NZ759983B2 - Detector with reduced fluorescence range noise - Google Patents
Detector with reduced fluorescence range noise Download PDFInfo
- Publication number
- NZ759983B2 NZ759983B2 NZ759983A NZ75998318A NZ759983B2 NZ 759983 B2 NZ759983 B2 NZ 759983B2 NZ 759983 A NZ759983 A NZ 759983A NZ 75998318 A NZ75998318 A NZ 75998318A NZ 759983 B2 NZ759983 B2 NZ 759983B2
- Authority
- NZ
- New Zealand
- Prior art keywords
- light
- detector surface
- metal complex
- complex dye
- filter material
- Prior art date
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Classifications
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
- G01N21/645—Specially adapted constructive features of fluorimeters
- G01N2021/6463—Optics
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
- G01N21/645—Specially adapted constructive features of fluorimeters
- G01N2021/6463—Optics
- G01N2021/6471—Special filters, filter wheel
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/01—Arrangements or apparatus for facilitating the optical investigation
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
- G01N21/6402—Atomic fluorescence; Laser induced fluorescence
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
- G01N21/6428—Measuring fluorescence of fluorescent products of reactions or of fluorochrome labelled reactive substances, e.g. measuring quenching effects, using measuring "optrodes"
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
- G01N21/645—Specially adapted constructive features of fluorimeters
- G01N21/6452—Individual samples arranged in a regular 2D-array, e.g. multiwell plates
- G01N21/6454—Individual samples arranged in a regular 2D-array, e.g. multiwell plates using an integrated detector array
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N21/00—Investigating or analysing materials by the use of optical means, i.e. using sub-millimetre waves, infrared, visible or ultraviolet light
- G01N21/62—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light
- G01N21/63—Systems in which the material investigated is excited whereby it emits light or causes a change in wavelength of the incident light optically excited
- G01N21/64—Fluorescence; Phosphorescence
- G01N21/6486—Measuring fluorescence of biological material, e.g. DNA, RNA, cells
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N2201/00—Features of devices classified in G01N21/00
- G01N2201/08—Optical fibres; light guides
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- G—PHYSICS
- G01—MEASURING; TESTING
- G01N—INVESTIGATING OR ANALYSING MATERIALS BY DETERMINING THEIR CHEMICAL OR PHYSICAL PROPERTIES
- G01N33/00—Investigating or analysing materials by specific methods not covered by groups G01N1/00 - G01N31/00
- G01N33/48—Biological material, e.g. blood, urine; Haemocytometers
- G01N33/50—Chemical analysis of biological material, e.g. blood, urine; Testing involving biospecific ligand binding methods; Immunological testing
- G01N33/53—Immunoassay; Biospecific binding assay; Materials therefor
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B19/00—Condensers, e.g. light collectors or similar non-imaging optics
- G02B19/0004—Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed
- G02B19/0019—Condensers, e.g. light collectors or similar non-imaging optics characterised by the optical means employed having reflective surfaces only (e.g. louvre systems, systems with multiple planar reflectors)
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B19/00—Condensers, e.g. light collectors or similar non-imaging optics
- G02B19/0033—Condensers, e.g. light collectors or similar non-imaging optics characterised by the use
- G02B19/0076—Condensers, e.g. light collectors or similar non-imaging optics characterised by the use for use with a detector
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B5/00—Optical elements other than lenses
- G02B5/20—Filters
- G02B5/22—Absorbing filters
- G02B5/223—Absorbing filters containing organic substances, e.g. dyes, inks or pigments
-
- H01L27/14621—
-
- H01L27/14625—
-
- H01L27/14643—
Abstract
There is set forth herein a device comprising structure defining a detector surface configured for supporting biological or chemical substances, and a sensor array comprising light sensors and circuitry to transmit data signals using photons detected by the light sensors. The device can include one or more features for reducing fluorescence range noise in a detection band of the sensor array. The device comprises: a structure defining a detector surface for supporting biological or chemical samples; a sensor array comprising light sensors, and circuitry to transmit data signals based on photons detected by the light sensors; and a guide array comprising light guides; wherein light guides of the guide array receive excitation light and emissions signal light from the detector surface, wherein the light guides extend toward respective light sensors of the sensor array and comprise filter material that blocks the excitation light and permits the emissions signal light to propagate toward the respective light sensors, wherein the detector surface includes a reaction recess, the reaction recess comprising an index of refraction and a dimension sufficient to cancel background light energy incident on the detector surface in a detection band of the sensor array. The filter material comprises a metal complex dye comprising a photon emission quencher and a transition metal complex dye. or more features for reducing fluorescence range noise in a detection band of the sensor array. The device comprises: a structure defining a detector surface for supporting biological or chemical samples; a sensor array comprising light sensors, and circuitry to transmit data signals based on photons detected by the light sensors; and a guide array comprising light guides; wherein light guides of the guide array receive excitation light and emissions signal light from the detector surface, wherein the light guides extend toward respective light sensors of the sensor array and comprise filter material that blocks the excitation light and permits the emissions signal light to propagate toward the respective light sensors, wherein the detector surface includes a reaction recess, the reaction recess comprising an index of refraction and a dimension sufficient to cancel background light energy incident on the detector surface in a detection band of the sensor array. The filter material comprises a metal complex dye comprising a photon emission quencher and a transition metal complex dye.
Description
(12) Granted patent specificaon (19) NZ (11) 759983 (13) B2
(47) Publicaon date: 2021.12.24
(54) DETECTOR WITH REDUCED FLUORESCENCE RANGE NOISE
(51) Internaonal Patent Classificaon(s):
G01N 21/64
(22) Filing date: (73) Owner(s):
2018.11.30 Illumina, Inc.
(23) Complete specificaon filing date: (74) Contact:
2018.11.30 Wrays Pty Ltd
(30) Internaonal Priority Data: (72) Inventor(s):
US 62/611,464 2017.12.28 KHURANA, Tarun
US 62/644,804 2018.03.19 PINTO, Joseph
FUNG, Tracy H.
(86) Internaonal Applicaon No.: SABOUNCHI, Poorya
HIRSCHBEIN, Bernard
SMITH, Randall
(87) Internaonal Publicaon number: FENG, Wenyi
WO/2019/133182
(57) Abstract:
There is set forth herein a device comprising structure defining a detector surface configured
for supporng biological or chemical substances, and a sensor array comprising light sensors
and circuitry to transmit data signals using photons detected by the light sensors. The device
can include one or more features for reducing fluorescence range noise in a detecon band of
the sensor array. The device comprises: a structure defining a detector surface for supporng
biological or chemical samples; a sensor array comprising light sensors, and circuitry to transmit
data signals based on photons detected by the light sensors; and a guide array comprising light
guides; wherein light guides of the guide array receive excitaon light and emissions signal light
from the detector surface, wherein the light guides extend toward respecve light sensors of the
sensor array and comprise filter material that blocks the excitaon light and permits the emissions
signal light to propagate toward the respecve light sensors, wherein the detector surface includes
a reacon recess, the reacon recess comprising an index of refracon and a dimension sufficient
to cancel background light energy incident on the detector surface in a detecon band of the
NZ 759983 B2
sensor array. The filter material comprises a metal complex dye comprising a photon emission
quencher and a transion metal complex dye.
DETECTOR WITH REDUCED FLUORESCENCE RANGE NOISE
CROSS-REFERENCE TO RELATED APPLICATION
This application claims priority to U.S. Patent Application No. 62/611,464, filed
28 December 2017, entitled, “Detector With Reduced Fluorescence Range Noise”, which is
incorporated herein by reference in its entirety. This application also claims priority to U.S.
Patent Application No. 62/644,804, filed 19 March 2018, entitled, “Detector With Reduced
Fluorescence Range Noise”, which is incorporated herein by reference in its entirety.
BACKGROUND
Various protocols in biological or chemical research involve performing controlled
reactions. The designated reactions can then be observed or detected and subsequent analysis can
help identify or reveal properties of chemicals involved in the reaction.
In some multiplex assays, an unknown analyte having an identifiable label (e.g.
fluorescent label) can be exposed to thousands of known probes under controlled conditions.
Each known probe can be deposited into a corresponding well of a microplate. Observing any
chemical reactions that occur between the known probes and the unknown analyte within the
wells can help identify or reveal properties of the analyte. Other examples of such protocols
include known DNA sequencing processes, such as sequencing-by-synthesis (SBS) or cyclic-
array sequencing.
