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Claims  |
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What is claimed is:
1. An apparatus for imaging a sample located on a support, said apparatus
comprising:
a body for immobilizing said support, said support comprising at least a
first surface having said sample thereon;
an electromagnetic radiation source for generating excitation radiation
having a first wavelength;
excitation optics for transforming a geometry of said excitation radiation
to an excitation line, said excitation line having a focal plane, and
directing said excitation line at said sample for exciting a plurality of
regions thereon, said excitation line causing a labeled material on said
sample to emit a response radiation, said response radiation having a
second wavelength, said first wavelength being different from said second
wavelength;
collection optics for collecting said response radiation from said
plurality of regions;
a detector for sensing said response radiation received by said collection
optics, said detector generating a signal proportional to the amount of
radiation sensed thereon, said signal representing an image associated
with said plurality of regions from said sample;
a translator for allowing a subsequent plurality of regions on said sample
to be excited;
a processor for processing and storing said signal so as to generate a
2-dimensional image of said sample;
a mirror for directing said excitation radiation to excite said plurality
of regions at a non-zero incident angle such that said response radiation
and said excitation line reflected from said support are decoupled from
each other; and
a focuser for automatically focusing said sample in said focal plane of
said excitation line, said focuser comprising first focusing optics for
receiving said reflected excitation line and focusing said reflected
excitation line to a first spot, a first slit located such that said first
spot traverses said first slit when said translator moves said support in
a direction relative to said excitation line, said first spot located at
substantially a center of said first slit when said support is
substantially in said focal plane, and a first radiation detector located
behind said first slit for generating a signal proportional to an amount
of radiation detected, said amount of radiation being greatest when said
support is located in said focal plane.
2. The apparatus as recited in claim 1, wherein said focusing optics
comprise:
a cylindrical lens for collimating said line reflected from said support;
and
a lens for focusing said line collimated by said cylindrical lens to a
spot.
3. The apparatus as recited in claim 1, further comprising a position
adjustor for locating said support automatically in a substantially
perpendicular position relative to an optical axis of said collection
optics, said position adjustor comprising:
a tilt stage for rotating said body until it reaches said substantially
perpendicular position relative to the optical axis of said collection
optics;
a beam splitter for directing a portion of said reflected excitation line
from said first focusing optics;
second focusing optics for receiving said portion of said reflected
excitation line from said beam splitter and focusing said reflected
excitation line to a second spot;
a second slit located such that said second spot traverses said slit
perpendicularly when said tilt stage rotates said support, said second
spot located at substantially a center of said second slit when said
support is substantially perpendicular relative to the optical axis of
said collection optics; and
a second radiation detector located behind said second slit for generating
a signal proportional to an amount of radiation detected, said amount of
radiation being greatest when said support is located substantially
perpendicular relative to the optical axis of said collection optics.
4. The apparatus as recited in claim 3, wherein said substantially
perpendicular position is substantially vertical.
5. The apparatus as recited in claim 3, wherein said tilt stage is
controlled by said processor.
6. The apparatus as recited in claim 3, wherein said position adjustor
comprises an air bearing system, said air bearing system comprising:
an optics head comprising a substantially planar plate, said planar plate
comprising a first surface having a plurality of holes disposed therein,
said plurality of holes being in communication with an air inlet;
a pump connected to said air inlet for flowing air through said plurality
of holes;
a valve for regulating a flow of air from said air pump through said
plurality of holes; and
an air ballast to dampen air pressure variations, said optics head
maintained in a relative position by air pressure through said plurality
of holes such that said support is maintained in a substantially
perpendicular position relative to said optical axis of said collection
optics.
7. The apparatus as recited in claim 6, wherein said electromagnetic
radiation source, excitation optics, collection optics and sensing
detector are enclosed in said optics head.
8. The apparatus of claim 1, further comprising a support immobilized on
said body, said support comprising at least a first surface having a
sample thereon, said sample on said first surface of said support
comprising a plurality of different oligonucleotide sequences, each of
said plurality of different oligonucleotide sequences being in a separate
known location on said first surface of said support.
