U.S. patent application number 15/347602 was filed with the patent office on 2018-05-10 for spatio-temporally incremental fiber swept source.
The applicant listed for this patent is The University of Hong Kong. Invention is credited to Xiaoming WEI, Kenneth Kin Yip WONG.
Application Number | 20180128972 15/347602 |
Document ID | / |
Family ID | 62064460 |
Filed Date | 2018-05-10 |
United States Patent
Application |
20180128972 |
Kind Code |
A1 |
WONG; Kenneth Kin Yip ; et
al. |
May 10, 2018 |
SPATIO-TEMPORALLY INCREMENTAL FIBER SWEPT SOURCE
Abstract
A spatio-temporally incremental fiber sweep source includes a
laser light pulse generator for generating light pulses and a fiber
array of individual optical fibers. The fiber array has an input
end and an output end, with the fibers at the input end receiving
the light pulses substantially simultaneously. The optical fibers
at the output end are arranged in a raster scan pattern, e.g., a
square pattern, wherein the optical delay in each fiber is greater
than the previous one in the scan pattern direction. As a result
light exits the array in a completely optical two dimensional
raster scan pattern. It has no moving parts, and thus no mechanical
inertia, so extremely high speed scanning can be achieved.
Inventors: |
WONG; Kenneth Kin Yip;
(Kowloon, HK) ; WEI; Xiaoming; (Whitty Street,
HK) |
|
Applicant: |
Name |
City |
State |
Country |
Type |
The University of Hong Kong |
Hong Kong |
|
CN |
|
|
Family ID: |
62064460 |
Appl. No.: |
15/347602 |
Filed: |
November 9, 2016 |
Current U.S.
Class: |
1/1 |
Current CPC
Class: |
H01S 3/1106 20130101;
H01S 3/1616 20130101; G02B 6/29359 20130101; H01S 3/094053
20130101; H01S 3/0092 20130101; G02B 6/32 20130101; H01S 3/0941
20130101; H01S 3/0057 20130101; G02B 6/4285 20130101; H04N 7/22
20130101; H01S 3/005 20130101; H01S 3/06791 20130101; H01S 3/09415
20130101; G02B 6/04 20130101; G02B 6/4204 20130101; G02B 2006/0098
20130101; H01S 3/1618 20130101; G02B 6/4296 20130101; H01S 3/1608
20130101; H04N 7/18 20130101; G02B 6/2938 20130101; H01S 3/094007
20130101; G02B 6/0008 20130101 |
International
Class: |
G02B 6/04 20060101
G02B006/04; G02B 6/42 20060101 G02B006/42; G02B 6/293 20060101
G02B006/293; H01S 3/11 20060101 H01S003/11; H01S 3/067 20060101
H01S003/067; H01S 3/0941 20060101 H01S003/0941; H01S 3/094 20060101
H01S003/094; G02B 6/32 20060101 G02B006/32; H04N 7/18 20060101
H04N007/18 |
Claims
1. A spatio-temporally incremental fiber sweep source comprising: a
light pulse generator for generating light pulses; a collimator and
a beam expander, wherein the collimator receive the light pulses
from the light pulse generator and passes them to the beam
expander, and a fiber array of individual optical fibers having an
input end and an output end, fibers at the input end receiving the
light pulses from the beam expander substantially simultaneously,
the optical fibers at the output end being arranged in a raster
scan pattern wherein the optical delay in each fiber is greater
than the previous one in the scan pattern direction whereby light
exits the array in the raster scan pattern as a sweep source.
2. The sweep source of claim 1 wherein the light pulse generator
comprises: a fiber ring cavity that performs polarization rotation
mode-locking; a laser diode that pumps light pulses into the fiber
ring cavity; a mode-locker inside the fiber cavity to insure the
delivery of ultra-short pulses; a fiber-based optical integrated
module that provides wavelength-division multiplexing for pump and
signal combining, and optical coupling for signal extraction said
integrated module providing an output pulse from said fiber ring
cavity; and a pre-chirp unit that received the output from the
integrated module and chirping ahead the pulse to compensate for
dispersion to be experienced during passage of the light through
the fiber array.
3. The sweep source of claim 2 wherein the fiber of the fiber ring
cavity is rare-earth-doped fiber with double cladding.
