Systems and methods for control of illumination or radiation collection for blood glucose and other analyte detection and measurement using collision computing
In a noninvasive system for detection/measurement of glucose and other analytes in a medium such as tissue, illumination is directed to the medium and corresponding radiation from the medium is collected. Spectral energy changes associated with fragment(s)/feature(s) obtained from the collected radiation are determined using collision computing. Such spectral energy changes generally represent analyte concentration. The collection of radiation and/or illumination is controlled either to target a particular volume of the medium or such that the spectral energy changes become directionally monotonic with respect to analyte concentration, or both. The collection parameters include: duration of collection, location and/or a size of a collection spot on the medium surface, and angle of a collector relative to the medium surface. The illuminated and/or collection spots may be treated to improve accuracy of analyte measurement.
1. A method for facilitating analysis of a medium, the method comprising the steps of:
directing illumination to a medium;
controlling a parameter of radiation collection corresponding to radiation to be collected from the medium;
collecting a first radiation fragment from the medium according to the parameter; and
determining, via a collision computer, a first renormalized spectral energy change associated with at least a portion of the first radiation fragment.
2. The method of claim 1 , wherein at least part of the first radiation fragment collected from the medium represents at least one of: (i) light transmitted through the medium, (ii) light emitted by the medium, and (iii) and light diffusely reflected from the medium.
3. The method of claim 1 , wherein the medium comprises a tissue.
4. The method of claim 1 , wherein the first renormalized spectral energy change corresponds to a quantity of an analyte present within the medium.
5. The method of claim 1 , further comprising:
collecting a second radiation fragment from the medium, at least one of: (i) a time of collection of the second fragment being different from a time of collection of the first fragment, and (ii) a spatial characteristic of the second fragment being different from a corresponding spatial characteristic of the first fragment; and
determining, via collision computing, a second renormalized spectral energy change associated with at least a portion of the second radiation fragment,
wherein one of:
(a1) the first renormalized spectral energy change comprises a first renormalized spectral energy gain and the second renormalized spectral energy change comprises a second renormalized spectral energy gain; and
(b1) controlling the parameter comprises adjusting the parameter to a value at which the second renormalized spectral energy gain is not less than the first renormalized spectral energy gain; and
(a2) the first renormalized spectral energy change comprises a first renormalized spectral energy loss and the second renormalized spectral energy change comprises a second renormalized spectral energy loss; and
(b2) controlling the parameter comprises adjusting the parameter to a value at which the second renormalized spectral energy loss is not less than the first renormalized spectral energy loss.
6. The method of claim 5 , wherein the parameter comprises at least one of: (i) a location of a spot on a surface of the medium from which the radiation is collected, (ii) a location of a component of a collector subsystem relative to the surface of the medium in a Z dimension, (iii) a focal length of a component of a collector subsystem, (iv) a focal point of the collected radiation, (v) an angle of collection relative to a normal to a surface of the medium, (vi) an area of a spot on a surface of the medium from which the radiation is collected, (vii) a duration of activation of a detector, and (viii) an area of a detector.
7. The method of claim 1 , wherein controlling the parameter of radiation collection comprises at least one of: (i) varying a location of a spot on a surface of the medium from which the radiation is collected in at least one of: an X dimension and a Y dimension, and (ii) varying a location of a component of a collector subsystem relative to the surface of the medium in a Z dimension.
8. The method of claim 1 , wherein controlling the parameter of radiation collection comprises at least one of:
varying an angle of collection relative to a normal to a surface of the medium;
varying an area of a spot on a surface of the medium from which the radiation is collected; and
adjusting at least one of: (i) duration of activation of a detector, and (ii) area of a detector.
9. The method of claim 1 , further comprising controlling a parameter of the illumination, by adjusting at least one of: (i) an amplitude of the illumination, comprising at least one of an intensity of the illumination and a duration of the illumination, (ii) a focal length of the illumination, (iii) a focal point of the illumination, (iv) a location of a target region of the medium to be illuminated by the illumination, (v) a size of the target region of the medium to be illuminated by the illumination, (vi) an angle of incidence of the illumination upon the medium, and (vii) a spectral characteristic, comprising at least one of a wavelength and a bandwidth of the illumination.
10. A method for facilitating analysis of a medium, the method comprising the steps of:
directing illumination to a medium;
collecting a plurality of radiation fragments from the medium;
dynamically controlling at least one of (i) a parameter of illumination and (ii) a parameter of collection of the radiation fragments; and
determining, a collision computer, respective renormalized spectral energy change values associated with the radiation fragments.