9. The apparatus of claim 8, wherein said sample comprises more than 100
different oligonucleotide sequences in a separate known location on said
first surface of said support.
10. The apparatus of claim 8, wherein said sample comprises more than 1000
different oligonucleotide sequences in a separate known location on said
first surface of said support.
11. The apparatus of claim 8, wherein said sample comprises more than
10,000 different oligonucleotide sequences in a separate known location on
said first surface of said support.
12. The apparatus of claim 8, wherein said sample comprises more than
100,000 different oligonucleotide sequences in a separate known location
on said first surface of said support.
13. The apparatus of claim 8, wherein said support is glass.
14. A method of imaging a sample on a support, said method comprising the
steps of:
immobilizing said support on a body;
exciting said sample on said support with an excitation radiation having a
first wavelength from an electromagnetic radiation source, said excitation
radiation having a focal plane and a linear geometry for exciting a
plurality of region on said sample;
detecting a response radiation having a second wavelength in response to
said excitation radiation, said response radiation representing an image
of said plurality of regions;
exciting a subsequent plurality of regions on said sample;
processing and storing said response radiation to generate a 2-dimensional
image of said sample; and
auto-focusing said sample in said focal plane of said excitation radiation,
said step of autofocusing comprising the steps of focusing a first surface
of said support, coarse focusing on a second surface said support and
finely focusing said second surface, wherein said step of focusing said
first surface comprises the steps of directing said excitation radiation
at said first surface of said support, said excitation radiation being
reflected by said support, focusing said reflected excitation radiation
through a slit, detecting an amount of reflected excitation radiation
passing through said slit, said slit configured such that said reflected
excitation radiation is located substantially at a center of said slit
when said first surface is located in substantially the focal plane of
said excitation radiation, determining if said amount of reflected
excitation radiation passing through said slit has peaked, moving said
support closer relative to said electromagnetic radiation source and
repeating the directing, focusing, detecting, determining, and moving
steps until said amount of reflected excitation radiation passing through
said slit has peaked.
15. The method as recited in claim 14, wherein said step of coarse focusing
said second surface comprises the steps of:
first moving said support closer relative to said electromagnetic radiation
source, the distance which the said support is moved being equal to about
half the thickness of said support;
directing said excitation radiation at said support, said excitation
radiation being reflected by said support;
focusing said excitation radiation reflected by said support through said
slit;
detecting an amount of said excitation radiation reflected by said support
and passing through said slit;
determining if said amount of excitation radiation reflected by said
support and passing through said slit has peaked;
second moving said support closer relative to said electromagnetic
radiation source and repeating the directing, focusing, detecting,
determining and moving steps until said amount of excitation radiation
reflected by said support and passing through said slit has peaked.
16. The method as recited in claim 14, wherein said step of finely focusing
said second surface comprises the steps of:
directing said excitation radiation at said support, said excitation
radiation being reflected by said support;
focusing said excitation radiation reflected by said support through said
slit;
detecting said amount of excitation radiation reflected by said support and
passing through said slit, said slit configured such that said excitation
radiation reflected by said support is located substantially at a center
of said slit when said second surface is located substantially in the
focal plane of said excitation radiation;
determining if said amount of excitation radiation reflected by said
support and passing through said slit has peaked; and
moving said support farther relative to said electromagnetic radiation
source and repeating the directing, focusing, detecting, determining and
moving steps until said amount of excitation radiation reflected by said
support passing through said slit has reached a desired value.
17. The method of claim 14, wherein said sample excited in said exciting
step comprises a plurality of different oligonucleotide sequences, each of
said plurality of different oligonucleotide sequences being in a separate
known location on said second surface of said support.
18. The method of claim 17, wherein said sample comprises more than 100
different oligonucleotide sequences in a separate known location on said
second surface of said support.
19. The method of claim 17, wherein said sample comprises more than 1000
different oligonucleotide sequences in a separate known location on said
second surface of said support.
