U.S. patent application number 13/385661 was filed with the patent office on 2013-08-29 for controlling the emissive properties of materials-improved lasers and upconversion materials.
This patent application is currently assigned to UChicago Argonne, LLC. The applicant listed for this patent is Nicholas G. Becker, Jeffrey W. Elam, Jeffrey Klug, Michael J. Pellin, Thomas Proslier. Invention is credited to Nicholas G. Becker, Jeffrey W. Elam, Jeffrey Klug, Michael J. Pellin, Thomas Proslier.
Application Number | 20130223469 13/385661 |
Document ID | / |
Family ID | 48999690 |
Filed Date | 2013-08-29 |
United States Patent
Application |
20130223469 |
Kind Code |
A1 |
Proslier; Thomas ; et
al. |
August 29, 2013 |
Controlling the emissive properties of materials-improved lasers
and upconversion materials
Abstract
Systems and methods for producing crystalline materials by
atomic layer deposition, allowing for high control of localized
doping. Such materials may be fibers or films suitable for use in
optoelectronics and lasers.
Inventors: |
Proslier; Thomas;
(Woodbridge, IL) ; Becker; Nicholas G.; (Chicago,
IL) ; Pellin; Michael J.; (Naperville, IL) ;
Klug; Jeffrey; (Westmont, IL) ; Elam; Jeffrey W.;
(Elmhurst, IL) |
|
Applicant: |
Name |
City |
State |
Country |
Type |
Proslier; Thomas
Becker; Nicholas G.
Pellin; Michael J.
Klug; Jeffrey
Elam; Jeffrey W. |
Woodbridge
Chicago
Naperville
Westmont
Elmhurst |
IL
IL
IL
IL
IL |
US
US
US
US
US |
|
|
Assignee: |
UChicago Argonne, LLC
|
Family ID: |
48999690 |
Appl. No.: |
13/385661 |
Filed: |
February 29, 2012 |
Current U.S.
Class: |
372/69 ;
252/301.4R; 427/162; 427/248.1; 427/58 |
Current CPC
Class: |
C30B 25/00 20130101;
H01S 3/1608 20130101; C04B 35/62231 20130101; C30B 29/16 20130101;
C04B 35/505 20130101; C23C 16/45531 20130101; C04B 2235/3224
20130101; H01S 3/163 20130101; C23C 16/405 20130101; H01S 3/067
20130101; C04B 35/62218 20130101; C23C 16/45553 20130101 |
Class at
Publication: |
372/69 ;
427/248.1; 427/162; 427/58; 252/301.4R |
International
Class: |
H01S 3/09 20060101
H01S003/09; C09K 11/78 20060101 C09K011/78; B05D 5/12 20060101
B05D005/12; C23C 16/40 20060101 C23C016/40; B05D 5/06 20060101
B05D005/06 |
Goverment Interests
[0002] The United States Government claims certain rights in this
invention pursuant to Contract No. DE-AC02-06CH11357 between the
United States Government and UChicago Argonne, LLC representing
Argonne National Laboratory. The United States Government also
claims certain rights in this invention pursuant to research
sponsored by the Army Research Lab, ANL Cost Code 8R26900.
Claims
1. A method for producing a final phase of a crystalline material
for use in a fiber laser of desired composition and thickness
through atomic layer deposition, comprising the steps of:
introducing a first precursor consisting of a Yttrium precursor
into a growth chamber; purging the growth chamber; introducing a
second precursor consisting of an Erbium precursor into the growth
chamber which acts as a dopant and forms a doping level of at least
0.5%; purging the growth chamber; introducing an oxygen co-reactant
into the growth chamber forming a phase of the crystalline
material; and annealing the phase of the crystalline material at or
above 600 up to 750.degree. C. to form the final phase of the
crystalline material, thereby achieving a crystalline material
having a fiber laser emission lifetime greater than 6 ms.
2. The method of claim 1 wherein the crystalline material has a
crystalline emission line, single exponential decay lines, and
lifetimes greater than 6 ms despite a high doping level that is
above 0.5%.
