The Z-Backlighter Laser Facility at Sandia National Laboratories was developed to enable high energy density physics experiments in conjunction with the Z Pulsed Power Facility at Sandia National Laboratories, with an emphasis on backlighting. Since the first laser system there became operational in 2001, the facility has continually evolved to add new capability and new missions. The facility currently has several high energy laser systems including the nanosecond/multi-kilojoule Z-Beamlet Laser (ZBL), the sub-picosecond/kilojoule- class Z-Petawatt (ZPW) Laser, and the smaller nanosecond/100 J-class Chaco laser. In addition to these, the backlighting mission requires a regular stream of coated consumable optics such as debris shields and vacuum windows, which led to the development of the Sandia Optics Support Facility to support the unique high damage threshold optical coating needs described.
Q-switch lasers are traditionally modeled using the rate equation approximation[1]. This model is effective in relating
the energy of the population inversion to the energy in the optical pulse. It is especially effective when augmented by the
Frantz-Nodvik theory that effectively builds in conservation of energy. However, the rate equation approximation theory
cannot independently describe the formation of longitudinal modes and, because it does not correctly consider the finite
response time of the medium, its accuracy in predicting the very fast rise time of Q-switch pulses is suspect. A more
powerful based on the laser gain in terms of radiating, resonant dipoles-the coherent gain model-is needed. This paper
reports progress to incorporate the more advanced coherent gain into a 3D, time resolved numerical model that can predict
both sub-nanosecond effects, the growth of longitudinal modes in the Q-switched laser, and other coherent effects. Work
remains to be done to explore the capabilities of this model to its full range of possibilities. Sandia National Laboratories
has been interested in short pulse modeling and provided support for the development of the coherent gain model which is
now being applied to the NASA Q-switch program to address fast rise times and the formation of longitudinal modes[2]-[6].
We discuss upgrades and development currently underway at the Z-Backlighter facility. Among them are a
new optical parametric chirped pulse amplier (OPCPA) front end, 94 cm 42 cm multi layer dielectric (MLD)
gratings, dichroic laser beam transport studies, 25 keV x-ray source development, and a major target area
expansion. These upgrades will pave the way for short/long pulse, multi-frame, multi-color x-ray backlighting
at the Z-Accelerator.
As high energy laser systems evolve towards higher energies, fundamental material properties such as the laserinduced
damage threshold (LIDT) of the optics limit the overall system performance. The Z-Backlighter Laser Facility
at Sandia National Laboratories uses a pair of such kiljoule-class Nd:Phosphate Glass lasers for x-ray radiography of
high energy density physics events on the Z-Accelerator. These two systems, the Z-Beamlet system operating at 527nm/
1ns and the Z-Petawatt system operating at 1054nm/ 0.5ps, can be combined for some experimental applications. In
these scenarios, dichroic beam combining optics and subsequent dual wavelength high reflectors will see a high fluence
from combined simultaneous laser exposure and may even see lingering effects when used for pump-probe
configurations. Only recently have researchers begun to explore such concerns, looking at individual and simultaneous
exposures of optics to 1064 and third harmonic 355nm light from Nd:YAG [1]. However, to our knowledge,
measurements of simultaneous and delayed dual wavelength damage thresholds on such optics have not been performed
for exposure to 1054nm and its second harmonic light, especially when the pulses are of disparate pulse duration.
The Z-Backlighter Facility has an instrumented damage tester setup to examine the issues of laser-induced
damage thresholds in a variety of such situations [2] . Using this damage tester, we have measured the LIDT of dual
wavelength high reflectors at 1054nm/0.5ps and 532nm/7ns, separately and spatially combined, both co-temporal and
delayed, with single and multiple exposures. We found that the LIDT of the sample at 1054nm/0.5ps can be
significantly lowered, from 1.32J/cm2 damage fluence with 1054/0.5ps only to 1.05 J/cm2 with the simultaneous
presence of 532nm/7ns laser light at a fluence of 8.1 J/cm2. This reduction of LIDT of the sample at 1054nm/0.5ps
continues as the fluence of 532nm/7ns laser light simultaneously present increases. The reduction of LIDT does not
occur when the 2 pulses are temporally separated. This paper will also present dual wavelength LIDT results of
commercial dichroic beam-combining optics simultaneously exposed with laser light at 1054nm/2.5ns and 532nm/7ns.
