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Dive into the research topics where Eddy A. Stappaerts is active.

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Featured researches published by Eddy A. Stappaerts.


Optics Express | 2008

Analysis of the scalability of diffraction-limited fiber lasers and amplifiers to high average power

Jay W. Dawson; Michael J. Messerly; Raymond J. Beach; Miroslav Y. Shverdin; Eddy A. Stappaerts; Arun Kumar Sridharan; Paul H. Pax; John E. Heebner; Craig W. Siders; C. P. J. Barty

We analyze the scalability of diffraction-limited fiber lasers considering thermal, non-linear, damage and pump coupling limits as well as fiber mode field diameter (MFD) restrictions. We derive new general relationships based upon practical considerations. Our analysis shows that if the fibers MFD could be increased arbitrarily, 36 kW of power could be obtained with diffraction-limited quality from a fiber laser or amplifier. This power limit is determined by thermal and non-linear limits that combine to prevent further power scaling, irrespective of increases in mode size. However, limits to the scaling of the MFD may restrict fiber lasers to lower output powers.


Fusion Science and Technology | 2009

ND:GLASS LASER DESIGN FOR LASER ICF FISSION ENERGY (LIFE)

John A. Caird; Vivek Agrawal; A. Bayramian; Ray Beach; J.A. Britten; Diana Chen; Robert R. Cross; Christopher A. Ebbers; Alvin C. Erlandson; Michael D. Feit; Barry L. Freitas; Chuni Ghosh; C. Haefner; Doug Homoelle; Tony Ladran; Jeff Latkowski; William A. Molander; J. R. Murray; Sasha Rubenchik; Kathleen I. Schaffers; Craig W. Siders; Eddy A. Stappaerts; S. Sutton; Steve Telford; John B. Trenholme; Christopher Barty

Abstract We have developed preliminary conceptual laser system designs for the Laser ICF (Inertial Confinement Fusion) Fission Energy (LIFE) application. Our approach leverages experience in high-energy Nd: glass laser technology developed for the National Ignition Facility (NIF)1, along with high-energy-class diode-pumped solid-state laser (HEC-DPSSL) technology developed for the DOE’s High Average Power Laser (HAPL) Program and embodied LLNL’s Mercury laser system.2 We present laser system designs suitable for both indirect-drive, hot spot ignition and indirect-drive, fast ignition targets. Main amplifiers for both systems use laser-diode-pumped Nd:glass slabs oriented at Brewster’s angle, as in NIF, but the slabs are much thinner to allow for cooling by high-velocity helium gas as in the Mercury laser system. We also describe a plan to mass-produce pump-diode lasers to bring diode costs down to the order of


Optics Letters | 2004

High-speed horizontal-path atmospheric turbulence correction with a large-actuator-number microelectromechanical system spatial light modulator in an interferometric phase-conjugation engine

K. L. Baker; Eddy A. Stappaerts; Donald T. Gavel; S. C. Wilks; J. Tucker; Dennis A. Silva; J. Olsen; S. Olivier; P. E. Young; M. Kartz; Laurence M. Flath; P. Kruelevitch; J. Crawford; Oscar Azucena

0.01 per Watt of peak output power, as needed to make the LIFE application economically attractive.


Optics Letters | 2006

A single-shot pixellated phase-shifting interferometer utilizing a liquid-crystal spatial light modulator

K. L. Baker; Eddy A. Stappaerts

Results of atmospheric propagation for a high-speed, large-actuator-number adaptive optics system are presented. The system uses a microelectromechanical system- (MEMS-) based spatial light modulator correction device with 1024 actuators. Tests over a 1.35-km path achieved correction speeds in excess of 800 Hz and Strehl ratios close to 0.5. The wave-front sensor was based on a quadrature interferometer that directly measures phase. This technique does not require global wave-front reconstruction, making it relatively insensitive to scintillation and phase residues. The results demonstrate the potential of large-actuator-number MEMS-based spatial light modulators to replace conventional deformable mirrors.


Optics Express | 2009

Interferometric adaptive optics testbed for laser pointing, wave-front control and phasing

K. L. Baker; Doug Homoelle; E. Utternback; Eddy A. Stappaerts; C. W. Siders; C. P. J. Barty

We introduce a novel phase-shifting pixellated interferometer based on a liquid-crystal spatial light modulator and simulate the expected performance. The phase-shifted frames are captured simultaneously, which reduces problems arising from vibrations and air turbulence. The liquid-crystal spatial light modulator is flexible and can be configured to provide a large number of phase-shift levels and geometries to reduce measurement error.


