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Volumn 324, Issue 5929, 2009, Pages 910-913

Achieving 1/20 resolution by one-color initiation and deactivation of polymerization

Author keywords

[No Author keywords available]

Indexed keywords

DIFFRACTION; FUNDAMENTAL PARTICLE; POLYMER; POLYMERIZATION; WAVELENGTH;

EID: 66149129610     PISSN: 00368075     EISSN: 10959203     Source Type: Journal    
DOI: 10.1126/science.1168996     Document Type: Article
Times cited : (491)

References (27)
  • 2
    • 17144368056 scopus 로고    scopus 로고
    • H. Ito, in Microlithography: Molecular Imprinting (Springer-Verlag, Berlin, 2005), 172, Advances in Polymer Science, pp. 37-245.
    • H. Ito, in Microlithography: Molecular Imprinting (Springer-Verlag, Berlin, 2005), vol. 172, Advances in Polymer Science, pp. 37-245.
  • 4
    • 54249089085 scopus 로고    scopus 로고
    • M. Rumi, S. Barlow, J. Wang, J. W. Perry, S. R. Marder, in Photoresponsive Polymers I (Springer-Verlag, Berlin, 2008), 213, Advances in Polymer Science, pp. 1-95.
    • M. Rumi, S. Barlow, J. Wang, J. W. Perry, S. R. Marder, in Photoresponsive Polymers I (Springer-Verlag, Berlin, 2008), vol. 213, Advances in Polymer Science, pp. 1-95.
  • 12
    • 34249945258 scopus 로고    scopus 로고
    • S. W. Hell, Science 316, 1153 (2007).
    • (2007) Science , vol.316 , pp. 1153
    • Hell, S.W.1
  • 16
    • 67649339968 scopus 로고    scopus 로고
    • Materials and methods are available as supporting material on Science Online.
    • Materials and methods are available as supporting material on Science Online.
  • 17
    • 67649384666 scopus 로고    scopus 로고
    • The maximum delay time of 13 ns is determined by the 76 MHz laser repetition rate.
    • The maximum delay time of 13 ns is determined by the 76 MHz laser repetition rate.
  • 18
    • 67649320456 scopus 로고    scopus 로고
    • Because MAIL from gold nanoparticles is a three-photon process at 800 nm, the images show the cubes of the PSFs.
    • Because MAIL from gold nanoparticles is a three-photon process at 800 nm, the images show the cubes of the PSFs.
  • 20
    • 67649320455 scopus 로고    scopus 로고
    • The deactivation laser was operated in fs pulsed mode for the purpose of measuring its PSF using MAIL but was operated in CW mode for all other experiments. The beam profile and direction did not change measurably in going from pulsed to CW mode, so we expect the PSF to be nearly identical in both modes
    • The deactivation laser was operated in fs pulsed mode for the purpose of measuring its PSF using MAIL but was operated in CW mode for all other experiments. The beam profile and direction did not change measurably in going from pulsed to CW mode, so we expect the PSF to be nearly identical in both modes.
  • 21
    • 67649358398 scopus 로고    scopus 로고
    • All powers were as measured at the sample position
    • All powers were as measured at the sample position.
  • 22
    • 67649358397 scopus 로고    scopus 로고
    • The slight asymmetry of the voxel is due to our use of linearly polarized light for fabrication. See (26).
    • The slight asymmetry of the voxel is due to our use of linearly polarized light for fabrication. See (26).
  • 23
    • 67649320329 scopus 로고    scopus 로고
    • AFM cannot measure reentrant (overhanging) features, so although the voxels appear to be tapered in these images, they are not
    • AFM cannot measure reentrant (overhanging) features, so although the voxels appear to be tapered in these images, they are not.
  • 27
    • 67649384665 scopus 로고    scopus 로고
    • We appreciate the support of the Maryland NanoCenter and its Nanoscale Imaging, Spectroscopy, and Properties Laboratory (NISPLab, NISPLab is supported in part by NSF as a Materials Research Science and Engineering Center (MRSEC) Shared Experimental Facility. This work was supported in part by the UMD-NSF-MRSEC under grant DMR 05-20471. We are grateful to E. Williams for the use of her AFM and to J. Goldhar, Y. Leng, and V. Yun for fabricating the phase mask used in this work. The University of Maryland has filed a provision patent based on the work presented in this paper
    • We appreciate the support of the Maryland NanoCenter and its Nanoscale Imaging, Spectroscopy, and Properties Laboratory (NISPLab). NISPLab is supported in part by NSF as a Materials Research Science and Engineering Center (MRSEC) Shared Experimental Facility. This work was supported in part by the UMD-NSF-MRSEC under grant DMR 05-20471. We are grateful to E. Williams for the use of her AFM and to J. Goldhar, Y. Leng, and V. Yun for fabricating the phase mask used in this work. The University of Maryland has filed a provision patent based on the work presented in this paper.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.