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 "title": "Laser lithography",
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 "excerpt": "Laser lithography is a maskless microfabrication technique that uses a focused laser beam to pattern photoresists and substrates directly, from nanometer features to centimeter-scale 3D structures.",
 "snippet": "Laser lithography is a maskless microfabrication technique that uses a focused laser beam to pattern photoresists and substrates directly, from nanometer features to centimeter-scale 3D structures.",
 "node": "technology.engineering.manufacturing.processes",
 "markdown": "# Laser lithography\n\nLaser lithography is a maskless microfabrication technique that uses a focused laser beam to pattern photoresists or substrates directly, producing resist patterns, deposited or etched microstructures, and free-form three-dimensional polymer and ceramic architectures. It spans single-photon direct writing with continuous-wave or pulsed visible and ultraviolet lasers, and multiphoton 3D lithography (MP3DL), a mesoscale additive manufacturing method that uses confined nonlinear light–matter interactions to build structures from nanometers to centimeters.<sup>[1](https://www.nature.com/articles/s43586-025-00386-y)</sup> By avoiding physical photomasks, it lowers production costs, increases process flexibility, and shortens development cycles compared with mask-based photolithography.<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup>\n\n| Key fact | Detail |\n|---|---|\n| Resolution mechanism | Single-photon writing resolution is set by the focused spot size; multiphoton writing adds thresholding that sharpens features beyond the diffraction limit<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup> |\n| Standard MP3DL feature size | 100 nm features with millimeter-scale object dimensions<sup>[1](https://www.nature.com/articles/s43586-025-00386-y)</sup> |\n| Typical light source | Ti:sapphire femtosecond laser, 690–1040 nm, 140 fs pulses, 80 MHz repetition rate<sup>[3](https://www.cell.com/iscience/pdf/S2589-0042%2823%2900451-0.pdf)</sup> |\n| Common resists | Negative-tone IP-series, PETIA, SU-8, and Ormocer, transparent at the writing wavelength with a large two-photon absorption cross-section<sup>[4](https://iopscience.iop.org/article/10.1088/2631-7990/ad943e)</sup> |\n| Serial-write speed | Commercial direct-write systems such as the DWL66+ write at 3 mm²/min with a 300 nm minimum feature; macroscale multiphoton prints can take hours to days<sup>[5](https://en.omedasemi.com/detail/218.html)</sup><sup> • </sup><sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup> |\n| Sub-diffraction records | 9 nm two-beam features<sup>[6](https://doi.org/10.1038/ncomms3061)</sup>; about 10 nm on semiconductor surfaces<sup>[7](https://iopscience.iop.org/article/10.1088/1361-648X/ae786d)</sup>; 5 nm for new-generation direct writing<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup> |\n\n## How it works\n\nLaser writing of microstructures rests on photolytic, pyrolytic, or photoelectrochemical microreactions between the laser light, the substrate surface, and molecules of the surrounding ambient; the same framework covers laser-based deposition and etching.<sup>[8](https://link.springer.com/article/10.1007/BF00617497)</sup> In single-photon writing, diffraction sets the floor: visible or infrared lasers cannot pattern materials with resolution better than about the diffraction limit, which motivates ultraviolet approaches.<sup>[9](https://pubs.aip.org/aip/jap/article/58/9/3649/173716/Submicrometer-resolution-etching-of-integrated)</sup>\n\nMultiphoton writing removes that floor differently. [Two-photon absorption](https://www.edgepedia.org/two-photon-absorption) is a nonlinear process in which the absorption rate is proportional to the square of the incident intensity, \\( I^{2} \\); a high-numerical-aperture objective confines the intensity to a sub-femtoliter voxel (3D pixel; tiny volume unit of a structure), and polymerization proceeds irreversibly only when the reactive-species concentration exceeds a critical threshold, which sharpens features beyond the diffraction limit.