“BEAMS”49 pages
- p. 3 …Free-Electron Laser Electron Beam Phase-Space Evolution ....................... 59
Figure 31. Recirculating-Beam FEL System ........................................................... 60…
- p. 4 …HEL Beam Pointer/Tracker ................................................................... 65
Figure 35. Basic Shared Aperture Beam Control System ......................................... 66
Figure 36…
- p. 7 …This can only be achieved via laser propulsion in
which the laser beam energy that is…
- p. 15 …By launching
spacecraft on a beam of electromagnetic radiation, researchers will have developed the
first new…
- p. 16 …The laser beam's pulse
interacts with the mirror, spreading out and focusing into an annular…
- p. 17 …1) power supply; 2) high-power (megawatt-class)
laser beam generator/transmitter using novel beam optics…
- p. 20 …is to the right and the laser beam strikes the stretched-out parabolic
mirror/propulsion section…
- p. 21 …It
requires a beam power of 0.1 to 1 MW per kg of vehicle mass…
- p. 22 …The ground-based
megawatt-class laser beam generator is state-of-the-art technology. The cost…
- p. 25 …Figure 8 illustrates the adverse beam
propagation geometry associated with ETO laser propulsion by means of…
- p. 26 …Attenuation Effects on Captured Laser Beam Power 261.
0.4
0.J
0.2
0.1…
- p. 27 …Unfortunately the demonstrated laser beam power levels for the attractive 1.62 μm
wavelength, which suffered…
- p. 28 …Beam combining
of several 1 MW (or higher) FELs can achieve a total combined beam output…
- p. 31 …Appropriate rotation of a high-energy laser beam,
emanating from a ground/sea-based laser, guides…
- p. 32 …Appropriate rotation and translation of a high-energy laser
beam, emanating from a moving aircraft, guides…
- p. 33 …But
multiple target interception within allowable time is limited by relatively long beam-
riding time needed…
- p. 37 …In this case, it is envisioned that the high-
pulsed power within high-energy laser beams…
- p. 39 …In this case, airborne laser beams at 12 km altitude will not suffer the
significant propagation…
- p. 41 …sidelobes, creates multiple beams, and steers the ensemble of the
individual beams anywhere on Earth. The…
- p. 42 …Each picosat is gravity-
gradient stable, has a dipole array facing Earth, and a broader beam…
- p. 43 …Commands for beam sweep delays are superimposed on the time delays of each
nanosat. Each nanosat…
- p. 44 …piezoelectric membrane kept flat by an electron beam in response to an optical figure
sensor. MEMS…
- p. 46 …technical issues include large wavelength and
atmospheric absorption of the laser beam.
• Carbon Monoxide (CO) Laser…
- p. 47 …125 Hz@ 20μs.
• Laser power, P = 2.5 MW/beam x 4 beams = 10 MW.
• Laser…
- p. 50 …Each power oscillator optics module transmitting a 2.5 MW beam of
10.6 μm wavelength…
- p. 52 …Adding an eight amplifier chain that the system was designed for will
increase the beam power…
- p. 53 …However,
BSSSL beam power can be scaled up further by improving presently known gain media
and…
- p. 54 …scalable
to 1 MW beam power within 2 years.
Typical solid-state lasers have the following…
- p. 55 …A new technology that enables the scaling-up of BSSSL beam power is a recently
developed…
- p. 56 …at the same time increasing the average
beam power.
Figure 21. Phase Change Materials Allow Storage…
- p. 57 …This exponential growth in beam output power is the result of many factors,
including the parallel…
- p. 58 …Microlens -O _
,:1
Incoherent Beam Combining 'Ind1vidually Incoherent Gaussian Beams i=L
Controlled
/_/Steering • ... o~bined…
- p. 59 …Neodymium
Thulium (Tm 3+), Holmium
- Range of beam wavelengths(),) produced: 0.48 μm to 2.9…
- p. 61 …Multlmode Fiber Lasers
50kW Multimode
Output beam quality BPP-1 o
M"2-33
DC EDE…
- p. 62 …The resulting laser beam photon energy depends on the
electron energy, the undulator period, and (weakly…
- p. 63 UNCLASSIFIED/ /F8~ 8FFl&I.«1k WliEii a,.klf
electron beam
( \ I,:--- ■■>ti■--
undulator
)
resonator mirror
0…
- p. 64 …The superconducting accelerator gives good
efficiency and gradient while recirculation of the electron beam recovers beam…
- p. 65 UNCLASSIFIED/ /F&~ 8FFHiil.«1k 1!181! &••kY
- K"' 1.5.t
• Electron Beam:
- Photocathode injector creates…
- p. 66 …HIGH ENERGY LASER BEAM CONTROL
··costs could be reduced to as low as $20 per kg…
- p. 67 …The typical HEL beam control system includes:++ 1) a gimbaled
beam director, 2) tracking and pointing…
- p. 68 UNCLASSIFIED//F&II. &FFiii,111!! l!llili &HI!¥
A novel new HEL beam control architecture being…
- p. 69 …HEL Beam Pointer/Tracker (courtesy of the Directed Energy Professional
Society).
