J. Goodberlet
Massachusetts Institute of Technology
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Featured researches published by J. Goodberlet.
Optics Letters | 1989
J. Goodberlet; J. Wang; James G. Fujimoto; Schulz Pa
Ultrashort pulses are generated in a Ti:Al(2)O(3) laser by using a coupled nonlinear external cavity. The external cavity uses self-phase modulation in an optical fiber to achieve passive mode locking without the need for synchronous pumping or acousto-optic modulation. A stable train of chirped 1.4-psec pulses is generated. After dispersive compensation, pulses as short as 200 fsec are obtained.
Applied Physics Letters | 2002
J. Goodberlet; Hamide Kavak
Sub-50 nm lines, holes, and posts have been patterned photolithographically using near-field embedded-amplitude masks and an exposing wavelength of 220 nm generated by an arc-lamp source. Interference in the optical near field is utilized to produce the fine patterns. In some cases, the feature sizes on the mask are more than six times larger than the size of the smallest features patterned on the substrate. Numerical simulations support the experimental results.
Journal of Vacuum Science & Technology B | 2002
J. T. Hastings; Michael H. Lim; J. Goodberlet; Henry I. Smith
We describe a technique to fabricate Bragg gratings in the sides of optical waveguides using a single lithographic step. This technique is particularly suited to the apodized gratings required for add/drop filters in dense-wavelength-division multiplexing. Apodization minimizes cross talk between channels and improves the filter response. Silicon-on-insulator rib waveguides with both uniform and apodized gratings were fabricated using direct-write spatial-phase-locked electron-beam lithography (SPLEBL). This approach combines SPLEBL’s pattern-placement accuracy with the flexibility of direct-write device prototyping. The resulting grating-based devices exhibited substantially reduced side-lobe levels.
Applied Physics Letters | 2000
J. Goodberlet
The extension of contact photolithography to pattern features at the 100 nm level, and below, is described. Isolated lines, nested L’s, and gratings with 100 nm linewidths are patterned using a conformable embedded-amplitude mask, a trilayer resist stack on the substrate, and a deep-ultraviolet radiation source having a wavelength of λ∼220 nm. A broad exposure latitude of ±21% for a linewidth control of ±10% is measured. Preliminary calculations indicate a practical resolution limit for the lithographic process. The patterning process is reliable and repeatable.
Optics Letters | 1990
J. Goodberlet; J. Wang; James G. Fujimoto; Peter A. Schulz
The starting dynamics of the additive-pulse mode-locked Ti:AI(2)O(3) laser are investigated. Mode locking develops from mode beating with pulse formation times of several hundred microseconds. A simple model based on additivepulse mode-locking theory is developed that describes self-starting and pulse evolution.
Journal of Vacuum Science & Technology B | 2001
J. Goodberlet; J. Todd Hastings; Henry I. Smith
The performance of a Raith 150 electron-beam lithography system is reported. The system’s resolution, stability, intrafield distortion, stitching, and overlay performance are evaluated. Patterning at low- and high-acceleration voltages is compared. The system was used to pattern sub-20 nm features, and the largest intrafield distortion for a 100 μm field was measured to be 15 nm. Pattern-placement accuracy below 35 nm, mean plus twice the standard deviation, was demonstrated.
Applied Physics B | 1993
Santanu Basu; Peter L. Hagelstein; J. Goodberlet; Martin H. Muendel; Sumanth Kaushik
We identified for the first time the 3d94d1S − 3d94p1P line in Ni-like Nb at 204.2 Å that was predicted to show gain. When pumped with a train of pulses containing less than 1 J per pulse, significant emission was recorded at 204.2 Å following the second and the third pulses. We measured the small signal gain coefficient per Joule of incident laser energy to be 1.49±0.42 cm−1 J−1 for this laser transition, which is higher by several orders of magnitude than that reported for other collisional laser systems in this wavelength range.
Journal of Vacuum Science & Technology B | 2000
J. T. Hastings; Feng Zhang; Mark Alan Finlayson; J. Goodberlet; Henry I. Smith
We report a new mode of spatial-phase-locked electron-beam lithography based on alignment of each e-beam deflection field to a fiducial grid on the substrate. Before exposing the pattern in a given field, the fiducial grid is sparsely sampled with the electron beam at a subexposure dose. These samples form a two-dimensional moire pattern that is analyzed to calculate field shift, scale, rotation, nonorthogonality, and trapezoidal distortion. Experimental verification of the approach was carried out with a scintillating fiducial grid quenched by interference lithography. Despite a poor signal-to-noise ratio, we achieved sub-beamstep field-stitching and pattern-placement accuracy.
Journal of Vacuum Science & Technology B | 1997
J. Goodberlet; Juan Ferrera; Henry I. Smith
A delay-locked loop is used in a one-dimensional demonstration of the global-fiducial-grid mode of spatial-phase-locked electron-beam lithography. A pattern-placement precision of σ∼5 nm is demonstrated under nonideal conditions. Results compare well with numerical simulations.
Journal of Vacuum Science & Technology B | 1998
J. Goodberlet; J. M. Carter; Henry I. Smith
An organic scintillator has been developed for use in electron-beam lithography. The scintillator can be deposited in a thin film ( 2) optical signal. It is expected that the signal from this type of grid will improve the pattern-placement precision to within 1 nm when used in conjunction with spatial-phase-locked electron-beam lithography.