Sandia's Large Optics Coating Operation has extensive results of laser induced damage threshold (LIDT) testing of its
anti-reflection (AR) and high reflection coatings on substrates pitch polished using ceria and washed in a process that
includes an alumina wash step. The purpose of the alumina wash step is to remove residual polishing compound to
minimize its role in laser damage. These LIDT tests are for multi longitudinal mode, ns class pulses at 1064 nm and
532 nm (NIF-MEL protocol) and mode locked, sub-ps class pulses at 1054 nm (Sandia measurements), and show
reasonably high and adequate laser damage resistance for coatings in the beam trains of Sandia's Z-Backlighter terawatt
and petawatt lasers. An AR coating in addition to coatings of our previous reports confirms this with LIDTs of 33.0
J/cm2 for 3.5 ns pulses and 1.8 J/cm2 for 350 fs pulses. In this paper, we investigate both ceria and zirconia in doublesided
polishing (common for large flat Z-Backlighter laser optics) as they affect LIDTs of an AR coating on fused silica
substrates washed with or without the alumina wash step. For these AR coated, double-sided polished surfaces, ceria
polishing in general affords better resistance to laser damage than zirconia polishing and laser damage is less likely with
the alumina wash step than without it. This is supported by specific results of laser damage tests with 3.5 ns, multi
longitudinal mode, single shot pulses at 1064 nm and 532 nm, with 7.0 ns, single and multi longitudinal mode, single
and multi shot pulses at 532 nm, and with 350 fs, mode-locked, single shot pulses at 1054 nm.
Sandia's Large Optics Coating Operation provides laser damage resistant optical coatings on meter-class optics required
for the ZBacklighter Terawatt and Petawatt lasers. Deposition is by electron beam evaporation in a 2.3 m × 2.3 m × 1.8
m temperature controlled vacuum chamber. Ion assisted deposition (IAD) is optional. Coating types range from antireflection
(AR) to high reflection (HR) at S and P polarizations for angle of incidence (AOI) from 0° to 47°.
This paper reports progress in meeting challenges in design and deposition of these high laser induced damage threshold
(LIDT) coatings. Numerous LIDT tests (NIF-MEL protocol, 3.5 ns laser pulses at 1064 nm and 532 nm) on the coatings
confirm that they are robust against laser damage. Typical LIDTs are: at 1064 nm, 45° AOI, Ppol, 79 J/cm2 (IAD 32
layer HR coating) and 73 J/cm2 (non-IAD 32 layer HR coating); at 1064 nm, 32° AOI, 82 J/cm2 (Ppol) and 55 J/cm2
(Spol ) (non-IAD 32 layer HR coating); and at 532 nm, Ppol, 16 J/cm2 (25° AOI) and 19 J/cm2 (45° AOI) (IAD 50 layer
HR coating). The demands of meeting challenging spectral, AOI and LIDT performances are highlighted by an HR
coating required to provide R > 99.6% reflectivity in Ppol and Spol over AOIs from 24° to 47° within ~ 1% bandwidth at
both 527 nm and 1054 nm.
Another issue is coating surface roughness. For IAD of HR coatings, elevating the chamber temperature to ~ 120 °C and
turning the ion beam off during the pause in deposition between layers reduce the coating surface roughness compared to
runs at lower temperatures with the ion beam on continuously. Atomic force microscopy and optical profilometry
confirm the reduced surface roughness for these IAD coatings, and tests show that their LIDTs remain high.
