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Dive into the research topics where A. Bayramian is active.

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Featured researches published by A. Bayramian.


Fusion Science and Technology | 2007

The mercury project : A high average power, gas-cooled laser for inertial fusion energy development

A. Bayramian; P. Armstrong; E. Ault; R. J. Beach; C. Bibeau; John A. Caird; R. Campbell; B. Chai; Jay W. Dawson; Christopher A. Ebbers; Alvin C. Erlandson; Y. Fei; Barry L. Freitas; R. Kent; Z. Liao; Tony Ladran; Joseph A. Menapace; B. Molander; Stephen A. Payne; N. Peterson; M. Randles; Kathleen I. Schaffers; S. Sutton; John B. Tassano; S. Telford; E. Utterback

Abstract Hundred-joule, kilowatt-class lasers based on diode-pumped solid-state technologies, are being developed worldwide for laser-plasma interactions and as prototypes for fusion energy drivers. The goal of the Mercury Laser Project is to develop key technologies within an architectural framework that demonstrates basic building blocks for scaling to larger multi-kilojoule systems for inertial fusion energy (IFE) applications. Mercury has requirements that include: scalability to IFE beamlines, 10 Hz repetition rate, high efficiency, and 109 shot reliability. The Mercury laser has operated continuously for several hours at 55 J and 10 Hz with fourteen 4 × 6 cm2 ytterbium doped strontium fluoroapatite amplifier slabs pumped by eight 100 kW diode arrays. A portion of the output 1047 nm was converted to 523 nm at 160 W average power with 73 % conversion efficiency using yttrium calcium oxy-borate (YCOB).


Journal of The Optical Society of America B-optical Physics | 2008

High-average-power femto-petawatt laser pumped by the Mercury laser facility

A. Bayramian; James P. Armstrong; Glenn Beer; R. Campbell; Bruce H. T. Chai; Robert R. Cross; Alvin C. Erlandson; Yting Fei; Barry L. Freitas; Robert Kent; Joseph A. Menapace; William A. Molander; Kathleen I. Schaffers; C. W. Siders; S. Sutton; John B. Tassano; Steve Telford; Christopher A. Ebbers; John A. Caird; C. P. J. Barty

The Mercury laser system is a diode-pumped solid-state laser that has demonstrated over 60 J at a repetition rate of 10 Hz (600 W) of near-infrared light (1047 nm). Using a yttrium calcium oxyborate frequency converter, we have demonstrated 31.7 J/pulse at 10 Hz of second harmonic generation. The frequency converted Mercury laser system will pump a high-average-power Ti:sapphire chirped pulse amplifier system that will produce a compressed peak power > 1 PW and peak irradiance > 1023W/cm2.


Fusion Science and Technology | 2011

Compact, Efficient Laser Systems Required for Laser Inertial Fusion Energy

A. Bayramian; S. Aceves; T. Anklam; K. Baker; E. Bliss; C. Boley; A. Bullington; John A. Caird; D. Chen; R. Deri; Mike Dunne; Alvin C. Erlandson; D. Flowers; Mark A. Henesian; Jeffery F. Latkowski; Kenneth R. Manes; William A. Molander; E. I. Moses; T. Piggott; S. Powers; S. Rana; S. Rodriguez; R. Sawicki; Kathleen I. Schaffers; L. Seppala; M. Spaeth; S. Sutton; S. Telford

Abstract This paper presents our conceptual design for laser drivers used in Laser Inertial Fusion Energy (LIFE) power plants. Although we have used only modest extensions of existing laser technology to ensure near-term feasibility, predicted performance meets or exceeds plant requirements: 2.2 MJ pulse energy produced by 384 beamlines at 16 Hz, with 18% wall-plug efficiency. High reliability and maintainability are achieved by mounting components in compact line-replaceable units that can be removed and replaced rapidly while other beamlines continue to operate, at up to ˜13% above normal energy, to compensate for neighboring beamlines that have failed. Statistical modeling predicts that laser-system availability can be greater than 99% provided that components meet reasonable mean-time-between-failure specifications.


