, it is desired that the concentration of glucose in the blood can be monitored at as short intervals as possible. Ordinarily, monitoring of the concentration of glucose in the blood is carried out by lancing the finger of the patient in order to obtain a drop of blood, analyzing the drop of blood, and thereby measuring the concentration of glucose in the blood. Since the lancing of the finger is painful, it is difficult to compel the patients to undergo the measurement procedure many times per day.

Accordingly, recently, in lieu of the invasive measurements having the drawbacks described above, various non-invasive measuring methods, which are not accompanied by pain, have been proposed.

The non-invasive measuring methods are primarily based upon the findings in that the concentration of glucose in the aqueous humor, which fills the anterior aqueous chamber located between the cornea and the crystalline lens of the human eyeball, has strong correlation with the concentration of glucose in the blood, though the level of correlation varies for different persons. With the non-invasive measuring methods, the concentration of glucose in the aqueous humor is measured non-invasively.

For example, a glucose sensor system, wherein the angle of rotation of infrared radiation having impinged upon the aqueous humor is measured, and the concentration of glucose having relationship with the angle of rotation is thereby determined, is proposed in, for example, U.S. Pat. No. 3,958,560.

Also, a technique for measuring stimulated Raman light from glucose is disclosed in, for example, WO 92/10131.

Further, a device for measuring the optical properties of light reflected from the crystalline lens of the eye is described in, for example, U.S. Pat. No. 5,535,743. Furthermore, a method for measuring the concentration of glucose in the aqueous humor is described in, for example, U.S. Pat. No. 5,433,197.

However, with the device described in U.S. Pat. No. 5,535,743, light reflected from the interface between the cornea and the aqueous humor cannot be eliminated, and information representing absorption at the cornea is detected together with the necessary information. Therefore, the accuracy, with which the concentration of glucose in the aqueous humor is determined, cannot be kept high.

Further, in U.S. Pat. No. 5,535,743, nothing is disclosed as to technical means to be used for measuring a minute change in absorbance. Therefore, the device described in U.S. Pat. No. 5,535,743 cannot be appropriately used in practice.

As for the glucose sensor system proposed in U.S. Pat. No. 3,958,560, many compounds other than glucose in the aqueous humor are optically active and take part in rotation of the plane of polarization. Also, the cornea exhibits birefringence and therefore causes rotation of the plane of polarization to occur. Accordingly, with the glucose sensor system proposed in U.S. Pat. No. 3,958,560, wherein the concentration of glucose in the aqueous humor is determined from the angle of rotation, the measurement accuracy cannot be kept high.

With the technique disclosed in WO 92/10131, in order for stimulated Raman light from glucose to be measured, a pump laser beam having a high intensity is introduced into the anterior aqueous chamber and in a direction normal to the vision line optical axis. Therefore, a practical measuring system cannot be constituted easily.

SUMMARY OF THE INVENTION

The primary object of the present invention is to provide a glucose concentration measuring method, wherein the concentration of glucose in the aqueous humor is measured non-invasively and with a high accuracy.

Another object of the present invention is to provide a glucose concentration measuring method, wherein the concentration of glucose in the blood is measured non-invasively from the non-invasively obtained concentration of glucose in the aqueous humor.

Another object of the present invention is to provide an apparatus for carrying out the glucose concentration measuring method.

The present invention provides a first glucose concentration measuring method, comprising the steps of:

i) splitting a low coherence light beam, which has been radiated out of a predetermined light source, into a signal light beam and a reference light beam, each of which travels along one of two different optical paths,

ii) modulating at least either one of the signal light beam and the reference light beam such that a slight difference in frequency may occur between them,

iii) irradiating the signal light beam to the eyeball lying at a predetermined position,

iv) causing a first backward scattered light beam of the signal light beam having been irradiated to the eyeball, the first backward scattered light beam coming from an interface between the cornea and the anterior aqueous chamber of the eyeball, and the reference light beam to interfere with each other by adjusting an optical path length of the reference light beam, a first interference light beam being thereby obtained,

v) measuring an intensity of the first interference light beam,

vi) calculating an intensity of the first backward scattered light beam from the intensity of the first interference light beam,