4. The sweep source of claim 2 wherein the laser diode is a high
power multimode fiber-pigtail pump laser diode.
5. The sweep source of claim 2 wherein the mode-locker is either
active (e.g. intensity modulator), or passive (e.g. semiconductor
saturable absorber and nonlinear polarization rotator).
6. (canceled)
7. The sweep source of claim 2 wherein the wavelength range of the
light pulse generator is changed by placing a nonlinear fiber optic
device before the fiber array.
8. The sweep source of claim 1 wherein the optical delay in the
fibers is controlled by controlling the fiber lengths.
9. The sweep source of claim 1 wherein the optical fibers of the
fiber array at the input are arranged randomly in a circular
pattern and at the output end they are arranged in a rectangular
raster scan pattern.
10. An image generator comprising: a sweep source according to
claim 1 a first lens system for forming collimated light from light
received from the sweep source and directing the collimated light
onto a specimen at an imaging plane; a second lens system after the
imaging plane for collecting light encoded by the specimen at the
imaging plane; and a photodetector for receiving the encoded light
and forming an image therefrom.
Description
FIELD OF THE INVENTION
[0001] The present invention relates to an optical fiber source for
providing ultrafast inertia-free spatially-scanning laser
pulses.
BACKGROUND OF THE INVENTION
[0002] Optical imaging has drawn great attention from various areas
in the past decade, particularly industrial inspection and
biomedical diagnosis. As the scientific research has gone deeper
and deeper into the details of these areas, people have become more
and more interested in dynamic behaviors, especially those involved
in life science, e.g. hemokinesis, cytology and neurology, which
provide information that may help provide a better understanding of
the human body. In particular there is great interest in ultrafast
dynamic diagnosis of disease and other tissue functionality. To
visualize high-speed dynamic events, an optical imager is required
to provide high sensitivity and high throughput. Modern
photo-receivers can offer excellent sensitivity, e.g. widely-used
CCD/CMOS cameras and photomultiplier tubes (PMT). Their imaging
speed, on the other hand, is largely limited, which results in
blurred images. Thus enhancing the speed of optical systems has
become a hot topic in recent years. Typically, there are two main
issues that have to be addressed for increasing the effective speed
of an optical system: scanning speed and signal readout speed.
[0003] The conventional way to perform two-dimensional (2D) imaging
is point-by-point scanning (i.e., raster-scanning) over the object
through multi-dimensional translation stages. Mechanical inertia,
unfortunately, limits the moving speed of these bulky stages,
typically to several mm/s. For an example of such mechanical stages
or actuators, see the LTA Precision Motorized Actuators, Series
300862, made by Newport Corporation.
https://www.newport.com/Precision-Motorized-Actuators,-LTA-Series/300862/-
1033/info.asp x#tab_Specifications. It thus takes 10 s of minutes
or even hours to finish a 2D image scan.
[0004] The object or sample can be moved by mechanical stages
through a beam or, rather than moving the sample, the more favored
way is to scan the laser beam over the object by using high-speed
scanning galvanometer mirrors (.about.kHz) or acousto-optic
deflectors (AOD, 10 s of kHz), which can boost the 2D imaging frame
rate to 100 Hz. See X. Chen, U. Leischner, Z. Varga, H. Jia, D.
Deca, N. L. Rochefort, and A. Konnerth, "LOTOS-based two-photon
calcium imaging of dendritic spines in vivo," Nat. Protoc. 7(10),
1818-1829 (2012), which is incorporated herein by reference in its
entirety. Although in the latter case, i.e., where the beam is
moved, can indeed perform the video rate imaging, it is still far
from the requirements for a 3D volumetric visualization of those
highly dynamic objects.
[0005] In addition to the scanning speed, the readout time of the
optical signal is another limitation on effectively boosting up the
imaging speed, and it must be fast enough to acquire the fast
scanning signal. Traditionally, the optical signal is read out
through CCD/CMOS cameras, which however exhibit an unacceptable
latency and result in a slow frame rate, typically 100 Hz, and
hence a long read-out time. See, the Hyper Vision HPV-2 high speed
video camera of Shimadzu Corporation of Kyoto Japan,
http://www.shimadzu.com/an/test/hpv/pv2_1.html, which is
incorporated herein by reference in its entirety. To overcome those
issues, the wavelength-swept source, e.g. Fourier-domain
mode-locking (FDML) swept source, has recently been proposed to
leverage those high-speed photodetectors (PDs) for fast imaging,
and to enable the video-rate necessary for 2D imaging. See R.