11. The method of claim 10 , wherein the medium comprises a tissue.
12. The method of claim 10 , wherein dynamically controlling the illumination parameter comprises at least one of:
(i) modifying a value of the illumination parameter until the illumination impinges upon a specified target volume within the medium
(ii) varying a location of a spot on a surface of the medium to which the illumination is directed in at least one of: an X dimension and a Y dimension; and
(iii) varying a location of a component of an illumination subsystem relative to the surface of the medium in a Z dimension.
13. The method of claim 10 , wherein dynamically controlling the collection parameter comprises at least one of:
(i) modifying a value of the collection parameter until at least one of the radiation fragment comprises radiation collected from a specified target volume within the medium;
(ii) varying a location of a spot on a surface of the medium from which the radiation fragments are collected in at least one of: an X dimension and a Y dimension; and
(iii) varying a location of a component of a collector subsystem relative to the surface of the medium in a Z dimension.
14. The method of claim 10 , wherein dynamically controlling of at least one of (i) the parameter of illumination and (ii) the parameter of collection of the radiation fragments comprises adjusting an interface associated with a spot on a surface of the medium.
15. The method of claim 14 , wherein adjusting the interface comprises at least one of:
changing a pressure applied by an optical probe to the spot; and
applying an index-matching material between an optical probe and the spot.
16. The method of claim 14 , wherein adjusting the interface comprises changing an optical property of the spot by at least one of: (i) electronic stimulation of the spot, (ii) radio frequency stimulation of the spot, (iii) mechanical stimulation of the spot, and (iv) application of a topical rubefacient to the spot.
17. The method of claim 14 , wherein the interface is further associated with at least one of: (i) a source of the illumination and (ii) a collector for collecting the radiation fragments.
18. The method of claim 10 , wherein at least one of the renormalized spectral energy change values corresponds to a quantity of an analyte present within the medium.
19. The method of claim 10 , wherein each respective spectral energy change value represents one of a spectral energy gain and a spectral energy loss.
20. A system for facilitating analysis of a medium, comprising:
an illumination subsystem for directing illumination to a medium;
an adjustable collector for collecting a radiation fragment from the medium according to a selected parameter of radiation collection; and
a collision computer programmed to compute renormalized spectral energy change associated with at least a portion of the collected radiation fragment.
21. The system of claim 20 , wherein the adjustable collector is adapted to collect, as at least a part of the radiation fragment, at least one of: (i) light transmitted through the medium, (ii) light emitted by the medium, and (iii) and light diffusely reflected from the medium.
22. The system of claim 20 , wherein:
the medium comprises a tissue; and
the adjustable collector is adapted to collect the radiation fragment from the tissue.
23. The system of claim 20 , wherein the collision computer is programmed to compute the renormalized spectral energy change as a measure of a quantity of an analyte present within the medium.
24. The system of claim 20 , wherein:
the parameter of radiation collection comprises a location parameter; and
the adjustable collector comprises a translator adapted to adjust, according to the location parameter, a location of a spot on a surface of the medium from which the radiation is collected in at least one of: an X dimension and a Y dimension.
25. The system of claim 24 , wherein the translator comprises at least one of a movable translator, an opto-mechanical translator, and an electro-optical translator.
26. The system of claim 20 , wherein:
the parameter of radiation collection comprises a size of a spot on a surface of the medium from which the radiation is collected; and
the adjustable collector comprises at least one of a movable detector and a movable lens assembly, movable according to the spot size in a Z dimension relative to the surface of the medium.
27. The system of claim 20 , wherein:
the parameter of radiation collection comprises a size of a spot on a surface of the medium from which the radiation is collected; and
the adjustable collector comprises an focus lens assembly adjustable according to the spot size.
28. The system of claim 20 , wherein:
the parameter of radiation collection comprises an angle of collection relative to a normal to a surface of the medium; and
the adjustable collector comprises at least one of:
(i) a radiation-collection conduit adjustable at a plurality of angles relative to the normal to the surface of the medium; and
(ii) a plurality of radiation-collection conduits each being oriented at a different respective angle relative to the surface of the medium.
29. The system of claim 20 , wherein the adjustable collector comprises at least one of: (i) a detector having adjustable activation duration, and (ii) a detector having adjustable area of detection.
30. The system of claim 20 , wherein the an illumination subsystem comprises an adjustable illumination system adapted to adjust at least one of: (i) an amplitude of the illumination, comprising at least one of an intensity of the illumination and a duration of the illumination, (ii) a focal length of the illumination, (iii) a focal point of the illumination, (iv) a location of a target region of the medium to be illuminated by the illumination, (v) a size of the target region of the medium to be illuminated by the illumination, (vi) an angle of incidence of the illumination upon the medium, and (vii) a spectral characteristic, comprising at least one of a wavelength and a bandwidth of the illumination.