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Volume VII–System Description

OMEGA EP Operations Manual

Page 6 of 35

1.1.3.2  OMEGA EP Fast-Ignition Program 

The key experiments needed to demonstrate the fast-ignition concept and determine the optimum 

parameters for the NIF will be carried out on OMEGA and OMEGA EP. The fundamental goal is to 
determine the coupling of the HEPW beam energy to the compressed core of a cryogenic implosion.  
Experiments will include the propagation of the high-intensity laser beam in the target, the conversion 
efficiency of the laser light to hot electrons (or ions), the intensity scaling of the hot-particle energy, the 
transport of these particles, and the heating of the compressed core.

1.1.3.2.1  Intensity Scaling of Hot-Electron Energy

The coupling efficiency to DT or plastic targets may be different than for high-

Z

 targets and is 

a major uncertainty in the fast-ignition scheme. In addition, the relationship between the hot-electron 
temperature 

T

hot

 and the ponderomotive potential 

U

pond

 of the high-intensity beam appears to be a 

function of target 

Z

. This will be determined experimentally in planar cryogenic target experiments in 

the OMEGA EP target chamber. The beam intensity will be varied by changing the compressed pulse 
duration in the 1- to 10-ps range. 

1.1.3.2.2  Electron-Beam Transport

HEPW-generated  electron-beam  propagation  without  excessive  divergence  is  important  for 

fast ignition. For example, the compressed core on OMEGA is only ~80 

n

m in diameter and remains 

assembled for less than ~100 ps, dictating a tight specification on the pointing accuracy of the channeling 
and ignitor beams. At the same time, the critical-electron-density (

n

c

) contour for 1-

n

m light has a 

430-

n

m radius while the 10 

n

c

 contour has a 150-

n

m radius. From this approximate characterization of 

the radial density profile, it is clear that the propagation of the high-intensity beams through the overdense 
plasma region requires good collimation and directionality of the electron beam that is generated at the 
end of the laser propagation. Studies of these processes will be carried out in the OMEGA EP chamber 
followed by full-scale, integrated implosion experiments in the OMEGA chamber with the compressed 
OMEGA EP beams used as the channeling and ignitor beams.  The cone-in-shell fast-ignitor concept 
will also be validated.

1.1.  SSP-Related High-Energy-Density Physics

Areas of high-energy-density physics of interest to NNSA’s Stockpile Stewardship Program (SSP) 

include (1) dynamic materials studies, including high-pressure equation-of-state (EOS) experiments of 
materials at high energy density, and (2) compressible hydrodynamics and radiative hydrodynamics 
experiments. The OMEGA EP target chamber design is optimal for both classes of experiments because 
all the laser energy is incident from one direction. The ability to heat compressed materials with high-
intensity beams and the advanced radiographic capabilities are equally valuable.

A related area is the study of matter near and above solid density at temperatures that can vary 

from a few electron volts to several hundred electron volts. There are applications in planetary and 
earth sciences, in addition to ICF and HED physics, including studies of the EOS and other materials 
properties  relevant  to  high-pressure  planetary  interiors.  Challenges  presented  by  this  field  include 
producing controlled conditions and their diagnosis. A number of complementary techniques can be 
used on OMEGA EP to access these conditions. 

Summary of Contents for Volume VII-System Description

Page 1: ...m 6 1 1 3 2 1 Intensity Scaling of Hot Electron Energy 6 1 1 3 2 2 Electron Beam Transport 6 1 1 4 SSP Related High Energy Density Physics 6 1 1 4 1 Equation of State Measurements of Materials 7 1 1 4...

Page 2: ...Structure 23 1 6 Timing Systems 24 1 7 Optical Alignment 26 1 8 Laser Diagnostics 29 1 8 1 Infrared Diagnostic Package IRDP 29 1 8 2 Short Pulse Diagnostics Package SPDP 29 1 8 3 Ultraviolet Diagnosti...

Page 3: ...irected into the OMEGA EP chamber with each beam capable of being operated in long pulse UV mode with independent temporal pulse shapes and pulse widths up to 10 ns It is also possible to send two com...

Page 4: ...nsity laser target interactions of the target improves with increased electrical conductivity No experiment to date has a target with conductivity within an order of magnitude of that of a DT plasma F...

Page 5: ...ts at 48 relative to the hohlraum axis allow the beams to be incident at an optimum angle for coupling to the hohlraum walls The 48 beam cone and options such as frequency converting the beams to 2 pr...

Page 6: ...hting with conventional OMEGA and NIF beams It will allow dedicated backlighting beams in both the OMEGA and OMEGA EP target chambers The short pulse capability of illuminating targets at 1020 W cm2 a...

Page 7: ...e full NIF but more than OMEGA possible and may relax requirements on efficiency and drive symmetry Fast ignition can also be used with drivers such as ion beam or Z pinch radiation sources that can c...

Page 8: ...on density nc contour for 1 nm light has a 430 nm radius while the 10 nc contour has a 150 nm radius From this approximate characterization of the radial density profile it is clear that the propagati...

Page 9: ...en unknown The OMEGA EP system will significantly extend the range of conditions and materials that can be tested with OMEGA because of the higher laser driver energy and the increased number of shots...

Page 10: ...on of 10 ps minimizes the hydrodynamic expansion of the sample and makes the heating close to isochoric It will be possible to study the opacities of warm dense matter using diagnostic techniques such...

Page 11: ...ne story high 14 ft concrete box beam which serves as a rigid optical table The first and second floors of the structure serve as the optical table and are 30 in thick concrete slabs The lower floor r...

