SEMICONDUCTOR-LASER-INTEGRATED ATOMIC FORCE MICROSCOPY OPTICAL PROBE
20220357360 · 2022-11-10
Assignee
Inventors
- ALEXANDER A. UKHANOV (ALBUQUERQUE, NM, US)
- GENNADY A. SMOLYAKOV (ALBUQUERQUE, NM, US)
- FEI HUNG CHU (FREMONT, CA, US)
Cpc classification
G01Q20/04
PHYSICS
G01Q80/00
PHYSICS
G01Q60/38
PHYSICS
International classification
G01Q60/38
PHYSICS
Abstract
A new semiconductor-laser-integrated Atomic Force Microscopy (AFM) optical probe integrates a semiconductor laser and a silicon cantilever AFM probe into a robust easy-to-use chip to enable AFM measurements, optical imaging, and spectroscopy at the nanoscale.
Claims
1. A semiconductor-laser-integrated silicon or silicon nitride atomic force microscopy optical probe comprising: a semiconductor laser chip providing a gain medium section; and a silicon or silicon nitride cantilever atomic force microscopy probe, all integrated into a single chip, wherein said silicon or silicon nitride cantilever atomic force microscopy probe is an atomic force microscopy probe comprising a base, a cantilever, a tip formed at the end of the cantilever, and wherein the laser light emitted by said semiconductor laser chip is coupled into the probe tip as a result of propagation of the laser light in free space or in air.
2. The atomic force microscopy optical probe of claim 1, wherein the semiconductor laser chip is bonded to the surface of the base or buried in the base of the silicon or silicon nitride cantilever atomic force microscopy probe right in front of the cantilever or at some distance from the cantilever and aligned with the probe tip to couple the laser light into the probe tip.
3. The atomic force microscopy optical probe of claim 2, wherein the semiconductor laser chip is fabricated from a specially designed semiconductor laser epitaxial structure with significantly improved divergence across the epitaxial layers to radically improve coupling of the laser light into the probe tip.
4. The atomic force microscopy optical probe of claim 3, wherein the semiconductor laser chip is a three-section device divided into electrically isolated gain section and two absorber sections, located on both sides of the gain section, and the two absorber sections are used as photodetectors for detection of external light.
5. The atomic force microscopy optical probe of claim 3, wherein the semiconductor laser chip is a two-section device divided into electrically isolated gain section and saturable absorber section to allow ultrafast pulse generation.
6. The atomic force microscopy optical probe of claim 5, wherein the saturable absorber section of the semiconductor laser chip is used as a photodetector for intracavity light detection.
7. The atomic force microscopy optical probe of claim 3, wherein a second semiconductor laser chip with the same epitaxial structure is bonded to the surface of the base or buried in the base of the silicon or silicon nitride cantilever atomic force microscopy probe alongside the first semiconductor laser chip.
8. The atomic force microscopy optical probe of claim 7, wherein the second laser chip is used for detection of the light scattered from the probe tip.
9. The atomic force microscopy optical probe of claim 7, wherein the first and second semiconductor laser chips are vertically integrated stacks of two or more semiconductor laser chips designed for laser emission at different wavelengths.
10. The atomic force microscopy optical probe of claim 9, wherein the first and second semiconductor laser chips are used for laser generation and light detection at multiple wavelengths in the first and second semiconductor laser chips, respectively.
11. The atomic force microscopy optical probe of claim 1, wherein the semiconductor laser chip is based on one of the following semiconductor materials: GaAs, InP, GaP, GaSb, and GaN.
12. The atomic force microscopy optical probe of claim 1, wherein the optical gain in the semiconductor laser chip is provided by bulk active region.
13. The atomic force microscopy optical probe of claim 1, wherein the optical gain in the semiconductor laser chip is provided by a single quantum well active layer or by multiple quantum well active layers.
14. The atomic force microscopy optical probe of claim 1, wherein the optical gain in the semiconductor laser chip is provided by a single layer or by multiple layers of quantum dots in the active region of the epitaxial structure.
15. The atomic force microscopy optical probe of claim 1, wherein the epitaxial structure of the semiconductor laser chip is that of quantum cascade semiconductor laser.