<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup> In practice, two-photon excitation sensitizes the photoinitiator, generating radicals that drive monomer cross-linking, chain growth, and termination, so the polymerized voxel becomes the building block of the structure.<sup>[3](https://www.cell.com/iscience/pdf/S2589-0042%2823%2900451-0.pdf)</sup> Quantitative resist models extend the Dill model to two-photon absorption with initiator depletion, \\( \\partial [\\mathrm{Init}]/\\partial t = -C_{\\mathrm{Dill}} \\cdot I^{2}(x,y,z) \\cdot [\\mathrm{Init}] \\), and add oxygen quenching and radical self-termination terms before a Mack-type development step converts the polymerization profile into the final binary structure.<sup>[10](https://proceedings.spiedigitallibrary.org/journals/journal-of-micro-nanopatterning-materials-and-metrology/volume-25/issue-3/031602/Differentiable-forward-modeling-and-inverse-lithography-for-two-photon-lithography/10.1117/1.JMM.25.3.031602.full)</sup>\n\nFeature sizes have improved by roughly a factor of 40, from about 0.2 μm linewidths in early direct writing to 5 nm in new-generation direct writing based on nonlinear laser–matter interaction, comparable to electron beam lithography, without masks or vacuum.<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup> Standard MP3DL reaches 100 nm features.<sup>[1](https://www.nature.com/articles/s43586-025-00386-y)</sup> Reported milestones include 65 nm features with visible-wavelength [multiphoton lithography](https://www.edgepedia.org/multiphoton-lithography), sub-50 nm features with sub-10 fs pulses, and a 9 nm feature size with two-beam optical beam lithography.<sup>[1](https://www.nature.com/articles/s43586-025-00386-y)</sup><sup> • </sup><sup>[6](https://doi.org/10.1038/ncomms3061)</sup> On inorganic substrates, carefully adjusted DLW parameters produce semiconductor surface features as small as about 10 nm, more than an order of magnitude below the far-field optical diffraction limit.<sup>[7](https://iopscience.iop.org/article/10.1088/1361-648X/ae786d)</sup> The limits are set by diffraction in single-photon systems and by reaction thresholds and nonlinear confinement in multiphoton systems.<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup><sup> • </sup><sup>[9](https://pubs.aip.org/aip/jap/article/58/9/3649/173716/Submicrometer-resolution-etching-of-integrated)</sup>\n\n## How it is done\n\nThe workflow runs from a CAD design, converted to STL, through slicing into layers and scan paths, to layer-by-layer polymerization and development.<sup>[11](https://pubs.rsc.org/no/content/articlehtml/2025/tc/d5tc02037a?page=search)</sup> A direct-write system typically comprises a femtosecond laser modulated by an acousto-optic modulator, beam expansion and collimation, a scanning galvanometer, a dynamic focusing module, a precision motion stage, real-time monitoring, and environmental control.<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup>\n\nA representative commercial setup uses a 780 nm Er-fiber frequency-doubled laser with 150 fs pulses at 100 MHz, an inverted microscope, a piezo XYZ stage, a 100× NA = 1.4 oil-immersion objective, and the negative resist IP-L.<sup>[12](https://reference-global.com/download/article/10.2478/lpts-2014-0026.pdf)</sup> Ti:sapphire oscillators tunable over 690–1040 nm are considered ideal excitation sources.<sup>[3](https://www.cell.com/iscience/pdf/S2589-0042%2823%2900451-0.pdf)</sup> Resists must be optically transparent at the writing wavelength, UV-curable, and preferably have a large two-photon absorption cross-section; negative-tone choices include the IP-series, PETIA, SU-8, and Ormocer.<sup>[4](https://iopscience.iop.org/article/10.1088/2631-7990/ad943e)</sup> Compact alternatives exist: a monolithically integrated mode-locked diode laser at 777 nm with 7.7 ps pulses and a 13.2 GHz repetition rate reaches 23 GW/cm² peak intensity with a 1.45 NA objective and writes complex 3D structures at up to 100 mm/s.<sup>[13](https://www.light-am.com/en/article/doi/10.37188/lam.2026.117)</sup>\n\n## Origin\n\nSpatial-light-modulator-based optical direct write traces to work on the deformable mirror device published in Optical Engineering in 1983 by Dennis R. Pape and Larry J. Hornbeck.<sup>[14](https://doi.org/10.1117/12.7973222)</sup> For three-dimensional writing, Maruo, Nakamura, and Kawata reported three-dimensional microfabrication with two-photon-absorbed photopolymerization in Optics Letters in 1997.