vii) causing a second backward scattered light beam of the signal light beam having been irradiated to the eyeball, the second backward scattered light beam coming from an interface between the anterior aqueous chamber and the crystalline lens of the eyeball, and the reference light beam to interfere with each other by adjusting the optical path length of the reference light beam, a second interference light beam being thereby obtained,

viii) measuring an intensity of the second interference light beam,

ix) calculating an intensity of the second backward scattered light beam from the intensity of the second interference light beam,

x) obtaining light absorption characteristics of constituents of the aqueous humor, which fills the anterior aqueous chamber, from the intensity of the first backward scattered light beam and the intensity of the second backward scattered light beam,

xi) obtaining light absorption characteristics of the constituents of the aqueous humor with respect to each of a plurality of other low coherence light beams, which are of wavelength bands different from the wavelength band of the low coherence light beam, in the same manner, and

xii) calculating a concentration of glucose in the constituents of the aqueous humor from the light absorption characteristics, which have been obtained with respect to the plurality of the low coherence light beams.

In the first glucose concentration measuring method in accordance with the present invention, as the light source for producing each of the low coherence light beams, a super-luminescent diode (SLD), a light emitting diode (LED), or the like, which produces a light beam having a coherence length of as short as approximately several tens of microns, may be employed. Practically, an SLD having a high directivity should preferably be used.

The term "measuring an intensity of an interference light beam" as used herein means the measurement of the intensity of the beat signal (i.e., the interference light beam), the intensity of which repeatedly becomes high and low at a frequency equal to the difference between the frequencies of the backward scattered light beam (i.e., the signal light beam) and the reference light beam.

In the first glucose concentration measuring method in accordance with the present invention, each of the low coherence light beams may be selected as a portion of light, which is of an emission wavelength band wider than the wavelength band of each low coherence light beam. Alternatively, each of the low coherence light beams may be radiated out of one of a plurality of different light sources.

In cases where a plurality of different light sources, which produce the low coherence light beams of different wavelength bands, are employed, the low coherence light beams may be radiated successively out of the plurality of the light sources, and the interference light beams corresponding to the low coherence light beams may be detected with a single photodetector.

The present invention also provides a second glucose concentration measuring method, comprising the steps of:

i) splitting a coherent light beam (e.g., a laser beam), which has been radiated out of a predetermined light source and the frequency of which is swept temporally in a sawtooth-like form (e.g., as illustrated in FIG. 6), into a signal light beam and a reference light beam, each of which travels along one of two different optical paths,

ii) irradiating the signal light beam to the eyeball lying at a predetermined position,

iii) causing a first backward scattered light beam of the signal light beam, the first backward scattered light beam coming from an interface between the cornea and the anterior aqueous chamber of the eyeball, and the reference light beam to interfere with each other, the reference light beam being constituted of the coherent light beam, which has been radiated out of the light source with a difference in time in accordance with a difference between an optical path length of the signal light beam (traveling from the position, at which the signal light beam is split from the reference light beam, to the interface between the cornea and the anterior aqueous chamber of the eyeball) and the first backward scattered light beam (traveling from the interface between the cornea and the anterior aqueous chamber of the eyeball to the position, at which the first backward scattered light beam interferes with the reference light beam) and an optical path length of the reference light beam (traveling from the position, at which the reference light beam is split from the signal light beam, to the position, at which the reference light beam interferes with the first backward scattered light beam), and which has a difference in frequency with respect to the first backward scattered light beam, a first interference light beam being thereby obtained,

iv) measuring an intensity of the first interference light beam,

v) calculating an intensity of the first backward scattered light beam from the intensity of the first interference light beam,

vi) causing a second backward scattered light beam of the signal light beam, the second backward scattered light beam coming from an interface between the anterior aqueous chamber and the crystalline lens of the eyeball, and the reference light beam to interfere with each other, the reference light beam being constituted of the coherent light beam, which has been radiated out of the light source with a difference in time in accordance with a difference between an optical path length of the signal light beam (traveling from the position, at which the signal light beam is split from the reference light beam, to the interface between the anterior aqueous chamber and the crystalline lens of the eyeball) and the second backward scattered light beam (traveling from the interface between the anterior aqueous chamber and the crystalline lens of the eyeball to the position, at which the second backward scattered light beam interferes with the reference light beam) and an optical path length of the reference light beam (traveling from the position, at which the reference light beam is split from the signal light beam, to the position, at which the reference light beam interferes with the second backward scattered light beam), and which has a difference in frequency with respect to the second backward scattered light beam, a second interference light beam being thereby obtained,