3. (canceled)
4. (canceled)
5. (canceled)
6. The method of claim 1 wherein the Yttrium precursor is selected
from the group consisting of: Y(Cp).sub.3 or Y(MeCp).sub.3.
7. The method of claim 1 wherein the Erbium precursor is selected
from the group consisting of: Er(MeCp).sub.3, Er(BA).sub.3, or
Er(TMHD).sub.3.
8. The method of claim 1 wherein the oxygen source is selected from
the group consisting of: H.sub.2O, H.sub.2O.sub.2, O.sub.3, oxygen
plasma, or mixtures of these oxygen sources.
9. The method of claim 1 wherein the crystalline material is
Erbium-Doped Yttrium Oxide (Er.sup.+3:Y.sub.2O.sub.3).
10. The method of claim 1 wherein the crystalline material is a
film.
11. (canceled)
12. (canceled)
13. (canceled)
14. The method of claim 1 wherein the crystalline material is
suitable for up conversion.
15. The method of claim 1 wherein the crystalline material is
suitable for use in down conversion.
16. The method of claim 1 wherein the crystalline material is
suitable for use in spintronics.
17. The method of claim 1 wherein the crystalline material is
suitable for use in thermoelectrics.
18. The method of claim 1 comprising the additional step of using a
B--reaction to burn off ligands to allow patterned as opposed to
random deposition.
19. A LASER comprising: a LASER pump; a reflective component; an
output coupler; and a gain medium, the gain medium comprising an
erbium-doped yttrium oxide.
20. A material for photon conversion comprising: an erbium-doped
yttrium oxide.
Description
RELATED APPLICATIONS
[0001] This application is related to U.S. patent application Ser.
No. 13/370,602, the entirety of which is incorporated herein by
reference.
FIELD OF THE INVENTION
[0003] The present invention is directed to a method and system for
production of crystalline materials through the use Atomic Layer
Deposition (ALD). More particularly, the method and system concern
production of crystalline materials with locally controlled doping
and high doping levels through ALD. In particular, bulk-like
lifetime values (.about.6 ms) obtained with Er doped Yttria fiber
made by ALD.
BACKGROUND OF THE INVENTION
[0004] The intentional introduction of impurities into a material
is fundamental to controlling and tuning the properties of bulk or
nanostructured matrices (whether they be insulators,
semiconductors, metals, semi-metals, or superconductors). Common
doping techniques include, but are not limited to, ion
implantation, electro-chemistry, chemical vapor deposition (CVD),
physical vapor deposition (PVD), molecular beam epitaxy, sol-gel
process, zone refinement crystal growth. These methods rely on a
statistical distribution of dopant and, therefore, often present
inhomogeneous local concentrations, chemical environments, and
properties that in turn hinder the fundamental understanding of the
underlying microscopic mechanism and limit the applications range
and performances of materials produced through these processes.
These methods provide no local control.
SUMMARY OF THE INVENTION
[0005] In the present invention, control, down to the atomic level,
of the three dimensional dopant distributions in a given bulk
material by using Atomic layer deposition (ALD) is described. The
main advantage of this technique is that it relies on the
self-assembly of the dopant induced by the hindrance effect, does
not require expensive nano-patterning in order to separate ions,
and can be scaled to arbitrary large surfaces and to a variety of
industries. Furthermore, the use of dual-pulsing of organometalic
precursors allows further separation.
[0006] Possible applications for materials produced by the present
invention include, but are not limited to, materials suitable for
use in lasers (as laser fibers or films), materials suitable for
use in up or down conversion, materials suitable for use in
spintronics, and materials suitable for use in thermoelectrics.
BRIEF DESCRIPTION OF THE DRAWING
[0007] The patent or application file contains at least one drawing
executed in color. Copies of this patent or patent application
publication with color drawing(s) will be provided by the Office
upon request and payment of necessary fee.
[0008] FIG. 1 illustrates Quartz Crystal Microbalance (QCM) mass
signals during alternating ALD pulses of tris-cyclopentadienyl
yttrium (III) (Y(Cp).sub.3) and O.sub.3.
[0009] FIG. 2 illustrates QCM mass signals during alternating ALD
pulses of Y(Cp).sub.3 and H.sub.2O.