In some fluorescent-detection protocols, an optical system is used to direct excitation
light onto fluorophores, e.g. fluorescently-labeled analytes and to also detect the fluorescent
emissions signal light that can emit from the analytes having attached fluorophores. However,
such optical systems can be relatively expensive and require a larger benchtop footprint. For
example, the optical system can include an arrangement of lenses, filters, and light sources.
In other proposed detection systems, the controlled reactions in a flow cell define by
a solid-state light sensor array (e.g. a complementary metal oxide semiconductor (CMOS)
detector or a charge coupled device (CCD) detector). These systems do not involve a large
optical assembly to detect the fluorescent emissions.
BRIEF DESCRIPTION
There is set forth herein a device comprising: structure defining a detector surface
configured for supporting biological or chemical substances, and a sensor array comprising light
sensors and circuitry to transmit data signals using photons detected by the light sensors. The
device can include one or more feature for reducing fluorescence range noise in a detection band
of the sensor array.
According to a first principal aspect, there is provided a device for detecting with
reduced fluorescence range noise comprising:
a structure defining a detector surface configured for supporting biological or
chemical samples;
a sensor array comprising light sensors and circuitry to transmit signals using
photons detected by the light sensors; and
a guide array comprising light guides;
wherein light guides of the guide array receive excitation light and emissions signal
light from the detector surface, wherein the light guides extend toward respective light sensors of
the sensor array and comprise filter material that blocks the excitation light and permits the
emissions signal light to propagate toward the respective light sensors, and wherein the filter
material comprises a metal complex dye comprising a photon emission quencher and a transition
metal complex dye.
Optionally, the filter material comprises metal complex dye suspended in a polymer
binder matrix.
Optionally, the filter material comprises a homogeneous matrix of metal complex
dye and a polymer binder and the homogeneous matrix comprises a weight concentration ratio of
metal complex dye to polymer binder in the range of from about 70:30 to about 90:10.
Optionally, the detector surface includes a reaction recess for supporting a sample,
the reaction recess comprises an index of refraction and dimension to cancel background
radiation in a detection band of the sensor array.
Optionally, the metal complex dye comprises a transition metal complex dye.
Optionally, the metal complex dye comprises a transition metal and a dye and the
transition metal has an absorption spectral profile overlapping a fluorescence emissions spectral
profile of the dye.
Optionally, the metal complex dye reduces an auto-fluorescence of the filter material.
Optionally, the filter material comprises a counter ion associated to the metal
complex dye.
Optionally, the counter ion comprises an alkyl amine.
Optionally, the alkyl amine comprises at least one hydrocarbon group of at least four
carbon atoms.
According to a second principal aspect, there is provided a method for manufacturing
a detecting device with reduced fluorescence range noise comprising:
providing a light sensor array comprising light sensors;
fabricating circuitry to transmit data signals using photons detected by the light
sensor array, wherein the method further comprises;
after forming cavities for a guide cavity array depositing filter material defining light
guides within the guide cavities of the guide cavity array that are aligned with and disposed
above respective light sensors of the light sensor array, wherein the filter material
comprises a transition metal complex dye suspended in a polymer matrix, the transition
metal complex dye comprising a photon emission quencher; and
fabricating a structure defining a detector surface for supporting biological or
chemical samples, wherein the fabricating the structure defining the detector surface
includes fabricating the structure defining the detector surface above cavities of the guide
cavity array and the light sensors of the light sensor array.
Optionally, the depositing filter material comprises using chemical vapour
deposition, and subsequent to the depositing, the deposited filter material is subject to processing
using one or more of etching and planarizing.
Optionally, the fabricating circuitry includes using complementary metal oxide
semiconductor CMOS fabrication technology.
Optionally, the filter material comprises a homogeneous matrix of metal complex
dye and polymer binder.
Optionally, the filter material comprises a matrix of metal complex dye and polymer
binder and a weight concentration of metal complex dye to polymer binder is in the range of
from about 70:30 to about 90:10.
Optionally, the fabricating a structure defining a sample supporting surface
comprises forming a reaction recess defined in the sample supporting surface, wherein the
forming includes configuring the reaction recess so that based on an index of refraction of the
detector surface and a dimensional characteristic of the reaction recess, an induced
electromagnetic field radiating from the detector surface cancels background light energy
incident on the detector surface in a detection wavelength band of the light sensor array.
Optionally, the method includes subjecting one or more test sample detectors to
testing to determine information relating a dimension of a detector surface to an electromagnetic
field cancellation effect and the fabricating the structure defining a detector surface includes
dimensioning, using the determined information, a reaction recess of the detector surface to
cancel light energy incident on the detector surface in a detection band of the light sensor array.
Optionally, the filter material comprises a counter ion associated to a metal complex
dye comprising the dye.
Optionally, the counter ion comprises an alkyl amine.
Optionally, the alkyl amine comprises at least one hydrocarbon group of at least four
carbon atoms.
According to a third principal aspect, there is provided a device comprising:
a structure defining a detector surface for supporting biological or chemical samples;
a sensor array comprising light sensors, and circuitry to transmit data signals based
on photons detected by the light sensors; and
a guide array comprising light guides;
wherein light guides of the guide array receive excitation light and emissions signal
light from the detector surface, wherein the light guides extend toward respective light
sensors of the sensor array and comprise filter material that blocks the excitation light and
permits the emissions signal light to propagate toward the respective light sensors, wherein
the detector surface includes a reaction recess, the reaction recess comprising an index of
refraction and a dimension sufficient to cancel background light energy incident on the
detector surface in a detection band of the sensor array.
Optionally, the reaction recess comprises an index of refraction and a dimension
sufficient to transmit a center wavelength of the excitation light.
Optionally, the reaction recess comprises an index of refraction and a dimension
sufficient to establish a critical wavelength λc so that λc is within a range of wavelengths of
between about λa and about λb, wherein wavelengths shorter than λc are transmitted by the
reaction recess and wherein wavelengths longer than λc are cancelled by the reaction recess,
wherein λa is the center wavelength of excitation light and wherein λb is the shortest detection
band wavelength of the sensor array.
Optionally, the filter material comprises a metal complex dye.
Optionally, the filter material comprises a matrix of metal complex dye and a
polymer binder and a weight concentration of metal complex dye to polymer binder in the matrix
is in the range of from about 70:30 to about 90:10.
Optionally, the filter material comprises the metal complex dye that comprises a
transition metal complex dye.
DRAWINGS
These and other features, aspects, and advantages of the present subject matter will
become better understood when the following detailed description is read with reference to the
accompanying drawings in which like characters represent like parts throughout the drawings,
wherein:
Fig. 1 is a schematic cutaway side view of a system for use in biological or chemical
analysis having a detector that includes a detector surface for supporting a biological or chemical
sample according to one example;
Fig. 2 spectral profile coordination diagram illustrating coordination between
excitation wavelengths, absorption wavelengths, fluorescence emissions signal wavelengths, and
detection band wavelengths according to one example;
Fig. 3 is spectral profile diagram illustrating autofluorescence characteristics of filter
materials according to one example;
Fig. 4 is an energy state transition diagram illustrating energy state transitions of a
radiant dye according to one example;
Fig. 5 is an energy state transition diagram illustrating energy state transitions of a
dye having a photon emission quencher according to one example;
Fig. 6 is an energy state transition diagram illustrating energy state transitions of a
metal complex dye having a photon emission quencher according to one example;
Fig. 7 depicts optical density (OD) by film thickness diagram illustrating dependence
of OD on film thickness for a filter material having a metal complex dye according to one
example;
Fig. 8 is a cutaway side view of a detector having a detector surface configured to
cancel incident light energy in selective wavelength bands according to one example;
Fig. 9 is a cutaway side view of a detector having a sensor array, a light guide array
and a reaction array according to one example; and
Fig. 10 is a cutaway side view of a detector having a light sensor, a light guide, and
reaction recess defined by a detector surface according to one example.
DETAILED DESCRIPTION
In Fig. 1 there is shown a system 100 for use in analysis, such as biological or
chemical analysis. System 100 can include light energy exciter 10 and a detector assembly 20.
Detector assembly 20 can include detector 200 and a flow cell 282. Detector 200 can include a
plurality of light sensors 202 and detector surface 206 for supporting samples 502 such as
biological or chemical samples subject to test. Detector 200 can also include a plurality of light
guides that guide light from detector surface 206 to light sensors 202. Detector surface 206,
sidewalls 284, and flow cover 288 can define and delimit flow cell 282. Detector surface 206 can
have an associated detector surface plane 130.