Huber, M. Wojtkowski, and J. G Fujimoto, "Fourier Domain Mode
Locking (FDML): A new laser operating regime and applications for
optical coherence tomography," Opt. Express 14, 3225-3237 (2006),
which is incorporated herein by reference in its entirety.
Unfortunately, the wavelength-swept source is a point source, and
it is still necessary to perform point scanning via, e.g.,
galvanometer scanning, for 2D/3D imaging.
[0006] Optical time-stretch is an emerging powerful all-optical
technique that can further enhance the wavelength-swept rate up to
the MHz range. See, K. Goda, K. K. Tsia, and B. Jalali, "Serial
time-encoded amplified imaging for real-time observation of fast
dynamic phenomena," Nature 458, 1145-1149 (2009), which is
incorporated herein by reference in its entirety. However, it has
the same issue as that of FDML, i.e., extra scanning is required.
In particular, mechanical or electronic scanning units are needed
to perform 2D imaging. More importantly, wavelength-swept sources
such as those used in traditional flow cytometers, operate at a kHz
level and exhibit a broad pulse waveform with limited instantaneous
peak power, typically at the mW level. The nature of the
time-stretch, i.e., high frequency chirping, also limits the
instantaneous peak power. Thus it cannot be used for those
applications requiring high peak power, for example multi-photon
imaging. See, N. G Horton, K. Wang, D. Kobat, C. G Clark, F. W.
Wise, C. B. Schaffer, and C. Xu, "In vivo three-photon microscopy
of subcortical structures within an intact mouse brain," Nature
Photon., 7, 205-209 (2013), which is incorporated herein by
reference in its entirety.
SUMMARY OF THE INVENTION
[0007] The present invention provides a 2D spatially-sweeping
source, as a new laser source, to overcome all of the limitations
mentioned above, and to boost the frame rate of 2D imaging to an
unprecedented level-10 s of MHz, i.e. 2D image capture within
<100 ns. The invention is implemented with a spatio-temporally
incremental fiber swept source (STIFSS). With STIFSS a laser beam
is applied to one end of a bunch of optical fibers. At the other
end of the bunch the fibers are arranged in a raster display. The
fibers of the display have different lengths in sequence such that
the light beam appears as a raster scan in the display without the
need for mechanical or electronic movement of a beam or object.
Such fast image capture is crucial for those applications where
traditional raster scanning is impossible, particularly for the
high-throughput flow cytometers.
[0008] Different from the traditional swept source with a low
instantaneous power (mW), the 2D spatially-sweeping STIFSS can
provide a peak power up to the kW level, which would allow use in
applications such as two-photon or even three-photon confocal
microscopy. The dwell time of a single spatial pixel, in addition,
is in the order of sub picoseconds (sub-ps)--several orders of
magnitude faster than that of CCD/CMOS cameras. Its ultra wide
operational wavelength range (more than an octave-spanning), in
addition, enables massive applications, e.g. ultrafast multi-photon
imaging, spectrally-encoded imaging, hyper-spectral imaging. More
importantly, it is a cost-effective solution for optical imaging
systems.
[0009] The main elements of STIFSS are (1) ultrafast femtosecond
(fs) pulse generation, (2) pulse pre-chirping; and (3) ultrafast
spatial sweeping. For the fs pulse generation, a simple fiber ring
cavity is employed to perform nonlinear polarization rotation (NPR)
mode-locking. This yields an fs pulse train. To simplify the
cavity, a compact optical integrated module (OIM) is designed to
provide multiple optical functions: pump combining,
polarization-sensitive unidirectional operation and signal tapping.
The gain medium is a piece of rare-earth-doped fiber, which is
pumped by a fiber-pigtail laser diode. The operating condition of
this fs laser cavity is optimized by an in-line polarization
controller. The cavity length L determines the 2D frame.