[0010] FIG. 3 illustrates QCM mass signals during alternating ALD
pulses of erbium(III) tetramethylheptanedionate (Er(TMHD).sub.3)
and O.sub.3.
[0011] FIG. 4 illustrates QCM mass signals during alternating ALD
pulses of Er(TMHD).sub.3, Y(Cp).sub.3 and O.sub.3.
[0012] FIG. 5 illustrates the dependence if the lifetime measured
at 1.5 .mu.m as a function of the ligand size of the Erbium
precursors used.
[0013] FIG. 6 illustrates the crystallinity of the as grown Yttria
film by Atomic layer deposition.
[0014] FIG. 7 illustrates the crystalline emission lines of Erbium
at 1.5 .mu.m in a Er doped Yttria films made by atomic layer
deposition and compared with a Er doped Yttria powder used as a
reference standard.
[0015] FIG. 8 illustrates the single exponential decay of the
lifetime of post-annealed Yttria films doped with various Er
precursor molecules.
[0016] FIG. 9 illustrates the dependence if the lifetime measured
at 1.5 .mu.m as a function of the Er doping concentration. In red
is a previous study of the lifetime of Er doped fiber grown by
ALD.
[0017] FIG. 10 illustrates an ALD specific method of producing
materials.
[0018] The patent or application file contains at least one drawing
executed in color. Copies of this patent or patent application
publication with color drawing(s) will be provided by the Office
upon request and payment of necessary fee.
DETAILED DESCRIPTION
[0019] The present invention introduced the application of atomic
patterning to optical fibers and other crystalline materials.
Through the present invention, one can organize doping and develop
crystalline materials with localized doping concentrations. The
present invention also allows for use of arbitrarily large Atomic
Layer Deposition (ALD) precursors molecules, which is an unexpected
result
[0020] In some embodiment, the present invention provides a method
for producing a crystalline material of desired composition and
thickness through atomic layer deposition. In some embodiments,
said method may comprise: introducing a first precursor into a
growth chamber; purging the growth chamber these two steps
constitute a cycle, the first cycle is refereed as the A cycle,
introducing a reducing or oxidizing agent into the growth chamber;
purging the growth chamber (refereed as cycle B); This A and B
cycles constitute the matrix material into which the dopant will be
introduced. The dopant is synthesized by introducing a second
precursor into the growth chamber, purging the growth chamber
(refereed as the cycle C), introducing a reducing or oxidizing
agent and purging the chamber (refereed as the cycle D). In some
embodiments the second precursor may comprise a precursor which
acts as a dopant. In some embodiments the first precursor is an
Yttrium precursor. In some embodiments, the second precursor is an
Erbium precursor. In some embodiments, the reducing or oxidizing
agent, also called co-reactant, can be an oxygen (O.sub.2), water
(H.sub.2O), ozone (O.sub.3), oxygen plasma or any combination of
these mentioned sources..
[0021] In some embodiments, an Yttrium precursor may be selected
from the group consisting of: tricyclopentadienyl yttrium(III)
(Y(Cp).sub.3) or tris-methylcyclopentadienyl yttrium(III)
(Y(MeCp).sub.3). In some embodiments an Erbium precursor may be
selected from the group consisting of: tris-methylcyclopentadienyl
erbium(III) (Er(MeCp).sub.3), erbium boranamide (Er(BA).sub.3), or
Er(TMHD).sub.3. In some embodiments, the crystalline material
produced by the present invention may be Erbium-Doped Yttrium Oxide
(Er.sup.+3:Y.sub.2O.sub.3). In some embodiments the crystalline
material produced by the present invention may be a film. In some
embodiments the crystalline material produced by the present
invention may be a fiber.
[0022] In some embodiments, use of the present invention in
producing laser fibers allows high doping levels without letting
the ions get so close as to quench the excitation. Doping through
the use of ALD allows control and spacing of the ions, to allow for
larger ions, and doping levels of up to 3% as opposed to the
customary 0.5%.