In a further aspect, detector surface 206 can be recessed to include reaction recesses
210 (nanowells). According to one example, each light sensor 202 can be aligned to one light
guide 214 and one reaction recess 210. Each reaction recess 210 can define therein one or more
reaction sites and samples 502 can be supported on such reaction sites according to one example.
In another aspect, detector 200 can include dielectric stack areas 218, intermediate of
the light guides 214. Dielectric stack areas 218 can have formed therein circuitry, e.g. for read
out of signals from light sensors 202 digitisation storage and processing.
According to one example, detector 200 can be provided by a solid-state integrated
circuit detector, such as complementary metal oxide semiconductor (CMOS) integrated circuit
detector or a charge coupled device (CCD) integrated circuit detector.
According to one example, system 100 can be used for performance of biological or
chemical testing with use of fluorophores. For example, a fluid having one or more fluorophores
can be caused to flow into and out of flow cell 282 through inlet port using inlet port 289 and
outlet port 290. Fluorophores can attract to various samples 502 and thus, by their detection
fluorophores can act as markers for the samples 502 e.g. biological or chemical analytes to which
they attract.
To detect the presence of a fluorophore within flow cell 282, light energy exciter 10
can be energised so that excitation light 101 in an excitation wavelength range is emitted by light
energy exciter 10. On receipt of excitation light 101 fluorophores attached to samples 502 radiate
emissions signal light 501, which is the signal of interest for detection by light sensors 202.
Emissions signal light 501 owing to fluorescence of a fluorophore attached to a sample 502 will
have a wavelength range red shifted relative to a wavelength range of excitation light 101.
Light energy exciter 10 can include at least one light source and at least one optical
components to illuminate samples 502. Examples of light sources can include e.g. lasers, arc
lamps, LEDs, or laser diodes. The optical components can be, for example, reflectors, dichroics,
beam splitters, collimators, lenses, filters, wedges, prisms, mirrors, detectors, and the like. In
examples that use an illumination system, the light energy exciter 10 can be configured to direct
excitation light 101 to reaction sites. As one example, fluorophores can be excited by light in the
green wavelength range, e.g. can be excited using excitation light 101 having a center (peak)
wavelength of about 523 nm.
Examples herein recognise that a signal to noise ratio of system 100 can be expressed
as set forth in the equation of (1) hereinbelow.
where “Signal” is the emissions signal light 501, i.e. the signal of interest light attributable to the
fluorescence of a fluorophore attached to a sample, “Excitation” is unwanted excitation light
reaching the light sensors 202, “AF” is the autofluorescence noise radiation of one or more
autofluorescence sources within detector 200, “Background” is unwanted light energy
transmitted into detector 200 from a source external to detector 200, “Dark Current” is current
flow is noise associated to random electron-hole pair generation in the absence of light and
“Read Noise” is noise associated to analogue-to-digital electronics.
Fig. 2 is a spectral profile coordination diagram illustrating targeted coordination
between a wavelength range of excitation light, a wavelength range of signal light and a
detection wavelength range. In the spectral profile coordination diagram of Fig. 2 spectral profile
1202 is the spectral profile of excitation light 101 as emitted by light energy exciter 10. Spectral
profile 1204 is the spectrum of absorption of a fluorophore being detected with use of excitation
light 101 having a spectral profile 1202 and spectral profile 1214 is the spectral profile of the
emissions signal light 501 caused by the fluorescence of a fluorophore on being excited by
excitation light 101. Spectral profile 1220 is the transmission profile (detection band) of detector
200 and light sensors 202 according to one example. Detector 200 can be configured to detect
light in the wavelength range indicated by spectral profile 1220. Thus, referring to the spectral
profile coordination diagram of Fig. 2, detector 200 is able to detect emissions signal light 501 in
the range of wavelengths wherein the spectral profile 1214 of the emissions signal light 501 and
the detection band spectral profile 1220 of detector 200 and light sensors 202 intersect.
Detector 200 can include one or more filters that block excitation light 101 so that
detector 200 having light sensors 202 does not detect excitation light 101. In one aspect, light
guides 214 that guide light from detector surface 206 can comprise filter material so that light
guides 214 block light in the wavelength range of excitation light 101. Light sensors 202
accordingly can receive emissions signal light 501 radiating from an excited fluorophore but not
excitation light 101.
Examples herein recognise that light guides 214 designed to improve a signal to
noise ratio of detector 200 can act as a source of noise within detector 200. Referring to the
spectral profile diagram of Fig. 3 spectral profile 1304 is a spectral profile of a filter material
having a dye that is without (absent) a photon emission quencher commonly used in optical
systems under test by excitation illumination in an expected wavelength range of excitation light
101 of system 100. In the specific spectral profile diagram of Fig. 3, spectral profile 1304
illustrates a spectral profile of a filter material under illumination by green excitation light, e.g.
according to the excitation light spectral profile 1202 depicted in the spectral profile coordination
diagram of Fig. 2, having a center (peak) wavelength of about 523 nm.
Referring to the spectral profile diagram of Fig. 3 it is seen that the filter material
having spectral profile characteristics depicted by spectral profile 1304 red shifts with respect to
the emission band of excitation light 101 depicted by spectral profile 1202 of the spectral profile
coordination diagram of Fig. 2, meaning that the material exhibits autofluorescence. Examples
herein recognise that with filter material of light guides 214 autofluorescing, signal detected by
light sensors 200 as an emissions signal can actually be noise radiation attributable to excitation
light 101 operating to excite autofluorescence of light guides 214.
Examples to address unwanted autofluorescence of light guides 214 are described
with reference to Figs. 3-7. Referring to the energy state transition diagrams of Figs. 4-6, light
guides 214 according to one example can comprise material having a photon emission quencher.
In another aspect, a filter material can include dye molecules to provide absorption in a
wavelength band of excitation light 101.
The energy state transition diagram of Fig. 4 depicts energy state transition of a dye
without a photon emission quencher. On excitation and after an excitation state relaxation period
the dye having the energy state transition characteristics as depicted in the energy state transition
diagram of Fig. 4 emits photons on return to a ground state. Fig. 5 is an energy state transition
diagram depicting energy state transitions of a dye having a photon emission quencher. Referring
to the energy state transition diagram of Fig. 5, the dye having a photon emission quencher on
excitation returns to a ground state after an excitation state relaxation period. However, by
operation of the photon emission quencher, photons are not released on return to the ground
state. Rather phonons are emitted on return to the ground state. The return to ground state is
accompanied by the release of thermal energy rather than photons.
Dyes having the energy state transition characteristics as shown in the energy state
transition diagram of Fig. 4 are radiant dyes and dyes having energy state transition
characteristics as shown in the energy state transition diagram of Fig. 5 are non-radiant dyes.
A chemical structure diagram of a dye, according to one example, having a suitable
photon emission quencher that quenches photon emissions is shown in (2).
Cr +
The chemical structural diagram of (2) illustrates structural characteristics of a metal
complex dye that functions as a photon emission quencher to quench photon emissions.
According to one example, a metal complex dye can be provided by an octahedral transition
metal complex dye as shown in (2). The specific metal complex dye shown in (2) includes two
dye molecules + chromium ion, and some complexes can include one dye molecule + one
chromium (Cr) ion or other metal ion. The structure depicted in (2) includes six ligand bonds: O,
N and a standard crystal field. According to the structure depicted in (2), there is a photon
emission quencher provided by a trivalent Cr transition metal ion. According to one example Cr3
+ can provide photon emission quenching functionality. Other transition metals can be used.
Transition metals for use in a metal complex dye herein can include e.g. Scandium, Titanium,
Vanadium, Chromium, Manganese, Iron, Cobalt, Nickel, Copper. For selection of alternative
metals, energy levels can be overlapping between the metal ion and a dye molecule. According
to one example, a transition metal for use in a metal complex dye can be selected to have an
absorption spectral profile overlapping a fluorescence emissions profile of the selected dye so
that the transition metal can provide photon emission quenching functionality through the
fluorescence emission spectral profile of the selected dye.
In the example of the metal complex dye depicted in the structural diagram of (2),
the metal complex dye has an associated proton depicted. The counter ion associated to the metal
complex dye is formed by absorbing the positive (+) charge specified by the proton of the metal
complex dye depicted in the structural diagram of (2) and can be selected according to one
example for hydrophobicity performance and UV absorption performance. In one example, an
alkyl amine, a primary amine, a secondary amine, or a tertiary amine may associate with the
metal complex dye forming a counter ion, which can include an alkylammonium when
associated with the metal complex dye.