16. A method for virus detection and identification, the method comprising: providing a semiconductor-laser-integrated silicon or silicon nitride atomic force microscopy optical probe comprising a semiconductor laser chip providing a gain medium section, a silicon or silicon nitride cantilever atomic force microscopy probe, and a photodetector, all integrated into a single chip; mounting the semiconductor-laser-integrated silicon or silicon nitride atomic force microscopy optical probe on an atomic force microscopy system; applying a direct current bias to the semiconductor laser chip such that the laser light power delivered to the tip apex of the probe is sufficient to do tip-enhanced Raman scattering or near-field scanning optical microscopy measurements; applying reverse voltage bias to the photodetector; performing a tip-enhanced Raman scattering measurement or near-field scanning optical microscopy measurement on a single virus particle.
17. The method of claim 16, wherein the semiconductor laser chip is a two-section device divided into electrically isolated gain section and saturable absorber section to allow ultrafast pulse generation, and the saturable absorber section is used as a photodetector for intracavity light detection in the near-field scanning optical microscopy measurement.
18. A method for DNA/RNA sequencing, the method comprising: providing a semiconductor-laser-integrated silicon or silicon nitride atomic force microscopy optical probe comprising a semiconductor laser chip providing a gain medium section, a silicon or silicon nitride cantilever atomic force microscopy probe, and a photodetector, all integrated into a single chip; mounting the semiconductor-laser-integrated silicon or silicon nitride atomic force microscopy optical probe on an atomic force microscopy system; applying a direct current bias to the semiconductor laser chip such that the laser light power delivered to the tip apex of the probe is sufficient to do tip-enhanced Raman scattering or near-field scanning optical microscopy measurements; applying reverse voltage bias to the photodetector; performing a tip-enhanced Raman scattering measurement or near-field scanning optical microscopy measurement on a single-stranded DNA, double-stranded DNA, or RNA molecules, stretched and attached to a fixed surface at both ends, by way of base-to-base readout necessary for DNA/RNA sequencing.
19. The method of claim 18, wherein the semiconductor laser chip is a two-section device divided into electrically isolated gain section and saturable absorber section to allow ultrafast pulse generation, and the saturable absorber section is used as a photodetector for intracavity light detection in the near-field scanning optical microscopy measurement.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION OF THE INVENTION
[0025] The semiconductor-laser-integrated AOP concept is based on integrating a semiconductor laser source into a cantilevered silicon AFM probe. Some preferred embodiments of the invention will be described below in detail based on the drawings.
Embodiment 1
[0026] In an illustrative embodiment of the present invention (
[0027] To allow light detection capability, the silicon-integrated semiconductor laser chip can be processed into a three-section device 15 divided into an electrically isolated gain section 16 and two parallel absorber sections 17 on both sides of the gain section (
[0028] Alternatively, a second semiconductor laser chip 20 with the same epitaxial structure is bonded directly to the top surface of the base 11 of a commercial AFM probe alongside the first semiconductor laser chip 10 (
[0029] The first and second semiconductor laser chips, in their turn, can be fabricated as vertically integrated stacks (22, 23) of two or more semiconductor laser chips with different epitaxial structures corresponding to different emission wavelengths (
Embodiment 2
[0030] In another illustrative embodiment of the present invention (
[0031] To allow light detection capability, the silicon-integrated semiconductor laser chip can be processed into a three-section device 15 divided into an electrically isolated gain section 16 and two parallel absorber sections 17 on both sides of the gain section (
[0032] Alternatively, a second semiconductor laser chip 20 with the same epitaxial structure is buried in the base 11 of a commercially available silicon AFM probe in front of the cantilever 12 alongside the first semiconductor laser chip 10 (
[0033] The first and second semiconductor laser chips, in their turn, can be fabricated as vertically integrated stacks (22, 23) of two or more semiconductor laser chips with different epitaxial structures corresponding to different emission wavelengths (
[0034]
Embodiment 3
[0035] Combining AFM probe with ultrafast near-field light source allows one to simultaneously achieve single-molecule spatial resolution and subpicosecond time resolution. The best way to achieve ultrafast laser pulse generation is to employ a passive mode-locking technique by dividing the laser cavity into two sections—a longer gain section and a shorter saturable absorber section. The gain section is forward biased, while the saturable absorber section is reverse biased. Electrical isolation between these two sections is achieved by using shallow dry etching to remove the heavily doped layers in the gap region.