[0010] The pre-chirp unit is essentially a piece of single-mode
fiber (SMF), .about.100 m in length. It is primarily utilized to
compensate for the chirping later induced by the spatially sweeping
unit (SSU). The system is designed so that dispersion in the
pre-chirp is opposite to that in the SSUs, respectively.
[0011] For the spatial sweeping, the pre-chirp pulse is launched
into a free-space telescope through a fiber collimator. The
telescope expands the beam size output from the collimator,
typically several mm, to match the aperture of the subsequent fiber
bundle or array. After the telescope, the expanded laser beam is
coupled into the 2D pixel-delay fiber bundle or array to achieve
the spatial sweeping based on the differential delay in the
fibers.
BRIEF DESCRIPTION OF THE DRAWINGS
[0012] The foregoing and other objects and advantages of the
present invention will become more apparent when considered in
connection with the following detailed description and appended
drawings in which like designations denote like elements in the
various views, and wherein:
[0013] FIG. 1A is a schematic diagram of the spatio-temporally
incremental fiber swept source (STIFSS) according to the present
invention and FIG. 1B is a schematic diagram of a 2D pixel-delay
fiber array according to the present invention;
[0014] FIG. 2 is a schematic diagram of a 1D pixel-delay fiber
array illustrating the principles of the present invention, where
inset shows white-light microscopic images of the input and output
ends of a one dimensional output fiber array;
[0015] FIG. 3A is a graph of the optical spectra of a Yb-gain fiber
STIFSS before spectral broadening and FIG. 3B is a graph of the
same spectra after spectral broadening;
[0016] FIG. 4A is an intensity graph of the temporal pulse train of
the one dimensional STIFSS with a Yb-gain fiber at 1.0 .mu.m before
the SSU, FIG. 4B is an enlarged version of FIG. 4A, FIG. 4C is an
intensity graph of the temporal pulse train of the one dimensional
STIFSS with a Yb-gain fiber after the SSU and FIG. 4D is an
enlarged version of FIG. 4C;
[0017] FIG. 5A is a diagram of the imaging setup for a one
dimensional STIFSS at a line-scan rate of 29 MHz. FIG. 5B shows the
optical illumination pattern at the imaging plane in FIG. 5A, FIG.
5C is a USAF 1951 resolution target used as a sample target in the
setup of FIG. 5A and FIG. 5D is the image of the target of FIG. 5C
captured with STIFSS of FIG. 5A;
[0018] FIG. 6A is an intensity graph of the temporal pulse train of
STIFSS at 530 nm by frequency doubling a Yb-gain fiber laser before
the SSU, FIG. 6B is an enlarged version of FIG. 6A with an inset
showing an optical spectrum of a mode-locked pulse after frequency
doubling, FIG. 6C is an intensity graph of the temporal pulse train
of STIFSS at 530 nm by frequency doubling a Yb-gain fiber laser
after the SSU and FIG. 6D is an enlarged version of FIG. 6C;
[0019] FIG. 7A is an intensity graph of the temporal pulse train of
STIFSS with an Er-gain fiber before the SSU, FIG. 7B is an enlarged
version of FIG. 7A with an inset showing the optical spectrum of a
mode-locked pulse from the laser cavity, FIG. 7C is an intensity
graph of the temporal pulse train of STIFSS with an Er-gain fiber
after the SSU and FIG. 7D is an enlarged version of FIG. 7C;
and
[0020] FIG. 8A is an intensity graph of the temporal pulse train of
STIFSS with a Tm-gain fiber before the SSU, FIG. 8B is an enlarged
version of FIG. 8A with an insert showing the optical spectrum of a
mode-locked pulse directly output from the laser cavity, FIG. 8C is
an intensity graph of the temporal pulse train of STIFSS with a
Tm-gain fiber after the SSU, FIG. 8D is an enlarged version of FIG.
8C.
DETAILED DESCRIPTION
[0021] The spatio-temporally incremental fiber swept source
(STIFSS) of the present invention provides an ultrafast
inertia-free spatially-scanning laser pulse for each frame of
imaging. The sub-ps pulse train is linearly mapped into a 2D
spatial distribution by a differential time delay in the fibers of
a fiber array as shown in FIG. 1B. Each spatial pixel offers a
sub-ps dwell time. This completely-new laser source can be directly
applied to existing optical imaging systems and it can perform 2D
imaging at a frame rate of 10 s MHz, which is several orders of
magnitude faster than that of mechanical raster scanning systems,
which typically operate in the range of kHz.