The metal complex dye according to one example may not be particularly soluble in
a solution on its own, and so the counter ion can be chosen to increase solubility. The counter ion
can be selected for hydrophobicity performance in order to promote transparency and visibility
of the polymer and/or solvent, and for reducing scattering. For instance, the counter ion can
allow for the metal complex dye to be more evenly distributed, enhancing the visibility and
transparency, and reducing scattering. The counter ion can be selected for UV absorption
performance e.g. so that the counter ion does not undesirably contribute to fluorescence. For
instance, absorption of the counter ion can affect the fluorescence characteristics by interfering
with the spectrum of the metal dye complex, and can be chosen so as not to have an interfering
spectrum. According to one example, a hydrophobic amine can be used as a counter ion.
According to another example, it will be understood that depending on the metal center and the
ligands chosen, a metal complex dye may have no charge, a net positive charge, or may have a
net negative charge as well.
According to one example a counter ion associated to the metal complex dye
depicted in the structural diagram of (2) can be provided by an alkyl amine. According to one
example a counter ion associated to the metal complex dye depicted in the structural diagram of
(2) can be provided by a tertiary amine. In a tertiary amine, a nitrogen has three organic
substituents. According to one example, a counter ion associated to the metal complex dye
depicted in the structural diagram of (2) can be provided by a tertiary alkyl amine.
Additionally, in other examples of a metal complex dye, a counter ion of appropriate
charge can be selected to be associated to the metal complex dye. In some embodiments, a
negatively or positively charged ion can be selected to counteract the net charge of the metal
complex dye molecule, and/or adding to the hydrophobicity in some embodiments to allow for
the metal complex dye to be incorporated into a solution. Additionally, when there is no charge,
no counter ion may be necessary in some embodiments. The counter ion may include any
charged particles, and in some embodiments includes primary, secondary, or tertiary amines. In
further embodiments, a quaternary ammonium ion can be selected.
According to one example, the counter ion associated to the metal complex dye as
depicted in (2) can include an amine, for instance an NR’R’’R’’’, where at least one of the R
groups is a chain, straight or branched, with at least four atoms. In some embodiments, there can
be at least 10 atoms in the chain. The chain can include a long chain, and can include a polymer.
The chain may be a mostly hydrocarbon group, or could include other moieties, such that the dye
can possibly be soluble in any solvent necessary, and the polymer can be soluble in a solvent
depending on the functional groups of the polymer. The other R groups can be the same or
hydrogen, or can comprise a different chain. The chain can be according to one example a C4 to
C20, including cyclic, chains or rings. In some embodiments, the counter ion can include more
than one type of counter ion. Examples herein recognise that some mixtures of counter ions are
convenient for use in solutions where more than one polymer material can be used. That is, some
alkyl groups can be different, and the counter ion can include a plurality of counter ions.
Fig. 6 is an energy state transition diagram illustrating properties of metal complex
dyes. Fig. 6 is an energy state transition diagram for Cr (CN Ar NC) . Referring to the energy
state transition diagram of Fig. 6, metal complexes can lead to ultrafast non-radiative (non-
autofluorescence) relaxation due to metal centered states being below the metalligand charge-
transfer (MLCT) complex. For Cr (CN Ar NC) ) depicted in the energy state transition
3d-d
diagram in Fig. 6, the ligand field can be sufficiently weak that metal centered excited states
can be energetically below the MLCT complex leading to ultrafast excited state. Metal complex
dyes can exhibit ultrafast excited state depopulation via non-radiative relaxation. According to
the energy state transition diagram of Fig. 6 a metal complex functioning as a photon emission
quencher quenches photons so that a return to ground state is accompanied by phonon emission
and release of thermal energy rather than photon emission.
To provide filter material, dye molecules in powder form, e.g. having photon
emission quencher, and according to one example provided by a metal complex dye, can be
dissolved with a solvent and added to a liquid polymer binder to form a liquid matrix having dye
molecules and polymer molecules. The liquid can be deposited into a dielectric stack cavity of
detector 200 and evapourated to form a filter material comprising a solid dye and polymer matrix
wherein dye molecules are suspended within a matrix of polymer binder molecules.
A filter material for forming light guide 214 according to one example can include
metal complex dye molecules suspended in a polymer binder matrix as set forth herein. A
formed filter material including metal complex dye molecules suspended in a polymer binder
matrix can exhibit spectral profile characteristics under illumination with excitation light 101
having a center wavelength of about 523 nm as set forth with reference to spectral profile 1404
as shown in the spectral profile diagram of Fig. 3. According to one example as set forth in
reference to Fig. 3 providing filter material to include a dye having a photon emission quencher
(as provided with use e.g. of a metal complex dye) can reduce autofluorescence emissions
signals radiating from filter material at wavelengths of about 570 nm or longer to values that are
about 5 percent (observing the respective autofluorescence emissions signal values of spectral
profile 1304 and spectral profile 1404 at a wavelength of about 570 nm) or less of their expected
values in the case filter material is provided that includes a dye without a photon emission
quencher.
Providing a matrix of dye molecules with a polymer binder molecule facilitates
processability with a range of semiconductor processes e.g. chemical vapour deposition (CVD),
spin coating, etching, planarizing, and the like.
According to one example filter material provided by a metal complex dye matrix
can have a weight ratio of between about 70:30 dye to polymer and about 90:10 dye to polymer.
At concentrations above this range, the structural integrity of the matrix can become
compromised and at concentrations below, filtering performance can become compromised.
According to one example filter material provided by a metal complex dye matrix can have a
molecule ratio of between about 1 dye molecule: 50 polymer molecules to about 1 dye
molecule:150 polymer molecules. According to one example filter material provided by a
polymer binder and metal complex dye matrix can have a molecule ratio of between about 1 dye
molecule: 100 polymer molecules.
While higher concentrations of dye molecules improve blockage of excitation light,
examples herein recognise that increased scattering can be observed at higher concentrations.
Light scattering can be addressed with further processes for filtering powder dye particles prior
to mixing with a polymer binder liquid.
Fig. 7 is an optical density (OD) film thickness diagram illustrating filtering
performance of a filter material herein comprising a matrix of metal complex dye suspended in a
polymer binder matrix. As seen in the OD film thickness diagram of Fig. 7, an OD of about 10
can be achieved within a spatial budget of 3.5μm. Referring again to the spectral profile
coordination diagram of Fig. 2, the spectral profile targeted for filtering is spectral profile 1202
for excitation light 101 having a center (peak) wavelength of about 523nm. Referring to the OD
film thickness diagram of Fig. 7, by configuring light guide 214 formed of a matrix of metal
complex dye suspended in a polymer binder matrix to have a thickness of about 3.5μm light
guide 214 can be configured to exhibit an OD of about 10 for the center (peak) excitation light
wavelength of about 523nm. By configuring light guide 214 formed of a matrix of metal
complex dye suspended in a polymer binder matrix to have a thickness of about 2μm light guide
214 can be configured to exhibit an OD of about 7 for the center (peak) excitation wavelength of
about 523nm.
For performance of light sensing, light sensor 202 can have a particular spacing
distance in reference to detector surface 206 (Fig. 1). According to one example, the particular
spacing distance can be a particular spacing distance in the range, e.g. of from about 4μm to
about 6μm. As seen in Fig. 1, light guides 214 can have space restrictions in dependence on the
spacing requirements between light sensors 202 and detector surface 206. In view of the OD
thickness data summarised in the OD film thickness diagram Fig. 7 material for construction of
light guides 214 can be provided to satisfy targeted optical density (OD) properties in
dependence on spatial properties of detector 200, and OD performance suitable for many
applications is achievable even where spatial budget is restricted.
As seen by the coordination depicted by the spectral profile coordination diagram of
Fig. 2, light sensors 202 can sense emissions signal light 501 attributable to fluorescence of a
fluorophore but, in accordance with ideal operation, cannot detect excitation light 101
represented by spectral profile 1202. For configuring of light sensors 202 to detect emissions
signal light 501 attributable to a fluorophore attached to a sample 502 without detecting
excitation light 101, system 100 can include one or more filters. For example, light guides 214
can be formed of filtering material that blocks light in the energy band of excitation light 101
represented by spectral profile 1202. Thus, emissions signal light 501 represented by spectral
profile 1214 is subject to detection with use of light sensors 202 without detection of excitation
light 101. However, as noted, filter material forming light guide 214 can autofluoresce in
response to excitation by excitation light 101. Examples herein provide light guides 214 to block
excitation light 101 to exhibit reduced autofluorescence so as to preserve desired spectral profile
coordination between excitation fluorescence emission and detection spectral profiles as depicted
in the spectral profile coordination diagram of Fig. 2.