20. The method of claim 17, wherein said sample comprises more than 10,000
different oligonucleotide sequences in a separate known location on said
second surface of said support.
21. The method of claim 17, wherein said sample comprises more than 100,000
different oligonucleotide sequences in a separate known location on said
second surface of said support.
22. The method of claim 17, wherein said support is glass. |
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Claims  |
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Description  |
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COPYRIGHT NOTICE
A portion of the disclosure of this patent document contains material which
is subject to copyright protection. The copyright owner has no objection
to the facsimile reproduction by anyone of the patent document or the
patent disclosure as it appears in the Patent and Trademark Office patent
file or records, but otherwise reserves all copyright rights whatsoever.
BACKGROUND OF THE INVENTION
The present invention relates to the field of imaging. In particular, the
present invention provides methods and apparatus for high speed imaging of
a sample containing labeled markers with high sensitivity and resolution.
Methods and systems for imaging samples containing labeled markers such as
confocal microscopes are commercially available. These systems, although
capable of achieving high resolution with good depth discrimination, have
a relatively small field of view. In fact, the system's field of view is
inversely related to its resolution. For example, a typical 40.times.
microscope objective, which has a 0.25 .mu.m resolution, has a field size
of only about 500 .mu.m. Thus, confocal microscopes are inadequate for
applications requiring high resolution and large field of view
simultaneously.
Other systems, such as those discussed in U.S. Pat. No. 5,143,854 (Pirrung
et al.), PCT WO 92/10092, and U. S. patent application Ser. No.
08/195,889, filed Feb. 10, 1994, incorporated herein by reference for all
purposes, are also known. These systems include an optical train which
directs a monochromatic or polychromatic light source to about a 5 micron
(.mu.m) diameter spot at its focal plane. A photon counter detects the
emission from the device in response to the light. The data collected by
the photon counter represents one pixel or data point of the image.
Thereafter, the light scans another pixel as the translation stage moves
the device to a subsequent position.
As disclosed, these systems resolve the problem encountered by confocal
microscopes. Specifically, high resolution and a large field of view are
simultaneously obtained by using the appropriate objective lens and
scanning the sample one pixel at a time. However, this is achieved by
sacrificing system throughput. As an example, an array of material formed
using the pioneering fabrication techniques, such as those disclosed in
U.S. Pat. No. 5,143,854 (Pirrung et al.), U.S. patent application Ser. No.
08/143,312, and U.S. patent application Ser. No. 08/255,682, incorporated
herein by reference for all purposes, may have about 10.sup.5 sequences in
an area of about 13 mm.times.13 mm. Assuming that 16 pixels are required
for each member of the array (1.6.times.10.sup.6 total pixels), the image
can take over an hour to acquire.
In some applications, a full spectrally resolved image of the sample may be
desirable. The ability to retain the spectral information permits the use
of multi-labeling schemes, thereby enhancing the level of information
obtained. For example, the microenvironment of the sample may be examined
using special labels whose spectral properties are sensitive to some
physical property of interest. In this manner, pH, dielectric constant,
physical orientation, and translational and/or rotational mobility may be
determined.
From the above, it is apparent that improved methods and systems for
imaging a sample are desired.
SUMMARY OF THE INVENTION
Methods and systems for detecting a labeled marker on a sample located on a
support are disclosed. The imaging system comprises a body for
immobilizing the support. Excitation radiation, from an excitation source
having a first wavelength, passes through excitation optics. The
excitation optics cause the excitation radiation to excite a region on the
sample. In response, labeled material on the sample emits radiation which
has a wavelength that is different from the excitation wavelength.
Collection optics then collect the emission from the sample and image it
onto a detector. The detector generates a signal proportional to the
amount of radiation sensed thereon. The signal represents an image
associated with the plurality of regions from which the emission
originated. A translator is employed to allow a subsequent plurality of
regions on said sample to be excited. A processor processes and stores the
signal so as to generate a 2-dimensional image of said sample.