[0022] As shown in FIG. 1A the STIFSS can be divided into three
parts: 1) high power ultra-short pulse generation (ultrafast
femtosecond (fs) pulse generation) with wavelength window
management, 2) pulse pre-chirp and 3) ultrafast spatial sweeping.
For the high power ultrashort pulse generation, a simple fiber ring
cavity 10 is employed to perform nonlinear polarization rotation
(NPR) mode-locking, providing a sub-ps or fs pulse train at 10 s of
MHz. To simplify the cavity, a fiber-based optical integrated
module (OIM) 12 is used to provide multiple optical functions:
wavelength-division multiplexing (WDM) for pump and signal
combining, and optical coupling (OC) for signal extraction. In
particular, OIM 12 provides pump combining, polarization-sensitive
unidirectional operation and signal tapping. The gain medium is a
piece of rare-earth-doped fiber 11, which is pumped by a
fiber-pigtail laser diode 14. To enable a high average output
power, the gain fiber 11 has a double-cladding design, including
inner and outer cladding, which has been commercially available.
The inner cladding mainly confines the signal in a small core
(.about.10 .mu.m) for single-mode operation, while the outer
cladding facilitates the propagation of the multimode pump laser
with a larger mode size (.about.100 .mu.m). In this way the laser
cavity can be pumped by using cost-effective high power multimode
pump laser diodes, typically offering 10 s of watts in power.
Benefiting from the high efficiency of state-of-the-art
double-cladding gain fibers, e.g. >70% at 1.0 .mu.m (see
https://www.thorlabs.com/newgrouppage9.cfm?objectgroup_id=336); the
average optical power of the output signal can reach several watts.
To ensure the laser cavity to deliver ultrashort pulses, a
mode-locker 16 is employed inside the fiber cavity. The mode-locker
can be active (e.g. intensity modulator), or passive (e.g.
semiconductor saturable absorber and nonlinear polarization
rotator). The cavity length L will determine the 2D frame rate.
Basically, the pulse laser can be bidirectional or unidirectional,
while the latter case requires an additional isolator.
[0023] In order to satisfy different wavelengths of interest for
specific applications, the operational wavelength of the laser
cavity has to be switchable or broad enough for selection by
different users. To meet this need, a STIFSS system can be designed
with two wavelength engineering schemes: First, the center
wavelength of the mode-locked pulse from the fiber cavity is
designed to be simply changed by choosing different doping fibers,
e.g. Nd-doped for 900 nm, Yb-doped for 1.0 .mu.m, Er-doped for 1.5
.mu.m and Tm-doped for 2.0 .mu.m. Second, the wavelength range
outside the fiber cavity can be further broadened by using a
highly-nonlinear fiber 18, e.g. photonic crystal fiber (PCF). With
these two schemes, the wavelength window is very flexible for
different applications.
[0024] To manage the pulse broadening effect due to the dispersion
issue in the optical fiber, and obtain an ultra-short pulse
approaching being transform-limited at the final output of STIFSS,
a pre-chirp unit 19 is utilized right after the spectral broadening
to chirp ahead the pulse with opposite dispersion, which can
compensate for the dispersion to be experienced during the later
propagation, mainly in the spatially sweeping unit (SSU) that
follows it. This pre-chirp can be achieved through dispersive
elements, e.g. single-mode fibers (SMFs) or chirped fiber Bragg
gratings (FBGs). It can be a piece of SMF, .about.100 m in length.
It should be noted that the goal is to make the dispersion in the
pre-chirp equal to and opposite from that introduced by the SSUs,
respectively.
[0025] For the spatially sweeping carried out by SSU 26, the
pre-chirp pulse is applied to a free-space telescope 22 through a
fiber collimator 20. The telescope, composed of two optical lenses,
expands the beam size of the fiber collimator, typically 1-2 mm, to
match the input aperture of the fiber array 24 (see FIG. 1B). After
the telescope, the expanded laser beam is coupled into the 2D
pixel-delay fiber array for spatially sweeping. As shown in FIG.