[0036] Another illustrative embodiment of the present invention is similar to Embodiment 1 and Embodiment 2, except that the semiconductor laser chip is a two-section device 28 divided into electrically isolated gain section 29 and saturable absorber section 30 to allow ultrafast pulse generation capability (
Method Embodiment for Virus Detection Using AOP
[0037] A method embodiment of the invention provides a method of virus detection and identification using AOP. The method embodiment includes the steps of providing a semiconductor-laser-integrated atomic force microscopy optical probe comprising a semiconductor laser chip providing a gain medium section, a silicon cantilever atomic force microscopy probe, and a photodetector, all integrated into a single chip; mounting the semiconductor-laser-integrated atomic force microscopy optical probe on an atomic force microscopy system; applying a direct current bias to the semiconductor laser chip such that the laser light power delivered to the tip apex of the probe is sufficient to do tip-enhanced Raman scattering or near-field scanning optical microscopy measurements; applying reverse voltage bias to the photodetector; and performing a tip-enhanced Raman scattering measurement or near-field scanning optical microscopy measurement on a single virus particle.
Method Embodiment for DNA/RNA Sequencing Using AOP
[0038] A method embodiment of the invention provides a method of DNA/RNA sequencing using AOP. The method embodiment includes the steps of providing a semiconductor-laser-integrated atomic force microscopy optical probe comprising a semiconductor laser chip providing a gain medium section, a silicon cantilever atomic force microscopy probe, and a photodetector, all integrated into a single chip; mounting the semiconductor-laser-integrated atomic force microscopy optical probe on an atomic force microscopy system; applying a direct current bias to the semiconductor laser chip such that the laser light power delivered to the tip apex of the probe is sufficient to do tip-enhanced Raman scattering or near-field scanning optical microscopy measurements; applying reverse voltage bias to the photodetector; and performing a tip-enhanced Raman scattering measurement or near-field scanning optical microscopy measurement on a single-stranded DNA, double-stranded DNA, or RNA molecules, stretched and attached to a fixed surface at both ends, by way of base-to-base readout necessary for DNA/RNA sequencing.
[0039] In all embodiments, the semiconductor laser chip can be based on one of the following semiconductor materials: GaAs, InP, GaP, GaSb, and GaN.
[0040] In all embodiments, the optical gain in the silicon-integrated laser chip can be provided by bulk active region, by single or multiple quantum well active layers, or by a single or multiple layers of quantum dots in the active region of the epitaxial structure. The epitaxial structure of the laser chip can be that of quantum cascade semiconductor laser.
[0041] In all embodiments, the silicon cantilever atomic force microscopy probe used for integration with the semiconductor laser chip can alternatively be a silicon nitride cantilever atomic force microscopy probe.
REFERENCES CITED