In one embodiment, excitation optics focus excitation light to a line at a
sample, simultaneously scanning or imaging a strip of the sample. Surface
bound labeled targets from the sample fluoresce in response to the light.
Collection optics image the emission onto a linear array of light
detectors. By employing confocal techniques, substantially only emission
from the light's focal plane is imaged. Once a strip has been scanned, the
data representing the 1-dimensional image are stored in the memory of a
computer. According to one embodiment, a multi-axis translation stage
moves the device at a constant velocity to continuously integrate and
process data. As a result, a 2-dimensional image of the sample is
obtained.
In another embodiment, collection optics direct the emission to a
spectrograph which images an emission spectrum onto a 2-dimensional array
of light detectors. By using a spectrograph, a full spectrally resolved
image of the sample is obtained.
The systems may include auto-focusing feature to maintain the sample in the
focal plane of the excitation light throughout the scanning process.
Further, a temperature controller may be employed to maintain the sample
at a specific temperature while it is being scanned. The multi-axis
translation stage, temperature controller, auto-focusing feature, and
electronics associated with imaging and data collection are managed by an
appropriately programmed digital computer.
In connection with another aspect of the invention, methods for analyzing a
full spectrally resolved image are disclosed. In particular, the methods
include, for example, a procedure for deconvoluting the spectral overlap
among the various types of labels detected. Thus, a set of images, each
representing the surface densities of a particular label can be generated.
A further understanding of the nature and advantages of the inventions
herein may be realized by reference to the remaining portions of the
specification and the attached drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 shows a block diagram of an imaging system;
FIG. 2 illustrates how the imaging system achieves good depth
discrimination;
FIG. 3 shows the imaging system according to the present invention;
FIGS. 4a-4d show a flow cell on which a substrate is mounted;
FIG. 5 shows a agitation system;
FIG. 6 is a flow chart illustrating the general operation of the imaging
system;
FIGS. 7a-7b are flow charts illustrating the steps for focusing the light
at the sample;
FIG. 8 is a flow chart illustrating in greater detail the steps for
acquiring data;
FIG. 9 shows an alternative embodiment of the imaging system;
FIG. 10 shows the axial response of the imaging system of FIG. 9;
FIGS. 11a-11b are flow charts illustrating the general operations of the
imaging system according to FIG. 9;
FIGS. 12a-12b are flow charts illustrating the steps for plotting the
emission spectra of the acquired image;
FIG. 12c shows the data structure of the data file according to the imaging
system in FIG. 9;
FIG. 13 shows the normalized emission spectra of four fluorophores whose
emission spectra are shown in FIG. 17, and scaled according to the steps
set forth in FIG. 12 a after they have been normalized;
FIG. 14 is a flow chart illustrating the steps for image deconvolution;
FIG. 15 shows the layout of the probe sample;
FIG. 16 shows examples of monochromatic images obtained by the imaging
system of FIG. 9;
FIGS. 17-18 show the emission spectra obtained by the imaging system of
FIG. 9;
FIG. 19 shows the emission cross section matrix elements obtained from the
emission spectra of FIG. 13;
FIG. 20 shows examples of images representing the surface density of the
fluorophores; and
FIG. 21 shows an alternative embodiment of an imaging system.
DESCRIPTION OF THE PREFERRED EMBODIMENT CONTENTS
I. Definitions
II. General
a. Introduction
b. Overview of the Imaging System
III. Detailed Description of One Embodiment of the Imaging System
a. Detection Device
b. Data acquisition
IV. Detailed Description of an Alternative Embodiment of the Imaging System
a. Detection Device
b. Data Acquisition
c. Postprocessing of the Monochromatic Image Set
d. Example of spectral deconvolution of a 4-fluorophore system
V. Detailed Description of Another Embodiment of the Imaging System
I. Definitions
The following terms are intended to have the following general meanings as
they are used herein:
1. Complementary: Refers to the topological compatibility or matching
together of interacting surfaces of a probe molecule and its target. Thus,
the target and its probe can be described as complementary, and
furthermore, the contact surface characteristics are complementary to each
other.