1B, the fiber array is an specially-designed fiber bundle of, for
example 400 fibers, and each has a 100 .mu.m core and 125 .mu.m
cladding. The input end 21 of the pixel-delay fiber bundle is
packaged in a round shape with a random order for the fibers order,
while the other end 23 is in a square shape (20.times.20 fibers in
a .about.2.5.times.2.5 mm size). Having the fibers at the input in
a random pattern reduces the possibility of light variation in the
output due to non-uniform input light. Also, the arrangement of the
fibers at the output end can be any convenient scan shape, e.g.,
rectangular for a wide screen display. The output fibers are
arranged in an order such that successive fibers are implemented
with an incremental length of .about.2 cm, corresponding to a time
delay of .about.100 ps. Thus the pulses exiting from the output end
of fiber bundle are sequenced in a raster fashion as shown in the
table inset 25 of FIG. 1B. Thus, the simultaneously input pulses
will exit the fiber bundle one by one with a time delay of 100 ps,
as shown in the right inset 13 of FIG. 1A, i.e. performing spatial
scanning in an all-optical manner. The optical fiber of the bundle
may have a numerical aperture (NA) of 0.22, and covers a wavelength
range from 400 nm to 2000 nm, see inset 27 of FIG. 1B. Since each
pulse from the fiber laser cavity will generate a 2D
spatially-sweeping pattern, the 2D scan rate is consistent with the
repetition rate of the fiber laser, as shown in right side of FIG.
1A, i.e., the repetition rate determined by the cavity length
L.
[0026] In order to prove the concept, a preliminary study was
conducted with a one dimensional (1D) version of STIFSS having an
optical wavelength ranging from 530 nm to 1900 nm. This design was
applied to perform ultrafast imaging. As shown in FIG. 2, 58-fibers
were constructed into a fiber bundle or array 30 in which, at the
input end 32, the 58 fibers were randomly bound together in a
circle, while at the output end 34 they were configured into a
1.times.58 array with a length increment of 2 cm. The fibers have a
size of 190/200 .mu.m for core/cladding, respectively. For a first
test the laser cavity was constructed with Yb-doped gain fiber. The
optical spectrum of the mode-locked pulse directly output from the
fiber cavity is illustrated in FIG. 3A, which is centered at 1064
nm with a bandwidth of .about.10 nm. The optical spectrum after
passing through a highly-nonlinear fiber was greatly broadened to
cover a range from .about.700 nm to .about.1700 nm as shown in FIG.
3B. The temporal waveforms before and after the SSU 26 are
illustrated in FIG. 4A (enlarged in FIG. 4B) and FIG. 4C (enlarged
in FIG. 4D), respectively. As shown in the FIGS. 4B and 4D, a
single narrow pulse, measured at the input of SSU 26, has been
spatially distributed onto a broad pulse waveform (around 5.8 ns,
corresponding to 100.times.58 ps). The sub-pulse from an individual
fiber pixel is also clearly shown, i.e. spatially sweeping along
the 1D fiber array facet. The temporal separation between adjacent
pixels is .about.100 ps, corresponding to the fiber length
increment of 2 cm. The line-scan rate was determined by the
repetition rate of the laser source, as shown in FIG. 4A and FIG.
4C, i.e. 29 MHz in this case. It is noted that the line-scan rate
is scalable by changing the repetition rate of the laser seed
source, e.g. changing the cavity length. The performance shown in
FIG. 4 is at 1.0 .mu.m.
[0027] Then, the STIFSS with the Yb-gain fiber was applied to
perform ultrafast microscopy, as shown in FIG. 5A. The
spatially-sweeping waveform train from STIFSS 50 was launched into
the optical imaging part (FIG. 5A) through two relay optical lenses
(L1 and L2) forming a beam expander. At the imaging plane there was
a linear illumination shower (single line raster light scan) as
shown in FIG. 5B, whose pixels are temporally stepping at an
interval of .about.100 ps. These pixels are encoded with the
spatial information of the sample. The sample used for this study
was a USAF 1951 resolution target, as shown in FIG. 5C. After the
sample, another optical lens (L3) was utilized to focus the STIFSS
pulse train onto a high-speed photodetector PD for optical
detection. The PD may be a single-pixel photodiode, which currently
has a bandwidth of 10 s of GHz. The image captured with this
ultrafast STIFSS is depicted in FIG. 5D. In this test the
illumination shower was in the horizontal direction, while
mechanical scanning was performed from top to bottom. The optical
line-scan rate was 29 MHz in this case.