<sup>[15](https://doi.org/10.1364/ol.22.000132)</sup>\n\n## Variants\n\n**Laser direct-write lithography** exposes patterns point-by-point or line-by-line with a focused beam, UV continuous-wave or femtosecond pulsed; its resolution depends on the focused spot size.<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup> Direct laser writing also divides by material outcome: subtractive DLW removes deposited material by ablation or etching, additive DLW synthesizes and patterns material from precursors, and transformative DLW converts material chemically or structurally without ablation.<sup>[16](https://advanced.onlinelibrary.wiley.com/doi/10.1002/adma.202402014)</sup>\n\n**Two-photon polymerization (2PP)**, a common type of MP3DL, builds true free-form 3D geometries voxel by voxel, reaching 100 nm feature sizes.<sup>[1](https://www.nature.com/articles/s43586-025-00386-y)</sup> Fischer and Wegener reviewed three-dimensional optical laser lithography beyond the diffraction limit in Laser & Photonics Review in 2012.<sup>[17](https://doi.org/10.1002/lpor.201100046)</sup> Gan and colleagues reported three-dimensional deep sub-diffraction optical beam lithography with 9 nm feature size in [Nature Communications](https://www.edgepedia.org/nature-communications) in 2013.<sup>[6](https://doi.org/10.1038/ncomms3061)</sup> Hahn and colleagues demonstrated high-throughput parallelized MP3DL using a static diffractive optical element in Advanced Functional Materials in 2020,<sup>[18](https://doi.org/10.1002/adfm.201907795)</sup> and Skliutas and colleagues reported X-photon laser direct write 3D nanolithography, with exposure-wavelength-independent writing in SZ2080, in Virtual and Physical Prototyping in 2023.<sup>[19](https://doi.org/10.1080/17452759.2023.2228324)</sup> In 2025, Gu and colleagues demonstrated 3D nanolithography with metalens arrays and spatially adaptive illumination in Nature.<sup>[20](https://doi.org/10.1038/s41586-025-09842-x)</sup>\n\n**Laser interference lithography** combines two or more coherent beams whose periodic intensity maxima and minima expose the resist; two-beam interference yields one-dimensional gratings, and rotating the sample by 90 degrees and repeating produces ordered 2D arrays of islands or holes, while metal-coated gratings support surface plasmon–polaritons for photonics and sensing.<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup><sup> • </sup><sup>[7](https://iopscience.iop.org/article/10.1088/1361-648X/ae786d)</sup> **Direct laser interference patterning** textures surfaces by melting or ablating the material and has been used extensively on steel, aluminum, copper, and nickel.<sup>[21](https://pmc.ncbi.nlm.nih.gov/articles/PMC11501624/)</sup> **Ablation and radical etching** are the subtractive branch: ultraviolet laser-induced radical etching with laser-generated atomic fluorine demonstrated submicrometer-resolution patterning of refractory metal/insulator and semiconductor/insulator combinations.<sup>[9](https://pubs.aip.org/aip/jap/article/58/9/3649/173716/Submicrometer-resolution-etching-of-integrated)</sup>\n\n## Applications\n\n[Two-photon lithography](https://www.edgepedia.org/two-photon-lithography) structures are used in tissue engineering, MEMS, biomedical implants, microfluidics, micro/nano-photonics, and drug delivery.<sup>[3](https://www.cell.com/iscience/pdf/S2589-0042%2823%2900451-0.pdf)</sup> The design freedom of TPL serves photonic crystals, biomedical scaffolds, and metamaterials.<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup> Direct laser writing fabricates functional metallic microstructures,<sup>[22](https://mdpi-res.com/d_attachment/micromachines/micromachines-10-00827/article_deploy/micromachines-10-00827-v2.pdf?version=1575513277)</sup> and femtosecond-laser methods extend to nanophotonics, sensing, optoelectronics, and 4D printing.<sup>[4](https://iopscience.iop.org/article/10.1088/2631-7990/ad943e)</sup> In semiconductor manufacturing, direct writing supports fast pattern modification during device development, when geometries change frequently,<sup>[7](https://iopscience.iop.org/article/10.1088/1361-648X/ae786d)</sup> and laser direct writing of interconnections during development is cheaper than a classical optical mask and permits layout adjustment before an expensive final mask is made.