vii) measuring an intensity of the second interference light beam,

viii) calculating an intensity of the second backward scattered light beam from the intensity of the second interference light beam,

ix) obtaining light absorption characteristics of constituents of the aqueous humor, which fills the anterior aqueous chamber, from the intensity of the first backward scattered light beam and the intensity of the second backward scattered light beam,

x) obtaining light absorption characteristics of the constituents of the aqueous humor with respect to each of a plurality of other coherent light beams, which have wavelengths different from the wavelength of the coherent light beam, in the same manner, and

xi) calculating a concentration of glucose in the constituents of the aqueous humor from the light absorption characteristics, which have been obtained with respect to the plurality of the coherent light beams.

In the second glucose concentration measuring method in accordance with the present invention, the reference light beam, which is caused to interfere with the first backward scattered light beam, has a difference in frequency with respect to the first backward scattered light beam. The reasons for this will be described hereinbelow.

The optical paths are set such that the sum of the length of the optical path, along which the signal light beam travels, and the length of the optical path, along which the first backward scattered light beam travels, may be different from the length of the optical path, along which the reference light beam travels. (The optical path length of the reference light beam may be shorter than the sum of the optical path lengths of the signal light beam and the first backward scattered light beam.

Alternatively, the optical path length of the reference light beam may be longer than the sum of the optical path lengths of the signal light beam and the first backward scattered light beam.) Due to the difference in optical path length, for example, in cases where the optical path length of the reference light beam is shorter than the sum of the optical path lengths of the signal light beam and the first backward scattered light beam, the reference light beam arrives at the position, at which the wavefront matching (the interference) is effected, with an earlier timing than the first backward scattered light beam does.

Specifically, at the time at which the first backward scattered light beam arrives at the position of interference, the reference light beam, which was split from the signal light beam that formed the first backward scattered light beam, has already passed through the position of interference, and the reference light beam, which is a portion of the coherent light beam radiated out of the light source with a later timing than the signal light beam was, arrives at the position of interference.

The frequency of the coherent light beam, which is radiated out of the light source with a later timing than the signal light beam was, is swept temporally. Therefore, there is a slight difference in frequency between the reference light beam, which is caused to interfere with the first backward scattered light beam, and the first backward scattered light beam.

The reference light beam, which is caused to interfere with the second backward scattered light beam, has a frequency different from the frequency of the reference light beam, which is caused to interfere with the first backward scattered light beam. Specifically, the first backward scattered light beam comes from the interface between the cornea and the anterior aqueous chamber, and the second backward scattered light beam comes from the interface between the anterior aqueous chamber and the crystalline lens, the latter interface being located at a position in the eyeball deeper than the former interface. Therefore, a difference in time, which corresponds to the difference in optical path length between the first backward scattered light beam and the second backward scattered light beam (the difference being two times as long as the thickness of the anterior aqueous chamber), occurs between when the first backward scattered light beam arrives at the position of interference and when the second backward scattered light beam arrives as the position of interference. As a result, the reference light beam, which is caused to interfere with the second backward scattered light beam, is the one constituted of a portion of the coherent light beam, which is radiated out of the light source with a later timing than the reference light beam caused to interfere with the first backward scattered light beam is.

In the second glucose concentration measuring method in accordance with the present invention, the coherent light beams may be selectively radiated out of a single light source. Alternatively, each of the coherent light beams may be radiated out of one of a plurality of different light sources.