Optics Letters | 2004

Open- and closed-loop aberration correction by use of a quadrature interferometric wave-front sensor

K. L. Baker; Eddy A. Stappaerts; S. C. Wilks; P. E. Young; Donald T. Gavel; J. Tucker; Dennis A. Silva; Scot S. Olivier

Implementing the capability to perform fast ignition experiments, as well as, radiography experiments on the National Ignition Facility (NIF) places stringent requirements on the control of each of the beams pointing, intra-beam phasing and overall wave-front quality. In this article experimental results are presented which were taken on an interferometric adaptive optics testbed that was designed and built to test the capabilities of such a system to control phasing, pointing and higher order beam aberrations. These measurements included quantification of the reduction in Strehl ratio incurred when using the MEMS device to correct for pointing errors in the system. The interferometric adaptive optics system achieved a Strehl ratio of 0.83 when correcting for a piston, tip/tilt error between two adjacent rectangular apertures, the geometry expected for the National ignition Facility. The interferometric adaptive optics system also achieved a Strehl ratio of 0.66 when used to correct for a phase plate aberration of similar magnitude as expected from simulations of the ARC beam line. All of these corrections included measuring both the upstream and downstream aberrations in the testbed and applying the sum of these two measurements in open-loop to the MEMS deformable mirror.


Optics Letters | 2005

Differential Synthetic Aperture Ladar

Eddy A. Stappaerts; E. T. Scharlemann

Experimental results are presented for an adaptive optics system based on a quadrature Twyman-Green interferometric wave-front sensor. The system uses a circularly polarized reference beam to form two interferograms with a pi/2 phase shift. The experiments conducted used Kolmogorov phase screens to simulate atmospheric phase distortions. Strehl ratio improvements by a factor of 8, to an absolute value of 0.45, are demonstrated.


Journal of Micro-nanolithography Mems and Moems | 2009

Interferometric adaptive optics for high-power laser pointing and wavefront control and phasing

K. L. Baker; Eddy A. Stappaerts; Doug Homoelle; Mark A. Henesian; Erlan S. Bliss; C. W. Siders; C. P. J. Barty

We report a differential synthetic aperture ladar concept that relaxes platform and laser requirements compared with those for conventional synthetic aperture ladar. Line-of-sight translation-vibration constraints are reduced by several orders of magnitude, while laser frequency stability is typically relaxed by an order of magnitude. The technique is most advantageous for shorter laser wavelengths, ultraviolet to mid-infrared. Analytical and modeling results, including the effect of speckle and atmospheric turbulence, are presented.


Optics Letters | 2004

Performance of a phase-conjugate engine implementing a finite-bit phase correction

K. L. Baker; Eddy A. Stappaerts; S. C. Wilks; Donald T. Gavel; P. E. Young; J. Tucker; S. Olivier; Dennis A. Silva; J. Olsen

Implementing the capability to perform fast ignition experiments, as well as, radiography experiments on the National Ignition Facility (NIF) places stringent requirements on the control of each of the beams pointing and overall wavefront quality. One quad of the NIF beams, four beam pairs, will be utilized for these experiments and hydrodynamic and particle-in-cell simulations indicate that for the fast ignition experiments, these beams will be required to deliver 50% (4.0 kJ) of their total energy (7.96 kJ) within a 40-µm-diam spot at the end of a fast ignition cone target. This requirement implies a stringent pointing and overall phase conjugation error budget on the adaptive optics system used to correct these beam lines. The overall encircled energy requirement is more readily met by phasing of the beams in pairs but still requires high Strehl ratios and root-mean-square tip/tilt errors of approximately 1 µrad. To accomplish this task we have designed an interferometric adaptive optics system capable of beam pointing, high Strehl ratio, and beam phasing with a single pixilated microelectromechanical systems deformable mirror and interferometric wavefront sensor. We present the design of a testbed used to evaluate the performance of this wavefront sensor along with simulations of its expected performance level.


Applied Optics | 2004

Breadboard testing of a phase-conjugate engine with an interferometric wave-front sensor and a microelectromechanical systems-based spatial light modulator

K. L. Baker; Eddy A. Stappaerts; Donald T. Gavel; S. C. Wilks; J. Tucker; Dennis A. Silva; J. Olsen; Scot S. Olivier; P. E. Young; Mike W. Kartz; Laurence M. Flath; Peter Krulevitch; Jackie Crawford; Oscar Azucena

The achievable Strehl ratio when a finite-bit correction to an aberrated wave front is implemented is examined. The phase-conjugate engine used to measure the aberrated wave front consists of a quadrature interferometric wave-front sensor, a liquid-crystal spatial light modulator, and computer hardware-software to calculate and apply the correction. A finite-bit approximation to the conjugate phase is calculated and applied to the spatial light modulator to remove the aberrations from the optical beam. The experimentally determined Strehl ratio of the corrected beam is compared with analytical expressions for the expected Strehl ratio and shown to be in good agreement with those predictions.

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K. L. Baker

Lawrence Livermore National Laboratory

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S. C. Wilks

Lawrence Livermore National Laboratory

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Donald T. Gavel

Lawrence Livermore National Laboratory

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Dennis A. Silva

Lawrence Livermore National Laboratory

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J. Tucker

Lawrence Livermore National Laboratory

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C. P. J. Barty

Lawrence Livermore National Laboratory

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J. Olsen

Lawrence Livermore National Laboratory

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P. E. Young

Lawrence Livermore National Laboratory

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Scot S. Olivier

Lawrence Livermore National Laboratory

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C. W. Siders

Lawrence Livermore National Laboratory

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