Photolithographically Defined Optical Cooling Devices for Electronic Cooling Plane Applications
Navy SBIR 2018.1 - Topic N181-081 ONR - Ms. Lore-Anne Ponirakis - [email protected] Opens: January 8, 2018 - Closes: February 7, 2018 (8:00 PM ET)
TECHNOLOGY AREA(S):
Electronics, Information Systems, Sensors ACQUISITION PROGRAM: 6.2
programs within ONR Code 31, building new HW systems in pre-FNC incubators The technology within this
topic is restricted under the International Traffic in Arms Regulation (ITAR),
22 CFR Parts 120-130, which controls the export and import of defense-related
material and services, including export of sensitive technical data, or the
Export Administration Regulation (EAR), 15 CFR Parts 730-774, which controls
dual use items. Offerors must disclose any proposed use of foreign nationals
(FNs), their country(ies) of origin, the type of visa or work permit possessed,
and the statement of work (SOW) tasks intended for accomplishment by the FN(s)
in accordance with section 5.4.c.(8) of the Announcement. Offerors are advised
foreign nationals proposed to perform on this topic may be restricted due to
the technical data under US Export Control Laws. OBJECTIVE: The objectives of
this topic are to invent a device that can be manufactured in an arrayed
geometry using whole wafer lithography techniques wherein anti-Stokes optical
upconversion can produce net cooling at each device and wherein well-verified
physics allows the upconverted photons to be caused to flow preferentially in
predefined directions away from the localized heat sinks, independent of the
local electronic temperature distribution. DESCRIPTION: In most
non-elemental solids, there are ground and excited state energy bands of the
electrons that contain sub-bands separated by the energies of thermally
excitable phonons of the crystal lattice.� If one of the ground state electrons
absorbs a photon that promotes it to such an excited state band and then it
subsequently also absorbs a phonon, and if the excitation decays by emitting a
photon, then the new photon will have more energy than the originally absorbed
one.� This is called the anti-Stokes process and the newly emitted photon will
be blue shifted.� The ability of this process to deliver net cooling of the
solid is determined by the branching ratio between the emission of the
upconverted photon and all other decay paths of the excitation and the
likelihood that the upconverted photon will escape from the local environment
which, for applications, we wish to cool.� Most demonstrations of this physics
have to date been done in bulk glasses where the re-radiated photons leave the
object being cooled isotropically.� Even if such devices could be made into a
planar geometry suitable for incorporation in a 3D stack of electronics, this
isotropy would mean that the vast majority of the upconverted photons would
have to pass through the devices we wish to cool in the adjacent planes, many
would be absorbed there, and the net cooling of the electronics would be
dramatically reduced.� What is needed is a way to cause the anti-Stokes photons
to leave their point of origin headed in a controllable, specific direction and
then to follow that path to a sink point which allows them to be removed from
the 3D stack in a convenient manner, such as via a low loss optical fiber.�
Fully optimized versions of such cooling planes would allow vertical
co-fabrication of the cooling structures and the active components being
cooled, but for the purposes of the Phase I proposal of this topic it will be
sufficient to define a device geometry and select materials to demonstrate net
optical cooling from a clearly defined starting temperature, produce a
technical approach that works to reduce the technical risk of the proposed
device, and argues how the integratable cooling plane would be built if the
individual device is successful in the materials chosen.� If the approach
proposed will be applicable to only a portion of the entire range of circuit
operating temperatures of ~4K to 400K (-289C to +125C), those limitations
should be discussed in the proposal. PHASE I: The purpose of the
Phase I effort is to refine the device concept presented in the initial
proposal and amplify the supporting scientific evidence about the behavior of
the selected materials to the point where the Phase II decision can be made
with realistic expectations of the performance possible at the end of Phase II
base.� For example, if the original proposal indicates there are two or three
candidate materials for use in the cooling volume, the Phase I should determine
which is in fact most promising.� Likely fabrication issues for the cooling
devices should be explored.� Detailed multi-physics simulations might be
attempted.� Demonstration of the method(s) proposed for controlling the
upconverted photon outflow are very desirable.� Fabrication of a first
prototype single device and proof it cools would be ideal.� The preliminary
Phase II proposal prepared at the end of Phase I should include a discussion of
the factors that could limit the energy efficiency of the chosen design and
what could be done to mitigate these limits if Phase II is awarded. PHASE II: The Phase II effort
will have four goals: optimization of the thermal performance of the chosen
single cooling device, planning the integration of a set of such devices into a
first array/cooling plane demonstrator, and fabrication and test thereof,
followed by further optimization.� The first goal must be completed in the base
portion of the award since the first option must be cost shared by a user who
wants to utilize this method of cooling and they must be convinced it is no
longer "high technical risk" work.� Further follow on efforts will
require user financial support and hence are expected to work toward the
sponsor's specified temperature range, thermal lift, and specific application,
and conceivably could become classified if the application is. PHASE III DUAL USE
APPLICATIONS: The central concept of this topic will, if successfully realized,
be considered as enabling, have many different uses, and ought to qualify as
"Dual use" for ITAR purposes.� The military applications should range
from cooling wiring and possibly power amplifiers in high-power transmitters (used
for surveillance and electronic attack) to the sensing of chemical, biologic,
or radioactive weapons at long wavelengths, to the provision of cryogenic
cooling for electronics dependent on low temperature environments.� However,
the application of local or general cooling, integrable with 3D stacked
electronics, has wide applicability in the consumer electronics fields where
heat removal often dictates maximum processor density for laptops and forces
strategies such as sequential depowering of circuit blocks to allow sufficient
cooling time for the stack not to over-heat and-or catch fire. REFERENCES: 1. Boriskina, S. V., Tong, J.
K., Hsu, W. C., Liao, B. L., Huang, Y., Chiloyan, V. and Chen, G. "Heat
meets light on the nanoscale", Nanophotonics 5 (#1), pp. 134-160, June
2016. (Open Access) 2. Nemova, G. "Laser
cooling of solids", https://arxiv.org/ftp/arxiv/papers/0907/0907.1926.pdf 3. Ruan, X. L. and Kaviany,
M. "Advances in laser cooling of solids", Journal of Heat Transfer
129 (#1), pp. 3-10, Jan. 2007, https://engineering.purdue.edu/NANOENERGY/publications/Ruan_JHT_2007.pdf KEYWORDS: Laser Cooling;
3-Dimensional Packaging; Anti-Stokes Radiation; Solid State Cooling; Cryogen
Free Cooling; Reradiation Branching Ratio
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