Examples herein recognise that left shifting of spectral profile 1220 of detector 200
can increase detection of emissions signal light 501 having a spectral profile indicated by
spectral profile 1214 in the spectral profile of the emissions signal light 501. It should be
understood that as used herein, left shifting refers to hypsochromic shifting, or blue shifting.
Filter material herein comprising a matrix of metal complex dye suspended in a polymer binder
matrix can be configured for left shifting of spectral profile 1220 by implementation of various
features. In order to left shift spectral profile 1220 certain substituents of the ligands surrounding
metal complex dye (2) can be altered. For instance, the phenyl groups and other moieties can act
as fluorophores, and can so be altered to left shift the spectrum. For instance, methyl groups can
be replaced with trifluoromethyl or other groups, and hydrogens be replaced with chlorine or
bromine, in some embodiments. The spectrum can be shifted left or right, depending on the
particular metal complex dye used, by replacing electron donating groups with electrons
withdrawing groups and vice versa. As used herein, right shifting refers to bathochromic
shifting, or red shifting, of the spectral wavelength. Thus, in any embodiment, the spectrum can
be adjusted with adjustments to the functional groups of the metal complex dye.
According to one example, a filter material can include a dye having a photon
emission quencher and the dye can be a non-radiant dye. According to one example, the photon
emission quencher can include chromium (Cr). According to one example, the dye can be a
metal complex dye having a photon emission quencher provided by a trivalent Cr transition
metal ion. According to one example the filter material can be provided by matrix having a dye
and polymer binder, wherein the dye has a photon emission quencher. According to one example
the filter material can be provided by matrix having a dye and polymer binder, wherein the dye is
a metal complex dye. According to one example the filter material can be provided by a dye
suspended in a polymer matrix, wherein the dye has a photon emission quencher. According to
one example the filter material can be provided by a dye suspended in a polymer matrix, wherein
the dye is a metal complex dye.
Examples herein recognise that performance of system 100 can be negatively
impacted by background noise, which herein refers to unwanted light energy radiating from a
source external to detector 200. Examples herein recognise that a signal to noise ratio of detector
200 can be negatively impacted by fluorescence range background light radiating for sources
external to detector 200. Fluorescence range noise emissions in system 100 can be attributable to
sources other than auto-fluorescing sources within detector 200.
Examples herein recognise for example that while light energy exciter 10 can be
configured to ideally emit light in a relatively shorter wavelength band, e.g. in a green
wavelength band, autofluorescent sources therein, e.g. optical components can autofluoresce and
light that is emitted by light energy exciter 10 can include unwanted light rays at longer
wavelengths in the fluorescence band of detector 200 and light sensors 202. Examples herein
recognise that fluorescence range light can enter system 100 from sources other than light energy
exciter 10.
In reference to Fig. 8 there are set forth additional features for increasing a signal to
noise ratio of detector 200. In reference to Fig. 8 there are described features for cancellation
(e.g. partial or entire cancellation) of fluorescence range background noise radiation that without
the described features would be received into detector 200. Cancellation features herein can
reduce fluorescence range wavelengths sensed by light sensors 202 not attributable to emissions
signal light 501.
The filter material features set forth in reference to Figs. 3-7 reduce fluorescence
range noise by reduction of internal autofluorescence within detector 200. Features of detector
surface 206 as set forth in connection with Fig. 8 reduce undesirable fluorescence range
background noise by cancellation (e.g. partial or entire) fluorescence range light energy incident
on detector surface 206. The features described with reference to Fig. 3-7 can be implemented
independently of the features of Fig. 8 or according to one example in combination with the
features of Fig. 8 to address the problem of fluorescence range noise with use of a combination
of detector internal (Figs. 3-7) and detector surface (Fig. 8) features.
Now referring to Fig. 8 detector 200 according to one example can be configured so
that light energy incident on detector surface 206 can induce electromagnetic fields radiating
from detector surface 206 that cancel (e.g. partially or entirely) incoming light energy which
would otherwise be transmitted through reaction recess 210. Examples herein recognise that
behaviour of induced fields radiating from detector surface 206 induced from light rays incident
on detector surface 206 can become more controllable and predictable as an index of refraction
ratio between a detector surface 206 and fluid within flow cell 282 increases. An index of
refraction of detector surface 206 can be defined by the index of refraction of the material of
passivation layer 258 adjacent flow cell 282 forming the detector surface 206. Examples herein
recognise that with a sufficiently high index of refraction ratio between detector surface 206 and
a fluid of flow cell 282 light rays of excitation light 101 can induce electromagnetic fields
radiating from detector surface 206 that cancel incoming light energy in dependence on a
dimension of detector surface 206.
Referring to Fig. 8, reaction recess 210 can include a dimension “D” provided by the
diameter of the reaction recess 210 at a top elevation of reaction recess 210. Examples herein
recognise that electromagnetic fields induced by incident light energy incident on reaction recess
210 can cancel incoming light energy in dependence on the dimension “D”, where an index of
refraction ratio between detector surface 206 and fluid within flow cell 282 is sufficiently high.
Detector 200 as shown in Fig. 8 can be an integrated circuit detector having structure 260
defining detector surface 206 which can include passivation layer 256 and passivation layer 258.
According to one example where passivation layer 258 having detector surface 206 is formed of
tantalum pentoxide (Ta2O5) having an index of refraction λ206 of about λ206 2.13 and where
fluid of flow cell 282 is water based and has an index of refraction λ282 of about λ282 1.33 the
index of refraction ratio λ206/ λ282 between a material forming detector surface 206 and a fluid
of flow cell 282 is about λ206/ λ282 1.60. According to one example where passivation layer
258 having detector surface 206 is formed of silicon nitride (SiN) having an index of refraction
λ206 of about λ206 2.02 and where fluid of flow cell 282 is water based and has an index of
refraction λ282 of about λ282 1.33 the index of refraction ratio λ206/ λ282 between a material
forming detector surface 206 and a fluid of flow cell 282 is about λ206/ λ282 1.52. A three-
dimensional shape of reaction recess 210 can be cylindrical or frustro-conical in some examples
such that a cross-section taken along a horizontal plane that extends into the page of Fig. 8 is
substantially circular. A longitudinal axis 268 can extend through a geometric center of the
cross-section.
Examples herein recognise that for a detector surface 206 as set forth in Fig. 8 having
a reaction recess 210 (nanowell) with the dimension D and with an index of refraction ratio
λ206/ λ282 suitably high there is a critical wavelength λc wherein wavelengths shorter than the
critical wavelength λc are transmitted into an interior of reaction recess 210 and detector 200 and
wherein wavelengths longer than the critical wavelength λc are cancelled (e.g. partially cancelled
or entirely cancelled) by detector surface 206 having reaction recess 210. Examples herein
further recognise that the described critical wavelength λc is in dependence of the dimension D
so that the dimension D can be controlled to tune the critical dimension λc to a desired value.
More specifically the critical wavelength λc can be increased by increasing the dimension D and
the critical wavelength λc can be decreased by decreasing the dimension D. Without being bound
to a particular theory in regard to the recognised effect, light rays incident on detector surface
206 may induce electromagnetic fields radiating from detector surface 206 that cancel (e.g.
partially or entirely) incoming light energy which would otherwise be transmitted through
reaction recess 210.
Light energy cancellation features can be advantageously incorporated into the
design of detector surface 206. According to one example described with reference to Fig. 8 the
dimension D can be selected to establish the critical wavelength λc so that wavelengths at about
the center (peak) wavelength λa of excitation light 101 and shorter are transmitted through
reaction recess 210 and into detector 200 and further so that wavelengths of about the shortest
detection band wavelength λb and longer are cancelled by detector surface 206. Transmission of
wavelengths at about the center (peak) wavelength λa of excitation light 101 and shorter can
assure that fluorophores are properly excited according to the design of system 100 and
cancellation of wavelengths of about the shortest detection band wavelength λb and longer can
increase a signal to noise ratio of detector 200.
While λc can be tuned in dependence on D, the precise relationship between D and
cancellation effects in dependence thereon can vary depending on materials, configuration
(including light energy exciter 10 configuration), and process control parameters of a particularly
fabricated system 100. Notwithstanding, information of the relationship between the dimension
D and a cancellation effect in dependence thereon for a particular design of detector 200 can be
determined by experimentation. On determination of information by experimentation that
specifies a relationship between D and a cancellation effect for a particular design of detector
200, the information can be used to establish a value for D; that is, D=d1 where D=d1 is selected
to establish the critical wavelength λc so that wavelengths at about a center (peak) wavelength λc
of excitation light 101 and shorter are transmitted into reaction recess 210 and detector 200 and
further so that wavelengths of about the shortest detection band wavelength λb and longer (i.e. in
the fluorescence range) are cancelled by detector surface 206.