To enable laser-based radiography of high energy density physics events on the Z-Accelerator[4,5] at Sandia
National Laboratories, a facility known as the Z-Backlighter has been developed. Two Nd:Phosphate glass lasers are
used to create x-rays and/or proton beams capable of this radiographic diagnosis: Z-Beamlet (a multi-kilojoule laser
operating at 527nm in a few nanoseconds) and Z-Petawatt (a several hundred joule laser operating at 1054nm in the subpicosecond
regime) [1,2]. At the energy densities used in these systems, it is necessary to use high damage threshold
optical materials, some of which are poorly characterized (especially for the sub-picosecond pulse). For example,
Sandia has developed a meter-class dielectric coating capability for system optics. Damage testing can be performed by
external facilities for nanosecond 532nm pulses, measuring high reflector coating damage thresholds >80J/cm2 and antireflection
coating damage thresholds >20J/cm2[3]. However, available external testing capabilities do not use
femtosecond/picosecond scale laser pulses. To this end, we have constructed a sub-picoseond-laser-based optical
damage test system. The damage tester system also allows for testing in a vacuum vessel, which is relevant since many
optics in the Z-Backlighter system are used in vacuum. This paper will present the results of laser induced damage
testing performed in both atmosphere and in vacuum, with 1054nm sub-picosecond laser pulses. Optical
materials/coatings discussed are: bare fused silica and protected gold used for benchmarking; BK7; Zerodur; protected
silver; and dielectric optical coatings (halfnia/silica layer pairs) produced by Sandia's in-house meter-class coating
capability.
High intensity lasers require novel debris mitigation techniques in laser-target experiments. For a PW class
system (500 J in 500 fs at 1054 nm), the debris shield thickness is limited by the accumulated B-integral that the laser
acquires in transmission. In our case, this sets an upper limit of 500 micron for the debris shield thickness if the added Bintegral
is to stay below 1.5.
Therefore we have started to investigate the optical properties of various thin films such as Nitrocellulose,
Mylar, and Polyimide with respect to their application as laser debris shields. Those results were presented during the
last conference in 2007[1] and it was shown that Nitrocellulose and Polyimide are well suited. Damage testing was not
performed at this time. We now present short pulse (500 fs at 1054 nm) laser damage testing on these thin films in
vacuum. Energy, pulsewidth, beamsize and phase were closely monitored during the damage testing experiments.
Nitrocellulose was measured to damage at 1.33 J/cm2. Polyimide showed signs of damage at 133 mJ/cm2 and began to
fully penetrate the film at 670 mJ/cm2. Surprisingly, these films do not rupture with tens of closely spaced damage sites
being present which makes them ideal candidates for short pulse laser debris shields. Damage testing procedure and
apparatus as well as the damage site morphology will also be discussed.
Optical properties of various thin films such as Nitrocellulose, Mylar, and Polyimide were investigated with respect to their application as laser debris shields. Studies on optical and spectral transmission quality, absorption, stress induced birefringence, and damage threshold have been performed. Scalability to large apertures was also considered. Studies were performed of how focusing geometry, target alignment, and mechanical components can help mitigate target debris traveling back to the focusing optic.
We use two Pockels cells in series to achieve simple temporal pulse shaping. This technique is used in our optical parametric chirp pulse amplification (OPCPA) system to optimize the temporal shape of the pump pulse. It also offers a low cost alternative to arbitrary waveform generators.
Using a micro channel plate (MCP), we have developed a sensitive method for measuring the onset of laser damage by detecting liberated surface ions and XUV radiation from the laser induced surface plasma. This method is insensitive to optical alignment and therefore assures good repeatability over numerous measurements.
We will briefly summarize our experimental results obtained for 1 ps long filaments. Theoretical studies show that scaling those filaments to ns should enable us to trap up 1 J in a single channel. Applications for laser induced lightning and high aspect ratio hole drilling will be discussed.
We present a review of our experimental studies on picosecond UV (248.6 nm) filaments and give a motivation for scaling them to longer pulsewidths. An analytical solution for the propagation of nanosecond UV filaments shows their feasibility for directed energy applications.
Pulses of 500 fs or greater duration and several tens of millijoules at 248 nm are used to trigger discharges in air. We will discuss the influence of beam geometry, the minimum field strength that can be triggered, and the electrical discharge guiding properties. The latest measurements have concentrated on DC discharges in air at up to 200 kV. Thanks to a new technique of background free, single shot interferometry, 2D snapshots of the evolving plasma can be recorded. This will lead to further insight about the dynamics involved in the discharge process. The existing laser system is costly and difficult to use in the field. We will show however that similar performance can be achieved with a solid state laser and frequency conversion by nonlinear optics. Such a compact system can be tuned to cover the wavelength range from 240 nm to 350 nm.
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