2. Probe: A probe is a surface-immobilized molecule that is recognized by a
particular target. Examples of probes that can be investigated by this
invention include, but are not restricted to, agonists and antagonists for
cell membrane receptors, toxins and venoms, viral epitopes, hormones
(e.g., opioid peptides, steroids, etc.), hormone receptors, peptides,
enzymes, enzyme substrates, cofactors, drugs, lectins, sugars,
oligonucleotides, nucleic acids, oligosaccharides, proteins, and
monoclonal antibodies.
3. Target: A molecule that has an affinity for a given probe. Targets may
be naturally-occurring or manmade molecules. Also, they can be employed in
their unaltered state or as aggregates with other species. Targets may be
attached, covalently or noncovalently, to a binding member, either
directly or via a specific binding substance. Examples of targets which
can be employed by this invention include, but are not restricted to,
antibodies, cell membrane receptors, monoclonal antibodies and antisera
reactive with specific antigenic determinants (such as on viruses, cells
or other materials), drugs, oligonucleotides, nucleic acids, peptides,
cofactors, lectins, sugars, polysaccharides, cells, cellular membranes,
and organelles. Targets are sometimes referred to in the art as
anti-probes. As the term targets is used herein, no difference in meaning
is intended. A "Probe Target Pair" is formed when two macromolecules have
combined through molecular recognition to form a complex.
II. General
a. Introduction
The present invention provides methods and apparatus for obtaining a highly
sensitive and resolved image at a high speed. The invention will have a
wide range of uses, particularly, those requiring quantitative study of a
microscopic region from within a larger region, such as 1 .mu.m.sup.2 over
100 mm.sup.2. For example, the invention will find application in the
field of histology (for studying histochemical stained and immunological
fluorescent stained images), video microscopy, or fluorescence in situ
hybridization. In one application, the invention herein is used to image
an array of probe sequences fabricated on a support.
The support on which the sequences are formed may be composed from a wide
range of material, either biological, nonbiological, organic, inorganic,
or a combination of any of these, existing as particles, strands,
precipitates, gels, sheets, tubing, spheres, containers, capillaries,
pads, slices, films, plates, slides, etc. The substrate may have any
convenient shape, such as a disc, square, sphere, circle, etc. The
substrate is preferably flat but may take on a variety of alternative
surface configurations. For example, the substrate may contain raised or
depressed regions on which a sample is located. The substrate and its
surface preferably form a rigid support on which the sample can be formed.
The substrate and its surface are also chosen to provide appropriate
light-absorbing characteristics. For instance, the substrate may be a
polymerized Langmuir Blodgett film, functionalized glass, Si, Ge, GaAs,
GaP, SiO.sub.2, SIN.sub.4, modified silicon, or any one of a wide variety
of gels or polymers such as (poly)tetrafluoroethylene,
(poly)vinylidenedifluoride, polystyrene, polycarbonate, or combinations
thereof. Other substrate materials will be readily apparent to those of
skill in the art upon review of this disclosure. In a preferred embodiment
the substrate is flat glass or silica.
According to some embodiments, the surface of the substrate is etched using
well known techniques to provide for desired surface features. For
example, by way of the formation of trenches, v-grooves, mesa structures,
or the like, the synthesis regions may be more closely placed within the
focus point of impinging light. The surface may also be provided with
reflective "mirror" structures for maximization of emission collected
therefrom.
Surfaces on the solid substrate will usually, though not always, be
composed of the same material as the substrate. Thus, the surface may be
composed of any of a wide variety of materials, for example, polymers,
plastics, resins, polysaccharides, silica or silica-based materials,
carbon, metals, inorganic glasses, membranes, or any of the above-listed
substrate materials. In one embodiment, the surface will be optically
transparent and will have surface Si-0H functionalities, such as those
found on silica surfaces.