[0023] In particular, the present invention can be used to produce
materials for Erbium (Er) doped fiber lasers with significantly
increased gains, much higher thermal conductivity than glass and
better spectroscopy than that of rare-earth ions in glass (in terms
of absorptivity and emission cross-sections). Atomic Layer
Deposition can be used to create crystalline Er doped Yttria films
that efficiently use Erbium (each Erbium may be in its optimum
valence state) and for the first time show radiative lifetimes
suitable for laser use (i.e. .about.6 millisecond range). Moreover,
lifetime value above 4 ms is achieved for concentrations 6 times
higher than the standard 0.5% doping limit. To achieve such high
lifetime the films need to be annealed at or above temperature of
600 C. The optimal post-annealing temperature depends on the dopant
level, films thickness, precursor molecule used for the dopant and
the presence of a seed layer of pure Yttria grown by atomic layer
deposition prior to the crystalline doped film.
[0024] Bulk like lifetime (>6 ms) has been achieved in Er doped
Y2O3 films with a thickness of 100 nm grown on 10, 25, 50 or 75 nm
thick pure Yttria films that acts as a seed layer for Yttria
crystallite growth. For such thin films, the improvement of the
lifetime didn't saturate for the post-annealing temperature up to
750 C. For Er doped Y2O3 films grown without seeding layer, the
annealing temperature is found to be around 700 C for an optimal
lifetime, before decreasing upon annealing at higher temperature.
The origin of such different post annealing behavior between the Er
doped Yttria films grown on a seed layer or not lies in the grain
size of the matrix, here Yttria, when the first dopant cycle is
introduced: for films grown without seed layers the Yttria
crystallites are smaller than 1 nm and therefore highly defected
when the first dopant cycle is introduced. Upon annealing at too
high temperature these dopants that do not have a clear
crystallographic cage around them will diffuse and gather, inducing
a decrease of the emission lifetime. On the contrary, it is found
that introducing dopant on at least 10 nm thick seed layer of
Yttria do not induce a decrease of the lifetime upon annealing at
temperature up to 750 C.
[0025] In one embodiment of the present invention, Atomic Layer
Deposition may be used as a unique synthesis method for the growth
of crystalline, highly doped, erbium-doped Yttrium oxide fibers.
Such films may have narrow crystalline emission lines, single
exponential decay lines, and with lifetimes greater than 6
milliseconds despite doping levels of around 3%. Such materials can
be formed into low loss fibers using standard semiconductor
patterning techniques to greatly shorten fiber lengths to achieve
high power with a consequent reduction in many non-linear losses
associated with fiber matrix materials, such as from Brillouin
scattering.
[0026] The rationale for using crystalline core Er fiber laser is
based on the following: 1) Er cross-sections in glass fibers are
low, so absorption is low; 2) significant increases in Er doping
level is not an option--due to the well-known Er up-conversion and
3) the consequent fiber lengths requires (of about tens of meters)
produce unacceptable stimulated Brillouin scattering (SBS) and
other non-linear losses. With utilization of crystalline
(single-crystalline or polycrystalline) core, absorption
cross-section will increase by at least an order of magnitude.
Moreover, using ALD as a deposition method, Er lifetime of value
greater than 6 ms at 1.5 .mu.m has been controlled for the first
time with up to 3% Er doping levels from the conventional 0.5%
limit of current materials utilizing ALD's non-random doping.
Combining these two advances into new fiber materials may reduce
fiber lengths by almost a factor of 50.
[0027] Producing Erbium-Doped Yttrium Oxide via ALD
[0028] In one embodiment of the present invention, Erbium-Doped
Yttrium Oxide is produced through the use of ALD. Erbium doped
Yttria can have applications in optoelectronics and lasers. In
lasers, Erbium doped Yttria can provide eye-safe down conversion
and higher concentrations of water absorption. Yttrium oxide
provides for high solubility of Erbium and grows poly-crystalline
via ALD. Yttrium oxide features a wide band gap of about 5.6 eV and
alleviates thermal quenching. Yttrium oxide also features a
relatively high index of refraction.