According to one process, one or more test sample detectors according to detector
200 can be fabricated and subject to test. The test can include testing for transmission of
excitation light 101 by reaction recess 210. One or more test samples can be provided and
subject to testing to determine the smallest dimension of D, D=dc at which reaction recess 210
transmits excitation light 101 in accordance with one or more transmission criterion. The one or
more transmission criterion can be e.g. that a threshold amount (e.g. 90 percent, 100 percent) of
maximum energy excitation light 100 is transmitted through reaction recess 210. One or more
test samples can be provided and subject to testing to determine the largest dimension of D,
D=de at which reaction recess 210 cancels fluorescence range light (e.g. a discernible amount of
fluorescence range light) in a detection band of light sensors 102. For such testing signals read
out by light sensors 202 can be examined with light guides 214 fabricated according to their
production specifications. With one or more of dimensions D=dc or D=de determined, detector
200 according to a production design can be provided. In the production design according to one
example, D=d1 can be provided to be in the range of from about D=dc to about D=de. In the
production design according to one example, D=d1 can be provided to be at about the midpoint
distance of between D=dc and D=De. In the production design according to one example, D=d1
can be provided to be about D=dc. In the production design according to one example, D=d1 can
be provided to be about D=de. In the described examples, the dimension D can be provided to
establish a critical wavelength λc so that λc is within a range of wavelengths of between about λa
and about λb, wherein wavelengths shorter than λc are transmitted by reaction recess 210 and
wherein wavelengths longer than λc are cancelled by reaction recess 210, wherein λa is the
center wavelength of excitation light 101 and wherein λb is the shortest detection band
wavelength of the sensor array 201.
Referring to the spectral profile coordination diagram of Fig. 2, excitation light 101
can have a center (peak) wavelength of about 523 nm (λa), and detector 200 with light sensors
202 can have a detection band commencing at about 580 nm (shortest detection band wavelength
λb). Thus, reaction recess 210 according to one example, configured to have a suitable index of
refraction, can be dimensioned to permit entry of incident light energy at wavelengths of about
523 nm and shorter and can be dimensioned to cancel incident light energy at wavelengths of
about 580 nm and longer. In the case where detector 200 is of a configuration wherein D=d1
λc so that the distance d1 is in common with the critical wavelength λc, D can be dimensioned
according to D=550 nm to transmit excitation light 101 into reaction recess 210 and to cancel
unwanted fluorescence range wavelengths according to the spectral profile coordination diagram
of Fig. 2. With the described configuration, the detector surface 206 can be dimensioned to
permit entry of incident light energy at wavelengths of about 523 nm and shorter and can be
dimensioned to cancel incident light energy at wavelengths of about 580 nm and longer.
There is set forth herein a method including subjecting a test sample detector
according to detector 200 (having a structure 260 defining detector surface 206) to determine
information that specifies a relationship between a dimension e.g. D of detector surface 206 and
an electromagnetic field cancellation effect (e.g. including information such dc, de and/or other
information relating D to λc ) and wherein the fabricating the structure 260 defining a detector
surface 206 includes dimensioning, using the determined information, a reaction recess 210 of
the detector surface 206 to transmit excitation light 101 in an excitation wavelength band of
excitation light 101 (including at the center (peak) wavelength λa) and to cancel light energy
incident on the detector surface 206 in a detection band of the light sensor array 201.
A three-dimensional shape of reaction recess 210 can be cylindrical or frustro-
conical in some examples such that a cross-section taken along a horizontal plane that extends
into the page of Fig. 8 is circular. A longitudinal axis 268 can extend through a geometric center
of the cross-section. However, other geometries can be used in alternative examples. For
example, the cross-section can be square-shaped or octagonal. According to one example, shield
structure 250 can have a thickness of from about 100 nm to about 600 nm, passivation layer 256
can have a thickness of from about 100 nm to about 600 nm, passivation layer 256 can have a
thickness of from about 50 nm to about 500 nm, aperture 252 can have a diameter of from about
700 nm to about 1.5 um, and reaction recess 210 if present can have a height H of from about 50
nm to about 500 nm.
Figs. 9 and 10 illustrate further details of an example of detector 200 having one or
more fluorescence range noise reducing features as set forth herein.
Referring to Figs. 9-10 there is set forth herein a detector surface 206 for supporting
biological or chemical substances; a sensor array 201 comprising light sensors 202, and circuitry
246 to transmit data signals based on photons detected by the light sensors 202; a guide array
213 comprising light guides 214; wherein light guides 214 of the guide array 213 receive
excitation light 101 and emissions signal light 501 from the detector surface 206, wherein the
light guides 214 extend toward respective light sensors 202 of the sensor array 201 and comprise
filter material that blocks the excitation light 101 and permits emissions signal light 501
radiating from fluorescing fluorophores to propagate toward the respective light sensors 202,
wherein the detector surface includes a reaction recess 210, the reaction recess comprising an
index of refraction and a dimension to cancel background light energy incident on the detector
surface in a detection band of the sensor array 201.
Detector 200 can include a sensor array 201 of light sensors 202, a guide array 213 of
light guides 214, and a reaction array 209 of reaction recesses 210. In certain examples, the
components are arranged such that each light sensor 202 aligns with a single light guide 214 and
a single reaction recess 210. However, in other examples, a single light sensor 202 can receive
photons through more than one light guide 214. In some examples there can be provided more
than one light guide and/or reaction recess for each light sensor of a light sensor array. In some
examples there can be provided more than one light guide and/or light sensors aligned to a
reaction recess of a reaction recess array. The term “array” does not necessarily include each and
every item of a certain type that the detector can have. For example, the sensor array of light
source may not include each and every light sensor of detector 200. As another example, the
guide array 213 may not include each and every light guide of detector 200. As another example,
the reaction array 209 may not include each and every reaction recess 210 of detector 200. As
such, unless explicitly recited otherwise, the term “array” may or may not include all such items
of detector 200.
In the illustrated example, flow cell 282 is defined by sidewall 284 and a flow cover
288 that is supported by the sidewall 284 and other sidewalls (not shown). The sidewalls are
coupled to the detector surface 206 and extend between the flow cover 288 and the detector
surface 206. In some examples, the sidewalls are formed from a curable adhesive layer that
bonds the flow cover 288 to detector 200.
The flow cell 282 can include a height H1. By way of example only, the height H1
can be between about 50-400 μm or, more particularly, about 80-200 μm. The flow cover 288
can include a material that is light transmissive to excitation light 101 propagating from an
exterior of the detector assembly 20 into the flow cell 282.
Also shown, the flow cover 288 can define inlet and outlet ports 289, 290 that are
configured to fluidically engage other ports (not shown). For example, the other ports can be
from a cartridge (not shown) or a workstation (not shown).
Detector 200 has a detector surface 206 that can be functionalised (e.g. chemically or
physically modified in a suitable manner for conducting designated reactions). For example, the
detector surface 206 can be functionalised and can include a plurality of reaction sites having one
or more biomolecules immobilised thereto. The detector surface 206 can have a reaction array
209 of reaction recesses 210. Each of the reaction recesses 210 can include one or more of the
reaction sites. The reaction recesses 210 can be defined by, for example, an indent or change in
depth along the detector surface 206. In other examples, the detector surface 206 can be planar.
Fig. 10 is an enlarged cross-section of detector 200 showing various features in
greater detail. More specifically, Fig. 10 shows a single light sensor 202, a single light guide 214
for directing emissions signal light 501 toward the light sensor 202, and associated circuitry 246
for transmitting signals based on emissions signal light 501 (e.g. photons) detected by the light
sensor 202. It is understood that the other light sensors 202 of the sensor array 201 (Fig. 9) and
associated components can be configured in an identical or similar manner. It is also understood,
however, the detector 200 is not required to be manufactured identically or uniformly
throughout. Instead, one or more light sensors 202 and/or associated components can be
manufactured differently or have different relationships with respect to one another.
The circuitry 246 can include interconnected conductive elements (e.g. conductors,
traces, vias, interconnects, etc.) that are capable of conducting electrical current, such as the
transmission of data signals that are based on detected photons. Detector 200 comprises an
integrated circuit having a planar array of the light sensors 202. The circuitry 246 formed within
detector 200 can be configured for at least one of read out signals from light sensors 202 after an
exposure period (integration period) in which charge accumulates on light sensor 202, signal
amplification, digitisation, storage, and processing. The circuitry 246 can collect and analyse the
detected emissions signal light 501 and generate data signals for communicating detection data
to a bioassay system. The circuitry 246 can also perform additional analogue and/or digital signal
processing in detector 200. Light sensors 202 can be electrically coupled to circuitry 246 through
gates 241-243.