Applied Physics B | 1995

Laser properties of a new average-power Nd-doped phosphate glass

Steve Payne; Christopher D. Marshall; A. Bayramian; Gary D. Wilke; J. S. Hayden

The Nd-doped phosphate laser glass described herein can withstand 2.3 times greater thermal loading without fracture, compared to APG-1 (commercially available Average-Power Glass from Schott Glass Technologies). The enhanced thermal loading capability is established on the basis of the intrinsic thermomechanical properties (expansion, conduction, fracture toughness, and Youngs modulus), and by direct thermally induced fracture experiments using Ar-ion laser heating of the samples. This Nd-doped phosphate glass (referred to as APG-t) is found to be characterized by a 29% lower gain cross section and a 25% longer low-concentration emission lifetime. Other measurements pertaining to the concentration quenching, thermal lensing, and saturation of the extraction are also described in this article. It is note-worthy that APG-t offers increased bandwidth near the peak of the 1054 nm gain spectrum, suggesting that this material may have special utility as a means of generating and amplifying ultrashort pulses of light.


Optical Materials Express | 2011

Comparison of Nd:phosphate glass, Yb:YAG and Yb:S-FAP laser beamlines for laser inertial fusion energy (LIFE) [Invited]

Alvin C. Erlandson; S. Aceves; A. Bayramian; Amber L. Bullington; Raymond J. Beach; C. D. Boley; John A. Caird; Robert J. Deri; A. M. Dunne; D. Flowers; Mark A. Henesian; Kenneth R. Manes; E. I. Moses; S. Rana; Kathleen I. Schaffers; M. Spaeth; C. J. Stolz; S. J. Telford

We present the results of performance modeling of diode-pumped solid state laser beamlines designed for use in Laser Inertial Fusion Energy (LIFE) power plants. Our modeling quantifies the efficiency increases that can be obtained by increasing peak diode power and reducing pump-pulse duration, to reduce decay losses. At the same efficiency, beamlines that use laser slabs of Yb:YAG or Yb:S-FAP require lower diode power than beamlines that use laser slabs of Nd:phosphate glass, since Yb:YAG and Yb:S-FAP have longer storage lifetimes. Beamlines using Yb:YAG attain their highest efficiency at a temperature of about 200K. Beamlines using Nd:phosphate glass or Yb:S-FAP attain high efficiency at or near room temperature.


Fusion Science and Technology | 2011

Timely Delivery of Laser Inertial Fusion Energy (LIFE)

Mike Dunne; E. I. Moses; Peter A. Amendt; Thomas M. Anklam; A. Bayramian; E. Bliss; B. Debs; R. Deri; T. Diaz de la Rubia; Bassem S. El-Dasher; Joseph C. Farmer; D. Flowers; Kevin J. Kramer; L. Lagin; J.F. Latkowski; J. D. Lindl; Wayne R. Meier; Robin Miles; Gregory A. Moses; S. Reyes; V. Roberts; R. Sawicki; M. Spaeth; E. Storm

Abstract The National Ignition Facility (NIF), the world’s largest and most energetic laser system, is now operational at Lawrence Livermore National Laboratory. A key goal of the NIF is to demonstrate fusion ignition for the first time in the laboratory. Its flexibility allows multiple target designs (both indirect and direct drive) to be fielded, offering substantial scope for optimization of a robust target design. In this paper we discuss an approach to generating gigawatt levels of electrical power from a laser-driven source of fusion neutrons based on these demonstration experiments. This “LIFE” concept enables rapid time-to-market for a commercial power plant, assuming success with ignition and a technology demonstration program that links directly to a facility design and construction project. The LIFE design makes use of recent advances in diode-pumped, solid-state laser technology. It adopts the paradigm of Line Replaceable Units utilized on the NIF to provide high levels of availability and maintainability and mitigate the need for advanced materials development. A demonstration LIFE plant based on these design principles is described, along with the areas of technology development required prior to plant construction.