In summary, this new architecture…
- p. 70 …The BILL is a solid-state, kilowatt-class laser
that measures atmospheric conditions, allowing the beam…
- p. 71 …All of these HEL beam control innovations can be quickly adapted to laser propulsion
applications with…
- p. 72 …The entire Lightcraft launch
system is comprised of a ground, sea, or airborne laser beam generator…
- p. 73 …New beam
control devices and high-power optical train combinations have a resulting beam line
that…
- p. 75 …N. (1983), "Advanced Beamed-Energy and Field Propulsion Concepts,"
BDM/W-83-225-TR, BDM Corp…
- p. 76 …N. (2001), "World Record Flights of Beam-Riding Rocket Lightcraft:
Demonstration of 'Disruptive' Propulsion Technology," AIAA…
- p. 77 …of the 6 th Int'! Symposium on Beamed Energy
Propulsion, edited by C. R. Phipps, AIP…
UNCLASSIFIED/ ,CFQA: QFFI&l11J.k W&liii Q•lklf
Table 5. Influence of Lightcraft and Target Velocity on Impact Energy and
Required Mass [261.
Lightcraft Lightcraft Impact Ballistic Missile Threat
Intercept Intercept Energy 1--SRBM IRBM ICBM-
Aspect Velocity and R~lO00 km R~2500 km R~l0,000 km
Weight V=2 km/s V=4 km/s V=6km/s
Impact E for 16MJ 36MJ 641\IJ
2 km/s 1.0 kg Wt.
Wt for 10 .63 kg
MJ ofE .28 kg .16 kg
0° from Impact E for 25MJ 49MJ 81 MJ
Head-on 3 km/s 1.0 kg Wt.
Collision Wt. For 10 .40 kg .20 kg .12 kg
MJ ofE
Impact E for 36 MJ 64MJ 100 }IJ
1.0 kg Wt.
4 km/, Wt. for 10 .28 kg .16 kg .l0kg
MJ ofE
RECOMMENDED LIGHTCRAFT MISSIONS FOR BALLISTIC MISSILE
DEFENSE
Laser-powered Lightcraft, flown on air-to-space trajectories, show much promise for
performing exo-atmospheric BMD missions, especially if the laser can also be used to
discriminate warhead-carrying vehicles from decoys and non-threatening debris. Such
Lightcraft also appear capable of eliminating enemy satellites in LEO, if the Lightcraft
laser can illuminate them. But a significant effort would be required to analyze the
engagement scenarios for such a system, and fully investigate the decoy discrimination
and satellite tracking capabilities of the Lightcraft's pulsed laser and the hit-to-kill
guidance requirements for the Lightcraft itself.
Locating lasers and Lightcraft on existing aircraft, such as the Boeing 747, B-1 Lancer,
or C-130, appears to be an attractive alternative to ground/sea-based laser Lightcraft
systems. In this case, airborne laser beams at 12 km altitude will not suffer the
significant propagation losses that occur when guiding and propelling Lightcraft through
the lower atmosphere, and greater Lightcraft flight range should therefore be
achievable. (The increase in laser range, due to reduced propagation losses, for high
altitude operation will be somewhat diminished because of the smaller allowable
apertures on aircraft-mounted laser optics, which are on the order of 1.0 m as
compared to apertures on the order of 10.0 m for large ground/sea-based laser
installations.) Furthermore, airborne laser Lightcraft systems possess much greater
operational flexibility since their carrier aircraft can fly over significant distances to
reach desired launch locations, and can be based at almost any major Air Force facility
35
UNCLASSIFIED/ ,'P8R:: 8ffl@Itlit Wlili IUIL\f