The present invention further provides a third glucose concentration measuring method, comprising the steps of:

i) irradiating an ultrashort pulsed light beam, which has been radiated out of a predetermined light source, to the eyeball,

ii) measuring each of an intensity of a first backward scattered light beam of the ultrashort pulsed light beam, the first backward scattered light beam coming from an interface between the cornea and the anterior aqueous chamber of the eyeball, and an intensity of a second backward scattered light beam of the ultrashort pulsed light beam, the second backward scattered light beam coming from an interface between the anterior aqueous chamber and the crystalline lens of the eyeball,

iii) obtaining light absorption characteristics of constituents of the aqueous humor, which fills the anterior aqueous chamber, from the intensity of the first backward scattered light beam and the intensity of the second backward scattered light beam,

iv) obtaining light absorption characteristics of the constituents of the aqueous humor with respect to each of a plurality of other ultrashort pulsed light beams, which have wavelengths different from the wavelength of the ultrashort pulsed light beam, in the same manner, and

v) calculating a concentration of glucose in the constituents of the aqueous humor from the light absorption characteristics, which have been obtained with respect to the plurality of the ultrashort pulsed light beams having different wavelengths.

The term "ultrashort pulsed light beam" as used herein means the pulsed light beam, which is emitted for a very short time (e.g., on the order of femtoseconds to picoseconds) such that the intensity of the first backward scattered light beam and the intensity of the second backward scattered light beam coming from the interface between the anterior aqueous chamber and the crystalline lens can at least be separated temporally and measured respectively. The ultrashort pulsed light beam may be produced by a mode locked Ti:sapphire laser, or the like. In cases where the ultrashort pulsed light beam is employed, the second backward scattered light beam, which lags behind the first backward scattered light beam by a length of time corresponding to the distance two times as long as the thickness of the anterior aqueous chamber, can be detected separately from the first backward scattered light beam by using a photodetector capable of effecting time resolution, such as a streak camera.

In the third glucose concentration measuring method in accordance with the present invention, the ultrashort pulsed light beams may be selectively radiated out of a single light source. Alternatively, each of the ultrashort pulsed light beams may be radiated out of one of a plurality of different light sources.

The present invention still further provides a fourth glucose concentration measuring method, comprising the steps of:

with respect to concentrations of glucose in the constituents of the aqueous humor, which concentrations have been measured with the aforesaid first, second, or third glucose concentration measuring method in accordance with the present invention, invasively measuring the corresponding concentrations of glucose in the blood, correlation between the concentrations of glucose in the constituents of the aqueous humor and the concentrations of glucose in the blood being thereby determined previously, and

thereafter non-invasively determining a concentration of glucose in the blood from a concentration of glucose in the constituents of the aqueous humor, which concentration is newly measured with the aforesaid first, second, or third glucose concentration measuring method in accordance with the present invention, and the correlation.

The present invention also provides an apparatus for carrying out the aforesaid first glucose concentration measuring method in accordance with the present invention. Specifically, the present invention also provides a first glucose concentration measuring apparatus, comprising:

i) a light source device for radiating out a plurality of low coherence light beams, which are of different emission wavelength bands,

ii) an optical path splitting means for splitting each of the low coherence light beams, which has been radiated out of the light source device, into a signal light beam irradiated to the eyeball and a reference light beam, each of which travels along one of two different optical paths,

iii) a modulation means, which is located in at least either one of the two different optical paths and modulates at least either one of the signal light beam and the reference light beam such that a slight difference in frequency may occur between them,

iv) an optical path length adjusting means for adjusting the length of the optical path, along which the reference light beam travels,

v) a wavefront matching means for:

matching a wave front of a first backward scattered light beam of the signal light beam having been irradiated to the eyeball, the first backward scattered light beam coming from an interface between the cornea and the anterior aqueous chamber of the eyeball, and a wave front of the reference light beam with each other, and

matching a wave front of a second backward scattered light beam of the signal light beam having been irradiated to the eyeball, the second backward scattered light beam coming from an interface between the anterior aqueous chamber and the crystalline lens of the eyeball, and a wave front of the reference light beam with each other,

vi) a photodetector for photoelectrically detecting an intensity of a first interference light beam, which is obtained from the matching of the wave front of the first backward scattered light beam and the wave front of the reference light beam with each other, and an intensity of a second interference light beam, which is obtained from the matching of the wave front of the second backward scattered light beam and the wave front of the reference light beam with each other,