The array of probe sequences may be fabricated on the support according to
the pioneering techniques disclosed in U.S. Pat. No. 5,143,854, PCT WO
92/10092, or U. S. application Ser. No. 07/624,120, filed Dec. 6, 1990,
incorporated herein by reference for all purposes. The combination of
photolithographic and fabrication techniques may, for example, enable each
probe sequence ("feature") to occupy a very small area ("site") on the
support. In some embodiments, this feature site may be as small as a few
microns or even a single molecule. For example, about 10.sup.5 to 10.sup.6
features may be fabricated in an area of only 12.8 mm.sup.2. Such probe
arrays may be of the type known as Very Large Scale Immobilized Polymer
Synthesis (VLSIPS.TM.).
The probe arrays will have a wide range of applications. For example, the
probe arrays may be designed specifically to detect genetic diseases,
either from acquired or inherited mutations in an individual DNA. These
include genetic diseases such as cystic fibrosis, diabetes, and muscular
dystrophy, as well as acquired diseases such as cancer (P53 gene relevant
to some cancers), as disclosed in U.S. Pat. application Ser. No.
08/143,312, already incorporated by reference.
Genetic mutations may be detected by a method known as sequencing by
hybridization. In sequencing by hybridization, a solution containing one
or more targets to be sequenced (i.e., samples from patients) contacts the
probe array. The targets will bind or hybridize with complementary probe
sequences. Generally, the targets are labeled with a fluorescent marker,
radioactive isotopes, enzymes, or other types of markers. Accordingly,
locations at which targets hybridize with complimentary probes can be
identified by locating the markers. Based on the locations where
hybridization occur, information regarding the target sequences can be
extracted. The existence of a mutation may be determined by comparing the
target sequence with the wild type.
The interaction between targets and probes can be characterized in terms of
kinetics and thermodynamics. As such, it may be necessary to interrogate
the array while in contact with a solution of labeled targets.
Consequently, the detection system must be extremely selective, with the
capacity to discriminate between surface-bound and solution-born targets.
Also, in order to perform a quantitative analysis, the high-density volume
of the probe sequences requires the system to have the capacity to
distinguish between each feature site.
b. Overview of the Imaging System
An image is obtained by detecting the electro-magnetic radiation emitted by
the labels on the sample when it is illuminated. Emission from
surface-bound and solution-free targets is distinguished through the
employment of confocal and auto-focusing techniques, enabling the system
to image substantially only emission originating from the surface of the
sample. Generally, the excitation radiation and response emission have
different wavelengths. Filters having high transmissibility in the label's
emission band and low transmissibility in the excitation wavelength may be
utilized to virtually eliminate the detection of undesirable emission.
These generally include emission from out-of-focus planes or scattered
excitation illumination as potential sources of background noise.
FIG. 1 is an optical and electronic block diagram illustrating the imaging
system according to the present invention. Illumination of a sample 1500
may be achieved by exposing the sample to electromagnetic radiation from
an excitation source 1100. Various excitation sources may be used,
including those which are well known in the art such as an argon laser,
diode laser, helium-neon laser, dye laser, titanium sapphire laser, Nd:YAG
laser, arc lamp, light emitting diodes, any incandescent light source, or
other illuminating device.
Typically, the source illuminates the sample with an excitation wavelength
that is within the visible spectrum, but other wavelengths (i.e., near
ultraviolet or near infrared spectrum) may be used depending on the
application (i.e., type of markers and/or sample). In some embodiments,
the sample is excited with electromagnetic radiation having a wavelength
at or near the absorption maximum of the species of label used. Exciting
the label at such a wavelength produces the maximum number of photons
emitted. For example, if fluorescein (absorption maximum of 488 nm) is
used as a label, an excitation radiation having a wavelength of about 488
nm would induce the strongest emission from the labels.
In instances where a multi-labeling scheme is utilized, a wavelength which
approximates the mean of the various candidate labels' absorption maxima
may be used. Alternatively, multiple excitations may be performed, each
using a wavelength corresponding to the absorption maximum of a specific
label. Table I lists examples of various types of fluorophores and their
corresponding absorption maxima.