Detector 200 according to one example can be provided by a solid-state integrated
circuit detector such as a CMOS integrated circuit detector or a CCD integrated circuit detector.
Detector 200 according to one example can be an integrated circuit chip manufactured using
integrated circuit manufacturing processes such as complementary metal oxide semiconductor
(CMOS) fabrication processes.
The resolution of the sensor array 201 defined by light sensors 202 can be greater
than about 0.5 megapixels (Mpixels). In more specific examples, the resolution can be greater
than about 5 Mpixels and, more particularly, greater than about 14 Mpixels.
Detector 200 can include a plurality of stacked layers 231-237 including a sensor
layer 231, which can be a silicon layer. The stacked layers can include a plurality of dielectric
layers 232-237. In the illustrated example, each of the dielectric layers 232-237 includes metallic
elements (e.g. W (tungsten), Cu (copper), or Al (aluminum)) and dielectric material, e.g. SiO2.
Various metallic elements and dielectric material can be used, such as those suitable for
integrated circuit manufacturing. However, in other examples, one or more of the dielectric
layers 232-237 can include only dielectric material, such as one or more layers of SiO2.
With respect to the specific example of Fig. 10, the dielectric layers 232-237 can
include metallisation layers that are labeled as layers M1-M5 in Fig. 10. As shown, the
metallisation layers, M1-M5, can be configured to form at least a portion of the circuitry 246.
In some examples, detector 200 includes a shield structure 250 having one or more
layers that extend throughout an area above metallisation layer M5. In the illustrated example,
the shield structure 250 can include a material that is configured to block, reflect, and/or
significantly attenuate the light signals that are propagating from the flow cell 282. The light
signals can be the excitation light 101 and/or emissions signal light 501. By way of example
only, the shield structure 250 can comprise tungsten (W). By way of specific example only, the
excitation light 101 may have a center (peak) wavelength of about 523 nm and emissions signal
light 501 can include wavelengths of about 570 nm and longer (Fig. 2).
As shown in Fig. 10, shield structure 250 can include an aperture 252 therethrough.
The shield structure 250 can include an array of such apertures 252. Aperture 252 is dimensioned
to allow signal emission light to propagate to light guide 214. Detector 200 can also include a
passivation layer 256 that extends along the shield structure 250 and across the apertures 252.
Detector 200 can also include a passivation layer 258 comprising detector surface 206 that
extends along passivation layer 256 and across the apertures 252. Shield structure 250 can extend
over the apertures 252 thereby directly or indirectly covering the apertures 252. Passivation layer
256 and passivation layer 258 can be configured to protect lower elevation layers and the shield
structure 250 from the fluidic environment of the flow cell 282. According to one example,
passivation layer 256 is formed of SiN or similar. According to one example, passivation layer
258 is formed of tantalum pentoxide (Ta2O5) or similar. Structure 260 having passivation layer
256 and passivation layer 258 can define detector surface 206 having reaction recesses 210.
Structure 260 defining detector surface 206 can have any number of layers such as one to N
layer.
Structure 260 can define a solid surface (i.e. the detector surface 206) that permits
biomolecules or other analytes-of-interest to be immobilised thereon. For example, each of the
reaction sites of a reaction recess 210 can include a cluster of biomolecules that are immobilised
to the detector surface 206 of the passivation layer 258. Thus, the passivation layer 258 can be
formed from a material that permits the reaction sites of reaction recesses 210 to be immobilised
thereto. The passivation layer 258 can also comprise a material that is at least transparent to a
desired fluorescent light. Passivation layer 258 can be physically or chemically modified to
facilitate immobilising the biomolecules and/or to facilitate detection of the emissions signal
light 501.
In the illustrated example, a portion of the passivation layer 256 extends along the
shield structure 250 and a portion of the passivation layer 256 extends directly along filter
material defining light guide 214. The reaction recess 210 can be aligned with and formed
directly over light guide 214. According to one example each of reaction recess 210 and light
guide 214 can have geometric centers centered on longitudinal axis 268.
As set forth herein in connection with Fig, 8 detector surface 206 can be dimensioned
so that light energy incident on detector surface 206 in a fluorescence range can be cancelled by
the operation of induced electromagnetic fields. According to one example, shield structure 250
can have a thickness of from about 100 nm to about 600 nm, passivation layer 256 can have a
thickness of from about 100 nm to about 600 nm, passivation layer 256 can have a thickness of
from about 50 nm to about 500 nm, aperture 252 can have a diameter of from about 700 nm to
about 1.5 um, and reaction recess 210 if present can have a height of from about 50 nm to about
500 nm.
In some cases, prior to the passivation layer 256 being deposited along the shield
structure 250, and prior to a depositing of shield structure 250 a cavity defined by sidewalls 254
can be formed the dielectric stack defined by dielectric layers 232-237. For example, the
dielectric stack defined by dielectric layers 232-237 can be etched to form an array of the
cavities defined by sidewalls 254, wherein one cavity is formed for each light sensor 202 of light
sensor array 201. In particular examples, a cavity defined by sidewalls 254 is a vertically
elongated space that extends from proximate the aperture 252 toward the light sensor 202.
The cavity can extend vertically along longitudinal axis 268. A three-dimensional
shape of cavity defined by sidewalls 254 can be cylindrical or frustro-conical in some examples
such that a cross-section taken along a horizontal plane that extends into the page of Fig. 10 is
circular. The longitudinal axis 268 can extend through a geometric center of the cross-section.
However, other geometries can be used in alternative examples. For example, the cross-section
can be square-shaped or octagonal. According to one example the longitudinal axis 268 which is
the longitudinal axis of light guide 214 can extend through a geometric center of light sensor 202
and reaction recess 210.
The filter material defining light guide 214 can be deposited within the cavity
defined by sidewalls 254 after the cavity defined by sidewalls 254 is formed. For fabrication of
light guide 214 according to one example, dye molecules in powder form, e.g. having photon
emission quencher, can be dissolved with a solvent and added to a liquid polymer binder to form
a homogeneous liquid matrix having dye molecules and polymer molecules. According to one
example the dye molecules in powder form can be metal complex dye particles.
The homogeneous liquid matrix can be deposited into a dielectric stack cavity of
detector 200 and evapourated to form a filter material comprising a solid dye and polymer matrix
wherein dye molecules are suspended within a matrix of polymer binder molecules. The
homogeneous polymer binder and dye matrix filter material can be deposited into the cavity
defined by sidewalls 254, using e.g. chemical vapour deposition (CVD) physical vapour
deposition (PVD). The depositing can be performed to overfill the cavity defined by sidewalls
254 with filter material and then subject to patterning such as by planarization or etching to
reduce the elevation of the filter material defining light guide 214. A filter material for forming
light guide 214 according to one example can include metal complex dye molecules suspended
in a polymer binder molecule matrix.
The filter material can form (e.g. after curing) a light guide 214. The light guide 214
can be configured to block the excitation light 101 and permit emissions signal light 501 (Fig. 1)
to propagate therethrough toward the corresponding light sensor 202. The light guide 214 can be
formed of filter material described in reference to Figs. 2-7 herein. The filter material can include
a homogeneous matrix of dye and polymer binder, wherein the dye can include a photon
emission quencher and according to one example is provided by a metal complex dye. The dye
and polymer matrix according to one example can include a weight concentration in the range of
from about 70:30 dye to polymer to about 90:10 dye to polymer. The filter material mixture can
have a molecule ratio of about 1 dye molecule to about 100 polymer molecules.
The light guide 214 can be configured relative to surrounding material of the
dielectric stack defined by dielectric layers 231-237 to form a light-guiding structure. For
example, the light guide 214 can have a refractive index of at least about 2.0 so that light energy
propagating through light guide is reflected at an interface between light guide 214 and the
surrounding dielectric stack defined by dielectric layers 231-237. In certain examples, the light
guide 214 is configured such that the optical density (OD) or absorbance of the excitation light
101 is at least about 4 OD. More specifically, the filter material can be selected and the light
guide 214 can be dimensioned to achieve at least 4 OD. In more particular examples, the light
guide 214 can be configured to achieve at least about 5 OD or at least about 6 OD. In more
particular examples, the light guide 214 can be configured to achieve at least about 5 OD or at
least about 6 OD. Other features of the detector 200 can be configured to reduce electrical and
optical crosstalk.