[0042] [1] J. M. Klingsporn, M. D. Sonntag, T. Seideman, R. P. Van Duyne, “Tip-enhanced Raman spectroscopy with picosecond pulses”, J. Phys. Chem. Lett. 5 (#1), pp. 106-110, 2014. [0043] [2] X. Huang, A. Stintz, H. Li, L. F. Lester, J. Cheng, and K. J. Malloy, “Passive mode-locking in 1.3 μm two-section InAs quantum dot lasers,” Appl. Phys. Lett. 78(#19), pp. 2825-2827, 2001. [0044] [3] E. U. Rafailov, M. A. Cataluna, W. Sibbett, “Mode-locked quantum-dot lasers”, Nature Photonics 1, pp. 395-401, 2007. [0045] [4] J. Kneipp, H. Kneipp, K. Kneipp, “Two-photon vibrational spectroscopy for biosciences based on surface-enhanced hyper-Raman scattering”, Proc. Natl. Acad. Sci. USA 103(#46), pp. 17149-17153, 2006. [0046] [5] F. Madzharova, Z. Heiner, J. Kneipp, “Surface enhanced hyper Raman scattering (SEHRS) and its applications”, Chem. Soc. Rev. 46(#13), pp. 3980-3999, 2017. [0047] [6] C. Dab, C. Awada, A. Ruediger, “Tip-enhanced second harmonic generation: an approach for hyper-Raman spectroscopy”, Plasmonics 14(#3), pp. 653-661, 2019. [0048] [7] W. R. Zipfel, R. M. Williams, W. W. Webb, “Nonlinear magic: multiphoton microscopy in the biosciences”, Nat. Biotechnol. 21(#11), pp. 1368-1376, 2003. [0049] [8] F. Madzharova, Z. Heiner, J. Kneipp, “Surface enhanced hyper-Raman scattering of the amino acids tryptophan, histidine, phenylalanine, and tyrosine”, J. Phys. Chem. C 121(#2), pp. 1235-1242, 2017. [0050] [9] L. D. Ziegler, “Hyper-Raman spectroscopy”, J. Raman Spectrosc. 21(#12), pp. 769-779, 1990. [0051] [10] R. Shimada, H. Kano, H. O. Hamaguchi, “Hyper-Raman microspectroscopy: a new approach to completing vibrational spectral and imaging information under a microscope”, Opt. Lett. 31(#3), pp. 320-322, 2006. [0052] [11] H. Kneipp, K. Kneipp, F. Seifert, “Surface-enhanced hyper-Raman scattering (SEHRS) and surface-enhanced Raman scattering (SERS) by means of mode-locked Ti-sapphire laser excitation”, Chem. Phys. Lett. 212 (#3-4), pp. 374-378, 1993. [0053] [12] D. Cialla, T. Deckert-Gaudig, C. Budich, M. Laue, R. Moller, D. Naumann, V. Deckert, J. Popp, “Raman to the limit: tip-enhanced Raman spectroscopic investigations of a single tobacco mosaic virus”, J. Raman Spectrosc. 40(#3), pp. 240-243 (2009). [0054] [13] J. D. Driskell, Y. Zhu, C. D. Kirkwood, Y. P. Zhao, R. A. Dluhy, R. A. Tripp, “Rapid and sensitive detection of rotavirus molecular signatures using surface enhanced Raman spectroscopy”, PLoS ONE 5(#4), e10222 (2010). [0055] [14] P. Hermann, A. Hermelink, V. Lausch, G. Holland, L. Moller, N. Bannert, D. Naumann, “Evaluation of tip-enhanced Raman spectroscopy for characterizing different virus strains”, Analyst 136(#6), pp. 1148-1152 (2011). [0056] [15] X. X. Han, B. Zhao, Y. Ozaki, “Label-free detection in biological applications of surface-enhanced Raman scattering”, TRAC-Trend. Anal. Chem. 38, pp. 67-78 (2012). [0057] [16] H. Sato, M. Ishigaki, A. Taketani, B. B. Andriana, “Raman spectroscopy and its use for live cell and tissue analysis”, Biomed. Spectrosc. Imaging 7(#3-4), pp. 97-104 (2018). [0058] [17] K. Moor, Y. Terada, A. Taketani, H. Matsuyoshi, K. Ohtani, H. Sato, “Early detection of virus infection in live human cells using Raman spectroscopy”, J. Biomed. Opt. 23(#9), 097001 (2018). [0059] [18] X. Zhang, X. L. Zhang, C. L. Luo, Z. Q. Liu, Y. Y. Chen, S. L. Dong, C. Z. Jiang, S. K. Yang, F. B. Wang, X. H. Xiao, “Volume-enhanced Raman scattering detection of viruses”, Small 15(#11), 1805516 (2019). [0060] [19] Y. T. Yeh, K. Gulino, Y. H. Zhanga, A. Sabestien, T. W. Chou, B. Zhou, Z. Lin, I. Albert, H. G. Lu, V. Swaminathan, E. Ghedin, M. Terrones, “A rapid and label-free platform for virus capture and identification from clinical samples”, Proc. Natl. Acad. Sci. USA 117(#2), pp. 895-901 (2020). [0061] [20] K. Olschewski, E. Kaemmer, S. Stoeckel, T. Bocklitz, T. Deckert-Gaudig, R. Zell, D. Cialla-May, K. Weber, V. Deckert, J. Popp, “A manual and an automatic TERS based virus discrimination”, Nanoscale 7(#10), pp. 4545-4552 (2015). [0062] [21] J. Y. Lim, J. S. Nam, S. E. Yang, H. Shin, Y. H. Jang, G. U. Bae, T. Kang, K. I. Lim, Y. Choi, “Identification of newly emerging influenza viruses by surface-enhanced Raman spectroscopy”, Anal. Chem. 87(#23), pp. 11652-11659 (2015). [0063] [22] V. Hoang, R. A. Tripp, P. Rota, R. A. Dluhy, “Identification of individual genotypes of measles virus using surface enhanced Raman spectroscopy”, Analyst 135(#12), pp. 3103-3109 (2010). [0064] [23] L. Hamm, A. Gee, A. S. D. Indrasekara, “Recent advancement in the surface-enhanced Raman spectroscopy-based biosensors for infectious disease diagnosis”, Appl. Sci.