[0029] In some embodiments, Yttrium precursors for use in ALD may
include Y(Cp).sub.3 or Y(MeCp).sub.3. In some embodiments, Erbium
precursors for use in ALD may include Er(MeCp).sub.3, Er(BA).sub.3,
or Er(TMHD).sub.3. In some embodiments, a co-reactant or oxygen
source for use in ALD may include H.sub.2O, H.sub.2O.sub.2,
O.sub.3, an oxygen plasma, or mixtures of these oxygen sources. For
example, H.sub.2O, H.sub.2O.sub.2, or O.sub.3 may be used with
Y(Cp).sub.3 or Er(MeCp).sub.3 precursors; H.sub.2O, H.sub.2O.sub.2
may be used with Y(MeCp).sub.3 precursors; H.sub.2O.sub.2 may be
used with Er(BA).sub.3 precursors; or O.sub.3 may be used with
Er(TMHD).sub.3 precursors.
[0030] In some embodiments, Erbium-doped Yttrium Oxide
(Er.sup.+3:Y.sub.2O.sub.3) may be produced through the use of
Y(Cp).sub.3 and Er(TMHD).sub.3 precursors and O.sub.3 as an oxygen
source. In such an embodiments, a pulse of Y(Cp).sub.3 may be
followed by a purge, then a pulse of Er(TMHD).sub.3, followed by a
purge, then a pulse of O.sub.3. The QCM mass signals for such an
ALD process is illustrated in FIG. 4. Additionally, the QCM mass
signals for ALD growth of Y(Cp).sub.3 and Er(TMHD).sub.3 with
varying oxygen sources is illustrated in FIGS. 1-3.
[0031] The Erbium-doped Yttrium Oxide produced by the invention may
have poly-crystalline physical properties. In some embodiments, the
grain size of the Erbium-doped Yttrium Oxide may increase with the
overall thickness of the material.
[0032] Materials for Use in Lasers
[0033] fiber grown by Atomic layer deposition require a substrate
such as sapphire, seed Yttria crystals or any substrate that have
high thermal conductivity. The laser fiber utilizing ALD has to be
crystalline, with a thermal conductivity higher than amorphous
fibers. The ALD fiber can be grown on high aspect ratio structures.
Materials produced by the present invention may be used in lasers,
and laser fibers or films. In prior art materials for use in
lasers, the dopant (for example, erbium) concentration is
determined by diffusion processes in both preform and drawing steps
of fiber fabrication. In some commercial samples the dopant may
diffuse outside the laser cavity and does not contribute to the
lasing process, but does remain as a source of inefficiency and
waste heat. As such fiber performance is limited to low dopant
concentration (.about.0.5%). Through use of ALD by the present
invention, the quenching concentration can be increased by up to 3%
while maintaining the integrity of single dopant emission
properties (for example, lifetimes above 4 ms). This discovery will
not only increase (by about six-fold) the power of a laser fiber
but also reduce its size for a given power requirement as compared
to conventional fibers.
[0034] Materials for Use in Up or Down Conversion
[0035] Materials produced by the present invention may be used as
materials for up-conversion or down-conversion. Up-conversion (UC)
refers to the emission of one high energy photon upon the
absorption of two or more lower energy photons, and down-conversion
(DC) refers to the analogous process of "cutting" one high energy
photon into multiple photons with lower energy. UC and DC may be
referred to as forms of photon conversion. In photovoltaic
applications, UV-visible to near-infrared (NIR) DC and IR to NIR UC
are both of considerable interest as a means to increase solar cell
efficiency by reducing the so-called "spectral mismatch" which
refers to the large portion of the solar spectrum which falls
outside the energy range suitable for photovoltaic absorption. For
example, in silicon-based photovoltaic cells .about.35% of the
solar photon intensity is below the Si band gap energy, Eg, and
cannot be absorbed. Another .about.32% has energy greater than 2 Eg
which results in large energy losses due to charge carrier
thermalization. Converting these sections of the solar spectrum to
easily absorbed photons through DC and UC, such as through
rare-earth enable DC and UC, can enable photovoltaic efficiencies
above the Shockley-Queisser theoretical efficiency limit
.about.30%.