<sup>[23](https://hal.science/jpa-00249394v1/document)</sup> Žukauskas and colleagues reported tuning the refractive index during 3D direct laser writing toward gradient-index (GRIN) micro-optics in Laser & Photonics Review in 2015.<sup>[24](https://doi.org/10.1002/lpor.201500170)</sup>\n\n## Limitations and alternatives\n\nThe main limitation of serial multiphoton writing is throughput: point-by-point scanning means macroscale structures can take hours or days, unsuitable for mass production, and polymerization shrinkage can deform final structures.<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup> Commercial maskless direct write reflects the same constraint: the DWL66+ handles linewidths above about 500 nm (300 nm minimum feature) with ≤100 nm overlay at 3 mm²/min, and is often used for proofing during trial production because of low throughput and poor cost-performance ratio at scale.<sup>[5](https://en.omedasemi.com/detail/218.html)</sup>\n\nAgainst alternatives: electron-beam lithography offers nanometer-scale precision but is constrained by low throughput and difficulty processing resists on non-planar surfaces;<sup>[7](https://iopscience.iop.org/article/10.1088/1361-648X/ae786d)</sup> nanoimprint lithography reaches low-nanometer resolution and generally higher throughput for replicated patterns, while TPA-based laser systems offer sub-micron resolution with maskless design flexibility and convenient digital prototyping;<sup>[16](https://advanced.onlinelibrary.wiley.com/doi/10.1002/adma.202402014)</sup> and two-photon lithography needs no mask, mold, or stamp and no vacuum or cleanroom.<sup>[11](https://pubs.rsc.org/no/content/articlehtml/2025/tc/d5tc02037a?page=search)</sup>\n\nFailure modes include the optical proximity effect, where the finite spot size and non-uniform field intensity make each pixel's exposure dose depend on surrounding pixels;<sup>[2](https://link.springer.com/article/10.1007/s44275-026-00046-7)</sup> ablation damage, since nanosecond and picosecond pulses cause molten ejecta, recast layers, micro-cracks, and larger heat-affected zones while femtosecond ablation induces minimal damage;<sup>[4](https://iopscience.iop.org/article/10.1088/2631-7990/ad943e)</sup> and the general drawbacks of TPL: low processing speed, a limited selection of commercially available resists and a need for further material development, low processing volume, and low dynamic range.<sup>[3](https://www.cell.com/iscience/pdf/S2589-0042%2823%2900451-0.pdf)</sup> The dominant recent trend is parallel throughput: 2024 brought holographic multi-foci high-speed scanning and ultrahigh-printing-speed photoresists,<sup>[1](https://www.nature.com/articles/s43586-025-00386-y)</sup> and in 2025 a 12-cm² metalens array produced more than 120,000 cooperative focal spots, a throughput exceeding \\( 10^{8} \\) voxels per second, with parallel printing of more than 50 million microparticles per day, centimeter-scale architectures with features down to 113 nm, and a spatial light modulator for greyscale linewidth modulation.<sup>[20](https://doi.org/10.1038/s41586-025-09842-x)</sup> On the modeling side, differentiable forward modeling and inverse lithography for two-photon lithography now allow calibrated, gradient-based correction of the written pattern.<sup>[10](https://proceedings.spiedigitallibrary.org/journals/journal-of-micro-nanopatterning-materials-and-metrology/volume-25/issue-3/031602/Differentiable-forward-modeling-and-inverse-lithography-for-two-photon-lithography/10.1117/1.JMM.25.3.031602.full)</sup>\n\n## References\n\n1. [Multiphoton 3D lithography | Nature Reviews Methods Primers](https://www.nature.com/articles/s43586-025-00386-y)\n2. [Maskless photolithography for micro- and nanofabrication (Moore and More)](https://link.springer.com/article/10.1007/s44275-026-00046-7)\n3. [S2589 0042(23)00451 0 (cell.com)](https://www.cell.com/iscience/pdf/S2589-0042%2823%2900451-0.pdf)\n4. [Femtosecond laser micro/nano processing: from fundamental to applications](https://iopscience.iop.org/article/10.1088/2631-7990/ad943e)\n5. [Comparison of contact lithography, stepper lithography, laser direct writing, electron beam lithography, and nanoimprint