Journal of Luminescence | 1996

Ce : LiSrAlF6 laser performance with antisolarant pump beam

A. Bayramian; Christopher D. Marshall; J.H. Wu; Joel A. Speth; Stephen A. Payne; Gregory J. Quarles; V.K. Castillo

Abstract We have explored the impact of 266 nm pump-induced solarization on the 290 nm laser performance of Ce: LiSrAlF 6 crystals. Among the issues considered are the incorporation of codopants (e.g. Na + , Mg 2+ , Zn 2+ ), and the use of an additional 532 nm beam to rapidly destroy the interfering color centers. The solarization mechanism has been unraveled and found to involve two-photon creation of color centers (via the 4f→ 5d→ conduction band pathway of Ce 3+ ), followed by the one-photon bleaching of the color centers. Ce : LiSrAlF 6 (Ce : LiSAF) laser slope efficiencies as high as 47% can be achieved with the simultaneous introduction of the 266 nm pump and 532 nm bleaching beams; 33% with the 266 nm beam only.


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


IEEE Journal of Quantum Electronics | 1999

Characterization of Yb/sup 3+/:Sr/sub 5-x/Ba/sub x/(PO/sub 4/)/sub 3/F crystals for diode-pumped lasers

A. Bayramian; Christopher D. Marshall; Kathleen I. Schaffers; Stephen A. Payne

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


Proceedings of SPIE | 2015

ELI-Beamlines: development of next generation short-pulse laser systems

Bedrich Rus; P. Bakule; D. Kramer; J. Naylon; J. Thoma; J. T. Green; R. Antipenkov; M. Fibrich; J. Novák; F. Batysta; T. Mazanec; M. A. Drouin; K. Kasl; R. Baše; D. Peceli; L. Koubíková; P. Trojek; R. Boge; J. C. Lagron; Š. Vyhlídka; J. Weiss; J. Cupal; J. Hřebíček; P. Hříbek; M. Durák; J. Polan; M. Košelja; G. Korn; M. Horáček; J. Horáček

Ytterbium-doped Sr/sub 5/(PO/sub 4/)/sub 3/F (S-FAP) has been shown to be a useful material for diode pumping, since it displays high gain, low loss, and a long radiative lifetime. One of the issues with S-FAP is that it has a relatively narrow absorption bandwidth (/spl sim/5 nm) at 900 nm, the diode-pumping wavelength, while the diodes output bandwidth can be large (/spl sim/10 nm). By changing the host slightly, the absorption feature can be broadened to better match the pump bandwidth. Four mixed crystal boules of Yb/sup 3+/:Sr/sub 5-x/Ba/sub x/(PO/sub 4/)/sub 3/F were grown by the Czochralski method with x=0.25: 0.5, 1, and 2. The bandwidth of the 900-nm absorption feature was found to grow with increasing barium concentration from 4.7 nm to a maximum of 15.9 nm. Emission spectra showed a similar bandwidth increase with barium content from 4.9 nm to a maximum of 10 nm. Emission cross sections for these materials were deduced by the methods of reciprocity, the Einstein method, and small-signal gain. The absorption features homogeneity was probed using a tunable pump source which qualitatively showed that the barium broadened lines were at least partly inhomogeneous. Each of these materials lased with a variety of output couplers. This family of materials was found to provide suitable laser hosts where a broader absorption and/or emission bandwidth is desired.

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Kathleen I. Schaffers

Lawrence Livermore National Laboratory

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Christopher A. Ebbers

Lawrence Livermore National Laboratory

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Christopher D. Marshall

Lawrence Livermore National Laboratory

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C. Bibeau

Lawrence Livermore National Laboratory

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Barry L. Freitas

Lawrence Livermore National Laboratory

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S. Sutton

Lawrence Livermore National Laboratory

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Stephen A. Payne

Lawrence Livermore National Laboratory

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John A. Caird

Lawrence Livermore National Laboratory

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Alvin C. Erlandson

Lawrence Livermore National Laboratory

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S. Telford

Lawrence Livermore National Laboratory

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