Page 12: ...ed using optical parametric chirped pulse amplification OPCPA The injected pulse passes through the booster amplifier and is reflected off the fold mirror to the polarizer POL1 and into the main ampli...

Page 13: ...port H7 where an off axis f 1 8 parabolic mirror focuses them onto the target The focal spot can be shifted to any location within 1 cm of the center of the chamber to provide for flexible backlighti...

Page 14: ...mance limited by the damage threshold of the multilayer dielectric reflection gratings The use of improved grating technology provides up to 2 6 kJ of laser energy per beam The pulse width of Beam 2 w...

Page 15: ...ively assumed to be 85 The calculations used for Table 1 3 assume low risk existing technologies and demonstrated UV damage fluences for optical coatings In spite of the de rating of OMEGA EP energies...

Page 16: ...mplifier This OPCPA stage is critical to the performance of the short pulse beams Attractive features of OPCPA include a broad gain bandwidth high gain in a short optical path and reduced amplified sp...

Page 17: ...cy chirped The OPCPA pump laser starts with the same components as the long pulse beam up to and including the spatial shaping stage It also includes a high repetition rate 5 Hz crystal large aperture...

Page 18: ...modulator The pulse is further amplified in a glass amplifier before injection into the transport spatial filter of the beamlines The optical image plane of the LP apodizer is relayed throughout the...

Page 19: ...a diagnostic beamsplitter mirror DBS to provide a path to beam diagnostics and alignment packages In both the cavity and transport spatial filters the beam passes through a different pinhole on each p...

Page 20: ...in Fig 1 7 For short pulse experiments Beam 1 or Beam 2 may be routed to the upper or lower compressor in the GCC where four matched MLD tiled grating assemblies temporally compress the pulse A defor...

Page 21: ...pper compressor Lower compressor GCC VW DM DM BC Beamline 1 Beamline 2 Beamline 3 Beamline 4 From transport spatial filters FCC s 2 3 b e a m 4 8 b e a m Short pulse IR path default configuration To O...

Page 22: ...roduced just before the FCC s with the periscope mirror assembly PMA The placement of the FCC s before the target chamber rather than on the target chamber as in the NIF permits more convenient beam d...

Page 23: ...ure 1 9 Illustration of the inner workings of the GCC shows the locations of the TGA s G1 to G4 and the target chamber selection mirror The upper and lower compressors for Beams 1 and 2 are aligned at...

Page 24: ...ation of the upper compressor s optical path including the deformable mirror beam combiner and target chamber selection mirror The diagnostic mirror provides a 1 pickoff for the short pulse diagnostic...

Page 25: ...d in the SPDP table 1 5 3 Target Chamber and Target Area Structure The OMEGA EP target chamber is similar in design to the OMEGA target chamber and has the same 3 3 m diameter The chamber is located w...

Page 26: ...video cameras to capture the laser pulses 2 trigger signals for the electro optical devices that select and shape optical pulses in the laser portion of the system 3 trigger signals for the power cond...

Page 27: ...Shot Executive Shot Director OMEGA Power Conditioning Executive OMEGA EP Power Conditioning Executive Trigger generator selector TG S Reference frequency generator RFG 38 MHz Master timing generator...

Page 28: ...nchronized with each other In the independent mode each system functions as if it had an independent dedicated timing system In the joint mode the critical shot triggers originate from a single source...

Page 29: ...ssor to the short pulse diagnostic package SPDP table completing an alignment handoff with the SPDP ASP The SPDP also contains an alignment laser 1053 and 1047 nm that can be propagated through either...

Page 30: ...the tiles in each tiled grating assembly for each pulse compressor Insertable CAM s located before TGA1 between TGA s 2 and 3 and after TGA4 support alignment of the TGA s A two wavelength Littrow ali...

Page 31: ...tics suite comprised of at least ten individual diagnostic instruments These instruments diagnose the properties of the beams before they are co aligned and exit the GCC The SPDP provides information...

Page 32: ...ror During the alignment process a sample of the alignment beam is directed to the alignment sensor On a shot the 4 sample of the high energy pulse is directed to beam performance diagnostics on the U...

Page 33: ...ann wavefront sensors PEPC grating alignment and a new higher precision timing system etc The Control System architecture has been modified to reflect OMEGA EP as a subservient system to OMEGA when in...

Page 34: ...ds to prepare for the shot When a subsystem has been readied the operator signals the SD using a checklist button on the executive GUI The SD then reviews key details of the setup with the operator be...

Page 35: ...osed access areas during shot operations for safety reasons and to define the staffing requirements The specifics are defined in LFORM referenced above Like OMEGA there are seven shot types used for O...

Page 36: ...nto TSF Viewing Gallery Capacitor Bays Laser Target Bay 5 Charging driver and beam line heads Propagation to beyond stage A Terminates at F ASP s Amplified source injected into TSF Glass amplifier pum...

Page 37: ...EGA Operations page of the LLE Web site This interface consists of a series of pages or screens called forms that collect information of various types The SRF pages for OMEGA EP include General laser...

Page 38: ......

Page 39: ...fast ignitor FOA final optical assembly fs femtosecond FWHM full width at half maximum GCC grating compression chamber GUI graphical user interface HED high energy density HEPW high energy petawatt H...

Page 40: ...erence frequency generator RRM rate regenerator module SAC scanning autocorrelator SD Shot Director SE Shot Executive SHG second harmonic generation SP short pulse SPDP short pulse diagnostic package...

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