lithography](https://en.omedasemi.com/detail/218.html)\n6. [Zongsong Gan and colleagues (2013). Three-dimensional deep sub-diffraction optical beam lithography with 9 nm feature size. Nature Communications.](https://doi.org/10.1038/ncomms3061)\n7. [Advances in laser-based lithography and processing of semiconductors and insulators](https://iopscience.iop.org/article/10.1088/1361-648X/ae786d)\n8. [Laser generated microstructures | Applied Physics A](https://link.springer.com/article/10.1007/BF00617497)\n9. [Submicrometer-resolution etching of integrated circuit materials with laser-generated atomic fluorine](https://pubs.aip.org/aip/jap/article/58/9/3649/173716/Submicrometer-resolution-etching-of-integrated)\n10. [Differentiable forward modeling and inverse lithography for two-photon lithography (J. Micro/Nanopattern. Mater. Metrology 25(3), 031602, 2026)](https://proceedings.spiedigitallibrary.org/journals/journal-of-micro-nanopatterning-materials-and-metrology/volume-25/issue-3/031602/Differentiable-forward-modeling-and-inverse-lithography-for-two-photon-lithography/10.1117/1.JMM.25.3.031602.full)\n11. [Two-photon polymerization-assisted 3D laser nanoprinting: from fundamentals to modern applications (J. Mater. Chem. C)](https://pubs.rsc.org/no/content/articlehtml/2025/tc/d5tc02037a?page=search)\n12. [Latvian Journal of Physics and Technical Sciences 2014, N 5 (direct laser writing experimental)](https://reference-global.com/download/article/10.2478/lpts-2014-0026.pdf)\n13. [Compact diode laser-based multi-photon polymerization system for 3D microfabrication](https://www.light-am.com/en/article/doi/10.37188/lam.2026.117)\n14. [Dennis R. Pape, Larry J. Hornbeck (1983). Characteristics Of The Deformable Mirror Device For Optical Information Processing. Optical Engineering.](https://doi.org/10.1117/12.7973222)\n15. [Shoji Maruo, Osamu Nakamura, Satoshi Kawata (1997). Three-dimensional microfabrication with two-photon-absorbed photopolymerization. Optics Letters.](https://doi.org/10.1364/ol.22.000132)\n16. [Direct Laser Writing: From Materials Synthesis and Conversion to Electronic Device Processing](https://advanced.onlinelibrary.wiley.com/doi/10.1002/adma.202402014)\n17. [Joachim Fischer, Martin Wegener (2012). Three‐dimensional optical laser lithography beyond the diffraction limit. Laser & Photonics Review.](https://doi.org/10.1002/lpor.201100046)\n18. [Vincent Hahn and colleagues (2020). Rapid Assembly of Small Materials Building Blocks (Voxels) into Large Functional 3D Metamaterials. Advanced Functional Materials.](https://doi.org/10.1002/adfm.201907795)\n19. [Edvinas Skliutas and colleagues (2023). X-photon laser direct write 3D nanolithography. Virtual and Physical Prototyping.](https://doi.org/10.1080/17452759.2023.2228324)\n20. [Songyun Gu and colleagues (2025). 3D nanolithography with metalens arrays and spatially adaptive illumination. Nature.](https://doi.org/10.1038/s41586-025-09842-x)\n21. [Structuring and functionalization of non-metallic materials using direct laser interference patterning: a review](https://pmc.ncbi.nlm.nih.gov/articles/PMC11501624/)\n22. [Functional Metallic Microstructures via Direct Laser Writing (review, Micromachines)](https://mdpi-res.com/d_attachment/micromachines/micromachines-10-00827/article_deploy/micromachines-10-00827-v2.pdf?version=1575513277)\n23. [Laser Beam Lithography for Direct Patterning of Interconnections on Prediffused ASIC's](https://hal.science/jpa-00249394v1/document)\n24. [Albertas Žukauskas and colleagues (2015). Tuning the refractive index in 3D direct laser writing lithography: towards GRIN microoptics. Laser & Photonics Review.](https://doi.org/10.1002/lpor.201500170)\n\n---\n*Topic: Encyclopedia › Technology and the built world › Engineering and manufacturing › Manufacturing processes and fabrication*\n\n*Initially written Sep 29, 2026 · Edited: Oct 15, 2026*\n\n*Copyright 2026 EdgeChat AI, a subsidiary of Biostate AI.*\n\nLicense: Edgepedia Community License 1.0, https://www.edgepedia.org/edgepedia/license\n",
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 "speakable": "Laser lithography is a maskless microfabrication technique that uses a focused laser beam to pattern photoresists and substrates directly, from nanometer features to centimeter-scale 3D structures."
}