[0036] In both DC and UC luminescent materials, the local structure
and coordination of the rare earth dopants has critical
implications for the emission properties--insufficient distance
between adjacent emitters can lead to non-radiative
losses/quenching, and in the case of multiple co-dopants, the
distance between absorbing and emitting ions can strongly influence
the energy transfer between them. However, conventional methods of
depositing DC/UC materials (ion implantation, sintering, etc.) lack
local control, and instead rely on the overall statistical
concentration and distribution of dopants into the matrix or host
material. In contrast, the use of ALD by the present inventions
offers a unique opportunity to not only control at the atomic level
the dopant concentration, but also the distance between dopants and
their chemical environment.
[0037] The present invention enables the production of UC/DC
materials with more efficient use of rare earth metals--achieving
superior performance with the same amount of rare earths, or
maintaining equivalent performance while reducing consumption of
materials which may be declared critical due to their technological
importance or risk of supply disruption. Increased Quantum
efficiencies in DC phosphors are possible for vacuum ultraviolet
(VUV) to visible light conversion in plasma displays and
mercury-free fluorescent lamps, which could produce considerable
economic and environmental impact. With current government mandates
on the use of CFLs in homes, the mercury content in fluorescent
light bulbs has come under recent scrutiny. The present invention
would lead to an elimination of the need for mercury in those
products, while maintaining the high efficiency associated with
fluorescent lights. The current efficiencies of Plasma display
panels (PDP) are approximately half that of cathode ray tubes and
significant improvement can be made in the efficiency of the DC
phosphors used.
[0038] The use of Atomic layer deposition for UC and DC conversion
require the addition of a second dopant in the matrix of choice
(preferably a material that have low phonon density of states in
the optical range). The second dopant is used as the absorber that
transfer the excitation to the first dopant: For instance DC can be
achieve with Er:Yb doped Yttria. where Yb (Ytterbium) is used as
the absorber, The absorber (Yb) is generally present in higher
concentration than the first dopant (Er).
[0039] Materials for Use in Spintronics.
[0040] Materials produced by the present invention may be used as
materials for spintronics. Spintronics relies on the using spin
excitations or magnons to carry information and energy without
losses, a definitive advantage over the common charge-based
transport. Spintronics materials are often doped semiconductors
that rely also on the well-controlled dopant local concentration
and large scale homogeneity. It has been shown that inhomogeneous
dopant concentration acts as defects and leads to a shorter
excitation lifetime and therefore limits the range of application.
The present invention provides for the production
locally-controlled doped materials via ALD, thus providing for
spintronics materials with a wider range of applications.
[0041] Materials for Use in Thermoelectrics.
[0042] Materials produced by the present invention may be used as
materials for thermoelectrics. The dimensionless figure of merit,
ZT=S.sup.2.sigma. T/.kappa., is the preferred measure for the
performance or efficiency of thermoelectric materials, where S is
the thermo-power and .sigma. and .kappa. the electric and thermal
conductivities, respectively. Recently, ZT values of 2.4 in layered
nanoscale structures at 300K, and 3.2 for a bulk semiconductor with
nanoscale inclusions at about 600K were reported. However, these
high values of ZT (which would be in the range for applications)
are reached under quite restrictive conditions and are not suitable
for applications. The transport properties are very sensitive to
the local dopant concentration and chemical environment, as a
consequence inhomogeneous dopant distribution often leads to a
deterioration of the figure of merit. Through the present
invention, locally controlled dopant concentrations can be obtained
which can yield materials with a higher figure of merit, ZT. The
ability to control the doping, and therefore both .sigma. and
.kappa. of the material, through the present invention goes beyond
that previously possible and allows for focusing on multiphasic
materials which further improves the figure of merit, ZT, and thus
broader applications.
[0043] FIG. 5 illustrates an example method of carrying out the
invention through ALD.
[0044] The foregoing description of embodiments of the present
invention have been presented for purposes of illustration and
description. It is not intended to be exhaustive or to limit the
present invention to the precise form disclosed, and modifications
and variations are possible in light of the above teachings or may
be acquired from practice of the present invention. The embodiments
were chosen and described to explain the principles of the present
invention and its practical application to enable one skilled in
the art to utilize the present invention in various embodiments and
with various modifications as are suited to the particular user
contemplated. The features of the embodiments described herein may
be combined in all possible combinations of methods, apparatus,
modules and systems.
* * * * *