vii) a heterodyne operation means for calculating an intensity of the first backward scattered light beam from the intensity of the first interference light beam, and calculating an intensity of the second backward scattered light beam from the intensity of the second interference light beam,

viii) a light absorption characteristics analyzing means for obtaining light absorption characteristics of constituents of the aqueous humor, which fills the anterior aqueous chamber, from the intensity of the first backward scattered light beam and the intensity of the second backward scattered light beam, and

ix) a glucose concentration calculating means for calculating a concentration of glucose in the constituents of the aqueous humor from the light absorption characteristics, which have been obtained with respect to the plurality of the low coherence light beams.

In the first glucose concentration measuring apparatus in accordance with the present invention, the light source device may comprise a single light source for radiating out low coherence light, which is of an emission wavelength band wider than the wavelength band of each of the low coherence light beams, and a wavelength selecting means for selecting each of the low coherence light beams with respect to the wavelength from the low coherence light, which is of the wide emission wavelength band. Alternatively, the light source device may comprise a plurality of light sources, each of which radiates out one of the low coherence light beams.

The present invention further provides an apparatus for carrying out the aforesaid second glucose concentration measuring method in accordance with the present invention. Specifically, the present invention further provides a second glucose concentration measuring apparatus, comprising:

i) a light source device for radiating out a plurality of coherent light beams, which have different wavelengths and the frequencies of which are swept temporally in a sawtooth-like form (e.g., as illustrated in FIG. 6),

ii) an optical path splitting means for splitting each of the coherent light beams, which has been radiated out of the light source device and the frequency of which is swept, into a signal light beam irradiated to the eyeball and a reference light beam, each of which travels along one of two different optical paths,

iii) a wavefront matching means for:

matching a wave front of a first backward scattered light beam of the signal light beam, the first backward scattered light beam coming from an interface between the cornea and the anterior aqueous chamber of the eyeball, and a wave front of the reference light beam with each other, the reference light beam being constituted of the coherent light beam, which has been radiated out of the light source device with a difference in time in accordance with a difference between an optical path length of the signal light beam and the first backward scattered light beam and an optical path length of the reference light beam, and which has a difference in frequency with respect to the first backward scattered light beam, and

matching a wave front of a second backward scattered light beam of the signal light beam, the second backward scattered light beam coming from an interface between the anterior aqueous chamber and the crystalline lens of the eyeball, and a wave front of the reference light beam with each other, the reference light beam being constituted of the coherent light beam, which has been radiated out of the light source device with a difference in time in accordance with a difference between an optical path length of the signal light beam and the second backward scattered light beam and an optical path length of the reference light beam, and which has a difference in frequency with respect to the second backward scattered light beam,

iv) a photodetector for photoelectrically detecting an intensity of a first interference light beam, which is obtained from the matching of the wave front of the first backward scattered light beam and the wave front of the reference light beam, the reference light beam having the slight difference in frequency with respect to the first backward scattered light beam, with each other, and an intensity of a second interference light beam, which is obtained from the matching of the wave front of the second backward scattered light beam and the wave front of the reference light beam, the reference light beam having the slight difference in frequency with respect to the second backward scattered light beam, with each other,

v) a heterodyne operation means for calculating an intensity of the first backward scattered light beam from the intensity of the first interference light beam, and calculating an intensity of the second backward scattered light beam from the intensity of the second interference light beam,

vi) a light absorption characteristics analyzing means for obtaining light absorption characteristics of constituents of the aqueous humor, which fills the anterior aqueous chamber, from the intensity of the first backward scattered light beam and the intensity of the second backward scattered light beam, and

vii) a glucose concentration calculating means for calculating a concentration of glucose in the constituents of the aqueous humor from the light absorption characteristics, which have been obtained with respect to the plurality of the coherent light beams.

In the second glucose concentration measuring apparatus in accordance with the present invention, the light source device may comprise a single light source capable of selectively radiating out each of the plurality of the coherent light beams, and a control means for controlling the light source such that the light source may selectively radiate out one of the plurality of the coherent light beams. Alternatively, the light source device may comprise a plurality of light sources, each of which radiates out one