[0028] In addition to the STIFSS with Yb-gain fiber, tests were
also performed at other center wavelengths without spectral
broadening, which may be useful for applications in other fields.
In particular, the pulse output from the Yb-gain fiber cavity was
frequency-doubled to 530 nm, which was realized by inserting a KTP
nonlinear crystal right before the SSU. The performance of the
530-nm STIFSS is shown in FIG. 6. In particular, FIG. 6A shows the
temporal pulse train of STIFSS with Yb-gain fiber and frequency
doubling to 530 nm before the SSU. FIG. 6B is an enlarged version
of FIG. 6A with an inset showing the optical spectrum of a
mode-locked pulse after frequency doubling. FIG. 6C shows the
temporal pulse train of STIFSS with a Yb-gain fiber and frequency
doubling at 530 nm after the SSU. FIG. 6D is an enlarged version of
FIG. 6C. The spatial sweeping operation is clearly shown in FIGS.
6B and 6D. It should be pointed out that, the sub-pixel pulse
vanishes from the illustration due to the limited bandwidth of the
2-GHz silicon visible window PD being used.
[0029] FIGS. 7 and 8 show the performance of STIFSS at with Er- and
Tm-gain fiber, respectively. In particular, FIG. 7A shows the
temporal pulse train of STIFSS with an Er-gain fiber before the SSU
and FIG. 7B is an enlarged version of FIG. 7A with an inset showing
the optical spectrum of a mode-locked pulse from the laser cavity.
FIG. 7C illustrates the temporal pulse train of STIFSS with an
Er-gain fiber after the SSU and FIG. 7D is an enlarged version of
FIG. 7C. The performance shown in FIG. 7 is at 1.5 .mu.m.
[0030] FIG. 8A illustrates the temporal pulse train of STIFSS with
a Tm-gain fiber before the SSU and FIG. 8B is an enlarged version
of FIG. 8A with an insert showing the optical spectrum of a
mode-locked pulse directly output from the laser cavity. FIG. 8C
shows the temporal pulse train of STIFSS with a Tm-gain fiber after
the SSU and FIG. 8D is an enlarged version of FIG. 8C. The
performance shown in FIG. 8 is at 2.0 .mu.m.
[0031] For the tests illustrated in FIGS. 7 and 8, the fiber
cavities of the seed sources were constructed with Er- and Tm-doped
gain fibers, respectively. It should be pointed out that the
temporal pulse packet of these two cases is not as broad as that of
the 1.0-.mu.m version (FIG. 4). This is because the beam size at
the input of the SSU was not optimized due to the lack of a
telescope at 1.5 and 2.0 .mu.m during the test. In addition, the
disappearance of the sub-pulse in the case of 2.0 .mu.m STIFSS is
due to a broader pulse width (>300 ps) of the original seed
pulse from the fiber cavity, as shown in FIG. 8B. Thus, the results
can be improved upon. It should be remembered that a broad
wavelength range (530-2000 nm) has been achieved with a single
SSU.
[0032] The present invention thus provides an ultrafast single-shot
imaging systems to enhance the 2D imaging speed. Taking multiphoton
microscopy as an example, the sub-ps dwell time together with
inertia-free 2D scanning enables the unprecedented ultrafast
fluorescence imaging. Another application is real time 2D imaging
of flow cytometry. Different from conventional cytometry, which can
only provide a blurred dot, the 2D spatially-swept source of the
present invention can enable 10 s m/s flowing 2D images.
Furthermore, it can provide not only a morphological image via 2D
spatial-encoding, but also chemical information as a result of its
high peak power.
[0033] While the present invention has been particularly shown and
described with reference to preferred embodiments thereof; it will
be understood by those skilled in the art that various changes in
form and details may be made therein without departing from the
spirit and scope of the invention.
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References