-Basel 9(#7), 1448 (2019). [0065] [24] S. A. Camacho, R. G. Sobral-Filho, P. H. B. Aoki, C. J. L. Constantino, A. G. Brolo, “Zika immunoassay based on surface-enhanced Raman scattering nanoprobes”, ACS Sensors 3(#3), pp. 587-594 (2018). [0066] [25] M. Reyes, M. Piotrowski, S. K. Ang, J. Q. Chan, S. A. He, J. J. H. Chu, J. C. Y. Kah, “Exploiting the anti-aggregation of gold nanostars for rapid detection of hand, foot, and mouth disease causing enterovirus 71 using surface-enhanced Raman spectroscopy”, Anal. Chem. 89(#10), pp. 5373-5381 (2017). [0067] [26] A. M. Paul, Z. Fan, S. S. Sinha, Y. L. Shi, L. D. Le, F. W. Bai, P. C. Ray, “Bioconjugated gold nanoparticle based SERS probe for ultrasensitive identification of mosquito-borne viruses using Raman fingerprinting”, J. Phys. Chem. C 119(#41), pp. 23669-23675 (2015). [0068] [27] M. M. Joseph, N. Narayanan, J. B. Nair, V. Karunakaran, A. N. Ramya, P. T. Sujai, G. Saranya, J. S. Arya, V. M. Vijayan, K. K. Maiti, “Exploring the margins of SERS in practical domain: An emerging diagnostic modality for modern biomedical applications”, Biomater. 181, pp. 140-181 (2018). [0069] [28] X.-M. Lin, T. Deckert-Gaudig, P. Singh, M. Siegmann, S. Kupfer, Z. Zhang, S. Grafe and V. Deckert, arXiv:1604.06598 (2016). [0070] [29] Z. He, Z. H. Han, M. Kizer, R. J. Linhardt, X. Wang, A. M. Sinyukov, J. Z. Wang, V. Deckert, A. V. Sokolov, J. Hu, M. O. Scully, “Tip-enhanced Raman imaging of single-stranded DNA with single base resolution”, J. Am. Chem. Soc. 141(#2), pp. 753-757 (2019). [0071] [30] N. N. Ledentsov and V. A. Shchukin, “Novel concepts for injection lasers”, Opt. Eng. 41(#12), pp. 3193-3203, December 2002. [0072] [31] M. V. Maximov, Y. M. Shernyakov, I. I. Novikov, L. Y. Karachinsky, N. Yu. Gordeev, U. Ben-Ami, D. Bortman-Arbiv, A. Sharon, V. A. Shchukin, N. N. Ledentsov, T. Kettler, K. Posilovic, D. Bimberg, “High-power low-beam divergence edge-emitting semiconductor lasers with 1- and 2-D photonic bandgap crystal waveguide”, IEEE J. Sel. Topics Quantum Electorn. 14(#4), pp. 1113-1122, July-August 2008. [0073] [32] L. Liu, H. Qu, Y. Liu, Y. Zhang, Y. Wang, A. Qi, W. Zheng, “High-power narrow-vertical-divergence photonic band crystal laser diodes with optimized epitaxial structure”, Appl. Phys. Lett. 105(#23), Art. 231110, December 2014. [0074] [33] M. J. Miah, T. Kettler, K. Posilovic, V. P. Kalosha, D. Skoczowsky, R. Rosales, D. Bimberg, J. Pohl, M. Weyers, “1.9 W continuous-wave single transverse mode emission from 1060 nm edge-emitting lasers with vertically extended lasing area”, Appl. Phys. Lett. 105(#15), Art. 151105, October 2014. [0075] [34] X. L. Ma, A. J. Liu, H. W. Qu, Y. Liu, P. C. Zhao, X. J. Guo, W. H. Zheng, “Nearly diffraction-limited and low-divergence tapered lasers with photonic crystal structure”, IEEE Photon. Technol. Lett. 28(#21), pp. 2403-2406, November 2016. [0076] [35] F.-H. Chu, G. A. Smolyakov, K. J. Malloy, A. A. Ukhanov, “Novel semiconductor-laser-integrated active AFM optical probe with ultrashort pulses and nanoscale aperture”, Proc. SPIE 11967, Single Molecule Spectroscopy and Superresolution Imaging XV, 1196707, 2022.