TABLE I
______________________________________
Candidate Fluorophores
Absorption Maxima
______________________________________
Fluorescein 488 nm
Dichloro-fluorescein
525 nm
Hexachloro-fluorescein
529 nm
Tetramethylrhodamine
550 nm
Rodamine X 575 nm
Cy3 .TM. 550 nm
Cy5 .TM. 650 nm
Cy7 .TM. 750 nm
IRD40 785 nm
______________________________________
The excitation source directs the light through excitation optics 1200,
which focus the light at the sample. The excitation optics transform the
light into a "line" sufficient to illuminate a row of the sample. Although
the Figure illustrates a system that images one vertical row of the sample
at a time, it can easily be configured to image the sample horizontally or
to employ other detection scheme. In this manner, a row of the sample
(i.e., multiple pixels) may be imaged simultaneously, increasing the
throughput of the imaging systems dramatically.
Generally, the excitation source generates a beam with a Gaussian profile.
In other words, the excitation energy of the line peaks flatly near the
center and diminishes therefrom (i.e., non-uniform energy profile).
Illuminating the sample with a non-uniform energy profile will produce
undesirable results. For example, the edge of the sample that is
illuminated by less energetic radiation would appear more dim relative to
the center. This problem is resolved by expanding the line to permit the
central portion of the Gaussian profile to illuminate the sample.
The width of the line (or the slit aperture) determines the spatial
resolution of the image. The narrower the line, the more resolved the
image. Typically, the line width is dictated by the feature size of
sample. For example, if each probe sequence occupies a region of about 50
.mu.m, then the minimum width is about 50 .mu.m. Preferably, the width
should be several times less than the feature size to allow for
oversampling.
Excitation optics may comprise various optical elements to achieved the
desired excitation geometry, including but not limited to microscope
objectives, optical telescopes, cylindrical lens, cylindrical telescopes,
line generator lenses, anamorphic prisms, combination of lenses, and/or
optical masks. The excitation optics may be configured to illuminate the
sample at an angle so as to decouple the excitation and collection paths.
As a result, the burden of separating the light paths from each other with
expensive dichroic mirrors or other filters is essentially eliminated. In
one embodiment, the excitation radiation illuminates the sample at an
incidence of about 45.degree.. This configuration substantially improves
the system's depth discrimination since emission from out-of-focus planes
is virtually undetected. This point will subsequently be discussed in more
detail in connection with FIG. 2.
As the incident light is reflected from the sample, it passes through
focusing optics 1400, which focus the reflected illumination line to a
point. A vertical spatial slit 1405 and light detector 1410 are located
behind the focusing optics. Various light detectors may be used, including
photodiodes, avalanche photodiodes, phototransistors, vacuum photodiodes,
photomultiplier tubes, and other light detectors. The focusing optics,
spatial slit, and light detector serve to focus the sample in the focal
plane of the excitation light. In one embodiment, the light is focused at
about the center of the slit when the sample is located in the focal plane
of the incident light. Using the light detector to sense the energy, the
system can determine when the sample is in focus. In some applications,
the slit may be eliminated by employing a split photodiode (bi-cell or
quadrant detector), position-sensitive photodiode, or position-sensitive
photomultiplier.
The line illumination technique presents certain concerns such as
maintaining the plane of the sample perpendicular to the optical axis of
the collection optics. If the sample is not aligned properly, image
distortion and intensity variation may occur. Various methods, including
shims, tilt stage, gimbal mount, goniometer, air pressure or pneumatic
bearings or other technique may be employed to maintain the sample in the
correct orientation. In one embodiment, a beam splitter 1420 may be
strategically located to direct a portion of the beam reflected from the
sample. A horizontal spatial slit 1425 and light detector 1430, similar to
those employed in the auto-focusing technique, may be used to sense when
the plane of the sample is perpendicular to the optical axis of the
collection optics.
In response to the excitation light, the labeled targets fluoresce (i.e.,
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