It should be appreciated that all combinations of the foregoing concepts and
additional concepts discussed in greater detail below (provided such concepts are not mutually
inconsistent) are contemplated as being part of the subject matter disclosed herein. In particular,
all combinations of claims subject matter appearing at the end of this disclosure are
contemplated as being part of the subject matter disclosed herein. It should also be appreciated
that terminology explicitly employed herein that also may appear in any disclosure incorporated
by reference should be accorded a meaning most consistent with the particular concepts
disclosed herein.
This written description uses examples to disclose the subject matter, and also to
enable any person skilled in the art to practice the subject matter, including making and using
any devices or systems and performing any incorporated methods. The patentable scope of the
subject matter is defined by the claims, and can include other examples that occur to those
skilled in the art. Such other examples are intended to be within the scope of the claims if they
have structural elements that do not differ from the literal language of the claims, or if they
include equivalent structural elements with insubstantial differences from the literal languages of
the claims.
It is to be understood that the above description is intended to be illustrative, and not
restrictive. For example, the above-described examples (and/or aspects thereof) can be used in
combination with each other. In addition, many modifications can be made to adapt a particular
situation or material to the teachings of the various examples without departing from their scope.
While the dimensions and types of materials described herein are intended to define the
parameters of the various examples, they are by no means limiting and are merely exemplary.
Many other examples will be apparent to those of skill in the art upon reviewing the above
description. The scope of the various examples should, therefore, be determined with reference
to the appended claims, along with the full scope of equivalents to which such claims are
entitled. In the appended claims, the terms “including” and “in which” are used as the plain-
English equivalents of the respective terms “comprising” and “wherein”. Moreover, in the
following claims, the terms “first”, “second”, and “third”, etc. are used merely as labels, and are
not intended to impose numerical requirements on their objects. Forms of term “based on” herein
encompass relationships where an element is partially based on as well as relationships where an
element is entirely based on. Forms of the term “defined” encompass relationships where an
element is partially defined as well as relationships where an element is entirely defined. Further,
the limitations of the following claims are not written in means-plus-function format and are not
intended to be interpreted based on 35 U.S.C. § 112, sixth paragraph, unless and until such claim
limitations expressly use the phrase “means for” followed by a statement of function void of
further structure. It is to be understood that not necessarily all such objects or advantages
described above can be achieved in accordance with any particular example. Thus, for example,
those skilled in the art will recognise that the systems and techniques described herein can be
embodied or carried out in a manner that achieves or optimises one advantage or group of
advantages as taught herein without necessarily achieving other objects or advantages as can be
taught or suggested herein.
While the subject matter has been described in detail in connection with only a
limited number of examples, it should be readily understood that the subject matter is not limited
to such disclosed examples. Rather, the subject matter can be modified to incorporate any
number of variations, alterations, substitutions or equivalent arrangements not heretofore
described, but which are commensurate with the spirit and scope of the subject matter.
Additionally, while various examples of the subject matter have been described, it is to be
understood that aspects of the disclosure can include only some of the described examples. Also,
while some examples are described as having a certain number of elements it will be understood
that the subject matter can be practiced with less than or greater than the certain number of
elements. Accordingly, the subject matter is not to be seen as limited by the foregoing
description, but is only limited by the scope of the appended claims.
Claims (20)
1. A device for detecting with reduced fluorescence range noise comprising: a structure defining a detector surface configured for supporting biological or chemical samples; a sensor array comprising light sensors and circuitry to transmit signals using photons detected by the light sensors; and a guide array comprising light guides; wherein light guides of the guide array receive excitation light and emissions signal light from the detector surface, wherein the light guides extend toward respective light sensors of the sensor array and comprise filter material that blocks the excitation light and permits the emissions signal light to propagate toward the respective light sensors, and wherein the filter material comprises a metal complex dye comprising a photon emission quencher and a transition metal complex dye.
2. The device of claim 1, wherein the metal complex dye is suspended in a polymer binder matrix.
3. The device of claim 1, wherein the filter material comprises a homogeneous matrix of metal complex dye and a polymer binder and wherein the homogeneous matrix comprises a weight concentration ratio of metal complex dye to polymer binder in the range of from about 70:30 to about 90:10.
4. The device of any one of the preceding claims, wherein the detector surface includes a reaction recess for supporting a sample, wherein the reaction recess comprises an index of refraction and dimension to cancel background radiation in a detection band of the sensor array.
5. The device of any one of the preceding claims, wherein the metal complex dye is a non‐radiant dye, wherein the metal complex dye having a photon emission quencher on excitation quenches photons so that a return to ground state is accompanied by phonon emission and release of thermal energy, the metal complex dye leading to a non‐auto‐fluorescence of the filter material.
6. The device of any one of the preceding claims, wherein the metal complex dye comprises a transition metal and a dye and wherein the transition metal has an absorption spectral profile overlapping a fluorescence emissions spectral profile of the dye.
7. The device of claim 6, wherein the transition metal is octahedral and is selected from the group comprising Chromium, Scandium, Titanium, Vanadium, Manganese, Iron, Cobalt, Nickel and Copper.
8. The device of any one of the preceding claims, wherein the filter material comprises a counter ion associated to the metal complex dye.
9. The device of claim 8, wherein the counter ion comprises an alkyl amine.
10. The device of claim 9, wherein the alkyl amine comprises at least one hydrocarbon group of at least four carbon atoms.
11. A method for manufacturing a detecting device with reduced fluorescence range noise comprising: providing a light sensor array comprising light sensors; fabricating circuitry to transmit data signals using photons detected by the light sensor array, wherein the method further comprises; after forming cavities for a guide cavity array depositing filter material defining light guides within the guide cavities of the guide cavity array that are aligned with and disposed above respective light sensors of the light sensor array, wherein the filter material comprises dye suspended in a polymer matrix, wherein the dye comprises a transition metal complex dye, the transition metal complex dye comprising a photon emission quencher; and fabricating a structure defining a detector surface for supporting biological or chemical samples, wherein the fabricating the structure defining the detector surface includes fabricating the structure defining the detector surface above cavities of the guide cavity array and the light sensors of the light sensor array.
12. The method of claim 11, wherein the depositing filter material comprises using chemical vapour deposition, and wherein subsequent to the depositing, the deposited filter material is subject to processing using one or more of etching and planarizing.
13. The method of either claim 11 or claim 12, wherein the fabricating circuitry includes using complementary metal oxide semiconductor CMOS fabrication technology.
14. The method of any one of claims 11 to 13, wherein the filter material comprises a homogeneous matrix of the metal complex dye and polymer binder.
15. The method of claim 14, wherein the homogenous matrix comprises a weight concentration ratio of metal complex dye to polymer binder in the range of from about 70:30 to about 90:10.
16. The method of any one of claims 11 to 15, wherein the fabricating a structure defining a sample supporting surface comprises forming a reaction recess defined in the sample supporting surface, wherein the forming includes configuring the reaction recess so that based on an index of refraction of the detector surface and a dimensional characteristic of the reaction recess, an induced electromagnetic field radiating from the detector surface cancels background light energy incident on the detector surface in a detection wavelength band of the light sensor array.
17. The method of any one of claims 11 to 16, wherein the method includes subjecting one or more test sample detectors to testing to determine information relating a dimension of a detector surface to an electromagnetic field cancellation effect and wherein the fabricating the structure defining a detector surface includes dimensioning, using the determined information, a reaction recess of the detector surface to cancel light energy incident on the detector surface in a detection band of the light sensor array.
18. The method of any one of claims 11 to 17, wherein the filter material comprises a counter ion associated to a metal complex dye comprising the dye.
19. The method of claim 18, wherein the counter ion comprises an alkyl amine.
20. The method of claim 19, wherein the alkyl amine comprises at least one hydrocarbon group of at least four carbon atoms.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| NZ778619A NZ778619A (en) | 2017-12-28 | 2018-11-30 | Detector with reduced fluorescence range noise |
Applications Claiming Priority (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| US201762611464P | 2017-12-28 | 2017-12-28 | |
| US62/611,464 | 2017-12-28 | ||
| US201862644804P | 2018-03-19 | 2018-03-19 | |
| US62/644,804 | 2018-03-19 | ||
| PCT/US2018/063395 WO2019133182A1 (en) | 2017-12-28 | 2018-11-30 | Detector with reduced fluorescence range noise |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| NZ759983A NZ759983A (en) | 2021-08-27 |
| NZ759983B2 true NZ759983B2 (en) | 2021-11-30 |
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